Taylor expansion of likelihood function
$require{cancel}$
...For large samples, as a consequence of the central limit theorem, the
likelihood function approaches a gaussian, whose expected value is
equal to the maximum likelihood estimate. Indeed, expanding the
logarithm of the likelihood function around its maximum,
$$ln{mathscr{L}(theta)}=ln{mathscr{L}}(hattheta)-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2 + dots$$
for a "sufficient large" number of samples, the so called parabolic
approximation can be considered, such that the likelihood function can
be approximated by a gaussian-like expression, i.e.,
$$mathscr{L}(theta)propto e^{-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial {theta}^2}right|_hattheta(theta-hattheta)^2}...$$
I tried the Taylor expansion at $ hattheta$ as:
$$ln{mathscr{L}(theta)}=
ln{mathscr{L}}(hattheta)
+ cancel{left. dfrac{partial lnmathscr{L}}{partial theta}right|_{hattheta}left(theta-hatthetaright)}
color{red}+dfrac{1}{2}left. dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2
+ dots$$
Why the minus sign?
statistics taylor-expansion maximum-likelihood log-likelihood
add a comment |
$require{cancel}$
...For large samples, as a consequence of the central limit theorem, the
likelihood function approaches a gaussian, whose expected value is
equal to the maximum likelihood estimate. Indeed, expanding the
logarithm of the likelihood function around its maximum,
$$ln{mathscr{L}(theta)}=ln{mathscr{L}}(hattheta)-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2 + dots$$
for a "sufficient large" number of samples, the so called parabolic
approximation can be considered, such that the likelihood function can
be approximated by a gaussian-like expression, i.e.,
$$mathscr{L}(theta)propto e^{-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial {theta}^2}right|_hattheta(theta-hattheta)^2}...$$
I tried the Taylor expansion at $ hattheta$ as:
$$ln{mathscr{L}(theta)}=
ln{mathscr{L}}(hattheta)
+ cancel{left. dfrac{partial lnmathscr{L}}{partial theta}right|_{hattheta}left(theta-hatthetaright)}
color{red}+dfrac{1}{2}left. dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2
+ dots$$
Why the minus sign?
statistics taylor-expansion maximum-likelihood log-likelihood
Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
1
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36
add a comment |
$require{cancel}$
...For large samples, as a consequence of the central limit theorem, the
likelihood function approaches a gaussian, whose expected value is
equal to the maximum likelihood estimate. Indeed, expanding the
logarithm of the likelihood function around its maximum,
$$ln{mathscr{L}(theta)}=ln{mathscr{L}}(hattheta)-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2 + dots$$
for a "sufficient large" number of samples, the so called parabolic
approximation can be considered, such that the likelihood function can
be approximated by a gaussian-like expression, i.e.,
$$mathscr{L}(theta)propto e^{-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial {theta}^2}right|_hattheta(theta-hattheta)^2}...$$
I tried the Taylor expansion at $ hattheta$ as:
$$ln{mathscr{L}(theta)}=
ln{mathscr{L}}(hattheta)
+ cancel{left. dfrac{partial lnmathscr{L}}{partial theta}right|_{hattheta}left(theta-hatthetaright)}
color{red}+dfrac{1}{2}left. dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2
+ dots$$
Why the minus sign?
statistics taylor-expansion maximum-likelihood log-likelihood
$require{cancel}$
...For large samples, as a consequence of the central limit theorem, the
likelihood function approaches a gaussian, whose expected value is
equal to the maximum likelihood estimate. Indeed, expanding the
logarithm of the likelihood function around its maximum,
$$ln{mathscr{L}(theta)}=ln{mathscr{L}}(hattheta)-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2 + dots$$
for a "sufficient large" number of samples, the so called parabolic
approximation can be considered, such that the likelihood function can
be approximated by a gaussian-like expression, i.e.,
$$mathscr{L}(theta)propto e^{-dfrac{1}{2}left|dfrac{partial^2lnmathscr{L}}{partial {theta}^2}right|_hattheta(theta-hattheta)^2}...$$
I tried the Taylor expansion at $ hattheta$ as:
$$ln{mathscr{L}(theta)}=
ln{mathscr{L}}(hattheta)
+ cancel{left. dfrac{partial lnmathscr{L}}{partial theta}right|_{hattheta}left(theta-hatthetaright)}
color{red}+dfrac{1}{2}left. dfrac{partial^2lnmathscr{L}}{partial
{theta}^2}right|_hatthetaleft(theta-hatthetaright)^2
+ dots$$
Why the minus sign?
statistics taylor-expansion maximum-likelihood log-likelihood
statistics taylor-expansion maximum-likelihood log-likelihood
asked Dec 5 '18 at 16:12
FredFred
1031
1031
Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
1
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36
add a comment |
Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
1
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36
Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
1
1
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36
add a comment |
1 Answer
1
active
oldest
votes
The minus sign comes from the fact that at the maximum of ln(L), the second order condition requires that necessarily ln(L)''<=0. And the opposite of the absolute value of ln(L)'' is equal in this case to ln(L)''.
add a comment |
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1 Answer
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1 Answer
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active
oldest
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oldest
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active
oldest
votes
The minus sign comes from the fact that at the maximum of ln(L), the second order condition requires that necessarily ln(L)''<=0. And the opposite of the absolute value of ln(L)'' is equal in this case to ln(L)''.
add a comment |
The minus sign comes from the fact that at the maximum of ln(L), the second order condition requires that necessarily ln(L)''<=0. And the opposite of the absolute value of ln(L)'' is equal in this case to ln(L)''.
add a comment |
The minus sign comes from the fact that at the maximum of ln(L), the second order condition requires that necessarily ln(L)''<=0. And the opposite of the absolute value of ln(L)'' is equal in this case to ln(L)''.
The minus sign comes from the fact that at the maximum of ln(L), the second order condition requires that necessarily ln(L)''<=0. And the opposite of the absolute value of ln(L)'' is equal in this case to ln(L)''.
edited Dec 5 '18 at 17:13
answered Dec 5 '18 at 17:07
BertrandBertrand
813
813
add a comment |
add a comment |
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Where does the quote come from by the way?
– epimorphic
Dec 5 '18 at 16:29
1
“Métodos Estatísticos em Física Experimental, Oguri V, 2014” (Portuguese)
– Fred
Dec 5 '18 at 16:36