Contents

Withholding Verifiable Information

Denis Shishkin, Maria Titova, Kun Zhang

Revision requested by Theoretical Economics

Abstract

We study a class of finite-action disclosure games in which the sender's preferences are state-independent and the receiver's optimal action depends only on the expected state. While receiver-preferred equilibria in these games involve full revelation, other equilibria are less well understood. We show that any equilibrium payoff can be obtained with a disclosure strategy corresponding to a partition with a laminar structure that allows pooling of nonadjacent states. In a sender-preferred equilibrium, such a structure balances inducing more sender-favorable actions with deterring deviations. Leveraging this insight, we identify conditions under which the sender does not benefit from commitment power. We then apply these results to study selling with quality disclosure and influencing voters.

1 Introduction

A canonical prediction in disclosure games is unraveling (e.g., Grossman, 1981; Milgrom, 1981). Specifically, if a sender can credibly prove that a state is highly favorable, he reveals it to induce a higher action from a receiver. Once the most favorable states have been disclosed, slightly less favorable states must also be revealed to avoid being mistaken for worse ones, and this reasoning continues recursively until all states are revealed. This full-revelation result hinges on a crucial assumption: the receiver’s action space is sufficiently flexible, meaning that she can adjust her action continuously so that any marginal improvement in her belief leads to a strictly higher action.

However, this flexibility assumption often fails in settings where the receiver chooses among finitely many actions—for example, when a consumer decides between a few products or product versions or a policymaker chooses among a few policy alternatives. In such cases, the receiver cannot finely adjust her action in response to small changes in her belief. Previous studies (e.g., Giovannoni and Seidmann, 2007; Titova and Zhang, 2025) have shown that this discreteness may prevent full unraveling and allow the sender to withhold some information—that is, create a scope for pooling. Yet little is known about precisely which states are pooled in equilibrium or about the limits of what can be achieved through verifiable disclosure.

In this paper, we study a disclosure game in which the receiver’s preferred action is increasing in the expected state. The only essential difference from Milgrom (1981) is that our receiver’s action space is finite. We characterize the equilibrium payoff set, study the sender-preferred equilibrium payoff, and identify sufficient conditions under which the commitment payoff is achieved with verifiable disclosure. We illustrate our results with a motivating example.

Example. Consider a seller (he) promoting a product to a buyer (she) who chooses whether to buy nothing (action 1), buy the product (action 2), or buy the product bundled with an add-on (action 3). The players have a common prior that the product quality—which can be interpreted as either the sender’s type or the state of the world—is uniformly distributed on [0,1][0, 1]. The buyer’s payoff depends on the posterior expectation of product quality ω\omega and is such that she optimally buys the bundle if E[ω]∈[34,1]\mathbb{E}[\omega] \in [\frac{3}{4}, 1], only the standalone product if E[ω]∈[12,34]\mathbb{E}[\omega] \in [\frac{1}{2}, \frac{3}{4}], and nothing otherwise. The seller’s profit is 0 if he sells nothing, 1 if he sells the product with the add-on, and p∈[0,1]p \in [0, 1] if he sells the product only. To persuade the buyer, the seller can disclose a piece of hard evidence about product quality after privately observing it. In particular, he can send a message corresponding to any nonempty closed subset of [0,1][0, 1] containing the true quality ω\omega. We focus on partitional disclosure strategies associated with some (ordered) partition {B1,B2,B3}\{B_1, B_2, B_3\} of [0,1][0, 1] such that when the product quality is ω∈Bi\omega \in B_i, the seller sends a message BiB_i, which is interpreted as a recommendation for the buyer to take action ii. To determine whether a partition can arise in an equilibrium, one needs to ensure that no player can profitably deviate. First, the partition must satisfy obedience in the sense that the buyer is willing to follow the recommendation. Second, it must satisfy revelation proofness in the sense that the seller is never willing to deviate by revealing the true quality. One can show that these properties are not only necessary but also sufficient for a partitional strategy to be an equilibrium strategy.

First, note that the seller's equilibrium payoff is bounded from above by his commitment payoff in this environment—that is, his maximal expected payoff in the case in which he can commit to disclosing information about ω\omega using any experiment. The commitment problem can be seen as a relaxation of the problem of maximizing the seller's payoff across equilibria because the former does not require the disclosure strategy to be revelation-proof. Therefore, if the commitment payoff is attainable in some equilibrium, this equilibrium must be a seller-preferred equilibrium of the game.

Suppose first that p=0p = 0. Given the observation above, we start by identifying the commitment solution. Because p=0p = 0, the action space is effectively binary and the seller is maximizing the probability of selling the bundle. Every commitment-optimal experiment corresponds to a partition given by B1=[0,12]B_1 = [0, \frac{1}{2}], B2=∅B_2 = \emptyset, B3=[12,1]B_3 = [\frac{1}{2}, 1] so that the buyer is indifferent between buying and not buying the bundle following message B3B_3. It is easy to check that this partition is revelation-proof, as no seller type in B1B_1 can induce any action higher than 1 by deviating. We have thus found a seller-preferred equilibrium that attains the commitment payoff.

Suppose next that p=0.5p = 0.5. In this case, there are three nontrivial actions available to the buyer, and the seller faces a trade-off between the likelihood of selling the standalone product and the likelihood of selling the bundle. It turns out that the unique commitment-optimal partition is given by B1=[0,14]B_1 = [0, \frac{1}{4}], B2=[516,1116]B_2 = [\frac{5}{16}, \frac{11}{16}], B3=[14,516]∪[1116,1]B_3 = [\frac{1}{4}, \frac{5}{16}] \cup [\frac{11}{16}, 1] (see Figure 1). Note two important properties of this partition. First, while this partition must satisfy obedience, it does so only barely, in the sense that the means of B2B_2 and B3B_3 are the lowest posterior means compatible with obedience. Namely, their means are exactly the cutoffs 12\frac{1}{2} and 34\frac{3}{4} for actions 2 and 3, respectively. Intuitively, if the obedience constraint were slack, the seller would be able to perturb the partition and shift the probability toward higher actions. Second, in contrast to the case of p=0p = 0, the optimal partition here is not monotone in the sense that some elements are not intervals. Instead, it is associated with a class of bi-pooling distributions of posterior means, which are known to be optimal in a general class of linear persuasion problems (Kleiner, Moldovanu, and Strack, 2021; Arieli, Babichenko, Smorodinsky, and Yamashita, 2023). Such bi-pooling partitions generalize monotone partitions by allowing pooling of nonadjacent types as follows. Each partitional element BiB_i is an interval or consists of two intervals and “nests” a unique other interval BjB_j in the sense that co(Bi)⊇Bj\text{co}(B_i) \supseteq B_j. Intuitively, such bi-pooling partitions arise as commitment optima because among barely obedient partitions they always allow for optimally resolving the trade-off between the likelihoods of difference actions. To determine whether the commitment payoff is attainable in equilibrium, we need to verify that this partition is revelation-proof. It is sufficient to check that no type in B2B_2 can deviate by revealing their type and convincing the buyer to buy the bundle. Indeed, since the highest type 1116\frac{11}{16} in B2B_2 is below the threshold 34\frac{3}{4} of selling a bundle, this partition is a seller-preferred equilibrium partition.

Suppose next that p=0.6p = 0.6. The unique commitment-optimal partition can be shown to be given by a bi-pooling partition B1=[0,18]B_1 = [0, \frac{1}{8}], B2=[1164,5364]B_2 = [\frac{11}{64}, \frac{53}{64}], B3=[18,1164]∪[5364,1]B_3 = [\frac{1}{8}, \frac{11}{64}] \cup [\frac{53}{64}, 1]. Compared to the previous case, here the profit from selling the standalone product expands and the set B2B_2 of types selling the standalone product shrinks. In particular, there are now some types in B2B_2 that are above the bundle threshold of 34\frac{3}{4} and for whom revealing their type would be a profitable deviation. Therefore, the above partition is not revelation-proof and the maximal equilibrium seller profit in the disclosure game is strictly below the commitment benchmark. In this case, the seller-optimal equilibrium turns out to be associated with another bi-pooling partition given by B1=[0,3−54]B_1 = [0, \frac{3-\sqrt{5}}{4}], B2=[14,34]B_2 = [\frac{1}{4}, \frac{3}{4}], B3=[3−54,14]∪[34,1]B_3 = [\frac{3-\sqrt{5}}{4}, \frac{1}{4}] \cup [\frac{3}{4}, 1]. To see why the seller cannot do better in equilibrium, note that this partition has two constraints. First, it is barely obedient for the same reason as the commitment optima described above. Second, in contrast to the commitment solution, the upper bound of B2B_2 coincides with the threshold 34\frac{3}{4}, indicating that the seller revelation-proofness constraint is binding.

Our model generalizes this example to any absolutely continuous prior distribution of the state, an ordered finite action space, and monotone preferences of the players.1

Four horizontal diagrams showing equilibrium partitions for different values of p. Each diagram has a horizontal axis from 0 to 1 with labels 'buy nothing', 'product only', and 'with add-on'. Three partitions are shown: B1 (blue), B2 (red), and B3 (green). Dashed vertical lines indicate conditional means. 1. p = 0, with and without commitment: B1 is (0, 1/2), B2 is (0, 1/2), B3 is (1/2, 1). 2. p = 0.5, with and without commitment: B1 is (0, 1/4), B2 is (1/4, 3/4), B3 is (1/4, 1/2) and (3/4, 1). 3. p = 0.6, without commitment: B1 is (0, 1/4), B2 is (1/4, 3/4), B3 is (1/4, 1/2) and (3/4, 1). 4. p = 0.6, with commitment: B1 is (0, 1/4), B2 is (1/4, 3/4), B3 is (1/4, 1/2) and (3/4, 1).
Figure 1. Commitment-optimal and sender-preferred equilibrium partitions in the example. The dashed lines are the (conditional) means of the partitional elements.

Our first main result, Theorem 1, characterizes the sender's equilibrium payoff set by showing that every equilibrium payoff can be obtained in a laminar partitional equilibrium, that is, one associated with a laminar partition. The laminar property of a partition, introduced in Candogan and Strack (2023), generalizes the aforementioned bi-pooling property as follows. In a bi-pooling partition, each element's convex hull may nest at most one other lower-indexed element, while in a laminar partition, it may nest any number of lower-indexed elements. The key step in the characterization is showing that laminar partitions are the most revelation-proof among all obedient partitions in the sense that any equilibrium partition can be transformed into a laminar equilibrium partition with the same sender payoff.

Our next result, Theorem 2, characterizes sender-preferred laminar equilibrium partitions and, more generally, provides a sharp equilibrium test for barely obedient laminar partitions. First, sender-preferred laminar equilibrium partitions are barely obedient in the sense that they leave no slack in the receiver’s obedience constraints. Theorem 2 also bounds their complexity by showing that action ii is recommended on at most max⁡{i−1,1}\max\{i-1, 1\} intervals of states. Finally, for barely obedient laminar partitions, revelation proofness is simplified into a local condition: it suffices to check only a small subset of the non-lowest on-path actions and only at the highest state recommend each such action. In all other cases, revelation proofness is automatic.

Our remaining set of results discusses the attainability of the commitment payoff in the disclosure game. It is well known that generically every commitment problem admits a unique bi-pooling solution. We establish in Theorem 3 that, among all partitions yielding this solution, there is a unique barely obedient bi-pooling one. Moreover, this partition is most resistant to violations of revelation proofness; consequently, the revelation proofness of this partition determines whether the commitment payoff can be achieved in a disclosure game (Proposition 1). With binary actions, Titova and Zhang (2025) show that every bi-pooling commitment solution is implementable. Our Proposition 2 shows that for three or more actions, every bi-pooling commitment solution is implementable if the sender’s utility is sufficiently convex in the cutoffs for the receiver’s actions. In the above example with three actions, the sender’s utility is sufficiently convex when pp is sufficiently low.

Our results suggest that full revelation may not be the only relevant outcome, even in settings where the sender can prove any true fact. In particular, when the receiver has only finitely many actions, the emergence of a rich set of simple equilibria can help explain the variety of disclosure policies observed in practice. Even within the class of laminar partitional equilibria, the same environment can sustain a fully revealing equilibrium, a sender-preferred equilibrium with substantially more withholding of information, and every payoff in between. Our analysis of sender-preferred equilibria also informs the case of mandatory disclosure: in some environments, voluntary disclosure may lead to pooling of a large fraction of low states with high states and therefore a much lower receiver’s payoff.

We apply these insights to study selling with quality disclosure and influencing voters. In the former setting, Milgrom (1981) shows that when the buyer can purchase any fraction of the product, unraveling takes place and every equilibrium features full revelation. We show that if the buyer is restricted to purchasing integer units, the seller may be able to achieve the commitment payoff by withholding information. In the second application, we consider an expert who discloses verifiable information to a voter who chooses from three alternatives: the amended bill, the unamended bill, and the status quo. We demonstrate that the expert can be hurt even if, all else equal, the voter becomes more inclined toward the expert’s most preferred alternative.

Related literature. This paper belongs to a growing body of literature that characterizes the equilibrium payoff set in disclosure games.2 The most closely related paper is Titova and Zhang (2025), which studies a more general disclosure game with a finite number of receiver actions. We specialize their model by assuming the state space is the unit interval and the receiver has monotonic preferences that depend only on the expected state. These assumptions allow us to characterize sender-preferred equilibria, identify the limits of verifiable communication, and establish sufficient conditions on model primitives under which the sender achieves the commitment payoff. While we focus on environments in which the receiver’s action set is more limited than it is in Grossman (1981) and Milgrom (1981)—our receiver chooses from a finite set of actions—Ali, Kleiner, and Zhang (2024) study settings with greater flexibility, where full revelation prompts an action that makes the sender no better off than inducing any other beliefs. Consequently, revelation proofness is not a concern. They provide conditions under which the set of equilibrium payoff profiles is virtually the same as the set of achievable payoff profiles under commitment. Gieczewski and Titova (2025) consider disclosure games with a general message mapping, propose an equilibrium selection criterion related to neologism proofness, and characterize the sender’s ex-ante payoffs under this criterion when the sender has access to sufficiently rich stochastic evidence.3

Beyond expanding the work on disclosure games, our work contributes to the growing body of literature on the possibility of attaining the commitment payoff without full commitment in other communication environments, as in the cases of cheap talk (Lipnowski and Ravid, 2020; Lipnowski, 2020), repeated cheap talk (Best and Quigley, 2024; Kuvalekar, Lipnowski, and Ramos, 2022; Mathevet, Pearce, and Stacchetti, 2022; Pei, 2023), informed information design (Perez-Richet, 2014; Koessler and Skreta, 2023; Zapechelnyuk, 2023),4 the ability to covertly revise a message generated by an experi-ment (Min, 2021; Lipnowski, Ravid, and Shishkin, 2022), the ability to covertly revise an experiment without affecting the marginal distribution over messages (Lin and Liu, 2024), costly misreporting (Guo and Shmaya, 2021; Nguyen and Tan, 2021), disclosure following private experimentation (Arieli and Stewart, 2025; Dai, Fudenberg, and Pei, 2026), and Bayesian persuasion under sender-worst equilibrium selection (Lipnowski, Ravid, and Shishkin, 2025). In contrast to these studies, we study a one-shot communication game with verifiable information without any commitment.

In the literature, pooling of nonadjacent states has been obtained in settings with either sender commitment (e.g., Kleiner et al., 2021; Arieli et al., 2023), the receiver’s private information (e.g., Feltovich, Harbaugh, and To, 2002; Harbaugh and To, 2020)5, or both (e.g., Guo and Shmaya, 2019; Candogan and Strack, 2023). While our setting has neither sender commitment nor receiver private information, equilibria in our game feature a similar structure. The most closely related paper to ours is Candogan and Strack (2023), which studies linear persuasion with one or more privately informed receivers. In that paper, laminar partitions arise as solutions to standard linear maximization problems with a mean-preserving contraction constraint, in which the receivers’ incentive constraints are written as additional moment conditions. Despite the fact that our revelation-proofness constraint cannot be written as a moment condition, the laminar property likewise plays a key role in our disclosure game because, as we show, laminar partitions turn out to be the most revelation-proof.

2 The Model

We consider the following disclosure game between the sender (he) and the receiver (she).6 The state space is Ω=[0,1]\Omega = [0, 1], and the common prior belief μF∈ΔΩ\mu_F \in \Delta\Omega is induced by a CDF FF that admits a strictly positive density ff. First, the sender learns the state. Then the sender communicates with the receiver using verifiable messages. Specifically, the sender’s message space in state ω∈Ω\omega \in \Omega is M(ω)≔{m∈C:ω∈m}M(\omega) := \{m \in \mathcal{C} : \omega \in m\}, where C\mathcal{C} is the collection of all nonempty closed subsets of [0,1][0, 1]. Finally, the receiver observes the message, forms a posterior belief, and takes an action.

The receiver’s action space is N={1,…,n}N = \{1, \dots, n\}, where n>1n > 1. The receiver’s optimal evidence. action depends only on her posterior mean, denoted by x∈[0,1]x \in [0, 1]. We assume that the receiver's preferences are monotone in the sense that action ii is optimal if and only if x∈[γi,γi+1]=:Aix \in [\gamma_i, \gamma_{i+1}] =: A_i for some cutoffs 0=γ1<γ2<⋯<γn+1=10 = \gamma_1 < \gamma_2 < \dots < \gamma_{n+1} = 1.7 We also assume that the sender's state-independent payoff uiu_i from the receiver taking action ii is strictly increasing in ii.8 Without loss, we normalize u1=0u_1 = 0. Finally, let

v(x)={uiif x∈[γi,γi+1) for some i∈N∖{n},unif x∈[γn,γn+1]v(x) = \begin{cases} u_i & \text{if } x \in [\gamma_i, \gamma_{i+1}) \text{ for some } i \in N \setminus \{n\}, \\ u_n & \text{if } x \in [\gamma_n, \gamma_{n+1}] \end{cases}

denote the sender's value function, which maps the receiver's posterior mean to the highest attainable sender payoff. By construction, v(x)v(x) is upper semicontinuous.

We focus on perfect Bayesian equilibria of the disclosure game. An assessment is a triple (σ,τ,β)(\sigma, \tau, \beta), where σ:Ω→ΔC\sigma: \Omega \rightarrow \Delta \mathcal{C} is the sender's strategy, τ:C→ΔN\tau: \mathcal{C} \rightarrow \Delta N is the receiver's strategy, and β:C→ΔΩ\beta: \mathcal{C} \rightarrow \Delta \Omega is the receiver's belief system.9 An assessment (σ,τ,β)(\sigma, \tau, \beta) is a (perfect Bayesian) equilibrium if

  1. for every ω∈Ω\omega \in \Omega, σ(ω)\sigma(\omega) is supported on arg⁡max⁡m∈M(ω)∑i∈Nτ(i∣m)ui\arg \max_{m \in M(\omega)} \sum_{i \in N} \tau(i | m) u_i;
  2. for every m∈Cm \in \mathcal{C}, τ(i∣m)>0\tau(i | m) > 0 implies ∫Ωωdβ(ω∣m)∈Ai\int_{\Omega} \omega d\beta(\omega | m) \in A_i;
  3. β\beta is obtained from FF given σ\sigma using Bayes' rule;
  4. for every m∈Cm \in \mathcal{C}, supp(β(m))⊆m\text{supp}(\beta(m)) \subseteq m.

In words, the first condition requires that the sender choose verifiable messages that maximize his expected payoff. The second condition requires that the receiver chooses an action that is optimal given her posterior mean. The third condition requires that the receiver uses Bayes' rule to calculate posterior beliefs from the prior and the sender's strategy. The final condition requires that the receiver's belief system is consistent with disclosure: she deems impossible any state in which the observed (on- or off-path) message is unavailable.

3 Equilibrium Analysis

We begin the analysis by introducing the notion of a partition of the state space and its key properties. A sequence B≔{Bi}i∈N⊆C\mathcal{B} := \{B_i\}_{i \in N} \subseteq \mathcal{C} of closed subsets of [0,1][0, 1] is an (ordered) partition if ⋃i∈NBi=[0,1]\bigcup_{i \in N} B_i = [0, 1] and μF(Bi∩Bj)=0\mu_F(B_i \cap B_j) = 0 for all i,j∈Ni, j \in N. Note that we index partitions using the action set for notational convenience; we also allow partitional elements to have nonempty but null intersections.

We say that an assessment (σ,τ,β)(\sigma, \tau, \beta) and a partition B\mathcal{B} are associated if for each i∈Ni \in N,

  • (a) σ(Bi∣ω)=1(ω∈Bi and ω∉Bi+1∪⋯∪Bn)\sigma(B_i \mid \omega) = \mathbb{1}(\omega \in B_i \text{ and } \omega \notin B_{i+1} \cup \dots \cup B_n);
  • (b) τ(i∣Bi)=1\tau(i \mid B_i) = 1;
  • (c) β(⋅∣Bi)=μF(⋅∣Bi)\beta(\cdot \mid B_i) = \mu_F(\cdot \mid B_i).

In an assessment associated with a partition B\mathcal{B}, the sender's strategy is to reveal which element of the partition the state belongs to by sending message BiB_i when ω∈Bi\omega \in B_i.10 Such a message can be interpreted as a recommendation for the receiver to choose action ii. Then the receiver's strategy is to always follow the recommendation. Finally, the receiver's posterior beliefs on the path are computed using Bayes' rule. Note that a partition uniquely defines the players' on-path behavior: if a partition is associated with multiple assessments, all of those assessments differ only in the receiver's off-path beliefs and actions. If an assessment (σ,τ,β)(\sigma, \tau, \beta) associated with a partition B\mathcal{B} is an equilibrium, then we call (σ,τ,β)(\sigma, \tau, \beta) a partitional equilibrium and B\mathcal{B} an equilibrium partition. The following two properties are necessary and sufficient for B\mathcal{B} to be an equilibrium partition.11

Definition 1. A partition B\mathcal{B} is

  • obedient if E[ω∣ω∈Bi]∈Ai\mathbb{E}[\omega \mid \omega \in B_i] \in A_i for each i∈Ni \in N.
  • revelation-proof if ω∈Bi\omega \in B_i implies ω∈A1∪⋯∪Ai=[0,γi+1]\omega \in A_1 \cup \dots \cup A_i = [0, \gamma_{i+1}] for each i∈Ni \in N.

In words, obedience requires that the receiver indeed prefers to take action ii when she learns that ω∈Bi\omega \in B_i, that is, after message BiB_i. Revelation proofness ensures that fully revealing the state is not a profitable deviation for the sender. Indeed, in the disclosure game, the sender has the option to fully reveal the state by sending message {ω}\{\omega\} with probability one, thus convincing the receiver to take the action that she would take knowing ω\omega. Thus, if ω∈Bi\omega \in B_i —in other words, the partition prescribes that the receiver takes action ii when the realized state is ω\omega —then the receiver prefers to take at most action ii when fully informed.

Next we define a key structural property of partitions. Let cl(⋅)\text{cl}(\cdot) and co(⋅)\text{co}(\cdot) denote the closure and the convex hull operators, respectively.

Definition 2. A partition B\mathcal{B} is laminar if for each i∈Ni \in N,

Bi=cl(co(Bi)∖⋃j<ico(Bj)).(1)B_i = \text{cl} \left( \text{co}(B_i) \setminus \bigcup_{j < i} \text{co}(B_j) \right). \quad (1)

If an equilibrium is associated with a laminar partition B\mathcal{B}, we call this equilibrium a laminar partitional equilibrium.

The intuitive interpretation of the laminar property is that each element BiB_i either has no “gaps” and is therefore an interval or has “gaps” and these gaps belong to lower-indexed partitional elements B1,…,Bi−1B_1, \dots, B_{i-1} only. This implies that for each pair BiB_i and BjB_j with i>ji > j, the convex hull co(Bi)\text{co}(B_i) either nests or has a null intersection with co(Bj)\text{co}(B_j).12 When co(Bi)⊇co(Bj)\text{co}(B_i) \supseteq \text{co}(B_j), we say that action ii nests action jj. We illustrate this intuition in Figure 2.

The following observation is a direct consequence of the definition of a laminar partition.

Observation 1. If B\mathcal{B} is a laminar partition, then each BiB_i is either an empty set or a union of at most ii intervals.

One prominent example of an obedient and revelation-proof laminar partition is A≔{Ai}i∈N={[γi,γi+1]}i∈N\mathcal{A} := \{A_i\}_{i \in N} = \{[\gamma_i, \gamma_{i+1}]\}_{i \in N}, which we call the fully informative partition. Note that while A\mathcal{A} is not fully revealing, it provides the minimal information necessary for the receiver to take her complete-information optimal action in each state.

Two panels illustrating partitions on the interval (0, 1). Panel (a) shows a laminar partition with four sets: B1 (blue, (0, 0.2)), B2 (red, (0.3, 0.4)), B3 (green, (0.5, 0.6)), and B4 (orange, (0.7, 1)). The sets are non-overlapping and nested. Panel (b) shows a non-laminar partition with the same sets, but B3 is split into two intervals: (0.5, 0.6) and (0.7, 0.8), with B4 covering (0.7, 1).
Figure 2. A laminar partition in panel (a) and a non-laminar partition in panel (b).

Equilibrium Payoff Set

Next we turn to the characterization of the equilibrium payoff set. We say that an equilibrium is sender-preferred if it yields the highest ex-ante payoff for the sender across all equilibria. Analogously, we refer to the ex-ante payoff-minimizing equilibrium as sender-worst. Our first main result shows that every equilibrium ex-ante payoff of the sender is achievable in an equilibrium associated with an obedient and revelation-proof laminar partition.13

  • Theorem 1.** (a) There exists a sender-worst equilibrium that is associated with the fully informative partition A\mathcal{A} and yields V‾≔∑i∈NμF(Ai)ui\underline{V} := \sum_{i \in N} \mu_F(A_i)u_i.
  • (b) There exists a sender-preferred equilibrium that is associated with an obedient and revelation-proof laminar partition and yields Vˉ>V‾\bar{V} > \underline{V}.
  • (c) For any V∈[V‾,Vˉ]V \in [\underline{V}, \bar{V}], there exists an equilibrium associated with an obedient and revelation-proof laminar partition.

We provide the intuition for Theorem 1 below. Part (a) is straightforward: as in most disclosure games, there exists an equilibrium in which the receiver acts as if she is fully informed. In our setting, that equilibrium is associated with the fully informative partition A\mathcal{A}. The sender's ex-ante payoff cannot fall below V‾\underline{V}, or else the sender will have a profitable deviation toward fully revealing some state.

Part (b) follows from two key observations. First, note that it is without loss to focus on partitional equilibria. This is because in a sender-preferred equilibrium, the receiver breaks ties in favor of the sender. Hence, a single action is taken with probability one in each state.

Second, we show that for any equilibrium partition there exists an equilibrium laminar partition that induces the same posterior mean distribution (PMD) and hence yields the same ex-ante payoff to the sender. We first observe that any partition induces a PMD with support on at most nn points (posterior means); using the techniques from Candogan and Strack (2023), we show that any such PMD can be induced by a laminar partition. We further show that if a PMD is induced by an obedient and revelation-proof partition, then the laminar partition that induces the same PMD is guaranteed to be obedient and revelation-proof. In this sense, laminar partitions are the most revelation-proof partitions.

Two partitions, B (laminar) and W (non-laminar), on the interval (0, 1). Partition B has elements B1 (blue interval from 0 to gamma_2) and B2 (red intervals from 0 to a and from gamma_2 to 1). Partition W has elements W1 (blue intervals from 0 to a and from gamma_2 to 1) and W2 (red interval from a to gamma_2). A red dashed vertical line is at a, and a blue dashed vertical line is at gamma_2.
Figure 3. Two partitions, B\mathcal{B} (laminar) and W\mathcal{W} (non-laminar), that induce the same PMD and whose corresponding elements have the same prior mass. If W\mathcal{W} is revelation-proof, then so is B\mathcal{B}.

We illustrate the intuition behind laminar partitions as the most revelation-proof ones in Figure 3, which presents the simplest case, where n=2n = 2. Consider two partitions, B\mathcal{B} (laminar) and W\mathcal{W} (non-laminar), that induce the same PMD and whose corresponding elements have the same prior mass; that is, E[ω∣ω∈Bi]=E[ω∣ω∈Wi]\mathbb{E}[\omega \mid \omega \in B_i] = \mathbb{E}[\omega \mid \omega \in W_i] and μF(Bi)=μF(Wi)\mu_F(B_i) = \mu_F(W_i) for all i∈Ni \in N. Since B\mathcal{B} is laminar, its lowest-indexed element B1B_1 is an interval. If W1W_1 is not an interval, the only way to match BiB_i 's prior mass and expectation is to have max⁡B1≤max⁡W1\max B_1 \leq \max W_1. Consequently, if W\mathcal{W} is revelation-proof (which, in the case of two actions, reduces to max⁡W1≤γ2\max W_1 \leq \gamma_2), so is B\mathcal{B}.

Combining the two aforementioned observations, to solve for the sender-preferred equilibrium payoff, one can maximize the sender's expected payoff across all obedient and revelation-proof laminar partitions as follows:

Vˉ=max⁡B∑i∈NμF(Bi)ui(2)\bar{V} = \max_{\mathcal{B}} \sum_{i \in N} \mu_F(B_i) u_i \tag{2}

subject to: B\mathcal{B} is an obedient and revelation-proof laminar partition.

We show that problem (2) admits a solution,14 which implies that a sender-preferred equilibrium exists. To show that Vˉ>V‾\bar{V} > \underline{V}, we construct an obedient and revelation-proof (and hence equilibrium) laminar partition that yields a strictly higher payoff than V‾\underline{V}. For example, take the fully revealing partition {[γi,γi+1]}i∈N\{[\gamma_i, \gamma_{i+1}]\}_{i \in N} and “move” the interval [0,ε][0, \varepsilon] from the first element of the partition to the nn -th one. If ε>0\varepsilon > 0 is sufficiently small, the resulting partition will remain obedient, revelation-proof, and laminar, but the sender’s ex-ante utility in the associated equilibrium will be strictly higher than V‾\underline{V}. Therefore, the sender’s ex-ante payoff in his most preferred equilibrium will also exceed V‾\underline{V}.

To prove Part (c), we show that for any payoff between V‾\underline{V} and Vˉ\bar{V} there exists a laminar equilibrium partition that blends the sender-worst (fully informative and laminar) partition A\mathcal{A} and the sender-preferred laminar equilibrium partition B\mathcal{B}, and this blend yields the payoff.

Sender-Preferred Equilibrium

Next we characterize the sender-preferred laminar partitional equilibrium. We say that action ii is skipped in partition B\mathcal{B} if BiB_i is a null set and unskipped otherwise. We refer to partition B\mathcal{B} as barely obedient if E[ω∣ω∈Bi]=γi\mathbb{E}[\omega \mid \omega \in B_i] = \gamma_i for all but the lowest unskipped i∈Ni \in N.

Theorem 2. Every sender-preferred laminar equilibrium partition B\mathcal{B} is barely obedient, and BiB_i is the union of at most max⁡{i−1,1}\max\{i-1, 1\} closed intervals for all i∈Ni \in N. Furthermore, a barely obedient laminar partition is an equilibrium partition if and only if max⁡Bi≤γi+1\max B_i \leq \gamma_{i+1} for any unskipped action i<ni < n such that action i+1i+1 either nests ii or is skipped.

The first part of Theorem 2 characterizes problem (2)’s solution—that is, an obedient and revelation-proof laminar partition that maximizes the sender’s ex-ante payoff. First, B\mathcal{B} must be barely obedient; otherwise, one could pool additional low states with high states without violating obedience or revelation proofness, thereby obtaining an equilibrium with a strictly higher ex-ante sender payoff. Specifically, if jj is the lowest unskipped action, one can reassign a subset of BjB_j of strictly positive measure to BkB_k for some k>jk > j. To show that each partitional element is the union of at most max⁡{i−1,1}\max\{i-1, 1\} closed intervals, we first note that Bj=[0,d]B_j = [0, d] for some d≤γj+1d \leq \gamma_{j+1} for the lowest unskipped action jj. That is, the lowest unskipped action is an interval that is not in the convex hull of any other partitional elements. Then each partitional element with index k≥2k \geq 2 must be a union of at most k−1k - 1 intervals by the definition of a laminar partition.

Next, note that revelation proofness is equivalent to max⁡Bi≤γi+1\max B_i \leq \gamma_{i+1} for each action ii. The second part of Theorem 2 shows that for a barely obedient laminar partition, this constraint is only binding for an action in two specific scenarios, illustrated in Figure 4: either the next-highest action is skipped or the action's corresponding partitional element is nested within the convex hull of the partitional element for the next-highest action. In all other instances, revelation proofness is automatically satisfied. This finding further emphasizes that the laminar structure makes revelation proofness easier to fulfill.

Two diagrams illustrating violations of revelation proofness. Diagram (a) shows a partition on (0, 1) with intervals B1 (blue, (0, gamma2)), B2 (red, (gamma2, gamma3)), and B3 (green, (gamma3, 1)). Diagram (b) shows a partition on (0, 1) with intervals B1 (blue, (0, gamma3)), B2 (red, (gamma3, 1)), and B3 (green, (0, gamma3) union (gamma3, 1)).
Figure 4. Violations of revelation proofness ruled out in Theorem 2.

As in Candogan and Strack (2023), the laminar structure emerges in a sender-preferred equilibrium of our game due to incentive constraints. In Candogan and Strack (2023), where the receiver is privately informed, the laminar structure prevents the receiver from misreporting her private information. In our setting, however, it optimally balances the trade-off between deterring the sender's deviations and inducing the most desirable action distribution.

As discussed after Theorem 1, laminar partitions are the most revelation-proof among all obedient partitions. However, interval partitions—a special case of laminar partitions—often fail to be sender-preferred equilibrium partitions. This underscores the importance of pooling nonadjacent states in inducing the most desirable distribution over actions subject to obedience and revelation proofness. To illustrate, recall our introductory example with p=0.6p = 0.6. The interval partition that generates the highest sender's ex-ante payoff is given by B1I=[0,14]B_1^I = [0, \frac{1}{4}], B2I=[14,34]B_2^I = [\frac{1}{4}, \frac{3}{4}], B3I=[34,1]B_3^I = [\frac{3}{4}, 1]. Since E[ω∣ω∈B3I]>γ3=34\mathbb{E}[\omega \mid \omega \in B_3^I] > \gamma_3 = \frac{3}{4}, we can pool the states from the top of B1IB_1^I with B3IB_3^I until the partition becomes barely obedient. This process yields a sender-preferred equilibrium partition, B1=[0,3−54]B_1 = [0, \frac{3-\sqrt{5}}{4}], B2=[14,34]B_2 = [\frac{1}{4}, \frac{3}{4}], B3=[3−54,14]∪[34,1]B_3 = [\frac{3-\sqrt{5}}{4}, \frac{1}{4}] \cup [\frac{3}{4}, 1].

4 When Is Commitment Payoff Achievable?

While the extent to which the sender benefits from verifiable communication depends on the specific parameters, an upper bound on the sender's payoff is given by his commitment payoff—that is, his payoff when he can commit to what messages to send in each state. In this section, we identify conditions under which the sender can attain his commitment payoff in an equilibrium of the disclosure game.

4.1 Commitment Benchmark

We start by introducing the commitment problem, or information-design problem, as a benchmark. In this problem, the sender can commit to any experiment that reveals information about the state. An experiment is a mapping χ:Ω→Δ(S)\chi: \Omega \rightarrow \Delta(S), where SS is a sufficiently rich signal space. For each state ω∈Ω\omega \in \Omega, a signal s∈Ss \in S realizes according to χ(ω)\chi(\omega). Because the receiver's optimal action only depends on the expected state, it is without loss to restrict attention to the class of experiments in which S=[0,1]S = [0, 1] and each s∈Ss \in S is calibrated to equal the induced posterior mean: s=E[ω∣s]s = \mathbb{E}[\omega \mid s]. Such a calibrated experiment χ\chi induces the PMD with CDF G(x)=∫01∫0xdχ(s∣ω)dF(ω)G(x) = \int_0^1 \int_0^x d\chi(s \mid \omega) dF(\omega).

It is well known that a PMD GG is induced by some experiment if and only if GG is a mean-preserving contraction of the prior CDF FF.15 Consequently, the commitment problem can be stated as a maximization of the expected value vv with respect to the PMD,

max⁡G∈MPC(F)∫01v(x)dG(x),(3)\max_{G \in \text{MPC}(F)} \int_0^1 v(x) dG(x), \quad (3)

where MPC(F)\text{MPC}(F) is the set of all mean-preserving contractions of FF. We call any solution to problem (3) a commitment solution and call the value of problem (3) the commitment payoff. Clearly, the commitment payoff is an upper bound of the sender's equilibrium payoff in the disclosure game.

Finally, we say that a commitment solution GG is implementable with verifiable messages, or simply implementable for short, if there is an equilibrium in which the sender's strategy induces the receiver's PMD GG.

We say that an experiment χ\chi is associated with a partition B\mathcal{B} if it maps almost every ω∈Bi\omega \in B_i into the degenerate distribution centered on E[ω∣ω∈Bi]\mathbb{E}[\omega \mid \omega \in B_i]. In other words, such an experiment discloses only which element of the partition the state belongs to. In this case, we also say that the induced PMD GG is associated with this partition.

Next we define a refinement of the laminar property, which is key for optimality under commitment.

Definition 3. A laminar partition is a bi-pooling partition if for every i∈Ni \in N, either BiB_i is an interval or there exists a unique j<ij < i and Bj⊆co(Bi)B_j \subseteq \text{co}(B_i).

Two panels illustrating partitions on the interval (0, 1). Panel (a) shows a bi-pooling partition where B1, B2, and B3 are intervals, and B4 is a union of two intervals that contains B2 and B3. Panel (b) shows a laminar partition that is not a bi-pooling partition, where B4 is a single interval that contains B2 and B3, but B1 is not nested within B4.
Figure 5. A bi-pooling partition in panel (a) and a laminar partition that is not a bi-pooling partition in panel (b).

While laminar partitions allow any BjB_j with j<ij < i to be nested within co(Bi)\text{co}(B_i), bi-pooling partitions allow only for a single such BjB_j to be nested within co(Bi)\text{co}(B_i) (see Figure 5).

The following result regarding bi-pooling partitions is a direct consequence of the results in Kleiner et al. (2021), Candogan (2022), and Arieli et al. (2023). Say that the communication environment is generic if no three elements of the collection of points {(γi,ui)}i∈N\{(\gamma_i, u_i)\}_{i \in N} are collinear.

Theorem 3. There exists a commitment solution associated with a unique barely obedient bi-pooling partition. Moreover, the commitment solution is unique in generic communication environments.

Theorem 3 indicates that, despite the simplicity of bi-pooling partitions, there always exists a commitment solution associated with a bi-pooling partition. Moreover, under mild conditions, the unique commitment solution is associated with a bi-pooling partition.

4.2 Characterizing Implementability

The following result characterizes the implementability of a commitment solution associated with a bi-pooling partition.

Proposition 1. Let GG be a commitment solution associated with a bi-pooling partition B\mathcal{B}. Then GG is implementable if and only if B\mathcal{B} is revelation-proof.

It follows directly from Theorem 3 and Proposition 1 that in a generic communication environment, the unique commitment solution is implementable if and only if the associated bi-pooling partition is revelation-proof.

The “if” part of Proposition 1 is a direct consequence of Theorem 2 in Titova and Zhang (2025), which states that for a partition associated with a commitment solution, implementability is equivalent to revelation proofness. Our primary contribution in Proposition 1 is to show that of all sender strategies that induce a commitment solution, the one associated with a bi-pooling partition has the best shot at being an equilibrium strategy. Roughly, this stems from the fact that bi-pooling partitions are a special case of laminar partitions, which exhibit a similar property.

Proposition 1 is useful in that it suggests a “guess and verify” approach to finding the sender-preferred equilibrium. First, one finds the commitment solution using standard information-design methods. Second, one identifies the associated bi-pooling partition. If this partition proves to be revelation-proof, then the sender-preferred equilibrium has been successfully identified.

The next result, which is a corollary of Proposition 1 and Theorem 2, goes one step further: it reveals the exact features of bi-pooling partitions that fail revelation proofness and hence prevent the commitment solutions from being implementable.

Corollary 1. Let GG be a commitment solution associated with a bi-pooling partition B\mathcal{B}. Then GG is implementable if and only if B\mathcal{B} is such that max⁡Bi≤γi+1\max B_i \leq \gamma_{i+1} for any unskipped action i<ni < n such that action i+1i + 1 either nests ii or is skipped.

Compared to the definition of revelation proofness, the condition in Corollary 1 is easier to verify when determining whether a commitment solution is implementable. It also allows us to identify sufficient conditions under which commitment has no value in the subsequent Section 4.3.

To illustrate this result, recall our introductory example with A={1,2,3}A = \{1, 2, 3\}, u1=0u_1 = 0, u2=pu_2 = p, u3=1u_3 = 1, γ2=12\gamma_2 = \frac{1}{2}, γ3=34\gamma_3 = \frac{3}{4}, and uniform FF. When p=0p = 0, there is a unique commitment solution associated with a bi-pooling partition given by B1=[0,12]B_1 = [0, \frac{1}{2}], B2=∅B_2 = \emptyset, B3=[12,1]B_3 = [\frac{1}{2}, 1]. Note that the condition in Corollary 1 only applies to action 1 and is satisfied because max⁡B1=12≤12=γ2\max B_1 = \frac{1}{2} \leq \frac{1}{2} = \gamma_2. In other words, the commitment-optimal partition is revelation-proof because the sender cannot induce an action higher than 1 by fully revealing the state when it is in B1B_1.

When p=0.5p = 0.5, there is a unique commitment solution associated with a bi-pooling partition given by B1=[0,14]B_1 = [0, \frac{1}{4}], B2=[516,1116]B_2 = [\frac{5}{16}, \frac{11}{16}], B3=[14,516]∪[1116,1]B_3 = [\frac{1}{4}, \frac{5}{16}] \cup [\frac{11}{16}, 1]. Note that the condition in Corollary 1 only applies to action 2 and is satisfied because max⁡B2=1116≤34=γ3\max B_2 = \frac{11}{16} \leq \frac{3}{4} = \gamma_3.

Proposition 1 and Corollary 1 might suggest that implementing a commitment solution associated with a bi-pooling partition is relatively simple: one needs only to ensure that no action is recommended more often than revelation proofness allows. Indeed, Titova and Zhang (2025) showed that when a receiver is choosing between two actions, revelation proofness is automatically satisfied. When there are three or more actions, however, the restriction imposed by revelation proofness can be substantial. We illustrated this in our introductory example with p=0.6p = 0.6. In this case, the commitment-optimal bi-pooling partition is given by B1=[0,18]B_1 = [0, \frac{1}{8}], B2=[1164,5364]B_2 = [\frac{11}{64}, \frac{53}{64}], B3=[18,1164]∪[5364,1]B_3 = [\frac{1}{8}, \frac{11}{64}] \cup [\frac{53}{64}, 1]. Note that in this case the condition in Corollary 1 is violated for action 2, which is nested by action 3, but max⁡B2=5364>34=γ3\max B_2 = \frac{53}{64} > \frac{3}{4} = \gamma_3.

When there are two actions, the sender’s sole objective is to maximize the probability that the “high action” 2 is played. This in turn suggests that revelation proofness is never an issue: in any state in which action 2 is played under complete information, there is no reason to recommend action 1. However, when there are three actions, as Gentzkow and Kamenica (2016) note, the sender in the commitment problem faces a trade-off between inducing actions 2 and 3. When pp is high, the gap between u2u_2 and u3u_3 is significantly smaller than that between u1u_1 and u2u_2, and hence it is more profitable to induce action 2 more often: to guarantee obedience, recommending action 3 more often must come with action 1 being played more frequently. Consequently, the unique commitment-optimal partition recommends action 2 so frequently that max⁡B2>γ3\max B_2 > \gamma_3. In states strictly higher than γ3\gamma_3, the sender is strictly better off by fully revealing the state, rendering the commitment solution not implementable.

4.3 Sufficient Conditions for Implementability

In what follows, we identify conditions on model primitives that guarantee the existence of an implementable commitment solution. Under these conditions, the sender does not benefit from commitment relative to the sender-preferred equilibrium. The equilibrium payoff set and the sender-preferred equilibrium partition can thus be found by solving the corresponding commitment problem. Conversely, the commitment assumption is unnecessary for any information-design problem that satisfies these conditions.

To state the result, let h(γi;γi+1)h(\gamma_i; \gamma_{i+1}) denote the unique solution of E[ω∣ω∈[h(γi;γi+1),γi+1]]=γi\mathbb{E}[\omega \mid \omega \in [h(\gamma_i; \gamma_{i+1}), \gamma_{i+1}]] = \gamma_i if it exists, and set it to 0 otherwise. In words, h(γi;γi+1)h(\gamma_i; \gamma_{i+1}) is the state such that the conditional mean of the states between it and γi+1\gamma_{i+1} is exactly γi\gamma_i.

Proposition 2. Suppose there are three or more actions. Then every commitment solution associated with a bi-pooling partition is implementable if

ui+1−uiγi+1−γi>ui−ui−1γi−max⁡{γi−1,h(γi;γi+1)}(4)\frac{u_{i+1} - u_i}{\gamma_{i+1} - \gamma_i} > \frac{u_i - u_{i-1}}{\gamma_i - \max\{\gamma_{i-1}, h(\gamma_i; \gamma_{i+1})\}} \quad (4)

for all i=2,…,n−1i = 2, \dots, n-1. Consequently, the commitment payoff is attained in an equilibrium of the disclosure game.

In Condition (4), ui+1−uiu_{i+1} - u_i is the sender's marginal benefit of inducing a higher action evaluated at action ii and γi+1−γi\gamma_{i+1} - \gamma_i is the difference in cutoffs for inducing actions i+1i+1 and ii under complete information, respectively. Proposition 2 suggests that in a communication environment, if inducing a marginally higher action is either sufficiently more profitable or sufficiently more difficult (requiring a sufficiently larger expected state), or both, then the sender does not benefit from commitment power. Put differently, the sender does not value commitment when his value function increases sufficiently fast in the expected state.

The intuition behind Proposition 2 is as follows. To establish the sufficiency of (4), we argue that any partition that is not revelation-proof must also fail optimality in the commitment problem. Take any barely obedient bi-pooling partition B\mathcal{B} that is not revelation-proof. Then some action ii is recommended in some states in which the sender would prefer to fully reveal the state to induce a higher action instead; that is, max⁡Bi>γi+1\max B_i > \gamma_{i+1}. To illustrate how B\mathcal{B} can then be strictly improved, suppose BiB_i is an interval. Then max⁡Bi>γi+1\max B_i > \gamma_{i+1} and obedience implies γi+1∈Bi\gamma_{i+1} \in B_i. Next, modify the partition by shrinking BiB_i and shifting the probability of recommending action ii to actions i−1i-1 and i+1i+1. Recommending action i+1i+1 can still be made barely obedient by inducing belief γi+1\gamma_{i+1}. At the same time, action i−1i-1 can now be induced at γi−1\gamma_{i-1} if γi−1\gamma_{i-1} is not too low, and otherwise at h(γi;γi+1)h(\gamma_i; \gamma_{i+1}). Either way, condition (4) ensures that such a local mean-preserving spread is profitable by requiring the sender's utility to be “convex enough” with respect to the cutoffs {γi}i∈N\{\gamma_i\}_{i \in N}. Consequently, any barely obedient partition associated with a commitment solution must be revelation-proof, and thus every such commitment solution is implementable.

Imposing a further assumption on the prior, Condition (4) can be simplified.

Corollary 2. Suppose there are three or more actions. If ff is increasing, and ui+1−ui≥ui−ui−1u_{i+1} - u_i \geq u_i - u_{i-1} and γi+1−γi≤γi−γi−1\gamma_{i+1} - \gamma_i \leq \gamma_i - \gamma_{i-1} hold for all i=2,…,n−1i = 2, \dots, n-1, with at least one inequality being strict for some ii, then every commitment solution associated with a bi-pooling partition is implementable. Consequently, the commitment payoff is attained in an equilibrium.

An increasing prior density is equivalent to a convex prior CDF. This condition is satisfied by the uniform distribution and more generally by the family of power distributions on [0,1][0, 1], with the CDF given by F(x)=xαF(x) = x^\alpha, α≥1\alpha \geq 1.

4.4 The Special Case of Ternary Actions

It is instructive to take a deeper dive into the case in which the receiver has three actions. In this case, a partition can be written as B={B1,B2,B3}\mathcal{B} = \{B_1, B_2, B_3\}. As implied by Theorem 2, in a sender-preferred laminar equilibrium partition, B1B_1 must be an interval if it is not null. Moreover, B2B_2 and B3B_3 either are both intervals or are such that B2⊆co(B3)B_2 \subseteq \text{co}(B_3), meaning that B\mathcal{B} is a bi-pooling partition.16 Consequently, Theorem 2 implies that revelation proofness boils down to max⁡B1≤γ2\max B_1 \leq \gamma_2.

Armed with these observations, a sender-preferred equilibrium can be explicitly solved.

Proposition 3. Suppose that n=3n = 3. A sender-preferred equilibrium is associated with a barely obedient bi-pooling partition B\mathcal{B} that either is also associated with the commitment solution or is such that B1=[0,y]B_1 = [0, y], B2=[z,γ3]B_2 = [z, \gamma_3], and B3=[y,z]∪[γ3,1]B_3 = [y, z] \cup [\gamma_3, 1], where z>0z > 0 and y≥0y \geq 0 solve the following system of equations:

E[ω∣ω∈[z,γ3]]=γ2;E[ω∣ω∈[y,z]∪[γ3,1]]=γ3.\begin{aligned}\mathbb{E}[\omega \mid \omega \in [z, \gamma_3]] &= \gamma_2; \\ \mathbb{E}[\omega \mid \omega \in [y, z] \cup [\gamma_3, 1]] &= \gamma_3.\end{aligned}

When there are only three actions, the only reason that a commitment solution is not implementable is that the “middle” action, 2, is recommended too often. Therefore, if no commitment solution is implementable, in the bi-pooling partition associated with a sender-preferred equilibrium, action 2 is recommended as frequently as revelation proofness allows: that is, the upper bound of B2B_2 must coincide with γ3\gamma_3.

The sufficient conditions can be further simplified when ∣N∣=3|N| = 3.

Corollary 3. If n=3n = 3, ff is increasing, and u3>2u2u_3 > 2u_2, then all commitment solutions are implementable.

Applying Corollary 3 to our introductory example, since u2=pu_2 = p and u3=1u_3 = 1, as long as p<0.5p < 0.5, the seller does not benefit from commitment power. In other words, even prior to solving the commitment problem, we know that a sender-preferred equilibrium partition can be identified from the commitment solution.

5 Applications

5.1 Selling with Quality Disclosure

We first consider a variant of the sales encounter model studied in Section 5 of Milgrom (1981). The state of the world, ω\omega, is interpreted as the quality of the seller's product. Let p>0p > 0 be the unit price, and for simplicity, assume that there is no quantity discount. Denote the seller's constant unit cost by cc, where 0≤c<p0 \leq c < p. The product is indivisible: the buyer can only buy integer units of the product. The buyer's utility from purchasing qq units is ωU(q)−pq\omega U(q) - pq, where U:R+→RU: \mathbb{R}_+ \rightarrow \mathbb{R} is a bounded, strictly increasing, strictly concave three-times differentiable function with U(0)=0U(0) = 0. We further assume that U(q)−pqU(q) - pq is maximized at n>1n > 1. As a consequence, the buyer buys at most nn units of the product, and she buys nothing if ω\omega is close enough to 0.

The only significant difference between this model and that of Milgrom (1981) is that he considers a perfectly divisible product and hence the seller's value function is strictly increasing. In our case, however, indivisibility makes the seller's value function a step function with nn jumps. For a perfectly divisible product, Milgrom shows that every equilibrium of the game features full revelation: the seller sends m={ω}m = \{\omega\} for each ω∈(0,1]\omega \in (0, 1], resulting in the buyer-preferred outcome. With indivisibility, however, the seller may be able to gain considerably from verifiable communication, attaining his commitment payoff.

To state the result, let

AU(q)≔−U′′(q)U′(q)andPU(q)≔−U′′′(q)U′′(q)A^U(q) := -\frac{U''(q)}{U'(q)} \quad \text{and} \quad P^U(q) := -\frac{U'''(q)}{U''(q)}

denote the coefficients of absolute risk aversion and absolute prudence, respectively.

Proposition 4. If ff is increasing and PU>2AUP^U > 2A^U, there exists an equilibrium of this game in which the seller is as well off as he would be if he had commitment power.

The assumption of an increasing prior density can be interpreted as meaning that it is common knowledge that the consumer is relatively confident about the quality of the product. The condition PU>2AUP^U > 2A^U is satisfied by, for example, a constant relative risk aversion (CRRA) utility function with parameter 0<σ<10 < \sigma < 1.

5.2 Influencing a Voter

Consider an amendment voting setting where a voter chooses among three alternatives: maintaining the status quo (no bill, action 1); the amended bill (action 2); and the (unamended) bill (action 3).17 The state of the world is ω∈[0,1]\omega \in [0, 1]. The voter has linear preferences: her utility from action k∈{1,2,3}k \in \{1, 2, 3\} in state ω\omega is given by αk+λkω\alpha_k + \lambda_k \omega. Moreover, λ3>λ2>λ1=0\lambda_3 > \lambda_2 > \lambda_1 = 0 and 0=α1>α2>α30 = \alpha_1 > \alpha_2 > \alpha_3. Let γ2\gamma_2 and γ3\gamma_3 denote the cutoff states at which the voter is indifferent between actions 1 and 2, and actions 2 and 3, respectively:18 we impose γ2<γ3\gamma_2 < \gamma_3. The voter's preferences are illustrated in Figure 6.

In this model, the voter's preferences over action kk are characterized by two parameters: αk\alpha_k, her reference point for action kk (her cardinal utility when the state is zero), and λk\lambda_k, her state sensitivity for action kk (how fast her cardinal utility increases in the state). The voter agrees that when the state is low (intermediate, high), action 1 (action 2, action 3, respectively) is optimal.

There is an expert who observes the state and discloses verifiable information to the voter (e.g., Jackson and Tan, 2013). The expert's preferences satisfy u3>u2>u1=0u_3 > u_2 > u_1 = 0; that is, the expert strictly prefers the bill to the amended bill, and the amended bill to no bill. This is a direct application of our model with n=3n = 3 and cutoffs γ2,γ3\gamma_2, \gamma_3, as defined above.19 The expert-preferred equilibrium is therefore characterized by Proposition 3.

A graph showing the voter's utility as a function of the state ω. The vertical axis is labeled 'voter's utility' and the horizontal axis is labeled 'ω'. Three linear functions are plotted: 'action 1' (orange, horizontal), 'action 2' (blue, upward sloping), and 'action 3' (red, upward sloping). The intersection of action 1 and action 2 is marked with a vertical dashed line to the horizontal axis at γ₂. The intersection of action 2 and action 3 is marked with a vertical dashed line to the horizontal axis at γ₃.
Figure 6. The voter's utilities.

Proposition 5 shows that the expert can be hurt if the voter becomes “more inclined toward” the bill in the sense that, all else equal, either the reference point or the state sensitivity for action 3 increases.

Proposition 5. If no commitment solution is implementable and at least one of the following happens:

  • (i) the voter's state sensitivity for the bill, λ3\lambda_3, increases,
  • (ii) the voter's reference point for the bill, α3\alpha_3, increases,

then the expert's payoff in his preferred equilibrium may decrease.

When either (i) or (ii) occurs (or both), γ3\gamma_3 decreases. This implies that the expected state required to pass the bill is lowered, which benefits the expert directly: he can more frequently induce passage of the original bill. However, this also introduces an adverse indirect effect. Recall from the discussion after Proposition 3 that when no commitment solution is implementable, the upper bound of B2B_2 is pinned to γ3\gamma_3 by the binding revelation-proofness constraint. As γ3\gamma_3 falls, this constraint tightens, limiting the range of states over which the expert can credibly recommend action 2. The expert is therefore harmed when this indirect effect dominates the direct one. This may occur when the utility gap between the bill and the amended bill is smaller than that between the amended bill and the status quo (i.e., u3−u2<u2−u1u_3 - u_2 < u_2 - u_1), which is plausible in many voting scenarios.

6 Conclusion

This paper revisits a classic persuasion game (e.g., Milgrom, 1981) by changing one feature of the canonical model: the receiver has only finitely many actions. When the receiver can adjust her action finely, even a small improvement in beliefs leads to a better action for the sender, and the usual unraveling logic leaves little room for withholding information. With finitely many actions, by contrast, small changes in beliefs need not change the receiver’s action. This creates room for credible pooling even when the sender can prove any true fact, so full revelation is no longer the sole relevant equilibrium outcome. We show that the resulting set of equilibrium payoffs is organized by partitions of the state space with a simple geometric property—the laminar structure. Any sender-worst equilibrium is payoff equivalent to a fully revealing equilibrium, whereas a sender-preferred equilibrium often involves pooling nonadjacent states. We characterize such sender-preferred equilibria and use the characterization to compare sender-preferred equilibrium payoff with the commitment payoff: the payoff the sender would obtain if he could commit to an information structure, as in the information-design literature. This comparison identifies conditions under which the commitment payoff can be achieved in equilibrium.

The analysis yields broader lessons about disclosure and information design. The same environment can sustain a fully revealing equilibrium, a sender-preferred equilibrium with substantial pooling, and every payoff in between through simple laminar equilibria. This observation helps explain the variety of disclosure policies observed in practice and qualifies the welfare conclusions one can draw from the existence of a fully revealing equilibrium alone: observing that voluntary disclosure admits a fully revealing equilibrium does not imply that it delivers the receiver-preferred outcome; mandatory disclosure can still substantially improve receiver welfare by eliminating sender-preferred pooling. At the same time, our sufficient conditions for attaining the commitment payoff identify information-design problems for which the commitment assumption can be relaxed. On the other hand, if those conditions are met, the sender-preferred equilibrium and the equilibrium payoff set can be identified by solving the corresponding information-design problem. When the commitment payoff is unattainable, the sender-preferred equilibrium captures the trade-off between inducing actions more favorable to the sender and ensuring that no type wants to deviate by fully revealing the state.

A Omitted Proofs and Details

A.1 Proofs for Section 3

A.1.1 Preliminary characterization

In what follows, we employ the following result, which is essentially Theorem 1 in Titova and Zhang (2025) adapted to our setting.20 We provide a proof below for completeness.

Lemma 1. B\mathcal{B} is an equilibrium partition if and only if it is obedient and revelation-proof.

Proof. Necessity is straightforward: if B\mathcal{B} is not revelation-proof or obedient, then in every associated assessment, the sender has a profitable deviation to full revelation or the receiver is not best responding to an on-path message. For sufficiency, suppose that B\mathcal{B} is an obedient and revelation-proof partition. Let (σ,τ,β)(\sigma, \tau, \beta) be an associated assessment such that the receiver (1) has maximally skeptical off-path beliefs and (2) best responds according to her posterior mean and breaks ties in the sender-adversarial manner when indifferent. Specifically, for each m∉Bm \notin \mathcal{B}, let β(min⁡m∣m)=1\beta(\min m \mid m) = 1, and τ(j∣m)=1\tau(j \mid m) = 1 if min⁡m∈[γj−1,γj)\min m \in [\gamma_{j-1}, \gamma_j) and j∈N∖{n}j \in N \setminus \{n\}, or min⁡m∈[γn−1,γn]\min m \in [\gamma_{n-1}, \gamma_n] and j=nj = n. Then, (σ,τ,β)(\sigma, \tau, \beta) is an equilibrium, and thus B\mathcal{B} is an equilibrium partition. Indeed, equilibrium conditions 2, 3, and 4 are satisfied by construction. Equilibrium condition 1 (the sender has no profitable deviations at each ω\omega) is satisfied because if ω∈Bi\omega \in B_i and ω∉Bi+1∪⋯∪Bn\omega \notin B_{i+1} \cup \dots \cup B_n, then the sender's interim payoff is uiu_i; deviations to on-path messages with a higher index are not feasible, and deviations to on-path messages with a lower index or to off-path messages yield an interim payoff of at most uiu_i. ■

A.1.2 Towards the proof of Theorem 1

To prove Theorem 1, we will need four auxiliary results.

Claim 1. Let HH be a mean-preserving contraction of FF with ∣supp(H)∣≤n|\text{supp}(H)| \leq n. Then there exist cutoffs 0=:d0≤d1≤⋯≤dm−1≤dm≔10 =: d_0 \leq d_1 \leq \dots \leq d_{m-1} \leq d_m := 1 with m≤∣supp(H)∣m \leq |\text{supp}(H)| such that ∫0xH(q)dq≤∫0xF(q)dq\int_0^x H(q) dq \leq \int_0^x F(q) dq on [di−1,di][d_{i-1}, d_i] for all i=1,…,mi = 1, \dots, m and the inequality binds only at di−1d_{i-1} and did_i.

Proof of Claim 1. First, let supp(H)={γ~i}i=1k\text{supp}(H) = \{\tilde{\gamma}_i\}_{i=1}^k, where k≤nk \leq n since ∣supp(H)∣≤n|\text{supp}(H)| \leq n and γ~i<γ~j\tilde{\gamma}_i < \tilde{\gamma}_j if i<ji < j. Since F(0)=H(0)=0F(0) = H(0) = 0, FF is strictly increasing (since f>0f > 0), and HH is a step function, there exists ε>0\varepsilon > 0 such that F(x)>H(x)F(x) > H(x) for all x∈[0,ε]x \in [0, \varepsilon]. Since H∈MPC(F)H \in \text{MPC}(F), we have ∫01H(q)dq=∫01F(q)dq\int_0^1 H(q) dq = \int_0^1 F(q) dq, and hence the set

D1={x∈[ε,1]:∫0xH(q)dq=∫0xF(q)dq}D_1 = \left\{ x \in [\varepsilon, 1] : \int_0^x H(q) dq = \int_0^x F(q) dq \right\}

is nonempty. Let d1=inf⁡D1d_1 = \inf D_1. If d1=1d_1 = 1, then set m=1m = 1 and the proof is complete. For the rest of the proof, suppose that d1<1d_1 < 1.

Observe that γ~1<d1<γ~k\tilde{\gamma}_1 < d_1 < \tilde{\gamma}_k: if d1≤γ~1d_1 \leq \tilde{\gamma}_1, then F(x)>H(x)=0F(x) > H(x) = 0 for all x∈[0,d1]x \in [0, d_1], which contradicts the definition of d1d_1; if d1≥γ~kd_1 \geq \tilde{\gamma}_k, then F(x)<H(x)=1F(x) < H(x) = 1 for all x∈[d1,1]x \in [d_1, 1], so that ∫01H(q)dq≠∫01F(q)dq\int_0^1 H(q) dq \neq \int_0^1 F(q) dq, a contradiction.

Next, we argue that F(d1)≥H(d1)F(d_1) \geq H(d_1). Suppose to the contrary that F(d1)<H(d1)F(d_1) < H(d_1). Then, since HH is a CDF and hence right-continuous, there must exist δ>0\delta > 0 such that F(x)<H(x)=H(d1)F(x) < H(x) = H(d_1) for all x∈[d1,d1+δ]x \in [d_1, d_1 + \delta], where the equality follows from the fact that HH is a step function. Then,

∫0d1+δF(q)dq=∫0d1F(q)dq+∫d1d1+δF(q)dq=∫0d1H(q)dq+∫d1d1+δF(q)dq<∫0d1H(q)dq+∫d1d1+δH(q)dq,\begin{aligned} \int_0^{d_1+\delta} F(q) dq &= \int_0^{d_1} F(q) dq + \int_{d_1}^{d_1+\delta} F(q) dq = \int_0^{d_1} H(q) dq + \int_{d_1}^{d_1+\delta} F(q) dq \\ &< \int_0^{d_1} H(q) dq + \int_{d_1}^{d_1+\delta} H(q) dq, \end{aligned}

which contradicts the assumption that HH is a MPC of FF.

Now, let j=min⁡{i:γ~i>d1}j = \min\{i : \tilde{\gamma}_i > d_1\}. Given that d1<γ~jd_1 < \tilde{\gamma}_j, F(d1)≥H(d1)F(d_1) \geq H(d_1), FF is strictly increasing, and HH is a step function, there exists η>0\eta > 0 such that F(x)>H(x)F(x) > H(x) for all x∈[d1,d1+η]x \in [d_1, d_1 + \eta]. Consequently, ∫01H(q)dq=∫01F(q)dq\int_0^1 H(q) dq = \int_0^1 F(q) dq implies that the set

D2={x∈[d1+η,1]:∫0xH(q)dq=∫0xF(q)dq}D_2 = \left\{ x \in [d_1 + \eta, 1] : \int_0^x H(q) dq = \int_0^x F(q) dq \right\}

is nonempty. Let d2=inf⁡D2d_2 = \inf D_2. If d2=1d_2 = 1, then set m=2m = 2 and the proof is complete. For the remainder of the proof, suppose that d2<1d_2 < 1. Using the same steps as above, one can show that d2>γ~jd_2 > \tilde{\gamma}_j and F(d2)≥H(d2)F(d_2) \geq H(d_2). Proceeding inductively, one can find dtd_t with t≤k≤nt \leq k \leq n such that dt>γ~kd_t > \tilde{\gamma}_k. It must be that dt=1d_t = 1: suppose not, then because FF is strictly increasing, F(x)<1F(x) < 1 on (dk,1)(d_k, 1); but H(x)=1H(x) = 1 on the same interval, which implies that ∫01H(q)dq>∫01F(q)dq\int_0^1 H(q) dq > \int_0^1 F(q) dq, a contradiction. Now set m=tm = t, the proof is complete. ■

Claim 2. If HH is a mean-preserving contraction of FF with ∣supp(H)∣≤n|\text{supp}(H)| \leq n, then it induces a laminar partition.

Proof. By Claim 1, on each of the mm intervals such that the MPC constraint only binds at the endpoints, the mass is redistributed to at most nn points, and there can be at most mm such intervals. We show that every such interval admits a laminar partition; the definition of a laminar partition then implies that the resulting partition is still laminar by taking the union.

Denote an arbitrary interval on which the MPC constraint only binds at the endpoints by I≔[a,b]I := [a, b]; that is, ∫0xH(q)dq≤∫0xF(q)dq\int_0^x H(q) dq \leq \int_0^x F(q) dq for all q∈Iq \in I, and the inequality binds only at aa and bb.

The remainder of the proof is very similar to the proof of Lemma 11 in Candogan and Strack (2023), and hence we only provide an outline here; readers interested in details are directed to that paper. Let K=∣supp(H)∩I∣≤nK = |\text{supp}(H) \cap I| \leq n; the proof proceeds by induction on KK. If K=1K = 1, let supp(H)∩I={γ~ℓ}\text{supp}(H) \cap I = \{\tilde{\gamma}_\ell\}; then clearly {Bℓ}\{B_\ell\} where Bℓ=IB_\ell = I is a laminar partition of II. If K=2K = 2, let supp(H)∩I={γ~ℓ,γ~m}\text{supp}(H) \cap I = \{\tilde{\gamma}_\ell, \tilde{\gamma}_m\} where ℓ<m\ell < m; then by Lemma 4 in Arieli et al. (2023), {Bℓ,Bm}\{B_\ell, B_m\} can be chosen such that Bℓ=[c,d]B_\ell = [c, d] and Bm=[a,c]∪[b,d]B_m = [a, c] \cup [b, d], which is laminar.

Taking K=2K = 2 as the base case, consider K>2K > 2; the induction hypothesis holds for K−1K - 1. One can find a closed interval BℓB_\ell such that (i) μF(Bℓ)=h(γ~ℓ)\mu_F(B_\ell) = h(\tilde{\gamma}_\ell), where hh is the probability mass function (pmf) of HH, and γ~ℓ=min⁡(supp(H)∩I)\tilde{\gamma}_\ell = \min(\text{supp}(H) \cap I),21 and (ii) E[ω∣ω∈Bℓ]=γ~ℓ\mathbb{E}[\omega \mid \omega \in B_\ell] = \tilde{\gamma}_\ell. Consequently, conditional on ω∉Bℓ\omega \notin B_\ell, HH only has K−1K - 1 mass points, and Lemma 12 in Candogan and Strack (2023) shows that it is a MPC of FF. Invoking the inductive hypothesis, a laminar partition of II, {B^i}i∈T\{\hat{B}_i\}_{i \in \mathcal{T}}, is obtained, where T≔{k≠ℓ:γk∈supp(H)∩I}\mathcal{T} := \{k \neq \ell : \gamma_k \in \text{supp}(H) \cap I\}. For every i∈Ti \in \mathcal{T}, let Bi≔cl(B^i∖Bℓ)B_i := \text{cl}(\hat{B}_i \setminus B_\ell). Since {B^i}i∈T\{\hat{B}_i\}_{i \in \mathcal{T}} is laminar, and ℓ<i\ell < i for all i∈Ti \in \mathcal{T}, {Bi}i∈T∪{ℓ}\{B_i\}_{i \in \mathcal{T} \cup \{\ell\}} is also laminar. ■

Claim 3. Suppose that W⊆[0,1]W \subseteq [0, 1] and B=[x,y]⊆[0,1]B = [x, y] \subseteq [0, 1] such that μF(W)=μF(B)\mu_F(W) = \mu_F(B) and E[ω∣ω∈W]=E[ω∣ω∈B]\mathbb{E}[\omega \mid \omega \in W] = \mathbb{E}[\omega \mid \omega \in B]. Then, inf⁡W≤x\inf W \leq x and y≤sup⁡Wy \leq \sup W.

Proof. We prove that y≤sup⁡Wy \leq \sup W; the proof of inf⁡W≤x\inf W \leq x is analogous. Since μF(W)=μF(B)\mu_F(W) = \mu_F(B) and E[ω∣ω∈W]=E[ω∣ω∈B]\mathbb{E}[\omega \mid \omega \in W] = \mathbb{E}[\omega \mid \omega \in B], we have ∫W∖BωdF(ω)=∫B∖WωdF(ω)\int_{W \setminus B} \omega dF(\omega) = \int_{B \setminus W} \omega dF(\omega) and μF(W∖B)=μF(B∖W)\mu_F(W \setminus B) = \mu_F(B \setminus W).

Suppose, by contradiction, that sup⁡W<y\sup W < y. Then, W∖B⊆[0,x]W \setminus B \subseteq [0, x], B∖W⊆[x,y]B \setminus W \subseteq [x, y] and μF(W∖B)=μF(B∖W)>0\mu_F(W \setminus B) = \mu_F(B \setminus W) > 0. Furthermore,

∫W∖BωdF(ω)<xμF(W∖B)=xμF(B∖W)<∫B∖WωdF(ω),\int_{W \setminus B} \omega dF(\omega) < x \mu_F(W \setminus B) = x \mu_F(B \setminus W) < \int_{B \setminus W} \omega dF(\omega),

a contradiction. Therefore, y≤sup⁡Wy \leq \sup W. ■

Claim 4. Let (σ′,τ′,β′)(\sigma', \tau', \beta') be an equilibrium. Define τ′′\tau'' by

τ′′(i∣m)={1,if i=max⁡supp τ′(⋅∣m)0,otherwise\tau''(i \mid m) = \begin{cases} 1, & \text{if } i = \max \text{supp } \tau'(\cdot \mid m) \\ 0, & \text{otherwise} \end{cases}

for all m∈Cm \in \mathcal{C} and i∈Ni \in N. Then (σ′,τ′′,β′)(\sigma', \tau'', \beta') is also an equilibrium.

Proof. Equilibrium conditions 3 and 4 are unchanged because the sender's strategy and the belief system are identical to those in the original equilibrium. Condition 2 also remains true: if τ′′(i∣m)>0\tau''(i \mid m) > 0, then i∈supp τ′(⋅∣m)i \in \text{supp } \tau'(\cdot \mid m); since (σ′,τ′,β′)(\sigma', \tau', \beta') is an equilibrium, (σ′,τ′′,β′)(\sigma', \tau'', \beta') must also satisfy condition 2.

It remains to verify condition 1. To simplify notation, for each message mm, let

w′(m)≔∑i∈Nτ′(i∣m)ui,andw′′(m)≔∑i∈Nτ′′(i∣m)ui.w'(m) := \sum_{i \in N} \tau'(i \mid m) u_i, \quad \text{and} \quad w''(m) := \sum_{i \in N} \tau''(i \mid m) u_i.

Because the receiver is only indifferent between actions ii and i+1i + 1 when the expected state after seeing a message is exactly γi+1\gamma_{i+1}, for every message mm, supp τ′(⋅∣m)\text{supp } \tau'(\cdot \mid m) is either a singleton {i}\{i\} or a pair of adjacent actions {i,i+1}\{i, i + 1\}.

Define a function c:[0,un]→[0,un]c : [0, u_n] \rightarrow [0, u_n] by c(z)≔umin⁡{k∈N:z≤uk}c(z) := u_{\min\{k \in N: z \leq u_k\}}. Because uiu_i is strictly increasing in ii, cc is increasing. For every message mm we have w′′(m)=c(w′(m))w''(m) = c(w'(m)): indeed, if supp τ′(⋅∣m)={i}\text{supp } \tau'(\cdot \mid m) = \{i\}, then w′(m)=uiw'(m) = u_i and w′′(m)=ui=c(w′(m))w''(m) = u_i = c(w'(m)); if supp τ′(⋅∣m)={i,i+1}\text{supp } \tau'(\cdot \mid m) = \{i, i + 1\}, then w′(m)∈(ui,ui+1)w'(m) \in (u_i, u_{i+1}) and w′′(m)=ui+1=c(w′(m))w''(m) = u_{i+1} = c(w'(m)).

Now fix ω∈Ω\omega \in \Omega. Since (σ′,τ′,β′)(\sigma', \tau', \beta') is an equilibrium,

supp σ′(ω)⊆arg⁡max⁡m∈M(ω)w′(m).\text{supp } \sigma'(\omega) \subseteq \arg \max_{m \in M(\omega)} w'(m).

Because cc is increasing,

arg⁡max⁡m∈M(ω)w′(m)⊆arg⁡max⁡m∈M(ω)c(w′(m))=arg⁡max⁡m∈M(ω)w′′(m).\arg \max_{m \in M(\omega)} w'(m) \subseteq \arg \max_{m \in M(\omega)} c(w'(m)) = \arg \max_{m \in M(\omega)} w''(m).

Therefore

supp σ′(ω)⊆arg⁡max⁡m∈M(ω)w′′(m),\text{supp } \sigma'(\omega) \subseteq \arg \max_{m \in M(\omega)} w''(m),

so condition 1 also holds for (σ′,τ′′,β′)(\sigma', \tau'', \beta'). Thus, (σ′,τ′′,β′)(\sigma', \tau'', \beta') is an equilibrium. ■\blacksquare

A.1.3 Proof of Theorem 1

Proof of Part (a). First, observe that the fully revealing partition A\mathcal{A} is obedient and revelation-proof since Ai=[γi,γi+1]A_i = [\gamma_i, \gamma_{i+1}] for each i∈Ni \in N. By Lemma 1, it is an equilibrium partition. Next, we show that the sender's ex-ante payoff cannot be lower than V‾\underline{V} in any other equilibrium. Let w‾(ω)≔min⁡{ui:i∈N,ω∈Ai}\underline{w}(\omega) := \min\{u_i : i \in N, \omega \in A_i\} be the sender's payoff in state ω\omega when the receiver knows the state and breaks ties in the sender-adversarial manner. By definition, ∫Ωw‾(ω)dF(ω)=∑i∈NμF(Ai)ui=V‾\int_{\Omega} \underline{w}(\omega) dF(\omega) = \sum_{i \in N} \mu_F(A_i) u_i = \underline{V}. If the sender's ex-ante payoff is strictly below V‾\underline{V} in an equilibrium, then his interim payoff is strictly below w‾(ω)\underline{w}(\omega) in a positive measure of states. Then, in each of those states, the sender has a profitable deviation toward sending message {ω}\{\omega\} and receiving w‾(ω)\underline{w}(\omega). Therefore, the sender's ex-ante payoff in a sender-worst equilibrium is exactly V‾\underline{V}. This completes the proof of Part (a).

Proof of Part (b). We proceed in three steps. First, we show that if there exists a sender-preferred equilibrium, then there exists a sender-preferred laminar partitional equilibrium (Lemma 2). Second, we show that a sender-preferred laminar partitional equilibrium exists (Lemma 3). Third, we show that Vˉ>V‾\bar{V} > \underline{V} (Lemma 4).

Lemma 2. For any equilibrium in which the receiver plays pure strategy, there exists a laminar equilibrium partition that induces the same posterior mean distribution. Furthermore, if there exists a sender-preferred equilibrium, then there exists a sender-preferred laminar partitional equilibrium.

Proof of Lemma 2. Let (σ,τ,β)(\sigma, \tau, \beta) be an equilibrium in which the receiver plays pure strategies. For any state ω∈Ω\omega \in \Omega in which the sender mixes, i.e., ∣supp σ(⋅∣ω)∣>1|\text{supp } \sigma(\cdot | \omega)| > 1, since (σ,τ,β)(\sigma, \tau, \beta) is an equilibrium, there exists i∈Ni \in N such that τ(i∣m)=τ(i∣m′)=1\tau(i | m) = \tau(i | m') = 1 for every m,m′∈supp σ(⋅∣ω)m, m' \in \text{supp } \sigma(\cdot | \omega). Thus, in every ω∈Ω\omega \in \Omega, there is an action ii played with probability 1 in this equilibrium. For every i∈Ni \in N, let

Wi≔{ω∈Ω:τ(i∣m)=1 for all m∈supp σ(⋅∣ω)}.W_i := \{\omega \in \Omega: \tau(i | m) = 1 \text{ for all } m \in \text{supp } \sigma(\cdot | \omega)\}.

By construction, ∪i∈NWi=Ω\cup_{i \in N} W_i = \Omega, and Wi∩Wj=∅W_i \cap W_j = \emptyset for any i≠ji \neq j. By Theorem 1(a) of Titova and Zhang (2025), for every i∈Ni \in N, γ~i≔E[ω∣ω∈Wi]∈[γi,γi+1]\tilde{\gamma}_i := \mathbb{E}[\omega | \omega \in W_i] \in [\gamma_i, \gamma_{i+1}], and Wi⊆[0,γi+1]W_i \subseteq [0, \gamma_{i+1}].

Consider the PMD G~\tilde{G} with supp G~⊆{γ~i}i=1n\text{supp } \tilde{G} \subseteq \{\tilde{\gamma}_i\}_{i=1}^n whose probability mass function is given by g~(γ~i)=μF(Wi)\tilde{g}(\tilde{\gamma}_i) = \mu_F(W_i). By construction, G~\tilde{G} is a mean-preserving contraction of the PMD induced by the equilibrium (σ,τ,β)(\sigma, \tau, \beta). Since the PMD induced by an equilibrium is itself a mean-preserving contraction of FF, G~\tilde{G} is a mean-preserving contraction of FF with ∣supp(G~)∣≤n|\text{supp}(\tilde{G})| \leq n. Then by Claim 2, G~\tilde{G} is also induced by a laminar partition B\mathcal{B} with generic element BiB_i. By construction, for every i∈Ni \in N, E[ω∣ω∈Bi]=γ~i\mathbb{E}[\omega | \omega \in B_i] = \tilde{\gamma}_i, which implies obedience. Also by construction, μF(Bi)=μF(Wi)\mu_F(B_i) = \mu_F(W_i) for each i∈Ni \in N.

We show next that B\mathcal{B} is also revelation-proof, i.e., Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}] for all i∈Ni \in N. Fix i∈Ni \in N. Because B\mathcal{B} is laminar, there exists k≤ik \leq i such that for every action j∈{k,…,i}j \in \{k, \dots, i\}, co(Bj)⊆co(Bi)\text{co}(B_j) \subseteq \text{co}(B_i); and for every action j∈{1,…,k−1,i+1,…,n}j \in \{1, \dots, k-1, i+1, \dots, n\}, μF(Bj∩co(Bi))=0\mu_F(B_j \cap \text{co}(B_i)) = 0. This implies that B^i≔Bk∪⋯∪Bi=co(Bi)\hat{B}_i := B_k \cup \dots \cup B_i = \text{co}(B_i) is an interval. Let W^i≔Wk∪⋯∪Wi\hat{W}_i := W_k \cup \dots \cup W_i. Since for each j=k,…,ij = k, \dots, i, μF(Bj)=μF(Wj)\mu_F(B_j) = \mu_F(W_j) and E[ω∣ω∈Bj]=E[ω∣ω∈Wj]\mathbb{E}[\omega | \omega \in B_j] = \mathbb{E}[\omega | \omega \in W_j], and since Wj∩Wℓ=∅W_j \cap W_\ell = \emptyset and μF(Bj∩Bℓ)=0\mu_F(B_j \cap B_\ell) = 0 for any j≠ℓj \neq \ell, we have μF(B^i)=μF(W^i)\mu_F(\hat{B}_i) = \mu_F(\hat{W}_i) and E[ω∣ω∈B^i]=E[ω∣ω∈W^i]\mathbb{E}[\omega | \omega \in \hat{B}_i] = \mathbb{E}[\omega | \omega \in \hat{W}_i]. By Claim 3, we have B^i⊆co(W^i)⊆[0,γi+1]\hat{B}_i \subseteq \text{co}(\hat{W}_i) \subseteq [0, \gamma_{i+1}], where the last inclusion follows since Wi⊆[0,γi+1]W_i \subseteq [0, \gamma_{i+1}] for all i∈Ni \in N.

To prove the second statement, suppose that there exists a sender-preferred equilibrium. An immediate consequence of Claim 4 is that in a sender-preferred equilibrium, the receiver mixes on a null set of states. Therefore, we can focus on a sender-preferred equilibrium (σ,τ,β)(\sigma, \tau, \beta) in which the receiver breaks ties in favor of the sender. Then by the first statement, there must exist a sender-preferred laminar equilibrium partition. ■

Lemma 3. Among all obedient and revelation-proof laminar partitions, there is one that maximizes the sender's ex-ante payoff.

Proof. The problem of finding a laminar partitional equilibrium that maximizes the sender's ex-ante payoff can be written as

max⁡B laminar∑i∈NuiμF(Bi)s.t.⋃i∈NBi=[0,1]μF(Bi∩Bj)=∅ for all i≠jγi≤E[ω∣ω∈Bi]≤γi+1 for all i∈NBi⊆[0,γi+1] for all i∈N\begin{aligned} & \max_{\mathcal{B} \text{ laminar}} \sum_{i \in N} u_i \mu_F(B_i) \\ & \text{s.t.} \quad \bigcup_{i \in N} B_i = [0, 1] \\ & \quad \mu_F(B_i \cap B_j) = \emptyset \text{ for all } i \neq j \\ & \quad \gamma_i \leq \mathbb{E}[\omega \mid \omega \in B_i] \leq \gamma_{i+1} \text{ for all } i \in N \\ & \quad B_i \subseteq [0, \gamma_{i+1}] \text{ for all } i \in N \end{aligned}

To prove the lemma, it suffices to show that this problem has a solution, by Lemma 2.

Although an action jj may be never recommended, one can still assume that BjB_j is nonempty by setting μF(Bj)=0\mu_F(B_j) = 0. Because B\mathcal{B} is laminar, it is without loss of generality to assume that for each i∈Ni \in N, BiB_i is the union of at most nn intervals (cf. Observation 1). Consequently, adding singletons if necessary, one can always set BiB_i as the union of exactly nn convex sets {Bi,s}s=1n\{B_{i,s}\}_{s=1}^n such that μF(Bi,s′∩Bi,s′′)=0\mu_F(B_{i,s'} \cap B_{i,s''}) = 0 for all s′≠s′′s' \neq s''.

Let Cc([0,1])\mathcal{C}_c([0, 1]) denote the set of closed, nonempty, and convex subsets of [0,1][0, 1] endowed with the Hausdorff distance; to simplify notation, we write Cc\mathcal{C}_c henceforth. By Proposition 1 in Ely (2022), Cc\mathcal{C}_c is compact; by Tychonoff's theorem, Ccn2\mathcal{C}_c^{n^2} is compact in the product topology. The problem above can be transformed to

max⁡{Bi,s}∈Ccn2∑i∈Nui∑s=1nμF(Bi,s)s.t.⋃i,sBi,s=[0,1]μF(Bi′,s′∩Bi′′,s′′)=0 for all (i′,s′)≠(i′′,s′′)μF(⋃s=1nBi,s)γi≤∫⋃s=1nBi,sωdμF(ω)≤μF(⋃s=1nBi,s)γi+1⋃s=1nBi,s⊆[0,γi+1](5)\begin{aligned} & \max_{\{B_{i,s}\} \in \mathcal{C}_c^{n^2}} \sum_{i \in N} u_i \sum_{s=1}^n \mu_F(B_{i,s}) \\ & \text{s.t.} \quad \bigcup_{i,s} B_{i,s} = [0, 1] \\ & \quad \mu_F(B_{i',s'} \cap B_{i'',s''}) = 0 \text{ for all } (i', s') \neq (i'', s'') \\ & \quad \mu_F(\bigcup_{s=1}^n B_{i,s}) \gamma_i \leq \int_{\bigcup_{s=1}^n B_{i,s}} \omega d\mu_F(\omega) \leq \mu_F(\bigcup_{s=1}^n B_{i,s}) \gamma_{i+1} \\ & \quad \bigcup_{s=1}^n B_{i,s} \subseteq [0, \gamma_{i+1}] \end{aligned} \tag{5}

where the third constraint is equivalent to the conditional mean condition.

Define

D={{Bi,s}∈Ccn2:⋃i,sBi,s=[0,1], and μF(Bi′,s′∩Bi′′,s′′)=0 for all (i′,s′)≠(i′′,s′′)};\mathcal{D} = \left\{ \{B_{i,s}\} \in \mathcal{C}_c^{n^2} : \bigcup_{i,s} B_{i,s} = [0, 1], \text{ and } \mu_F(B_{i',s'} \cap B_{i'',s''}) = 0 \text{ for all } (i', s') \neq (i'', s'') \right\};

We claim that D\mathcal{D} is compact. To show this, it is enough to show that D\mathcal{D} is a closed subset of Ccn2\mathcal{C}_c^{n^2}. Take any {Bi,sm}\{B_{i,s}^m\} that converges to {Bi,s}\{B_{i,s}\} in the product topology, then Bi,sm→Bi,sB_{i,s}^m \rightarrow B_{i,s} for each ii and ss. Consequently, because the limit of convergence in Hausdorff distance is preserved under finite unions,22 ∪i,sBi,sm→∪i,sBi,s\cup_{i,s} B_{i,s}^m \rightarrow \cup_{i,s} B_{i,s}. Therefore, if ∪i,sBi,sm=[0,1]\cup_{i,s} B_{i,s}^m = [0, 1], it must be that ∪i,sBi,s=[0,1]\cup_{i,s} B_{i,s} = [0, 1]. Furthermore, if μF(Bi′,s′m∩Bi′′,s′′m)=0\mu_F(B_{i',s'}^m \cap B_{i'',s''}^m) = 0 for all mm and (i′,s′)≠(i′′,s′′)(i', s') \neq (i'', s''), the same argument as the second paragraph in the proof of Lemma 2 in Ely (2022) shows that μF(Bi′,s′∩Bi′′,s′′)=0\mu_F(B_{i',s'} \cap B_{i'',s''}) = 0 for all (i′,s′)≠(i′′,s′′)(i', s') \neq (i'', s''). Therefore, if {Bi,sm}∈D\{B_{i,s}^m\} \in \mathcal{D} for each mm and {Bi,sm}→{Bi,s}\{B_{i,s}^m\} \rightarrow \{B_{i,s}\}, it must be that {Bi,s}∈D\{B_{i,s}\} \in \mathcal{D}. Thus, D\mathcal{D} is a closed subset of Ccn2\mathcal{C}_c^{n^2}.

Problem (5) is equivalent to

max⁡{Bi,s}∈D∑i∈Nui∑s=1nμF(Bi,s)(6)\max_{\{B_{i,s}\} \in \mathcal{D}} \sum_{i \in N} u_i \sum_{s=1}^n \mu_F(B_{i,s}) \quad (6)
s.t.(∑s=1nμF(Bi,s))γi≤∑s=1n∫Bi,sω dμF(ω)≤(∑s=1nμF(Bi,s))γi+1(7)\text{s.t.} \quad \left( \sum_{s=1}^n \mu_F(B_{i,s}) \right) \gamma_i \leq \sum_{s=1}^n \int_{B_{i,s}} \omega \, d\mu_F(\omega) \leq \left( \sum_{s=1}^n \mu_F(B_{i,s}) \right) \gamma_{i+1} \quad (7)
∪s=1nBi,s⊆[0,γi+1](8)\cup_{s=1}^n B_{i,s} \subseteq [0, \gamma_{i+1}] \quad (8)

where constraint (7) supersedes the third constraint in problem (5) because for any {Bi,s}∈D\{B_{i,s}\} \in \mathcal{D}, μF(Bi′,s′∩Bi′′,s′′)=0\mu_F(B_{i',s'} \cap B_{i'',s''}) = 0 for all (i′,s′)≠(i′′,s′′)(i', s') \neq (i'', s'').

By the extreme value theorem, to show that a solution to problem (6) exists, it suffices to show that (i) the objective function is continuous, and (ii) the constraint set is nonempty and compact. Clearly, the constraint set is nonempty: for each i∈Ni \in N, consider

Bi,1=Ai, and Bi,s={γi+1} for all s=2,…,n,B_{i,1} = A_i, \text{ and } B_{i,s} = \{\gamma_{i+1}\} \text{ for all } s = 2, \dots, n,

then {Bi,s}\{B_{i,s}\} is feasible for this problem. Furthermore, by Proposition 1 in Ely (2022), μF\mu_F is continuous on Cc\mathcal{C}_c, and hence the objective is continuous.

Since D\mathcal{D} is compact, to show that the constraint set is compact, it suffices to show that each of the constraints, (7) and (8), defines a closed subset of D\mathcal{D}. Observe that if Cm→CC^m \rightarrow C and Dm→DD^m \rightarrow D with Cm⊆DmC^m \subseteq D^m for all mm, then C⊆DC \subseteq D.23 Then because the limit of convergence in Hausdorff distance is preserved under finite unions, if ∪s=1nBi,sm⊆[0,γi+1]\cup_{s=1}^n B_{i,s}^m \subseteq [0, \gamma_{i+1}] for each ii, it must be that ∪s=1nBi,s⊆[0,γi+1]\cup_{s=1}^n B_{i,s} \subseteq [0, \gamma_{i+1}] for each ii. Hence, (8) defines a closed subset of D\mathcal{D}.

Next, we show that (7) does the same, which is equivalent to showing that if {Bi,sm}→{Bi,s}\{B_{i,s}^m\} \rightarrow \{B_{i,s}\} where {Bi,sm}∈D\{B_{i,s}^m\} \in \mathcal{D} for each mm, then

(∑s=1nμF(Bi,sm))γi≤∑s=1n∫Bi,smω dμF(ω)≤(∑s=1nμF(Bi,sm))γi+1\left( \sum_{s=1}^n \mu_F(B_{i,s}^m) \right) \gamma_i \leq \sum_{s=1}^n \int_{B_{i,s}^m} \omega \, d\mu_F(\omega) \leq \left( \sum_{s=1}^n \mu_F(B_{i,s}^m) \right) \gamma_{i+1}

for all mm and ii implies that

(∑s=1nμF(Bi,s))γi≤∑s=1n∫Bi,sω dμF(ω)≤(∑s=1nμF(Bi,s))γi+1\left( \sum_{s=1}^n \mu_F(B_{i,s}) \right) \gamma_i \leq \sum_{s=1}^n \int_{B_{i,s}} \omega \, d\mu_F(\omega) \leq \left( \sum_{s=1}^n \mu_F(B_{i,s}) \right) \gamma_{i+1}

for all ii. Because μF\mu_F is continuous on Cc\mathcal{C}_c, ∑s=1nμF(Bi,sm)→∑s=1nμF(Bi,s)\sum_{s=1}^n \mu_F(B_{i,s}^m) \rightarrow \sum_{s=1}^n \mu_F(B_{i,s}) for all ii. Consequently, (∑s=1nμF(Bi,sm))γi→(∑s=1nμF(Bi,s))γi(\sum_{s=1}^n \mu_F(B_{i,s}^m)) \gamma_i \rightarrow (\sum_{s=1}^n \mu_F(B_{i,s})) \gamma_i, and (∑s=1nμF(Bi,sm))γi+1→(∑s=1nμF(Bi,s))γi+1(\sum_{s=1}^n \mu_F(B_{i,s}^m)) \gamma_{i+1} \rightarrow (\sum_{s=1}^n \mu_F(B_{i,s})) \gamma_{i+1} for each ii. Therefore, it only remains to show that

∑s=1n∫Bi,smω dμF(ω)→∑s=1n∫Bi,sω dμF(ω),\sum_{s=1}^n \int_{B_{i,s}^m} \omega \, d\mu_F(\omega) \rightarrow \sum_{s=1}^n \int_{B_{i,s}} \omega \, d\mu_F(\omega),

which is a consequence of E↦∫Eω dμF(ω)E \mapsto \int_E \omega \, d\mu_F(\omega) being continuous on Cc\mathcal{C}_c.

To prove this claim, we show that E↦∫Eω dμF(ω)E \mapsto \int_E \omega \, d\mu_F(\omega) is both upper- and lower-semicontinuous. To see that it is upper-semicontinuous, pick any ε>0\varepsilon > 0, and let E∈CcE \in \mathcal{C}_c; we show that there exists δ>0\delta > 0 such that for every E′∈N(E,δ)E' \in N(E, \delta), where N(E,δ)N(E, \delta) is the δ\delta -neighborhood of EE, ∫E′ω dμF(ω)<∫Eω dμF(ω)+ε\int_{E'} \omega \, d\mu_F(\omega) < \int_E \omega \, d\mu_F(\omega) + \varepsilon. Because E∈CcE \in \mathcal{C}_c, there exist a,b∈[0,1]a, b \in [0, 1] such that E=[a,b]E = [a, b]. The key observation here is that for any E′∈N(E,δ)E' \in N(E, \delta), it must be that E′⊆[a−δ,b+δ]E' \subseteq [a - \delta, b + \delta]. Then

∫a−δb+δω dμF(ω)=∫a−δaω dμF(ω)+∫abω dμF(ω)+∫bb+δω dμF(ω)≤μF([a−δ,a])+∫Eω dμF(ω)+μF([b,b+δ])\begin{aligned} \int_{a-\delta}^{b+\delta} \omega \, d\mu_F(\omega) &= \int_{a-\delta}^a \omega \, d\mu_F(\omega) + \int_a^b \omega \, d\mu_F(\omega) + \int_b^{b+\delta} \omega \, d\mu_F(\omega) \\ &\leq \mu_F([a - \delta, a]) + \int_E \omega \, d\mu_F(\omega) + \mu_F([b, b + \delta]) \end{aligned}

where the inequality holds because ω∈[0,1]\omega \in [0, 1]. For δ\delta small enough, since μF\mu_F is absolutely continuous with respect to the Lebesgue measure,

∫E′ω dμF(ω)≤∫a−δb+δω dμF(ω)<∫Eω dμF(ω)+ε.\int_{E'} \omega \, d\mu_F(\omega) \leq \int_{a-\delta}^{b+\delta} \omega \, d\mu_F(\omega) < \int_E \omega \, d\mu_F(\omega) + \varepsilon.

Next, we show that ∫Eω dμF(ω)\int_E \omega \, d\mu_F(\omega) is lower semicontinuous, that is, there exists δ>0\delta > 0 such that for every E′∈N(E,δ)E' \in N(E, \delta), ∫E′ω dμF(ω)>∫Eω dμF(ω)−ε\int_{E'} \omega \, d\mu_F(\omega) > \int_E \omega \, d\mu_F(\omega) - \varepsilon. Without loss of generality, assume δ<(b−a)/2\delta < (b - a)/2. Consequently, [a+δ,b−δ][a + \delta, b - \delta] is an interval of positive measure, and for any E′∈N(E,δ)E' \in N(E, \delta), [a+δ,b−δ]⊆E′[a + \delta, b - \delta] \subseteq E'. Then

∫a+δb−δω dμF(ω)=∫abω dμF(ω)−∫aa+δω dμF(ω)−∫b−δbω dμF(ω)≥∫Eω dμF(ω)−μF([a,a+δ])−μF([b−δ,b])\begin{aligned} \int_{a+\delta}^{b-\delta} \omega \, d\mu_F(\omega) &= \int_a^b \omega \, d\mu_F(\omega) - \int_a^{a+\delta} \omega \, d\mu_F(\omega) - \int_{b-\delta}^b \omega \, d\mu_F(\omega) \\ &\geq \int_E \omega \, d\mu_F(\omega) - \mu_F([a, a + \delta]) - \mu_F([b - \delta, b]) \end{aligned}

where the inequality follows from the fact that ω≥a\omega \geq a on [a,b][a, b]. Consequently, ∫Eω dμF(ω)\int_E \omega \, d\mu_F(\omega) is both upper- and lower-semicontinuous, and hence continuous. This completes the proof. ■\blacksquare

Let B\mathcal{B} denote a laminar partition associated with a sender-preferred equilibrium; by the previous two lemmas, such a partition exists. Denote the sender's ex-ante payoff from B\mathcal{B} by Vˉ\bar{V}.

Lemma 4. Vˉ>V‾\bar{V} > \underline{V}.

Proof. Let ε∈(0,γ2)\varepsilon \in (0, \gamma_2). Also, for each i∈N∖{1,n}i \in N \setminus \{1, n\}, let Biε=AiB_i^\varepsilon = A_i, B1ε=[ε,γ2]B_1^\varepsilon = [\varepsilon, \gamma_2] and Bnε=[0,ε]∪AnB_n^\varepsilon = [0, \varepsilon] \cup A_n. It is easy to see that B(ε)≔{Biε}i∈N\mathcal{B}(\varepsilon) := \{B_i^\varepsilon\}_{i \in N} is a revelation-proof partition. Furthermore, E[ω∣ω∈Biε]∈Ai\mathbb{E}[\omega \mid \omega \in B_i^\varepsilon] \in A_i for all i∈N∖{n}i \in N \setminus \{n\} by construction. Finally, the function ψ(ε)≔E[ω∣ω∈Bnε]\psi(\varepsilon) := \mathbb{E}[\omega \mid \omega \in B_n^\varepsilon] is continuous at 0 and ψ(0)>γn\psi(0) > \gamma_n. Consequently, there exists ε′>0\varepsilon' > 0 sufficiently small such that ψ(ε′)∈[γn,1]\psi(\varepsilon') \in [\gamma_n, 1], which makes B(ε′)\mathcal{B}(\varepsilon') an obedient partition. By Lemma 1, B(ε′)\mathcal{B}(\varepsilon') is an equilibrium partition; the sender's ex-ante payoff in that equilibrium is

V(B(ε′))=V‾+μF([0,ε′])(un−u1)>V‾,V(\mathcal{B}(\varepsilon')) = \underline{V} + \mu_F([0, \varepsilon'])(u_n - u_1) > \underline{V},

which completes the proof. ■\blacksquare

Proof of Part (c). For any V∈[V‾,Vˉ]V \in [\underline{V}, \bar{V}], we construct an obedient and revelation-proof laminar partition that yields VV by “blending” the fully informative partition A\mathcal{A} and a sender-preferred laminar equilibrium partition B\mathcal{B} (which exists by part (b)). For all z∈[0,γn]z \in [0, \gamma_n],

  • for every i∈Ni \in N such that γi+1≤z\gamma_{i+1} \leq z, let B^iz≔Ai\hat{B}_i^z := A_i;
  • if ii is such that γi≤z≤γi+1\gamma_i \leq z \leq \gamma_{i+1}, B^iz≔cl(Bi∖[0,γi])∪[γi,z]\hat{B}_i^z := \text{cl}(B_i \setminus [0, \gamma_i]) \cup [\gamma_i, z];
  • for every i∈Ni \in N such that z<γiz < \gamma_i, let B^iz≔cl(Bi∖[0,z])\hat{B}_i^z := \text{cl}(B_i \setminus [0, z]).

For any z∈[0,γn]z \in [0, \gamma_n], and any i∈Ni \in N, E[ω∣ω∈Bi]∈Ai\mathbb{E}[\omega \mid \omega \in B_i] \in A_i implies E[ω∣ω∈B^iz]∈Ai\mathbb{E}[\omega \mid \omega \in \hat{B}_i^z] \in A_i. Consequently, B^(z)≔{B^iz}i=1n\hat{\mathcal{B}}(z) := \{\hat{B}_i^z\}_{i=1}^n is obedient. It is also revelation-proof because both A\mathcal{A} and B\mathcal{B} are. Finally, because both A\mathcal{A} and B\mathcal{B} are laminar, it can be checked using (1) that B^(z)\hat{\mathcal{B}}(z) is a laminar partition.

Let V(z)V(z) denote the sender's ex-ante payoff from B^(z)\hat{\mathcal{B}}(z): V(z)≔∑i∈NuiμF(B^iz)V(z) := \sum_{i \in N} u_i \mu_F(\hat{B}_i^z); because f>0f > 0, V(z)V(z) is continuous in zz. Since V(0)=Vˉ≥V≥V‾=V(γn)V(0) = \bar{V} \geq V \geq \underline{V} = V(\gamma_n), by the intermediate value theorem, there exists zV∈[0,γn]z^V \in [0, \gamma_n] such that V(zV)=VV(z^V) = V. Thus, the partition B^(zV)\hat{\mathcal{B}}(z^V) is an obedient and revelation-proof laminar partition that yields VV.

A.1.4 Proof of Theorem 2

To establish Theorem 2, we first prove the following two preliminary results.

Claim 5. Let B\mathcal{B} be a laminar partition associated with a sender-preferred equilibrium, and let j=min⁡{i:μF(Bi)>0}j = \min\{i : \mu_F(B_i) > 0\}. If E[ω∣ω∈Bj]>γj\mathbb{E}[\omega \mid \omega \in B_j] > \gamma_j, then Bj=[0,d]B_j = [0, d] for some d≤γj+1d \leq \gamma_{j+1}.

Proof. Because B\mathcal{B} is a laminar partition, BjB_j must be an interval, and hence one can write Bj=[b‾j,bˉj]B_j = [\underline{b}_j, \bar{b}_j]. Furthermore, revelation proofness implies that [b‾j,bˉj]⊆[0,γj+1][\underline{b}_j, \bar{b}_j] \subseteq [0, \gamma_{j+1}].

To show that b‾j=0\underline{b}_j = 0, it suffices to show that int(Bj)∩co(Bk)=∅\text{int}(B_j) \cap \text{co}(B_k) = \emptyset for all k>jk > j.24 Suppose not, so Bj⊆co(Bk)B_j \subseteq \text{co}(B_k) for some k>jk > j. The laminar structure implies that BkB_k is the union of at most kk closed intervals; let [α,β][\alpha, \beta] be an interval such that β≤bˉj\beta \leq \bar{b}_j and [α,β]⊆Bk[\alpha, \beta] \subseteq B_k; this interval is well-defined because B\mathcal{B} is laminar and Bj⊆co(Bk)B_j \subseteq \text{co}(B_k). Because E[ω∣ω∈Bk]=γk\mathbb{E}[\omega \mid \omega \in B_k] = \gamma_k and E[ω∣ω∈Bj]≔γS>γj\mathbb{E}[\omega \mid \omega \in B_j] := \gamma_S > \gamma_j, for small enough ε>0\varepsilon > 0, one can find h(ε)h(\varepsilon) such that

E[ω∣ω∈(Bk∪[bˉj−h(ε),bˉj])∖(β−ε,β)]=γk,\mathbb{E}[\omega \mid \omega \in (B_k \cup [\bar{b}_j - h(\varepsilon), \bar{b}_j]) \setminus (\beta - \varepsilon, \beta)] = \gamma_k,

and

E[ω∣ω∈[β−ε,β]∪[b‾j,bˉj−h(ε)]]≥γj.\mathbb{E}\left[\omega \mid \omega \in [\beta - \varepsilon, \beta] \cup [\underline{b}_j, \bar{b}_j - h(\varepsilon)]\right] \geq \gamma_j.

Now define a new partition B~\tilde{\mathcal{B}} with generic element B~i\tilde{B}_i by B~i=Bi\tilde{B}_i = B_i if i≠j,ki \neq j, k, B~j=[β−ε,β]∪[b‾j,bˉj−h(ε)]\tilde{B}_j = [\beta - \varepsilon, \beta] \cup [\underline{b}_j, \bar{b}_j - h(\varepsilon)], and B~k=(Bk∪[bˉj−h(ε),bˉj])∖(β−ε,β)\tilde{B}_k = (B_k \cup [\bar{b}_j - h(\varepsilon), \bar{b}_j]) \setminus (\beta - \varepsilon, \beta). B~\tilde{\mathcal{B}} is obedient by construction, and it is also revelation-proof because B\mathcal{B} is; then by Lemma 1, B~\tilde{\mathcal{B}} is an equilibrium partition. Furthermore, it must be that μF(B~k)>μF(Bk)\mu_F(\tilde{B}_k) > \mu_F(B_k): this is because by construction, E[ω∣ω∈Bk]=E[ω∣ω∈B~k]=γk\mathbb{E}[\omega \mid \omega \in B_k] = \mathbb{E}[\omega \mid \omega \in \tilde{B}_k] = \gamma_k and ∫B~kωdF(ω)>∫BkωdF(ω)\int_{\tilde{B}_k} \omega dF(\omega) > \int_{B_k} \omega dF(\omega). Consequently, the sender's payoff is strictly higher in this new equilibrium since j<kj < k, which contradicts the assumption that B\mathcal{B} is a partition associated with a sender-preferred equilibrium. ■

Claim 6. Let B\mathcal{B} be a barely obedient laminar partition, and let i,ji, j be two unskipped actions with j<ij < i. Then if μF(co(Bi)∩co(Bj))=0\mu_F(\text{co}(B_i) \cap \text{co}(B_j)) = 0, then every ω′∈Bj\omega' \in B_j and ω′′∈Bi\omega'' \in B_i satisfy ω′≤ω′′\omega' \leq \omega''.

Proof of Claim 6. Because μF(co(Bi)∩co(Bj))=0\mu_F(\text{co}(B_i) \cap \text{co}(B_j)) = 0, either ω′≤ω′′\omega' \leq \omega'' for every ω′∈Bj\omega' \in B_j and ω′′∈Bi\omega'' \in B_i, or ω′≥ω′′\omega' \geq \omega'' for every ω′∈Bj\omega' \in B_j and ω′′∈Bi\omega'' \in B_i. The second possibility, however, cannot be true: by obedience, j<ij < i implies that b‾j≤γi\underline{b}_j \leq \gamma_i, and E[ω∣ω∈Bi]≥γi\mathbb{E}[\omega \mid \omega \in B_i] \geq \gamma_i. Consequently, bˉi>γi≥b‾j\bar{b}_i > \gamma_i \geq \underline{b}_j, a contradiction. Therefore, it must be that ω′≤ω′′\omega' \leq \omega'' for every ω′∈Bj\omega' \in B_j and ω′′∈Bi\omega'' \in B_i. ■

We are now ready to prove Theorem 2.

Proof of Theorem 2. We first show that B\mathcal{B} must be barely obedient. Suppose to the contrary that B\mathcal{B}, a laminar partition associated with a sender-preferred equilibrium, has E[ω∣ω∈Bk]>γk\mathbb{E}[\omega \mid \omega \in B_k] > \gamma_k for some non-null k>jk > j. By Lemma 1, B\mathcal{B} is both obedient and revelation-proof. Let b‾j≔min⁡Bj\underline{b}_j := \min B_j; because f>0f > 0, there exists x∈Bjx \in B_j with x>b‾jx > \underline{b}_j such that E[ω∣ω∈[b‾j,x]∪Bk]≥γk\mathbb{E}[\omega \mid \omega \in [\underline{b}_j, x] \cup B_k] \geq \gamma_k, and E[ω∣ω∈Bj∖[b‾j,x]]>γj\mathbb{E}[\omega \mid \omega \in B_j \setminus [\underline{b}_j, x]] > \gamma_j. Now consider the partition B~\tilde{\mathcal{B}} where B~j=Bj∖[b‾j,x]\tilde{B}_j = B_j \setminus [\underline{b}_j, x], B~k=[b‾j,x]∪Bk\tilde{B}_k = [\underline{b}_j, x] \cup B_k, and B~i=Bi\tilde{B}_i = B_i for i≠j,ki \neq j, k. B~\tilde{\mathcal{B}} is obedient and revelation-proof because B\mathcal{B} is, and the sender's ex-ante payoff from B~\tilde{\mathcal{B}}, V(B~)V(\tilde{\mathcal{B}}), satisfies

V(B~)−Vˉ=[F(x)−F(b‾j)](uk−uj)>0,V(\tilde{\mathcal{B}}) - \bar{V} = [F(x) - F(\underline{b}_j)](u_k - u_j) > 0,

a contradiction.

Next, we show that BiB_i is the union of at most max⁡{i−1,1}\max\{i - 1, 1\} closed intervals for all i∈Ni \in N. Recall that a laminar partition is defined by (1). Because co(Bk)\text{co}(B_k) must be an interval for all kk, ∪k<ico(Bk)\cup_{k < i} \text{co}(B_k) is the union of at most i−1i - 1 intervals. By Claim 5, since B\mathcal{B} is associated with a sender-preferred equilibrium, int(B1)∩Bk=∅\text{int}(B_1) \cap B_k = \emptyset for all k≥2k \geq 2. Thus, for any i≥2i \geq 2, by taking out ∪k<ico(Bk)\cup_{k < i} \text{co}(B_k) from co(Bi)\text{co}(B_i), at most i−2i - 2 intervals are removed, and hence the remainder, namely co(Bi)∖∪k<ico(Bk)\text{co}(B_i) \setminus \cup_{k < i} \text{co}(B_k), must be the union of at most max⁡{i−1,1}\max\{i - 1, 1\} intervals. By taking closure, BiB_i is also the union of at most max⁡{i−1,1}\max\{i - 1, 1\} intervals.

Finally, we prove the equivalence between revelation proofness of a barely obedient laminar partition B\mathcal{B} and the condition that max⁡Bi≤γi+1\max B_i \leq \gamma_{i+1} for all unskipped ii such that i+1i + 1 either nests ii or is skipped. For convenience, for any Bi∈BB_i \in \mathcal{B}, denote b‾i≔min⁡Bi\underline{b}_i := \min B_i and bˉi≔max⁡Bi\bar{b}_i := \max B_i.25

Suppose first that max⁡Bi≤γi+1\max B_i \leq \gamma_{i+1} for all unskipped ii such that i+1i + 1 either nests ii or is skipped, and we show that for any action i∈Ni \in N, Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}]. Since B\mathcal{B} is laminar, it is without loss of generality to assume that if action ii is skipped, Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}].

Now suppose ii is not skipped. There are two possibilities: either action i+1i + 1 is skipped or not. If i+1i + 1 is skipped, by assumption bˉi≤γi+1\bar{b}_i \leq \gamma_{i+1}, implying Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}]. If instead i+1i + 1 is not skipped, there are two cases: either Bi⊆co(Bi+1)B_i \subseteq \text{co}(B_{i+1}) or not. If Bi⊆co(Bi+1)B_i \subseteq \text{co}(B_{i+1}), then by assumption bˉi≤γi+1\bar{b}_i \leq \gamma_{i+1}, implying that Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}].

Suppose instead that BiB_i is not a subset of co(Bi+1)\text{co}(B_{i+1}), and suppose to the contrary that bˉi>γi+1\bar{b}_i > \gamma_{i+1}. Because B\mathcal{B} is laminar, since BiB_i is not a subset of co(Bi+1)\text{co}(B_{i+1}) (which means that co(Bi+1)\text{co}(B_{i+1}) does not nest co(Bi)\text{co}(B_i)), it must be that μF(co(Bi)∩co(Bi+1))=0\mu_F(\text{co}(B_i) \cap \text{co}(B_{i+1})) = 0. By Claim 6, for every ω′∈Bi\omega' \in B_i and every ω′′∈Bi+1\omega'' \in B_{i+1}, ω′≤ω′′\omega' \leq \omega''. This implies that ω≥bˉi>γi+1\omega \geq \bar{b}_i > \gamma_{i+1} for every ω∈Bi+1\omega \in B_{i+1}, violating bare obedience, a contradiction. Thus, bˉi≤γi+1\bar{b}_i \leq \gamma_{i+1}, which implies that Bi⊆[0,γi+1]B_i \subseteq [0, \gamma_{i+1}].

For the other direction, we prove the contrapositive. If the condition is violated, that is, if max⁡Bi>γi+1\max B_i > \gamma_{i+1} for some unskipped ii such that i+1i + 1 either nests ii or is skipped, then BiB_i is not a subset of [0,γi+1][0, \gamma_{i+1}]. Thus, B\mathcal{B} must violate revelation proofness. ■

A.2 Proofs and Details for Section 4

We first introduce the notion of a bi-pooling distribution.

Definition 4 (Bi-pooling distribution). A distribution G∈MPC(F)G \in \text{MPC}(F) is a bi-pooling distribution if there exists a collection of pairwise disjoint intervals {(ω‾i,ωˉi)}i∈I\{(\underline{\omega}_i, \bar{\omega}_i)\}_{i \in \mathcal{I}} such that

  • for all i∈Ii \in \mathcal{I}, G(ωˉi)−G(ω‾i)=F(ωˉi)−F(ω‾i)G(\bar{\omega}_i) - G(\underline{\omega}_i) = F(\bar{\omega}_i) - F(\underline{\omega}_i) and ∣supp(G∣(ω‾i,ωˉi))∣≤2|\text{supp}(G|_{(\underline{\omega}_i, \bar{\omega}_i)})| \leq 2;26
  • G∣[0,1]∖∪i∈I(ω‾i,ωˉi)=F∣[0,1]∖∪i∈I(ω‾i,ωˉi)G|_{[0,1] \setminus \cup_{i \in \mathcal{I}} (\underline{\omega}_i, \bar{\omega}_i)} = F|_{[0,1] \setminus \cup_{i \in \mathcal{I}} (\underline{\omega}_i, \bar{\omega}_i)}.

In particular, (ω‾i,ωˉi)(\underline{\omega}_i, \bar{\omega}_i) is called a pooling interval if ∣supp(G∣(ω‾i,ωˉi))∣=1|\text{supp}(G|_{(\underline{\omega}_i, \bar{\omega}_i)})| = 1, and it is called a bi-pooling interval if ∣supp(G∣(ω‾i,ωˉi))∣=2|\text{supp}(G|_{(\underline{\omega}_i, \bar{\omega}_i)})| = 2.

We call a bi-pooling distribution GBG_B that solves the commitment problem (3) a bi-pooling solution.

The following observation is useful.

Lemma 5 (Candogan, 2019). Every bi-pooling solution to the commitment problem satisfies supp(GB)⊆[0,γ~]∪{γi}i=2n\text{supp}(G_B) \subseteq [0, \tilde{\gamma}] \cup \{\gamma_i\}_{i=2}^n, where γ~∈[0,1]\tilde{\gamma} \in [0, 1] is such that γ~≤γ\tilde{\gamma} \leq \gamma for all γ∈supp(GB)∩{γi}i=2n\gamma \in \text{supp}(G_B) \cap \{\gamma_i\}_{i=2}^n.

An important consequence of Lemma 5 is that every signal realization can be identified by the action it induces. In particular, every x∈supp(GB)∩[0,γ~]x \in \text{supp}(G_B) \cap [0, \tilde{\gamma}] induces the lowest unskipped action, and γi\gamma_i induces action ii for each i=2,…,ni = 2, \dots, n. Moreover, if a bi-pooling solution is associated with a bi-pooling partition, then Lemma 5 implies that the partition must be barely obedient.

A.2.1 Proof of Theorem 3

By results in Kleiner et al. (2021) and Arieli et al. (2023), the commitment problem (3) admits a bi-pooling solution.

By Lemma 5, in any bi-pooling solution GBG_B, if supp(GB)∖{γi}i=2n\text{supp}(G_B) \setminus \{\gamma_i\}_{i=2}^n is nonempty but not a singleton, there must exist an interval [0,d][0, d] on which action 1 is recommended, and [d,1][d, 1] is comprised of pooling intervals and/or bi-pooling intervals; in this case, [0,d][0, d] can be viewed as a pooling interval. Otherwise, [0,1][0, 1] comprises pooling and/or bi-pooling intervals. The fact that every bi-pooling solution GBG_B is associated with a bi-pooling partition therefore follows from Lemma 4 in Arieli et al. (2023): on every pooling interval, a single signal realizes, which induces a single action and hence ties to a single partitional element. On every bi-pooling interval (ω‾,ωˉ)(\underline{\omega}, \bar{\omega}), there exists (q‾,qˉ)⊆(ω‾,ωˉ)(\underline{q}, \bar{q}) \subseteq (\underline{\omega}, \bar{\omega}) such that one (deterministic) signal realizes when ω∈(q‾,qˉ)\omega \in (\underline{q}, \bar{q}), and another signal realizes when ω∈(ω‾,q‾)∪(qˉ,ωˉ)\omega \in (\underline{\omega}, \underline{q}) \cup (\bar{q}, \bar{\omega}), with the latter signal recommending a higher action. Then [q‾,qˉ][\underline{q}, \bar{q}] and [ω‾,q‾]∪[qˉ,ωˉ][\underline{\omega}, \underline{q}] \cup [\bar{q}, \bar{\omega}] correspond to two partitional elements BℓB_\ell and BhB_h with ℓ<h\ell < h, respectively. This observation and Lemma 5 together imply that the bi-pooling partition is barely obedient.

Fix a bi-pooling solution GBG_B. To see that there is a unique barely obedient bi-pooling partition associated with it, we first note that every pooling interval necessarily ties to a unique partitional element. Hence, if a bi-pooling solution admits two distinct bi-pooling partitions, B1\mathcal{B}^1 and B2\mathcal{B}^2, they must differ on a bi-pooling interval (ω‾,ωˉ)(\underline{\omega}, \bar{\omega}). Then there must exist {Bℓ,Bh}\{B_\ell, B_h\} and {Bℓ′,Bh′}\{B'_\ell, B'_h\} such that Bℓ=[b‾ℓ,bˉℓ]B_\ell = [\underline{b}_\ell, \bar{b}_\ell], Bh=[ω‾,b‾ℓ]∪[bˉℓ,ωˉ]B_h = [\underline{\omega}, \underline{b}_\ell] \cup [\bar{b}_\ell, \bar{\omega}], Bℓ′=[b‾ℓ′,bˉℓ′]B'_\ell = [\underline{b}'_\ell, \bar{b}'_\ell], and Bh′=[ω‾,b‾ℓ′]∪[bˉℓ′,ωˉ]B'_h = [\underline{\omega}, \underline{b}'_\ell] \cup [\bar{b}'_\ell, \bar{\omega}], with either b‾ℓ′≠b‾ℓ\underline{b}'_\ell \neq \underline{b}_\ell, or bˉℓ′≠bˉℓ\bar{b}'_\ell \neq \bar{b}_\ell, or both. Since f>0f > 0 and ω‾\underline{\omega} and ωˉ\bar{\omega} are fixed, either E[ω∣ω∈Bℓ]≠γℓ\mathbb{E}[\omega \mid \omega \in B_\ell] \neq \gamma_\ell, or E[ω∣ω∈Bℓ′]≠γℓ\mathbb{E}[\omega \mid \omega \in B'_\ell] \neq \gamma_\ell, or both, a contradiction.

Finally, we show that the commitment solution is unique in generic communication environments. For any bi-pooling solution GBG_B, let μi≔GB(γi+1)−GB(γi)\mu_i := G_B(\gamma_{i+1}) - G_B(\gamma_i) for each i=2,…,ni = 2, \dots, n. If supp(GB)∖{γi}i=1n=∅\text{supp}(G_B) \setminus \{\gamma_i\}_{i=1}^n = \emptyset, set μ1=GB(γ2)\mu_1 = G_B(\gamma_2) and μ~=0\tilde{\mu} = 0; otherwise, let μ~=GB(γ~)\tilde{\mu} = G_B(\tilde{\gamma}) and μ1=GB(γ2)−μ~\mu_1 = G_B(\gamma_2) - \tilde{\mu}; Lemma 5 then indicates that every bi-pooling solution is identified by {μ~}∪{μi}i=1n\{\tilde{\mu}\} \cup \{\mu_i\}_{i=1}^n. By Lemma D.1 in Candogan (2022), the condition that no three elements of the collection of points {(γi,ui)}i=1n\{(\gamma_i, u_i)\}_{i=1}^n are collinear implies that any two bi-pooling solutions of problem (3) induce the same collection of {μ~}∪{μi}i=2n\{\tilde{\mu}\} \cup \{\mu_i\}_{i=2}^n. Then, because every bi-pooling solution is a mean-preserving spread of FF, any two such bi-pooling solutions must be identical. As noted in Kleiner et al. (2021) and Arieli et al. (2023), every extreme point of the set of solutions to problem (3) is a bi-pooling solution, and hence the solution to problem (3) must be a unique bi-pooling solution.

A.2.2 Proof of Proposition 1

Since the bi-pooling partition is barely obedient, the “if” direction follows from Lemma 1. For the other direction, suppose first that a bi-pooling solution GBG_B is implementable. Since the commitment payoff is an upper bound on equilibrium payoffs, GBG_B is the PMD induced by a sender-preferred equilibrium (σ,τ,β)(\sigma, \tau, \beta). By Theorem 3, GBG_B is associated with a unique barely obedient bi-pooling partition B\mathcal{B}; an argument analogous to the one in the proof of Lemma 2 shows that B\mathcal{B} is revelation-proof.

A.2.3 Proof of Proposition 2

We use the following result by Arieli et al. (2023) to prove Proposition 2. Say that {γℓ,γh}\{\gamma_\ell, \gamma_h\} is a feasible bi-pooling support for the interval (ω‾,ωˉ)(\underline{\omega}, \bar{\omega}) (or just feasible for simplicity) if there exists a mean preserving contraction of F∣[ω‾,ωˉ]F|_{[\underline{\omega}, \bar{\omega}]} whose support is {γℓ,γh}\{\gamma_\ell, \gamma_h\}.

Lemma 6 (Arieli et al., 2023). Fix an interval (ω‾,ωˉ)(\underline{\omega}, \bar{\omega}), and let y(γℓ)y(\gamma_\ell) satisfy E[ω∣ω∈[ω‾,y(γℓ)]]=γℓ\mathbb{E}[\omega \mid \omega \in [\underline{\omega}, y(\gamma_\ell)]] = \gamma_\ell. Then {γℓ,γh}\{\gamma_\ell, \gamma_h\} is feasible for the interval (ω‾,ωˉ)(\underline{\omega}, \bar{\omega}) if and only if

  • (i) ω‾≤γℓ≤E[ω∣ω∈[ω‾,ωˉ]]≤γh≤ωˉ\underline{\omega} \leq \gamma_\ell \leq \mathbb{E}[\omega \mid \omega \in [\underline{\omega}, \bar{\omega}]] \leq \gamma_h \leq \bar{\omega}, and
  • (ii) E[ω∣ω∈[y(γℓ),ωˉ]]≥γh\mathbb{E}[\omega \mid \omega \in [y(\gamma_\ell), \bar{\omega}]] \geq \gamma_h.

Proof of Proposition 2. Suppose to the contrary that there exists a bi-pooling solution GBG_B that is not implementable. Then by Corollary 1, the bi-pooling partition of GBG_B, B\mathcal{B}, must violate the condition therein. First suppose that there exists an unskipped action ii such that bˉi>γi+1\bar{b}_i > \gamma_{i+1}. There are two cases.

Case 1. BiB_i is an interval; i.e., Bi=[b‾i,bˉi]B_i = [\underline{b}_i, \bar{b}_i]. There are two subcases:

(I) γi−1∈int(Bi)\gamma_{i-1} \in \text{int}(B_i).

For z∈(γi+1,bˉi)z \in (\gamma_{i+1}, \bar{b}_i), let h(z)h(z) solve E[ω∣ω∈[b‾i,h(z)]∪[z,bˉi]]=γi+1\mathbb{E}[\omega \mid \omega \in [\underline{b}_i, h(z)] \cup [z, \bar{b}_i]] = \gamma_{i+1}. By Lemma 6, for zz close enough to bˉi\bar{b}_i, {γi−1,γi}\{\gamma_{i-1}, \gamma_i\} is feasible for [h(z),z][h(z), z]. Consequently, the sender's payoff on BiB_i, as a function of zz, is

P(z)≔ui+1[F(bˉi)−F(z)+F(h(z))−F(b‾i)]+[m(z)−γi−1γi−γi−1ui+γi−m(z)γi−γi−1ui−1](F(z)−F(h(z)))P(z) := u_{i+1}[F(\bar{b}_i) - F(z) + F(h(z)) - F(\underline{b}_i)] + \left[ \frac{m(z) - \gamma_{i-1}}{\gamma_i - \gamma_{i-1}} u_i + \frac{\gamma_i - m(z)}{\gamma_i - \gamma_{i-1}} u_{i-1} \right] (F(z) - F(h(z)))

where m(z)≔E[ω∣ω∈[z,h(z)]]m(z) := \mathbb{E}[\omega \mid \omega \in [z, h(z)]]. To show that this is a profitable deviation, it suffices to show that P′(bˉi)≔lim⁡z↗bˉiP′(z)<0P'(\bar{b}_i) := \lim_{z \nearrow \bar{b}_i} P'(z) < 0. To this end, we first calculate

P′(z)=f(z)γi−γi−1z−h(z)γi+1−h(z)[(ui−ui−1)γi+1+(ui+1−ui)γi−1−(ui+1−ui−1)γi].P'(z) = \frac{f(z)}{\gamma_i - \gamma_{i-1}} \frac{z - h(z)}{\gamma_{i+1} - h(z)} [(u_i - u_{i-1})\gamma_{i+1} + (u_{i+1} - u_i)\gamma_{i-1} - (u_{i+1} - u_{i-1})\gamma_i].

Letting z↗bˉiz \nearrow \bar{b}_i, then h(z)↘b‾ih(z) \searrow \underline{b}_i, and

P′(bˉi)=f(bˉi)γi−γi−1bˉi−b‾iγi+1−b‾i[(ui−ui−1)γi+1+(ui+1−ui)γi−1−(ui+1−ui−1)γi];P'(\bar{b}_i) = \frac{f(\bar{b}_i)}{\gamma_i - \gamma_{i-1}} \frac{\bar{b}_i - \underline{b}_i}{\gamma_{i+1} - \underline{b}_i} [(u_i - u_{i-1})\gamma_{i+1} + (u_{i+1} - u_i)\gamma_{i-1} - (u_{i+1} - u_{i-1})\gamma_i];

P′(bˉi)<0P'(\bar{b}_i) < 0 if and only if (ui+1−ui−1)γi−(ui−ui−1)γi+1−(ui+1−ui)γi−1>0(u_{i+1} - u_{i-1})\gamma_i - (u_i - u_{i-1})\gamma_{i+1} - (u_{i+1} - u_i)\gamma_{i-1} > 0, and this is equivalent to

ui+1−uiγi+1−γi>ui−ui−1γi−γi−1,\frac{u_{i+1} - u_i}{\gamma_{i+1} - \gamma_i} > \frac{u_i - u_{i-1}}{\gamma_i - \gamma_{i-1}},

which is implied by (4).

(II) γi−1∉int(Bi)\gamma_{i-1} \notin \text{int}(B_i) (and therefore γi−1≤b‾i\gamma_{i-1} \leq \underline{b}_i).

Define Biε=[b‾i+ε,bˉi]B_i^\varepsilon = [\underline{b}_i + \varepsilon, \bar{b}_i]; for small enough ε>0\varepsilon > 0, {γi,γi+1}\{\gamma_i, \gamma_{i+1}\} is feasible for BiεB_i^\varepsilon. Let m(ε)m(\varepsilon) denote the mean of BiεB_i^\varepsilon; note that m(0)=γim(0) = \gamma_i. Then the sender's payoff as a function of ε\varepsilon on BiB_i is

P(ε)≔[m(ε)−γiγi+1−γiui+1+γi+1−m(ε)γi+1−γiui][F(bˉi)−F(b‾i+ε)]+ui−1[F(b‾i+ε)−F(b‾i)].P(\varepsilon) := \left[ \frac{m(\varepsilon) - \gamma_i}{\gamma_{i+1} - \gamma_i} u_{i+1} + \frac{\gamma_{i+1} - m(\varepsilon)}{\gamma_{i+1} - \gamma_i} u_i \right] [F(\bar{b}_i) - F(\underline{b}_i + \varepsilon)] + u_{i-1}[F(\underline{b}_i + \varepsilon) - F(\underline{b}_i)].

To show that this is a profitable deviation, it suffices to show that P′(0)≔P'(0) := lim⁡ε↘0P′(ε)>0\lim_{\varepsilon \searrow 0} P'(\varepsilon) > 0. Algebra reveals that

P′(ε)=f(b‾i+ε)[ui−1−γi+1ui−γiui+1γi+1−γi−(b‾i−ε)ui+1−uiγi+1−γi];P'(\varepsilon) = f(\underline{b}_i + \varepsilon) \left[ u_{i-1} - \frac{\gamma_{i+1}u_i - \gamma_i u_{i+1}}{\gamma_{i+1} - \gamma_i} - (\underline{b}_i - \varepsilon) \frac{u_{i+1} - u_i}{\gamma_{i+1} - \gamma_i} \right];

consequently, as ε↘0\varepsilon \searrow 0,

P′(0)=f(b‾i)γi+1−γi[(γi−b‾i)(ui+1−ui)−(γi+1−γi)(ui−ui−1)].(9)P'(0) = \frac{f(\underline{b}_i)}{\gamma_{i+1} - \gamma_i} [(\gamma_i - \underline{b}_i)(u_{i+1} - u_i) - (\gamma_{i+1} - \gamma_i)(u_i - u_{i-1})]. \quad (9)

Because f(b‾i)>0f(\underline{b}_i) > 0 and γi+1−γi>0\gamma_{i+1} - \gamma_i > 0 by assumption, the sign of P′(0)P'(0) is the same as the sign of term in the square brackets in the right-hand side of (9). Thus, P′(0)>0P'(0) > 0 if and only if

ui+1−uiγi+1−γi>ui−ui−1γi−b‾i.\frac{u_{i+1} - u_i}{\gamma_{i+1} - \gamma_i} > \frac{u_i - u_{i-1}}{\gamma_i - \underline{b}_i}.

Because γi+1<bˉi\gamma_{i+1} < \bar{b}_i, h(γi;γi+1)>b‾ih(\gamma_i; \gamma_{i+1}) > \underline{b}_i. Thus, (4) implies the inequality above.

Case 2. There is a partitional element BjB_j with j<ij < i such that Bj⊆co(Bi)B_j \subseteq \text{co}(B_i). In this case, Bj=[b‾j,bˉj]B_j = [\underline{b}_j, \bar{b}_j], and Bi=[b‾i,b‾j]∪[bˉj,bˉi]B_i = [\underline{b}_i, \underline{b}_j] \cup [\bar{b}_j, \bar{b}_i]. WLOG, assume that b‾i<b‾j\underline{b}_i < \underline{b}_j; by Lemma 6, {γj,γi}\{\gamma_j, \gamma_i\} is feasible for [b‾i,bˉi][\underline{b}_i, \bar{b}_i], and

E[ω∣ω∈[y(γj),bˉi]]>γi.(10)\mathbb{E}[\omega \mid \omega \in [y(\gamma_j), \bar{b}_i]] > \gamma_i. \quad (10)

For z∈(max⁡{γi+1,bˉj},bˉi)z \in (\max\{\gamma_{i+1}, \bar{b}_j\}, \bar{b}_i), let h(z)h(z) solve E[ω∣ω∈[b‾i,h(z)]∪[z,bˉi]]=γi+1\mathbb{E}[\omega \mid \omega \in [\underline{b}_i, h(z)] \cup [z, \bar{b}_i]] = \gamma_{i+1}. By (10) and Lemma 6, for zz close enough to bˉi\bar{b}_i, {γj,γi}\{\gamma_j, \gamma_i\} is feasible for [h(z),z][h(z), z]. Consequently, one can find a profitable deviation similar to in Case 1 (I) mutatis mutandis.

Now suppose instead that there exists a pair of partitional elements BiB_i and Bi+1B_{i+1} with Bi⊆co(Bi+1)B_i \subseteq \text{co}(B_{i+1}), and γi+1<bˉi\gamma_{i+1} < \bar{b}_i. Since Bi=[b‾i,bˉi]B_i = [\underline{b}_i, \bar{b}_i], this case is isomorphic to Case 1 when action i+1i + 1 is skipped. Hence, we can similarly find a profitable deviation.

Therefore, every bi-pooling solution must satisfy the condition in Corollary 1, and hence implementable. This completes the proof. ■\blacksquare

A.2.4 Proof of Corollary 2

By definition of h(γi;γi+1)h(\gamma_i; \gamma_{i+1}), when ff is increasing, γi+1−γi≤γi−h(γi;γi+1)\gamma_{i+1} - \gamma_i \leq \gamma_i - h(\gamma_i; \gamma_{i+1}). Then since γi+1−γi≤γi−γi−1\gamma_{i+1} - \gamma_i \leq \gamma_i - \gamma_{i-1}, it must be that γi+1−γi≤min⁡{γi−γi−1,γi−h(γi;γi+1)}\gamma_{i+1} - \gamma_i \leq \min\{\gamma_i - \gamma_{i-1}, \gamma_i - h(\gamma_i; \gamma_{i+1})\}. Now there are two cases. If ui+1−ui>ui−ui−1u_{i+1} - u_i > u_i - u_{i-1}, (4) must hold; then by Proposition 2, every bi-pooling solution can be implemented. If instead γi+1−γi<γi−γi−1\gamma_{i+1} - \gamma_i < \gamma_i - \gamma_{i-1}, it must be that γi+1−γi<min⁡{γi−γi−1,γi−h(γi;γi−1)}\gamma_{i+1} - \gamma_i < \min\{\gamma_i - \gamma_{i-1}, \gamma_i - h(\gamma_i; \gamma_{i-1})\}; this inequality and ui+1−ui≥ui−ui−1u_{i+1} - u_i \geq u_i - u_{i-1} together imply (4). Again by Proposition 2, every bi-pooling solution can be implemented.

B Supplementary Appendix

This appendix is organized as follows:

  • Section B.1 proves supplementary results for the special case in which the receiver has three actions.
  • Section B.2 contains the proofs omitted from Appendix A.
  • Section B.3 establishes the robustness of the set of partitional equilibria to two standard refinements: the never-a-weak-best-response (NWBR) criterion (Cho and Kreps, 1987) and the Grossman–Perry–Farrell refinement (Bertomeu and Cianciaruso, 2018).

B.1 Supplementary Results for Ternary Actions

In this section, we study the special case where the receiver has three actions: N={1,2,3}N = \{1, 2, 3\}. Recall that {γL,γH}\{\gamma_L, \gamma_H\} is feasible for the interval [ω‾,ωˉ][\underline{\omega}, \bar{\omega}] if there exists a mean preserving contraction of F∣[ω‾,ωˉ]F|_{[\underline{\omega}, \bar{\omega}]} whose support is {γL,γH}\{\gamma_L, \gamma_H\}.

Claim 7. If there does not exist y∈[0,γ2]y \in [0, \gamma_2] such that {γ2,γ3}\{\gamma_2, \gamma_3\} is feasible for [y,1][y, 1], then every bi-pooling solution is implementable.

Proof of Claim 7. By Lemma 6, {γ2,γ3}\{\gamma_2, \gamma_3\} is feasible for the interval [y,1][y, 1] if and only if

  • (i) y≤γ2≤m(y)≤γ3≤1y \leq \gamma_2 \leq m(y) \leq \gamma_3 \leq 1, and
  • (ii) E[ω∣ω∈[η(γ2;y),1]]≥γ3\mathbb{E}[\omega \mid \omega \in [\eta(\gamma_2; y), 1]] \geq \gamma_3,

where m(y)≔E[ω∣ω∈[y,1]]m(y) := \mathbb{E}[\omega \mid \omega \in [y, 1]], and η(γ2;y)\eta(\gamma_2; y) is such that E[ω∣ω∈[y,η(γ2)]]=γ2\mathbb{E}[\omega \mid \omega \in [y, \eta(\gamma_2)]] = \gamma_2. Then if there does not exist y∈[0,γ2]y \in [0, \gamma_2] such that {γ2,γ3}\{\gamma_2, \gamma_3\} is feasible for [y,1][y, 1], there are two cases:

  • (a) (i) fails to hold for all y∈[0,γ2]y \in [0, \gamma_2];
  • (b) (i) holds for some y∈[0,γ2]y \in [0, \gamma_2], but (ii) fails for all such yy 's.

For Case (a), the only possibility is that m(y)≥γ3m(y) \geq \gamma_3. If this is the case, every bi-pooling solution GG has supp(G)⊆[γ3,1]\text{supp}(G) \subseteq [\gamma_3, 1], and hence the unique bi-pooling partition has B3=[0,1]B_3 = [0, 1], and revelation proofness holds.

For Case (b), let us introduce some notation first. For each i=1,2i = 1, 2, if there exists h≥0h \geq 0 such that E[ω∣ω∈[h,1]]=γi\mathbb{E}[\omega \mid \omega \in [h, 1]] = \gamma_i, set h(γi)=hh(\gamma_i) = h; otherwise let h(γi)=0h(\gamma_i) = 0. Then for every y∈[0,γ2]∩[h(γ2),h(γ3)]y \in [0, \gamma_2] \cap [h(\gamma_2), h(\gamma_3)], (i) holds. If (ii) fails for all such yy 's, it must be that E[ω∣ω∈[η(γ2;h(γ2)),1]]<γ3\mathbb{E}[\omega \mid \omega \in [\eta(\gamma_2; h(\gamma_2)), 1]] < \gamma_3. Note that this is not possible if h(γ2)>0h(\gamma_2) > 0: if this is the case, η(γ2;h(γ2))=1\eta(\gamma_2; h(\gamma_2)) = 1 by definition, so it must be that E[ω∣ω∈[η(γ2;h(γ2)),1]]≥γ3\mathbb{E}[\omega \mid \omega \in [\eta(\gamma_2; h(\gamma_2)), 1]] \geq \gamma_3, a contradiction. Consequently, in Case (b), (ii) must fail for y=0y = 0, and hence every bi-pooling solution GG has G(γ3)−G(γ3−)=1−F(h(γ3))G(\gamma_3) - G(\gamma_3^-) = 1 - F(h(\gamma_3)), and supp(G)⊆[γ2,γ3]\text{supp}(G) \subseteq [\gamma_2, \gamma_3]. Thus, the unique bi-pooling partition associated with GG has B2=[0,h(γ3)]B_2 = [0, h(\gamma_3)] and B3=[h(γ3),1]B_3 = [h(\gamma_3), 1]. Since h(γ3)<γ3h(\gamma_3) < \gamma_3 by definition, revelation proofness must hold. This completes the proof. ■\blacksquare

Claim 8. All bi-pooling solutions to the information design problem are associated with the same bi-pooling partition.

Proof of Claim 8. It can be readily seen from the proof of Claim 7 that, if there does not exist y∈[0,γ2]y \in [0, \gamma_2] such that {γ2,γ3}\{\gamma_2, \gamma_3\} is feasible for [y,1][y, 1], then all bi-pooling solutions are associated with the same bi-pooling partition. Now suppose there exists y∈[0,γ2]y \in [0, \gamma_2] such that {γ2,γ3}\{\gamma_2, \gamma_3\} is feasible for [y,1][y, 1]. Let YY denote the set of such yy 's; Lemma 6 implies that YY is a closed subset of [0,γ2][0, \gamma_2]. Consequently, the commitment payoff can be identified by the lower endpoint of the bi-pooling interval. Hence, each of them corresponds to a point in YY that maximizes the sender's ex-ante payoff (recall that u1=0u_1 = 0):

π(y)=(1−F(y))[γ3−m(y)γ3−γ2u2+m(y)−γ2γ3−γ2u3].\pi(y) = (1 - F(y)) \left[ \frac{\gamma_3 - m(y)}{\gamma_3 - \gamma_2} u_2 + \frac{m(y) - \gamma_2}{\gamma_3 - \gamma_2} u_3 \right].

Taking derivative,

π′(y)=−f(y)[γ3−m(y)γ3−γ2u2+m(y)−γ2γ3−γ2u3]+(1−F(y))u3−u2γ3−γ2m′(y),\pi'(y) = -f(y) \left[ \frac{\gamma_3 - m(y)}{\gamma_3 - \gamma_2} u_2 + \frac{m(y) - \gamma_2}{\gamma_3 - \gamma_2} u_3 \right] + (1 - F(y)) \frac{u_3 - u_2}{\gamma_3 - \gamma_2} m'(y),

where

m′(y)=(m(y)−y)f(y)1−F(y).m'(y) = \frac{(m(y) - y)f(y)}{1 - F(y)}.

Consequently,

π′(y)=f(y)γ3−γ2[(m(y)−y)(u3−u2)−(γ3−m(y))u2−(m(y)−γ2)u3],=f(y)γ3−γ2[u3(γ2−y)−u2(γ3−y)]\begin{aligned} \pi'(y) &= \frac{f(y)}{\gamma_3 - \gamma_2} [(m(y) - y)(u_3 - u_2) - (\gamma_3 - m(y))u_2 - (m(y) - \gamma_2)u_3], \\ &= \frac{f(y)}{\gamma_3 - \gamma_2} [u_3(\gamma_2 - y) - u_2(\gamma_3 - y)] \end{aligned}

and its sign is determined by the terms between the squared brackets, which implies that π\pi is single-peaked in yy. Therefore, there must exist a unique zz that maximizes π(y)\pi(y) on YY. As a consequence, all bi-pooling solutions are associated with the same bi-pooling partition B\mathcal{B} with B1=[0,z]B_1 = [0, z], B2=[b2,bˉ2]B_2 = [b_2, \bar{b}_2], and B3=[z,b2]∪[bˉ2,1]B_3 = [z, b_2] \cup [\bar{b}_2, 1]. ■

Claim 9. If no commitment solution is implementable, the sender-preferred laminar PE B\mathcal{B} is such that B1=[0,y]B_1 = [0, y], B2=[h,b]B_2 = [h, b], and B3=[y,h]∪[b,1]B_3 = [y, h] \cup [b, 1], where γ2<b≤γ3\gamma_2 < b \leq \gamma_3, and h>0h > 0 and y≥0y \geq 0 are defined by

E[ω∣ω∈[h,b]]=γ2andE[ω∣ω∈[y,h]∪[b,1]]=γ3.(11)\mathbb{E}[\omega \mid \omega \in [h, b]] = \gamma_2 \quad \text{and} \quad \mathbb{E}[\omega \mid \omega \in [y, h] \cup [b, 1]] = \gamma_3. \quad (11)

Furthermore,

u3≤γ3−yγ2−yu2.(12)u_3 \leq \frac{\gamma_3 - y}{\gamma_2 - y} u_2. \quad (12)

Proof of Claim 9. By Theorem 2, if B2B_2 has nonempty interior, it must be that E[ω∣ω∈B2]=γ2\mathbb{E}[\omega \mid \omega \in B_2] = \gamma_2, and E[ω∣ω∈B3]=γ3\mathbb{E}[\omega \mid \omega \in B_3] = \gamma_3.27 Then to obtain the statement it suffices to show three things: (1) b>γ2b > \gamma_2, namely B2B_2 has nonempty interior; (2) there exists such an hh; and (3) there exists such a yy.

We show that B2B_2 has nonempty interior first. Suppose to the contrary that int(B2)=∅\text{int}(B_2) = \emptyset, then by Claim 7, there are two cases: B3=[0,1]B_3 = [0, 1], and B3=[z,1]B_3 = [z, 1] for some z>0z > 0. If B3=[0,1]B_3 = [0, 1], since the sender attains highest possible payoff in equilibrium, it must be that a commitment outcome is implementable, a contradiction. If instead B3=[z,1]B_3 = [z, 1] for some z>0z > 0, it must be that z≤γ2z \leq \gamma_2, as otherwise recommending action 2 on [z,γ2][z, \gamma_2] is a profitable deviation. Consequently, this bi-pooling partition is revelation-proof, and hence a commitment outcome is implementable, again a contradiction. Therefore, it must be that B2B_2 has nonempty interior.

To see that there exists such an hh, we first claim that E[ω∣ω∈[0,γ3]]≤γ2\mathbb{E}[\omega \mid \omega \in [0, \gamma_3]] \leq \gamma_2. Suppose not, so

E[ω∣ω∈[0,γ3]]>γ2.(13)\mathbb{E}[\omega \mid \omega \in [0, \gamma_3]] > \gamma_2. \quad (13)

Without loss of generality, assume that there exists a bi-pooling solution features [y,1][y, 1] bi-pooled to {γ2,γ3}\{\gamma_2, \gamma_3\} for some y∈[0,γ2]y \in [0, \gamma_2].28 Consequently, there exist bˉ1\bar{b}_1 and b‾1\underline{b}_1 with y≤b‾1≤bˉ1y \leq \underline{b}_1 \leq \bar{b}_1 such that the (unique) bi-pooling partition associated with the bi-pooling solution B\mathcal{B} is given by B1=[0,y]B_1 = [0, y], B2=[b‾1,bˉ1]B_2 = [\underline{b}_1, \bar{b}_1], and B3=[y,b‾1]∪[bˉ1,1]B_3 = [y, \underline{b}_1] \cup [\bar{b}_1, 1]. Then because E[ω∣ω∈B2]=γ2\mathbb{E}[\omega \mid \omega \in B_2] = \gamma_2 and b‾1≥0\underline{b}_1 \geq 0, we must have bˉ1≤γ3\bar{b}_1 \leq \gamma_3 by (13). Thus, the bi-pooling solution must be implementable, a contradiction. As a consequence, it must be that E[ω∣ω∈[h,b]]=γ2\mathbb{E}[\omega \mid \omega \in [h, b]] = \gamma_2; it remains to show that h>0h > 0. If instead h=0h = 0, then E[ω∣ω∈[0,γ3]]=γ2\mathbb{E}[\omega \mid \omega \in [0, \gamma_3]] = \gamma_2. Consequently, it must be that B2=[0,γ3]B_2 = [0, \gamma_3] and B3=[γ3,1]B_3 = [\gamma_3, 1]. This cannot be optimal: for any ε∈(0,γ2)\varepsilon \in (0, \gamma_2), define B^1=[ε,γ3]\hat{B}_1 = [\varepsilon, \gamma_3], and B^2=[0,ε]∪[γ3,1]\hat{B}_2 = [0, \varepsilon] \cup [\gamma_3, 1]. Then for ε\varepsilon small enough, E[ω∣ω∈B^i]≥γi\mathbb{E}[\omega \mid \omega \in \hat{B}_i] \geq \gamma_i for each i=1,2i = 1, 2, and the sender's ex-ante payoff is strictly higher. Thus, it must be that h>0h > 0.

To show that there exists such a yy, it suffices to show that E[ω∣ω∈[0,h]∪[b,1]]≤γ3\mathbb{E}[\omega \mid \omega \in [0, h] \cup [b, 1]] \leq \gamma_3. Suppose not, so E[ω∣ω∈[0,h]∪[b,1]]>γ3\mathbb{E}[\omega \mid \omega \in [0, h] \cup [b, 1]] > \gamma_3. Let δ>0\delta > 0 be small enough, and let ϵ(δ)\epsilon(\delta) be such that

E[ω∣ω∈[h+ϵ(δ),b−δ]]=γ2.\mathbb{E}[\omega \mid \omega \in [h + \epsilon(\delta), b - \delta]] = \gamma_2.

Now define B~1=[h+ϵ(δ),b−δ]\tilde{B}_1 = [h + \epsilon(\delta), b - \delta], and B~2=[0,h+ϵ(δ)]∪[b−δ,1]\tilde{B}_2 = [0, h + \epsilon(\delta)] \cup [b - \delta, 1]. Because the density ff is strictly positive, for small enough δ\delta, E[ω∣ω∈B~2]≥γ3\mathbb{E}[\omega \mid \omega \in \tilde{B}_2] \geq \gamma_3, and μF(B~2)>μF(B3)\mu_F(\tilde{B}_2) > \mu_F(B_3). This creates a profitable deviation to the sender without violating revelation proofness.

Finally, to show that (12) must hold, suppose to the contrary that

u3>γ3−yγ2−yu2.u_3 > \frac{\gamma_3 - y}{\gamma_2 - y} u_2.

An argument analogous to Case 1 (II) in the proof of Proposition 2 shows that the sender has a profitable deviation, and hence the bi-pooling partition B\mathcal{B} with B1=[0,y]B_1 = [0, y], B2=[h,b]B_2 = [h, b], and B3=[y,h]∪[b,1]B_3 = [y, h] \cup [b, 1] cannot be associated with a sender-preferred laminar PE, a contradiction. ■\blacksquare

By Claim 9, the sender's ex-ante payoff in a sender-preferred equilibrium can be written as

Vˉ(b)=u2[F(b)−F(h(b))]+u3[1−F(b)+F(h(b))−F(y(b))],\bar{V}(b) = u_2[F(b) - F(h(b))] + u_3[1 - F(b) + F(h(b)) - F(y(b))],

where h(b)h(b) and y(b)y(b) are implicitly defined by the two equations in (11).

Claim 10. If no commitment outcome is implementable, the sender's ex-ante payoff in a sender-preferred equilibrium, Vˉ(b)\bar{V}(b), is increasing in bb.

Proof of Claim 10. Directly,

Vˉ′(b)=(u2−u3)[f(b)−f(h)dhdb]−u3f(y)dydb.(14)\bar{V}'(b) = (u_2 - u_3) \left[ f(b) - f(h) \frac{dh}{db} \right] - u_3 f(y) \frac{dy}{db}. \quad (14)

Using (11), by the implicit function theorem,

dhdb=−(b−γ2)f(b)(γ2−h)f(h),(15)\frac{dh}{db} = - \frac{(b - \gamma_2) f(b)}{(\gamma_2 - h) f(h)}, \quad (15)
dydb=−(b−h)(γ3−γ2)f(b)(γ2−h)(γ3−y)f(y).(16)\frac{dy}{db} = - \frac{(b - h) (\gamma_3 - \gamma_2) f(b)}{(\gamma_2 - h) (\gamma_3 - y) f(y)}. \quad (16)

Plugging (15) and (16) into (14),

Vˉ′(b)=(u2−u3)f(b)(1+b−γ2γ2−h)+u3f(b)(b−h)(γ3−γ2)(γ2−h)(γ3−y)=[(u2−u3)b−hγ2−h+u3(γ3−γ2)(b−h)(γ2−h)(γ3−y)]f(b)=[u2b−hγ2−h−u3(b−h)(γ2−y)(γ2−h)(γ3−y)]f(b)=[u2(γ3−y)−u3(γ2−y)](b−h)f(b)(γ2−h)(γ3−y),\begin{aligned} \bar{V}'(b) &= (u_2 - u_3) f(b) \left( 1 + \frac{b - \gamma_2}{\gamma_2 - h} \right) + u_3 f(b) \frac{(b - h) (\gamma_3 - \gamma_2)}{(\gamma_2 - h) (\gamma_3 - y)} \\ &= \left[ (u_2 - u_3) \frac{b - h}{\gamma_2 - h} + u_3 \frac{(\gamma_3 - \gamma_2) (b - h)}{(\gamma_2 - h) (\gamma_3 - y)} \right] f(b) \\ &= \left[ u_2 \frac{b - h}{\gamma_2 - h} - u_3 \frac{(b - h) (\gamma_2 - y)}{(\gamma_2 - h) (\gamma_3 - y)} \right] f(b) \\ &= [u_2 (\gamma_3 - y) - u_3 (\gamma_2 - y)] \frac{(b - h) f(b)}{(\gamma_2 - h) (\gamma_3 - y)}, \end{aligned}

and we see that Vˉ′(b)≥0\bar{V}'(b) \geq 0 if and only if u2(γ3−y)≥u3(γ2−y)u_2 (\gamma_3 - y) \geq u_3 (\gamma_2 - y). Then since no commitment solution is implementable, by Claim 9, (12) implies that Vˉ′(b)≥0\bar{V}'(b) \geq 0, and hence the sender's ex-ante payoff in a sender-preferred equilibrium is increasing in bb. ■

B.2 Remaining Omitted Proofs

B.2.1 Proof of Proposition 3

To solve for a sender-preferred equilibrium, we find a bi-pooling solution to the corresponding information design problem first, and check whether it is implementable using Corollary 1. If it is, a sender-preferred equilibrium is associated with a barely obedient bi-pooling partition B\mathcal{B} that is also associated with the commitment solution.29

Now suppose that no commitment solution is implementable. By Theorem 2, there exist yy, zz, and bb such that B2=[z,b]B_2 = [z, b], and B3=[y,z]∪[b,1]B_3 = [y, z] \cup [b, 1].30 By Claim 9, there exist y≥0y \geq 0 and z>0z > 0 such that

E[ω∣ω∈[z,b]]=γ2andE[ω∣ω∈[y,z]∪[b,1]]=γ3.\mathbb{E}[\omega \mid \omega \in [z, b]] = \gamma_2 \quad \text{and} \quad \mathbb{E}[\omega \mid \omega \in [y, z] \cup [b, 1]] = \gamma_3.

Consequently, yy and zz can be implicitly defined as functions of bb, and hence the sender's ex-ante payoff can be parametrized by bb, so long as b≤γ3b \leq \gamma_3:

Vˉ(b)=u2[F(b)−F(z(b))]+u3[1−F(b)+F(z(b))−F(y(b))].\bar{V}(b) = u_2[F(b) - F(z(b))] + u_3[1 - F(b) + F(z(b)) - F(y(b))].

By Claim 10, Vˉ\bar{V} is increasing in bb. Hence, the partition corresponding to the sender's preferred equilibrium can be found by setting b=γ3b = \gamma_3, which yields the expression in the statement of the claim.

B.2.2 Proof of Corollary 3

Recall that γ1≔0\gamma_1 := 0 and u0u_0 is normalized to zero; hence when n=3n = 3, Equation (4) in the main text reduces to

u3−u2γ3−γ2>u2γ2−max⁡{0,h(γ2;γ3)}(17)\frac{u_3 - u_2}{\gamma_3 - \gamma_2} > \frac{u_2}{\gamma_2 - \max\{0, h(\gamma_2; \gamma_3)\}} \quad (17)

And because h(γ2;γ3)≥0h(\gamma_2; \gamma_3) \geq 0, the right-hand side of (17) further reduces to u2/(γ2−h(γ2;γ3))u_2/(\gamma_2 - h(\gamma_2; \gamma_3)). Then since ff is increasing, γ3−γ2≥γ2−h(γ2;γ3)\gamma_3 - \gamma_2 \geq \gamma_2 - h(\gamma_2; \gamma_3); thus, if u3−u2>u2u_3 - u_2 > u_2, or u3>2u2u_3 > 2u_2, (17) must hold. Consequently, by Proposition 2, every bi-pooling solution can be implemented. By Claim 7, all bi-pooling solutions induce the same bi-pooling partition. Then because the set of bi-pooling solutions is the set of extreme points of the solution correspondence of the information design problem, all commitment solutions must be associated with the same bi-pooling partition. Thus, every commitment outcome is implementable.

B.2.3 Proof of Proposition 4

Let ωq\omega_q denote the cutoff quality that the buyer is indifferent between purchasing q−1q - 1 and qq units: it solves

ωqU(q)−pq=ωqU(q−1)−p(q−1),\omega_q U(q) - pq = \omega_q U(q - 1) - p(q - 1),

so ωq=p/[U(q)−U(q−1)]\omega_q = p/[U(q) - U(q - 1)]. Letting ω0=0\omega_0 = 0 and ωn+1=1\omega_{n+1} = 1, the buyer buys q∈{0,1,…,n}q \in \{0, 1, \dots, n\} units of the product if and only if ω∈[ωq,ωq+1]\omega \in [\omega_q, \omega_{q+1}]. If PU>2AUP^U > 2A^U, U′′(q)/[U′(q)]2U''(q)/[U'(q)]^2 is strictly decreasing in qq, and thus

ωq+1−ωq=pU(q+1)−U(q)−pU(q)−U(q−1)\omega_{q+1} - \omega_q = \frac{p}{U(q+1) - U(q)} - \frac{p}{U(q) - U(q-1)}

is strictly decreasing in qq. Since the seller's gain from the buyer purchasing one more unit is p−cp - c, Proposition 4 follows from Corollary 3.

B.2.4 Proof of Proposition 5

If either α3\alpha_3 increases, or λ3\lambda_3 increases, or both, γ3\gamma_3 decreases. By Proposition 3, when no commitment outcome can be implemented, the sender's ex-ante payoff is given by

Vˉ(γ3)=u2[F(γ3)−F(h(γ3))]+u3[1−F(γ3)+F(h(γ3))−F(y(γ3))],\bar{V}(\gamma_3) = u_2[F(\gamma_3) - F(h(\gamma_3))] + u_3[1 - F(\gamma_3) + F(h(\gamma_3)) - F(y(\gamma_3))],

where hh and yy are implicitly defined by

E[ω∣ω∈[h,γ3]]=γ2andE[ω∣ω∈[y,h]∪[γ3,1]]=γ3.\mathbb{E}[\omega \mid \omega \in [h, \gamma_3]] = \gamma_2 \quad \text{and} \quad \mathbb{E}[\omega \mid \omega \in [y, h] \cup [\gamma_3, 1]] = \gamma_3.

Now

Vˉ′(γ3)=(u2−u3)[f(γ3)−f(h)dhdγ3]−u3f(y)dydγ3.(18)\bar{V}'(\gamma_3) = (u_2 - u_3) \left[ f(\gamma_3) - f(h) \frac{dh}{d\gamma_3} \right] - u_3 f(y) \frac{dy}{d\gamma_3}. \quad (18)

By the implicit function theorem,

dhdγ3=−(γ3−γ2)f(γ3)(γ2−h)f(h),(19)\frac{dh}{d\gamma_3} = - \frac{(\gamma_3 - \gamma_2) f(\gamma_3)}{(\gamma_2 - h) f(h)}, \quad (19)
dydγ3=(γ2−h)[1−f(γ3)+F(h)−F(y)](γ2−h)(γ3−y)f(y)−(γ3−h)(γ3−γ2)f(γ3)(γ2−h)(γ3−y)f(y).(20)\frac{dy}{d\gamma_3} = \frac{(\gamma_2 - h) [1 - f(\gamma_3) + F(h) - F(y)]}{(\gamma_2 - h) (\gamma_3 - y) f(y)} - \frac{(\gamma_3 - h) (\gamma_3 - \gamma_2) f(\gamma_3)}{(\gamma_2 - h) (\gamma_3 - y) f(y)}. \quad (20)

Plug (19) and (20) into (18),

Vˉ′(γ3)=−(γ2−h)[1−f(γ3)+F(h)−F(y)]u3(γ2−h)(γ3−y)−(γ3−h)(γ2−y)f(γ3)(γ2−h)(γ3−y)u3+(γ3−h)(γ3−y)f(γ3)(γ2−h)(γ3−y)u2,\begin{aligned}\bar{V}'(\gamma_3) = & -\frac{(\gamma_2 - h) [1 - f(\gamma_3) + F(h) - F(y)] u_3}{(\gamma_2 - h) (\gamma_3 - y)} - \frac{(\gamma_3 - h) (\gamma_2 - y) f(\gamma_3)}{(\gamma_2 - h) (\gamma_3 - y)} u_3 \\ & + \frac{(\gamma_3 - h) (\gamma_3 - y) f(\gamma_3)}{(\gamma_2 - h) (\gamma_3 - y)} u_2,\end{aligned}

whose sign is determined by

−(γ2−h)(1−F(γ2)+F(h)−F(y))−(γ3−h)f(γ3)[(γ2−y)u3−(γ2−y)u2].(21)-(\gamma_2 - h) (1 - F(\gamma_2) + F(h) - F(y)) - (\gamma_3 - h) f(\gamma_3) [(\gamma_2 - y) u_3 - (\gamma_2 - y) u_2]. \quad (21)

By Claim 9, if no comment outcome is implementable, it must be that (γ2−y)u3≤(γ3−y)u2(\gamma_2 - y)u_3 \leq (\gamma_3 - y)u_2. Consequently, the sign of the second term of (21) must be positive, and the first term has a strictly negative sign. Hence as γ3\gamma_3 decreases, the expert's ex-ante payoff in her preferred equilibrium strictly decreases if the second term is larger in absolute value, which establishes the statement.

B.3 Equilibrium Refinement

It is natural to ask whether the equilibria of the disclosure game considered in this paper are credible in that they survive certain equilibrium refinements. We consider the following two equilibrium refinements:

  • The Never-a-Weak-Best-Response (NWBR) Criterion, proposed by Cho and Kreps (1987), is a strengthening of a few equilibrium refinements that are extensively used in the literature, which includes the Intuitive Criterion, D1, and D2.31
  • The Grossman-Perry-Farrell equilibrium, proposed by Bertomeu and Cianciaruso (2018), is based on the perfect sequential equilibrium of Grossman and Perry (1986) and neologism-proofness of Farrell (1993).

It can be shown that every PE of the disclosure game we study is a Grossman-Perry-Farrell equilibrium, and every PE outcome survives the NWBR Criterion. We use the term “type” instead of “state” henceforth to ease exposition.

B.3.1 Never-a-Weak-Best-Response (NWBR) Criterion

We introduce some notation first. For any m∈Cm \in \mathcal{C}, let MBR(m)MBR(m) denote the set of all mixed strategy best responses for the receiver to message mm for any belief β(⋅∣m)\beta(\cdot | m).32 Moreover, let vω∗v_\omega^* denote the equilibrium payoff of type ω\omega. Finally, for any equilibrium and an off-path message mm, define

D(ω,m)={ρ∈MBR(m):vω∗<∑i∈Nuiρi},D(\omega, m) = \left\{ \rho \in MBR(m) : v_\omega^* < \sum_{i \in N} u_i \rho_i \right\},

and

D0(ω,m)={ρ∈MBR(m):vω∗=∑i∈Nuiρi};D^0(\omega, m) = \left\{ \rho \in MBR(m) : v_\omega^* = \sum_{i \in N} u_i \rho_i \right\};

in words, D(ω,m)D(\omega, m) is the set of mixed strategy best responses that make type ω\omega strictly prefer mm to her equilibrium message, and D0(ω,m)D^0(\omega, m) is the set of mixed strategy best responses that make type ω\omega exactly indifferent.

Definition 5. An equilibrium (σ,τ,β)(\sigma, \tau, \beta) survives the NWBR criterion if for every m∈Cm \in \mathcal{C} and any ω,ω′∈[0,1]\omega, \omega' \in [0, 1], D0(ω′,m)⊆∪ω≠ω′D(ω,m)D^0(\omega', m) \subseteq \cup_{\omega \neq \omega'} D(\omega, m) implies that ω′∉supp β(⋅∣m)\omega' \notin \text{supp } \beta(\cdot | m).

Claim 11. For every PE (σ,τ,β)(\sigma, \tau, \beta), there exists β′\beta' such that (σ,τ,β′)(\sigma, \tau, \beta') survives the NWBR criterion.

Proof. Fix a PE (σ,τ,β)(\sigma, \tau, \beta), and let B\mathcal{B} denote the associated partition. For every m∉Bm \notin \mathcal{B}, let ℓ=min⁡{i:m∩Bi≠∅}\ell = \min\{i : m \cap B_i \neq \emptyset\}. Let β′\beta' be such that β′(⋅∣Bi)=β(⋅∣Bi)\beta'(\cdot | B_i) = \beta(\cdot | B_i) for all i=0,…,n−1i = 0, \dots, n-1, and for any m∉Bm \notin \mathcal{B}, let

β′(min⁡m∩Bℓ∣m)=1.(22)\beta'(\min m \cap B_\ell | m) = 1. \tag{22}

By the definition of PE, the receiver never mixes on path, and hence for any ω′∈[0,1]\omega' \in [0, 1], D0(ω′,m)={δk}D^0(\omega', m) = \{\delta_k\} if and only if ω∈Bk∖(∪i>kBi)\omega \in B_k \setminus (\cup_{i>k} B_i), where δk\delta_k is the Dirac measure at action kk. Furthermore, define

M={k∈N:k is such that m∩Bk≠∅};M = \{k \in N : k \text{ is such that } m \cap B_k \neq \emptyset\};

then the lowest action in MM is ℓ\ell. Now for any ω′∈[0,1]\omega' \in [0, 1],

⋃ω≠ω′D(ω,m)={ρ∈Δ(M):supp ρ⊆{ak,ak+1} with k≥ℓ, and ρ(aℓ)<1}.\bigcup_{\omega \neq \omega'} D(\omega, m) = \{\rho \in \Delta(M) : \text{supp } \rho \subseteq \{a_k, a_{k+1}\} \text{ with } k \geq \ell, \text{ and } \rho(a_\ell) < 1\}.

Then D0(ω′,m)⊆⋃ω≠ω′D(ω,m)D^0(\omega', m) \subseteq \bigcup_{\omega \neq \omega'} D(\omega, m) if and only if D0(ω′,m)={δk}D^0(\omega', m) = \{\delta_k\} with k>ℓk > \ell, which is in turn equivalent to ω′∈⋃k>ℓ(Bk∖(⋃i>kBi))\omega' \in \bigcup_{k > \ell} (B_k \setminus (\bigcup_{i > k} B_i)). Then (22) implies that ω′∉supp β′(⋅∣m)\omega' \notin \text{supp } \beta'(\cdot | m). Consequently, (σ,τ,β′)(\sigma, \tau, \beta') survives the NWBR criterion. ■

B.3.2 Grossman-Perry-Farrell Equilibrium

Definition 6. Fix a PE (σ,τ,β)(\sigma, \tau, \beta). Say that m∗∈Cm^* \in \mathcal{C} is a self-signaling set if33

m∗={ω∈m∗:v(E[ω∣ω∈m∗])>v(E[ω∣ω∈σ(ω)])}.m^* = \{\omega \in m^* : v(\mathbb{E}[\omega | \omega \in m^*]) > v(\mathbb{E}[\omega | \omega \in \sigma(\omega)])\}.

An PE is a Grossman-Perry-Farrell equilibrium if there does not exist a self-signaling set.

Claim 12. Every PE is a Grossman-Perry-Farrell equilibrium.

Proof. Fix a PE (σ,τ,β)(\sigma, \tau, \beta), and let B\mathcal{B} denote the associated partition. Suppose there exists a self-signaling set m∗m^*. Let

kˉ≔max⁡{i∈N:there exists ω∈m∗ such that σ(ω)=Bi}.\bar{k} := \max \{i \in N : \text{there exists } \omega \in m^* \text{ such that } \sigma(\omega) = B_i\}.

Because m∗m^* is a self-signaling set, it must be that E[ω∣ω∈m∗]≥γkˉ+1\mathbb{E}[\omega | \omega \in m^*] \geq \gamma_{\bar{k}+1}. But then revelation proofness of B\mathcal{B} implies that there must exist ω′∈m∗\omega' \in m^* such that σ(ω′)=Bj\sigma(\omega') = B_j with j≥kˉ+1j \geq \bar{k} + 1, a contradiction. ■

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