Lecture 2

Lecture 2#

Likelihood Function#

Assuming a gaussian error distribution for the data,

\[ P(D \mid \theta) = \prod_{i=1}^n{\frac{1}{\sqrt{2\pi\sigma_i^2}}\exp\left(\frac{-(y_i - \hat y_i)^2}{2\sigma_i^2}\right)} \]

Markov Chain Monte Carlo (MCMC)#

A method to sample the posterior \(P(\theta | D)\).

MCMC Hasting#

  1. Begin with starting point \(\theta_0\)

  2. Propose \(\theta_{t+1}\) based on sampling a random proposal distribution \(J(\theta_{t+1} \mid \theta_t)\).

  3. Keep it with a probability proportional to if it improves the posterior ratio else try again:

    \[\frac{P(\theta_{t+1} | D)}{P(\theta_{t} | D)}\]

Affine Invariant MCMC#

Adding multiple samplers (aka walkers) we group each walk as a pairs. The next step step for a walker is towards its partner’s line of sight. A new partner is assigned at every step.

Goodness of Fit#

  • Geweke Score:

    Take the end and begining of the chain and computer the score as, $\( \frac{\bar \theta_e - \bar \theta_b}{\sqrt{\text{Var}[\theta_e]\text{Var}[\theta_b]}} \)$

  • G-R Statistics

  • Acceptance Fraction

  • Autocorrelation Function

    • Typicall have burn-in period 5 times larger than the ACF convergence number.

Periodogram#

A periodogram can be produced by a fourier transform of some time-series data:

\[ \hat y(f) \equiv \int_{-\infty}^{\infty}y(t)e^{-i2\pi ft}~\mathrm d t \]

When plotting a periodogram, we often plot the power spectrum over frequency,

\[ \mathcal P(f) \equiv |\hat y(f)|^2 \]

Pratically, an unbounded infinite signal is not possible thus we apply whats called fast fourier transform,

\[ \hat y(f) = \sum_{n=1}^N y(n\Delta t)e^{-i2\pi fn\Delta t} \]

  • \(\Delta t\) : Sampling interval.

In irregular sampling interval you get the Lomb-Scargle Periodogram. To model data with a single frequency,

\[ \hat y = y_0 + A_f \sin\left(2\pi f\left[t - \phi_f\right]\right) \]
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