How does push-forward of inverse map look like?
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In the post Differential of the multiplication and inverse maps on a Lie group, second answer, appears the following solution for the push-forward of the inverse map:
$iota_{*,a}(Y_a) = -(r_{a^{-1}})_* (ell_{a^{-1}})_* Y_a tag1$
In the second answer it is explained that applying the chain rule to
$iota(x) = r_{a^{-1}} circ iota circ l_{a^{-1}}(x) tag2$
you obtain Eq. (1). I guess that the chain rule has to be applied by derivation respect to some parameter $t$. Doing that I get:
$$frac{diota(x)}{dt} = frac{dr_{a^{-1}}(iota(l_a^{-1}(x)))}{d(iota(l_a^{-1}(x)))}cdot frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}cdot frac{dl_{a^{-1}}(x)}{dx}cdot frac{dx}{dt} = r_{a^{-1}}frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}l_{a^{-1}}frac{dx}{dt} tag3$$
And I don't know how to continue, so, I don't see how Eq. (1) can be obtained by this method.
differential-geometry lie-groups lie-algebras
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up vote
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In the post Differential of the multiplication and inverse maps on a Lie group, second answer, appears the following solution for the push-forward of the inverse map:
$iota_{*,a}(Y_a) = -(r_{a^{-1}})_* (ell_{a^{-1}})_* Y_a tag1$
In the second answer it is explained that applying the chain rule to
$iota(x) = r_{a^{-1}} circ iota circ l_{a^{-1}}(x) tag2$
you obtain Eq. (1). I guess that the chain rule has to be applied by derivation respect to some parameter $t$. Doing that I get:
$$frac{diota(x)}{dt} = frac{dr_{a^{-1}}(iota(l_a^{-1}(x)))}{d(iota(l_a^{-1}(x)))}cdot frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}cdot frac{dl_{a^{-1}}(x)}{dx}cdot frac{dx}{dt} = r_{a^{-1}}frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}l_{a^{-1}}frac{dx}{dt} tag3$$
And I don't know how to continue, so, I don't see how Eq. (1) can be obtained by this method.
differential-geometry lie-groups lie-algebras
The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17
add a comment |
up vote
0
down vote
favorite
up vote
0
down vote
favorite
In the post Differential of the multiplication and inverse maps on a Lie group, second answer, appears the following solution for the push-forward of the inverse map:
$iota_{*,a}(Y_a) = -(r_{a^{-1}})_* (ell_{a^{-1}})_* Y_a tag1$
In the second answer it is explained that applying the chain rule to
$iota(x) = r_{a^{-1}} circ iota circ l_{a^{-1}}(x) tag2$
you obtain Eq. (1). I guess that the chain rule has to be applied by derivation respect to some parameter $t$. Doing that I get:
$$frac{diota(x)}{dt} = frac{dr_{a^{-1}}(iota(l_a^{-1}(x)))}{d(iota(l_a^{-1}(x)))}cdot frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}cdot frac{dl_{a^{-1}}(x)}{dx}cdot frac{dx}{dt} = r_{a^{-1}}frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}l_{a^{-1}}frac{dx}{dt} tag3$$
And I don't know how to continue, so, I don't see how Eq. (1) can be obtained by this method.
differential-geometry lie-groups lie-algebras
In the post Differential of the multiplication and inverse maps on a Lie group, second answer, appears the following solution for the push-forward of the inverse map:
$iota_{*,a}(Y_a) = -(r_{a^{-1}})_* (ell_{a^{-1}})_* Y_a tag1$
In the second answer it is explained that applying the chain rule to
$iota(x) = r_{a^{-1}} circ iota circ l_{a^{-1}}(x) tag2$
you obtain Eq. (1). I guess that the chain rule has to be applied by derivation respect to some parameter $t$. Doing that I get:
$$frac{diota(x)}{dt} = frac{dr_{a^{-1}}(iota(l_a^{-1}(x)))}{d(iota(l_a^{-1}(x)))}cdot frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}cdot frac{dl_{a^{-1}}(x)}{dx}cdot frac{dx}{dt} = r_{a^{-1}}frac{d(iota(l_a^{-1}(x)))}{d(l_{a^{-1}}(x))}l_{a^{-1}}frac{dx}{dt} tag3$$
And I don't know how to continue, so, I don't see how Eq. (1) can be obtained by this method.
differential-geometry lie-groups lie-algebras
differential-geometry lie-groups lie-algebras
edited Nov 15 at 17:45
asked Nov 15 at 16:35
Vicky
1387
1387
The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17
add a comment |
The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17
The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17
add a comment |
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The chain rule for pushforwards is just that $(F circ G)_{ast} = F_{ast} circ G_{ast}$.
– Travis
Nov 15 at 16:47
How do you prove it? Sorry, I'm a roockie in this branch of maths
– Vicky
Nov 15 at 16:49
In coordinates this is just the multivariable chain rule.
– Travis
Nov 15 at 17:17