Intersection of two independent events

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Discussion Overview

The discussion centers around the concept of independent events in probability theory, specifically focusing on the intersection of two independent events and the corresponding sample space. Participants explore the definitions and implications of independence, conditional probability, and the construction of sample spaces through Cartesian products.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant states that for independent events A and B, the probability of their intersection is given by P(A intersection B) = P(A) * P(B), but expresses confusion regarding the sample space.
  • Another participant explains that the sample space for independent events can be represented as the Cartesian product of the two sets, C = A X B.
  • A different participant questions how the sample space would work if A and B were dependent, suggesting that the sample space would differ for each event.
  • One participant asserts that the sample space consists of combinations such as {h,1}, {t,1}, {h,2}, etc., indicating a direct product space.
  • Another participant clarifies that to discuss joint probabilities, the event spaces must be combined into a Cartesian product, emphasizing the relationship between the independent event spaces and their probability functions.
  • One participant notes that their discussion was focused on the event space without delving into probability measures, suggesting that applying probabilities is a subsequent step.

Areas of Agreement / Disagreement

Participants express varying interpretations of the sample space and the implications of independence and dependence. There is no consensus on the specifics of the sample space or the treatment of probabilities in relation to the Cartesian product.

Contextual Notes

The discussion includes assumptions about independence and the structure of sample spaces that may not be universally accepted. The relationship between event spaces and their probability measures is also noted as a complex layer not fully resolved in the conversation.

Avichal
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If A and B are two independent events then P(A intersection B) = P(A).P(B)
I don't refute this but it confuses me. What is the sample space in this?
For eg: - If A is the event that we get Head while tossing a coin and B is the event that we get 2 while throwing a die, then what will we be the sample space? Is it {H, T} or {1, 2, 3, 4, 5, 6}?
 
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Hey Avichal.

If you have two sets A and B that are independent, then the state space for all combinations is the Cartesian product C = A X B (a belonging to A, B belonging to b, c = (a,b) belonging to C).

With regards to independence, the way you get the definition is the following:

P(A|B) = P(A and B)/P(B) [definition of conditional probability].

If A is independent from any other random variable then P(A|B) = P(A). This implies:

P(A|B) = P(A) = P(A and B)/P(B). Multiplying everything by P(B) gives

P(A and B) = P(A)*P(B) and thus proved.
 
Hmm ... If A and B are dependent then P(A|B) = P(A and B) / P(B)
Here what will be the sample space? For B it will be different compared to A and B. So how does it work?
 
The sample space is the direct product space, i.e. the elements are {h,1}, {t,1}, {h,2}, etc.
 
chiro said:
If you have two sets A and B that are independent, then the state space for all combinations is the Cartesian product C = A X B (a belonging to A, B belonging to b, c = (a,b) belonging to C).
Hi Chiro,
I think that's a bit confusing. Perhaps you meant this:
If you have two sets A and B that are subsets of apparently unrelated event spaces Ω1, Ω2, then in order to discuss joint probabilities etc. you must first combine the event spaces. Given their independence as spaces (not to be confused with independence of events within a space), the appropriate combination is the Cartesian product ΩC = Ω1 X Ω2. Each space has its own probability function, but they are related. A ⊂ Ω1 maps naturally to A X Ω2 ⊂ ΩC. P1(A) = PC(A X Ω2) etc. Now we can understand the joint event "A and B" as (A X Ω2) ∩ (Ω1 X B) = A X B.
 
I was only talking about the event space without reference to a probability measure. The measure and filtration/sigma-algebras come on top of this, but I wasn't really getting specifically into this (as you have).

This was just a way to say that if you can have every permutation of possibilities from both sets, then the cartesian product will give you a state-space that describes such possibilities.

Applying zero probabilities or other constraints is further step on top of this.
 

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