User:IssaRice/Aumann's agreement theorem: Difference between revisions
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In the form of <math>E</math> above, we can change <math>A</math> to be any subset of <math>\Omega</math> and <math>q_1, q_2</math> to be any numbers in <math>[0,1]</math>. We can also set the state of the world to be any <math>\omega\in\Omega</math>. The agreement theorem says that as we vary these parameters, if we ever find that <math>(I\wedge J)(\omega) \subset E</math>, then we must have <math>q_1 = q_2</math>. | In the form of <math>E</math> above, we can change <math>A</math> to be any subset of <math>\Omega</math> and <math>q_1, q_2</math> to be any numbers in <math>[0,1]</math>. We can also set the state of the world to be any <math>\omega\in\Omega</math>. The agreement theorem says that as we vary these parameters, if we ever find that <math>(I\wedge J)(\omega) \subset E</math>, then we must have <math>q_1 = q_2</math>. | ||
Define <math>X((x,y)) = x+y</math>. | |||
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! <math>\omega</math> !! <math>A</math> !! <math>q_1</math> !! <math>q_2</math> !! Explanation | |||
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| (2, 3) || <math>2 \leq X \leq 6</math> || 1 || 1 || Given these parameters, <math>E = (I\wedge J)(\omega)</math> so <math>E</math> is common knowledge. This satisfies the requirement of the agreement theorem, and indeed 1=1. | |||
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| (2, 3) || <math>X = 4</math> || 1/3 || 1/3 || Given these parameters, <math>E = (I\wedge J)(\omega)</math> so <math>E</math> is common knowledge. This satisfies the requirement of the agreement theorem, and indeed 1/3=1/3. | |||
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| (2, 3) || <math>X = 4</math> || 1/3 || 1/3 || Given these parameters, <math>E = \{2,3\}\times\{2,3\}</math>, which is not a superset of <math>(I\wedge J)(\omega)</math>, so <math>E</math> is not common knowledge. Nonetheless, 1/3=1/3. (Is this a case of mutual knowledge that is not common knowledge?) | |||
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<ref>Tyrrell McAllister. [https://web.archive.org/web/20110725162431/http://dl.dropbox.com/u/34639481/Aumann_agreement_theorem.pdf "Aumann's agreement theorem"]. July 7, 2011.</ref> | <ref>Tyrrell McAllister. [https://web.archive.org/web/20110725162431/http://dl.dropbox.com/u/34639481/Aumann_agreement_theorem.pdf "Aumann's agreement theorem"]. July 7, 2011.</ref> | ||
Revision as of 23:31, 24 August 2018
Hal Finney's example
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One of the assumptions in the agreement theorem is that is common knowledge. This seems like a pretty strange requirement, since it seems like the posterior probability of can never change no matter what else the agents condition on in addition to . For example, what if we bring in agent 3 and make the posteriors common knowledge again?
What if we take and say that agent 1 knows ?
In the form of above, we can change to be any subset of and to be any numbers in . We can also set the state of the world to be any . The agreement theorem says that as we vary these parameters, if we ever find that , then we must have .
Define .
| Explanation | ||||
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| (2, 3) | 1 | 1 | Given these parameters, so is common knowledge. This satisfies the requirement of the agreement theorem, and indeed 1=1. | |
| (2, 3) | 1/3 | 1/3 | Given these parameters, so is common knowledge. This satisfies the requirement of the agreement theorem, and indeed 1/3=1/3. | |
| (2, 3) | 1/3 | 1/3 | Given these parameters, , which is not a superset of , so is not common knowledge. Nonetheless, 1/3=1/3. (Is this a case of mutual knowledge that is not common knowledge?) |
References
- ↑ Tyrrell McAllister. "Aumann's agreement theorem". July 7, 2011.
- ↑ Wei Dai. "Probability Space & Aumann Agreement". December 10, 2009.
- ↑ Robert J. Aumann. "Agreeing to Disagree". November 1976.
- ↑ https://math.stackexchange.com/questions/303834/common-knowledge-and-concept-of-coarsening-partition
- ↑ John Geanakoplos. "Common Knowledge".