Lecture 1 (1/5)

Lecture 2 (1/7)

Example 1:

Let be a particle with the following ODE

Let . Then

such that

Upon solving this ODE, we get

So, as .

Example 2:

We could have a double well

Desmos Graph

In the SDE case, given

In order, the terms are:

  • is the change
  • is the deterministic force
  • is some “random” force. In particular, is the Brownian increment, or “white noise”.

So when we calculate the position of the particle via , the term tells us how we move via the force, with some randomness via . This leads to

  • new frequency in a system

what does frequency mean?

  • new types of resonance/transport effects.

Lecture 3 (1/9)

Reference for this section is Rubinstein Ch.2

Lecture 4 (1/12)

Reference: Rubinstein Ch. 2, 2.4, 2.3.4

Lecture 5 (1/14)

  • Acceptance-Rejection
  • [[Acceptance-Rejection#theorem-uniformity-on-region-a|Theorem (Uniformity on Region )]]
  • [[Acceptance-Rejection#theorem-from-uniformity-on-a-to-target-fx|Theorem (From Uniformity on to Target )]]
  • [[Acceptance-Rejection#theorem-a-r-generates-z-sim-f|Theorem (A-R Generates )]]

Lecture 6 (1/16)

Lecture 7 (1/21)

Lecture 8 (1/23)

Lecture 9 (1/26)

  • Review of previous lectures.
  • Markov Chains. For the purposes of this class we only consider Discrete Time/State Homogeneous Markov Chains
  • Stochastic Process

Lecture 10 (1/28)

Lecture 11 (1/31)

Lecture 12 (2/2)

Lecture 13 (2/4)

Lecture 14 (2/6)

Lecture 15 (2/9)

  • Review for midterm

Lecture 16 (2/13)

Lecture 17 (2/19)

Lecture 18 (2/20)

Lecture 19 (2/23)

Lecture 20 (2/25)

Lecture 21 (2/27)

Lecture 22 (3/2)

Lecture 23 (3/4)

Lecture 24 (3/6)

Lecture 25 (3/9)

Lecture 26 (3/11)

Lecture 27 (3/13)

  • Finals review