Rearranging a formula (Multivariate Gaussian function)

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The discussion focuses on rearranging the multivariate Gaussian likelihood function, specifically the expression p(y|θ). The user expands the exponent in the original function and attempts to express it in a new form involving constants and a matrix L. They derive relationships for L and θ0, noting that L = A^TA and θ0 = L^(-1)A^Tb. However, they encounter difficulties in determining the constant L0 and express confusion about the exponential component in the context of their calculations. The conversation highlights the complexities involved in matching coefficients and ensuring the correct formulation of the Gaussian function.
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Homework Statement


See image, p(y|θ) is the Likelihood function which has to be rearranged in the form of equation (3). θ is a vector variable.
1zobx9u.png


Homework Equations


None?

The Attempt at a Solution


I first expanded the exponent in the original function, equation (2).

(b-A\theta)^T(b-A\theta)=b^Tb - b^TA\theta - \theta^T A^T b + \theta^T A^T A \theta

Now suppose I can write the function equivalently as

C \exp\left( -\frac{1}{2} (\theta - \theta_0)^T L (\theta - \theta_0) \right)

where C represents the same constant multiplying with exp in equation (2). In this case, the exponential parts must be the same. So:

b^Tb - b^TA\theta - \theta^T A^T b + \theta^T A^T A \theta = \theta^TL\theta - \theta^TL\theta_0 - \theta_0^TL\theta + \theta_0^TL\theta_0

If this this expression is true for all θ, then all coefficients of (...)θ , θT(...) , θT(...)θ and the constants must match.

So L = ATA and θ0=L-1ATb.

Now I don't know how to get L0. (equation (5) ). I only have this condition left from my assumption about the constants above:

bTb=θT00

There just don't seem to be enough terms in either exponent to allow the exponential part of L0. I don't think I can add and subtract anything either...

Any ideas?
 
Last edited:
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Pi-Bond said:

Homework Statement


See image, p(y|θ) is the Likelihood function which has to be rearranged in the form of equation (3). θ is a vector variable.
1zobx9u.png


Homework Equations


None?

The Attempt at a Solution


I first expanded the exponent in the original function, equation (2).

(b-A\theta)^T(b-A\theta)=b^Tb - b^TA\theta - \theta^T A^T b + \theta^T A^T A \theta

Now suppose I can write the function equivalently as

C \exp\left( -\frac{1}{2} (\theta - \theta_0)^T L (\theta - \theta_0) \right)

where C represents the same constant multiplying with exp in equation (2). In this case, the exponential parts must be the same. So:

b^Tb - b^TA\theta - \theta^T A^T b + \theta^T A^T A \theta = \theta^TL\theta - \theta^TL\theta_0 - \theta_0^TL\theta + \theta_0^TL\theta_0

If this this expression is true for all θ, then all coefficients of (...)θ , θT(...) , θT(...)θ and the constants must match.

So L = ATA and θ0=LATb.

Now I don't know how to get L0. (equation (5) ). I only have this condition left from my assumption about the constants above:

bTb=θT00

There just don't seem to be enough terms in either exponent to allow the exponential part of L0. I don't think I can add and subtract anything either...

Any ideas?

Try to show that
(b-A\theta)^T(b-A\theta) = (\theta - \theta_0)^T L (\theta - \theta_0) + K for some matrix L and some constant K, and for ##\theta_0## as given in the question.
 
Ok.

(b-A\theta)^T(b-A\theta)=b^Tb - b^TA\theta - \theta^T A^T b + \theta^T A^T A \theta
= b^Tb - (L L^{-1}A^T b)^T\theta - \theta^T L( L^{-1}A^T b) + \theta^T L \theta
= b^Tb + \theta_0^T L \theta - \theta^T L \theta_0 + \theta^T L \theta
= b^Tb + (\theta-\theta_0)^T L \theta - \theta^T L \theta_0
= b^Tb + (\theta-\theta_0)^T L \theta - (\theta-\theta_0)^T L \theta_0 -\theta_0^T L \theta_0
= b^Tb + (\theta-\theta_0)^T L (\theta-\theta_0)-\theta_0^T L \theta_0

I used the fact that LT=L=ATA.

On the basis of this it seems K = bTb - θ0T0

I still can't see the origin of L0 here though..
 
Bump. I haven't been able to find any leads. Anyone have an idea?
 
I'm somewhat confused by the fact that if L = A^TA and \theta_0 = L^{-1}A^Tb then L^{-1} = A^{-1}(A^T)^{-1} so that
A\theta_0 = AL^{-1}A^Tb = A(A^{-1}(A^T)^{-1})A^Tb = b
which means that b - A\theta_0 = b - b = 0. So I'm at a loss to explain why the author has included the exponential in \mathcal{L}_0, when its value appears to be \exp(0) = 1.

On the other hand, I was able to show (using the additional fact that L is symmetric so that (L^T)^{-1} = (L^{-1})^T = L^{-1}) that
(\theta - \theta_0)^TL(\theta - \theta_0) = (A\theta - b)^T(A\theta - b)<br /> = (b - A\theta)^T(b - A\theta)
It's just a case of expanding the left hand side, substituting the definitions of L and \theta_0 and simplifying.
 
pasmith said:
I'm somewhat confused by the fact that if L = A^TA and \theta_0 = L^{-1}A^Tb then L^{-1} = A^{-1}(A^T)^{-1}
Ignore that: A is not square, so cannot be invertible.

The aim is to show that (b - A\theta)^T(b - A\theta) = (b - A\theta_0)^T(b - A\theta_0) + (\theta - \theta_0)^T(\theta - \theta_0)

Now the left hand side is
b^Tb - b^TA\theta - \theta^TA^Tb + \theta^TA^TA\theta

The right hand side is
b^Tb - b^TA\theta_0 - \theta_0^TA^Tb + \theta_0^TA^TA\theta_0<br /> + \theta^TL\theta - \theta^TL\theta_0 - \theta_0^TL\theta + \theta_0^TL\theta_0\\<br /> = b^Tb - (b^TA\theta_0 + \theta_0^TA^Tb) + 2\theta_0^TL\theta_0<br /> + \theta^TL\theta - \theta^TL\theta_0 - \theta_0^TL\theta \\<br /> = b^Tb - 2b^TAL^{-1}A^Tb + 2b^TAL^{-1}A^Tb<br /> + \theta^TA^TA\theta - \theta^TA^Tb - b^TA\theta \\<br /> = b^Tb -b^TA\theta - \theta^TA^Tb + \theta^TA^TA\theta<br />
as required.
 
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Edit: there seems to be a mistake between the second and third lines. You go from -(bT0 + θ0TATb) to -2bT(...)+2bT(...)

The plus sign should be minus, and I'm not sure of where the factor of 2 comes from. Anyway I will investigate your approach.
 
Last edited:

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