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Talk:Quadratic form (statistics)

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cov [ ε T Λ 1 ε , ε T Λ 2 ε ] = 2 tr [ Λ 1 Σ Λ 2 Σ ] + 4 μ T Λ 1 Σ Λ 2 μ {\displaystyle \operatorname {cov} \left[\epsilon ^{T}\Lambda _{1}\epsilon ,\epsilon ^{T}\Lambda _{2}\epsilon \right]=2\operatorname {tr} \left[\Lambda _{1}\Sigma \Lambda _{2}\Sigma \right]+4\mu ^{T}\Lambda _{1}\Sigma \Lambda _{2}\mu } {\displaystyle \operatorname {cov} \left[\epsilon ^{T}\Lambda _{1}\epsilon ,\epsilon ^{T}\Lambda _{2}\epsilon \right]=2\operatorname {tr} \left[\Lambda _{1}\Sigma \Lambda _{2}\Sigma \right]+4\mu ^{T}\Lambda _{1}\Sigma \Lambda _{2}\mu }

If Λ 1 T = Λ 2 {\displaystyle \Lambda _{1}^{T}=\Lambda _{2}} {\displaystyle \Lambda _{1}^{T}=\Lambda _{2}} and they are not symmetric, the above formula contradicts the variance formula, since in that case ε T Λ 1 ε = ε T Λ 2 ε {\displaystyle \epsilon ^{T}\Lambda _{1}\epsilon =\epsilon ^{T}\Lambda _{2}\epsilon } {\displaystyle \epsilon ^{T}\Lambda _{1}\epsilon =\epsilon ^{T}\Lambda _{2}\epsilon }. How to resolve this? Btyner 04:48, 3 April 2006 (UTC) [reply ]

Yikes, the expression was wrong in the case of nonsymmetric Λ {\displaystyle \Lambda } {\displaystyle \Lambda }s. I have noted the symmetric requirement, and added a section showing how to derive the general expression. Btyner 18:24, 6 April 2006 (UTC) [reply ]

Is symmetry really necessary for the expectation result?

[edit ]

Nothing in the usual proof of the result for expectation seems to require symmetry of Λ {\displaystyle \Lambda } {\displaystyle \Lambda }:

E ( ε T Λ ε ) {\displaystyle \operatorname {E} (\epsilon ^{T}\Lambda \epsilon )} {\displaystyle \operatorname {E} (\epsilon ^{T}\Lambda \epsilon )} = E [ tr ( ε T Λ ε ) ] {\displaystyle \operatorname {E} [\operatorname {tr} (\epsilon ^{T}\Lambda \epsilon )]} {\displaystyle \operatorname {E} [\operatorname {tr} (\epsilon ^{T}\Lambda \epsilon )]}
= E [ tr ( Λ ε ε T ) ] {\displaystyle \operatorname {E} [\operatorname {tr} (\Lambda \epsilon \epsilon ^{T})]} {\displaystyle \operatorname {E} [\operatorname {tr} (\Lambda \epsilon \epsilon ^{T})]}
= tr ( Λ E [ ε ε T ] ) {\displaystyle \operatorname {tr} (\Lambda \operatorname {E} [\epsilon \epsilon ^{T}])} {\displaystyle \operatorname {tr} (\Lambda \operatorname {E} [\epsilon \epsilon ^{T}])}
= tr ( Λ [ μ μ T + Σ ] ) {\displaystyle \operatorname {tr} (\Lambda [\mu \mu ^{T}+\Sigma ])} {\displaystyle \operatorname {tr} (\Lambda [\mu \mu ^{T}+\Sigma ])}
= μ T Λ μ + tr ( Λ Σ ) {\displaystyle \mu ^{T}\Lambda \mu +\operatorname {tr} (\Lambda \Sigma )} {\displaystyle \mu ^{T}\Lambda \mu +\operatorname {tr} (\Lambda \Sigma )}

Geomon 23:30, 21 December 2006 (UTC) [reply ]

Good call. I must have been thinking about bilinear forms when I wrote that. Btyner 00:16, 23 January 2007 (UTC) [reply ]

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