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 Post subject: Odd basic problem
PostPosted: Wed, 25 Apr 2012 13:54:42 UTC 
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A friend of mine posed the question if I have a basis v_1,\ldots, v_k of V=\mathbb{R}^k and a dual basis \phi_1,\ldots,\phi_k which has the usual pairing rule \phi_i(v_j)=\delta_{ij} and ||v_i||=1 for every i, can we conclude that ||\phi_j||=||\phi_k|| for every j,k? Note the assumption is only that the original basis is normal, nothing about orthogonality is assumed, otherwise this is trivial. I personally feel like it should just come from the transpose isomorphism, but he feels there might be something more subtle. If there's a reference or a really solid proof that actually has the maximization via the analysis definition taking the sup over unit vectors, that would probably be most convincing. Thanks, and any help appreciated.

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 Post subject: Re: Odd basic problem
PostPosted: Wed, 25 Apr 2012 14:23:00 UTC 
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Shadow wrote:
A friend of mine posed the question if I have a basis v_1,\ldots, v_k of V=\mathbb{R}^k and a dual basis \phi_1,\ldots,\phi_k which has the usual pairing rule \phi_i(v_j)=\delta_{ij} and ||v_i||=1 for every i, can we conclude that ||\phi_j||=||\phi_k|| for every j,k? Note the assumption is only that the original basis is normal, nothing about orthogonality is assumed, otherwise this is trivial. I personally feel like it should just come from the transpose isomorphism, but he feels there might be something more subtle. If there's a reference or a really solid proof that actually has the maximization via the analysis definition taking the sup over unit vectors, that would probably be most convincing. Thanks, and any help appreciated.


No.

Take \mathbb{R}^3 with v_1=e_1, v_2=\cos(\theta) e_1+\sin(\theta) e_2, v_3=e_3, where \theta is tiny. Then obviously \phi^3=e^3 (lifting the indices to show it is the dual), but \phi^1=e^1-\cot(\theta) e^2 has norm \lvert\csc(\theta)\rvert\gg1.

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\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


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 Post subject: Re: Odd basic problem
PostPosted: Wed, 25 Apr 2012 14:33:30 UTC 
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outermeasure wrote:
Shadow wrote:
A friend of mine posed the question if I have a basis v_1,\ldots, v_k of V=\mathbb{R}^k and a dual basis \phi_1,\ldots,\phi_k which has the usual pairing rule \phi_i(v_j)=\delta_{ij} and ||v_i||=1 for every i, can we conclude that ||\phi_j||=||\phi_k|| for every j,k? Note the assumption is only that the original basis is normal, nothing about orthogonality is assumed, otherwise this is trivial. I personally feel like it should just come from the transpose isomorphism, but he feels there might be something more subtle. If there's a reference or a really solid proof that actually has the maximization via the analysis definition taking the sup over unit vectors, that would probably be most convincing. Thanks, and any help appreciated.


No.

Take \mathbb{R}^3 with v_1=e_1, v_2=\cos(\theta) e_1+\sin(\theta) e_2, v_3=e_3, where \theta is tiny. Then obviously \phi^3=e^3 (lifting the indices to show it is the dual), but \phi^1=e^1-\cot(\theta) e^2 has norm \lvert\csc(\theta)\rvert\gg1.


Excellent. Thanks a lot. He found that it was true for \mathbb{R}^2 and it seems I was wrong to doubt that it must be true for all finite dimensional spaces.

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 Post subject: Re: Odd basic problem
PostPosted: Wed, 25 Apr 2012 14:51:07 UTC 
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Shadow wrote:
outermeasure wrote:
Shadow wrote:
A friend of mine posed the question if I have a basis v_1,\ldots, v_k of V=\mathbb{R}^k and a dual basis \phi_1,\ldots,\phi_k which has the usual pairing rule \phi_i(v_j)=\delta_{ij} and ||v_i||=1 for every i, can we conclude that ||\phi_j||=||\phi_k|| for every j,k? Note the assumption is only that the original basis is normal, nothing about orthogonality is assumed, otherwise this is trivial. I personally feel like it should just come from the transpose isomorphism, but he feels there might be something more subtle. If there's a reference or a really solid proof that actually has the maximization via the analysis definition taking the sup over unit vectors, that would probably be most convincing. Thanks, and any help appreciated.


No.

Take \mathbb{R}^3 with v_1=e_1, v_2=\cos(\theta) e_1+\sin(\theta) e_2, v_3=e_3, where \theta is tiny. Then obviously \phi^3=e^3 (lifting the indices to show it is the dual), but \phi^1=e^1-\cot(\theta) e^2 has norm \lvert\csc(\theta)\rvert\gg1.


Excellent. Thanks a lot. He found that it was true for \mathbb{R}^2 and it seems I was wrong to doubt that it must be true for all finite dimensional spaces.


Well, for \mathbb{R}^2 it is true because you have an (orientation-reversing) isometry swapping v_1 and v_2, but it is not true in general that any permutation of v_i is an isometry when in higher dimensions. ;)

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\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


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