Cardinality of Sample Space for Brownian Motion

In summary, the conversation discusses the cardinality of the sample space Ω in a Brownian Motion process, with the conclusion that it is an uncountable set. The comparison is made to a discrete time stochastic process with a countable set of outcomes, and the possibility of continuous stock prices being samples from an underlying continuous process is also mentioned. The question of whether the Brownian motion sigma algebra adequately models the evolution of the stock price process is raised.
  • #1
J.P.
5
0
Hello,

Given a Brownian Motion process B(t) for 0≤t≤T,
we can write it more explicitly as B(t,ω) where ω[itex]\in[/itex]Ω,
where Ω is the underlying sample space.

My question is: what is the cardinality of Ω. I.e. what is |Ω|?

My thoughts are that it is an uncountable set, based on the observation
that B(t) ~ N(0,t), and thus takes values in the real numbers.

Am I correct, is this simple observation enough, or is a more rigorous
proof needed?
 
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  • #2
J.P. said:
Hello,

My question is: what is the cardinality of Ω. I.e. what is |Ω|?

My thoughts are that it is an uncountable set, based on the observation
that B(t) ~ N(0,t), and thus takes values in the real numbers.

It depends on whether you want to consider the space in terms of points or trajectories. In a Euclidean space, you need only consider the points in what could be considered a vector space with every point being described by a tuple. You would consider the particle as "jumping" from point to point. The history of the particle's motion would be the ordered progression of tuples. In this case you are dealing with a countable set.

If you want to consider it terms of a diffusion model based on a normal distribution around the point of origin, the space could be considered as an uncountable set or continuum.
 
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  • #3
Thanks for the response SW VandeCarr.
SW VandeCarr said:
The history of the particle's motion would be the ordered progression of tuples. In this case you are dealing with a countable set.

I'm not sure if I understand what "countable set" you mean. Certainly the ordered list of tuples would be countable. But I'm interested in Ω.

Even if we are dealing with an ordered list of tuples (let's assume we are dealing with one dimension), wouldn't each element of this list be chosen out of ℝ? I.e. if we choose the n-th tuple with the random variable X:Ω→ℝ then we would need an ω[itex]\in[/itex]Ω for every possible x[itex]\in[/itex]ℝ, and thus |Ω|=|ℝ|.

Thanks again.
 
  • #4
J.P. said:
Hello,

Given a Brownian Motion process B(t) for 0≤t≤T,
we can write it more explicitly as B(t,ω) where ω[itex]\in[/itex]Ω,
where Ω is the underlying sample space.

My question is: what is the cardinality of Ω. I.e. what is |Ω|?

My thoughts are that it is an uncountable set, based on the observation
that B(t) ~ N(0,t), and thus takes values in the real numbers.

Am I correct, is this simple observation enough, or is a more rigorous
proof needed?

The set of sample paths in a Brownian motion is uncountable. B(t) is the height of the path at time t. It is normally distributed. So there must be uncountably many different paths at time,t
 
  • #5
Ok, thanks lavinia. Makes sense.

The reason I ask is because I have only dealt with stochastic processes in discrete time, in the case of stock prices. For example, we may have a stock St where t=0,1,2, that can go up or down between time 0 and 1, and again up or down between time 1 and 2. Thus there would be four possible outcomes (up up, up down, down up, down down) corresponding to ω1, ω2, ω3 and ω4. So it is easy to visualize how the "state of the world" (ω) corresponds to the value of S2.

I have been trying to get an analogous understanding in the continuous case for Brownian motion. So I guess it works exactly the same, except there are now an uncountable number of different "states of the world" corresponding to the terminal value B(T) . But even further, for a given B(T) there would be an uncountable number of "states of the world" corresponding to the different paths that could potentially get there.
 
  • #6
J.P. said:
Ok, thanks lavinia. Makes sense.

The reason I ask is because I have only dealt with stochastic processes in discrete time, in the case of stock prices. For example, we may have a stock St where t=0,1,2, that can go up or down between time 0 and 1, and again up or down between time 1 and 2. Thus there would be four possible outcomes (up up, up down, down up, down down) corresponding to ω1, ω2, ω3 and ω4. So it is easy to visualize how the "state of the world" (ω) corresponds to the value of S2.

I have been trying to get an analogous understanding in the continuous case for Brownian motion. So I guess it works exactly the same, except there are now an uncountable number of different "states of the world" corresponding to the terminal value B(T) . But even further, for a given B(T) there would be an uncountable number of "states of the world" corresponding to the different paths that could potentially get there.

That is correct.

BTW: One might be able to think of actual stock prices, prices where the stock actually trades, as samples from an underlying continuous process. The continuous Brownian motion is always taking place but only observed when it materializes in a trade price. The advantage of this point of view is that you do not need to have a fixed time increment to describe the successive prices. In a discrete model it seems that you would need to assume that the stock trades at specific points in time.

Such a model could also allow for sudden prices changes e.g. reactions to unexpected economic reports, as a sample from an outlier continuous path in the tail of the normal distribution.

So what would the stochastic process be? One starts with a Brownian motion then samples it at random times?

The question I would ask is whether the evolution of the underlying sigma algebra of the stock price process is adequately modeled by the Brownian motion sigma algebra which is generated entirely by paths of prices.
 
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  • #7
J.P. said:
Thanks for the response SW VandeCarr.I'm not sure if I understand what "countable set" you mean. Certainly the ordered list of tuples would be countable. But I'm interested in Ω.

Even if we are dealing with an ordered list of tuples (let's assume we are dealing with one dimension), wouldn't each element of this list be chosen out of ℝ? I.e. if we choose the n-th tuple with the random variable X:Ω→ℝ then we would need an ω[itex]\in[/itex]Ω for every possible x[itex]\in[/itex]ℝ, and thus |Ω|=|ℝ|.

Thanks again.

Sorry I didn't back to you sooner. Yes, I agree with you and Lavinia that [itex]\Omega[/itex] is an uncountable set and I referred to the diffusion model myself in my previous post. My only point was that in two or more dimensions, the physical model of Brownian motion is imagined in terms of directed line segments joined at (countable) singular points. I guess one could argue that the space itself is continuous, if that's what you mean. However, wouldn't that argument imply that discrete probability distributions, such as the binomial distribution, are in some sense continuous since each of n points maps to R in terms of its probability?
 
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  • #8
lavinia said:
So what would the stochastic process be? One starts with a Brownian motion then samples it at random times?

Well I understand that the standard stock price model is given by the stochastic differential equation dSt = μStdt + σStdWt with solution St = S0exp(Wt + (-0.5σ2)t). So this would be a stochastic processes, depending on Brownian motion, and I suppose the times that investors needed access to prices could be considered random. Is this what you had in mind? However this does not capture the jumps due to sudden events etc. I don't know how to incorporate that into the above.

lavinia said:
The question I would ask is whether the evolution of the underlying sigma algebra of the stock price process is adequately modeled by the Brownian motion sigma algebra which is generated entirely by paths of prices.

I'm going to guess that the information revealed over time by the Brownian motion is the same information needed to model the stock price (since the Brownian motion is the only random part of the stock price), but I don't know enough to be sure I understand what you're asking.

SW VandeCarr said:
My only point was that in two or more dimensions, the physical model of Brownian motion is imagined in terms of directed line segments joined at (countable) singular points.
Ok, such as if you were simulating a Brownian path numerically on a computer.

SW VandeCarr said:
I guess one could argue that the space itself is continuous, if that's what you mean. However, wouldn't that argument imply that discrete probability distributions, such as the binomial distribution, are in some sense continuous since each of n points maps to R in terms of its probability?

I don't think so. It is part of the definition of Brownian Motion that it depends continuously on its parameter.
 
  • #9
J.P. said:
Well I understand that the standard stock price model is given by the stochastic differential equation dSt = μStdt + σStdWt with solution St = S0exp(Wt + (-0.5σ2)t). So this would be a stochastic processes, depending on Brownian motion, and I suppose the times that investors needed access to prices could be considered random. Is this what you had in mind? However this does not capture the jumps due to sudden events etc. I don't know how to incorporate that into the above.

What i meant was that a continuous Brownian motion can never be observed in actual prices. So if you believed that such a process was correct then actual stock prices are a random time sampling of this process. So the observed process is not Brownian motion. I am sure what it is.

Outlier events have some probability in Brownian motion. So what appears to be a jump might actually be the discrete time observation of a continuous path that happens to moved rapidly away from the current price.

Actual stock returns do not appear to follow a Brownian motion. Much statistical evidence suggests that outlier events occur too frequently. the distribution has fat tails.

Also it is possible that the volatility is not constant but actually stochastic. There is a large body of statistical research on that question as well.

The usual model that you wrote down is useful for the pricing of options and is not at all considered to be a true model especially over medium to longer time frames. First of all, the riskless rate will change significantly over long time periods and secondly it is not at all clear that the drift rate should be constant except over short time periods.

I'm going to guess that the information revealed over time by the Brownian motion is the same information needed to model the stock price (since the Brownian motion is the only random part of the stock price), but I don't know enough to be sure I understand what you're asking.

In an efficient market,all of the information relevant to the stock price is incorporated into the price. In a Brownian motion the only information is the history of the stock price. I just said that this may not actually model the information set.
 
  • #10
Thanks lavinia, you've given me a bit to think/read about.
 

Related to Cardinality of Sample Space for Brownian Motion

What is the "Cardinality of Sample Space" for Brownian Motion?

The "Cardinality of Sample Space" refers to the number of possible outcomes in a given experiment or scenario. In the case of Brownian Motion, this refers to the number of possible paths that a particle can take as it moves randomly in a fluid.

Why is the "Cardinality of Sample Space" important in Brownian Motion?

The "Cardinality of Sample Space" is important in Brownian Motion because it helps us understand the behavior of particles in a fluid. By knowing the number of possible paths a particle can take, we can make predictions about its movement and better understand the phenomena of diffusion.

How is the "Cardinality of Sample Space" calculated for Brownian Motion?

The "Cardinality of Sample Space" for Brownian Motion can be calculated by using a mathematical formula that takes into account the number of dimensions in the system, the time interval, and the step size of the particle. This formula is known as the Wiener–Kolmogorov equation.

Can the "Cardinality of Sample Space" change in Brownian Motion?

Yes, the "Cardinality of Sample Space" can change in Brownian Motion. This is because the number of possible paths a particle can take depends on the time interval and the step size, which can vary depending on the conditions of the system. As these variables change, the "Cardinality of Sample Space" can also change.

What is the relationship between the "Cardinality of Sample Space" and the diffusion coefficient in Brownian Motion?

The "Cardinality of Sample Space" and the diffusion coefficient in Brownian Motion are directly related. The diffusion coefficient is a measure of the rate at which a particle diffuses in a fluid, and it is inversely proportional to the "Cardinality of Sample Space". This means that as the "Cardinality of Sample Space" increases, the diffusion coefficient decreases, and vice versa.

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