What is the “right” extra information needed to define the trace of a map between two different vector spaces?

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Let $V,W$ be real vector spaces of dimension $d$, and let $T in textHom(V,W)$.




Is there a "natural piece of additional information" required in order to give a meaningful interpretation of the trace of $T$? (which is "less than" choosing an isomorphism $V cong W$).




Let me explain a bit what do I mean by "additional information" through other examples:



Suppose we want to define the determinant of $T$. Then sufficient additional information is a choice of preferred volume forms on $V,W$. Assuming we are given such forms, we can then define $det T$ by requiring
$$T^*(textVol_W)=det T cdot textVol_V.$$



Perhaps an even more economical option would be to provide an isomorphism $bigwedge^d V simeq bigwedge^d W$. Since $bigwedge^d T:bigwedge^d V to bigwedge^d W
$, by composing it with the given isomorphism we can identify $bigwedge^d T$ with a map $bigwedge^d V to bigwedge^d V$ which can then be naturally identified with a scalar.



(Choosing a volume form is equivalent to choosing an isomorphism $bigwedge^d V cong mathbbR$).



Of course, we could be given an isomorphism $V simeq W$ and consider $T$ as a map $V to V$, but my point is that this is much more than we really need.



In the same spirit, in order to define the singular values of a map, we need to choose inner products on both spaces. (Which is again less information then choosing isomorphisms of $V,W$ to $mathbbR^d$).




The question is whether there is an "analogous" piece of extra structure which naturally fits into the definition of the trace. Of course, when $V=W$ (or when we are given some isomorphism between $V$ and $W$) we can define the trace of $T$ as a map $V to V$.




(A coordinate-free version would be using the natural identification $V^* otimes V cong textHom(V,V)$, and the contraction map $V^* otimes V to F$. Alternatively we can choose a basis, and use the fact the trace of a matrix is invariant under conjugation).



I am aware that it's not entirely clear whether the trace can be given a purely "geometric meaning" (in the sense that it's not invariant under isometries for instance). This is different than the situation with the determinant, or the singular values.



Edit:



In a slight contrast to the last contrast, here is some evidence that the trace is at least "partially" a geometric creature: The space of trace-free matrices is the tangent space at the identity to $SL_d$ (the group of volume preserving matrices). Thus, I am guessing that we shall need at least something like an isomorphism $bigwedge^d V simeq bigwedge^d W$ (in order to define a notion of volume preservation for maps). Using this isomorphism, we can now identify $bigwedge^d T$ as a map $bigwedge^d V to bigwedge^d V$, and define
$$
"SL"= , bigwedge^d T=textId_bigwedge^d V .
$$



The problem is that I am not sure if we can "single out" which element is the analog of the "identity map" among all these elements of our $"SL"$. Thus, I am not sure that a choice of an isomorphism $bigwedge^d V simeq bigwedge^d W$ would suffice to even define what is "trace=$0$"...







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    up vote
    11
    down vote

    favorite
    4












    Let $V,W$ be real vector spaces of dimension $d$, and let $T in textHom(V,W)$.




    Is there a "natural piece of additional information" required in order to give a meaningful interpretation of the trace of $T$? (which is "less than" choosing an isomorphism $V cong W$).




    Let me explain a bit what do I mean by "additional information" through other examples:



    Suppose we want to define the determinant of $T$. Then sufficient additional information is a choice of preferred volume forms on $V,W$. Assuming we are given such forms, we can then define $det T$ by requiring
    $$T^*(textVol_W)=det T cdot textVol_V.$$



    Perhaps an even more economical option would be to provide an isomorphism $bigwedge^d V simeq bigwedge^d W$. Since $bigwedge^d T:bigwedge^d V to bigwedge^d W
    $, by composing it with the given isomorphism we can identify $bigwedge^d T$ with a map $bigwedge^d V to bigwedge^d V$ which can then be naturally identified with a scalar.



    (Choosing a volume form is equivalent to choosing an isomorphism $bigwedge^d V cong mathbbR$).



    Of course, we could be given an isomorphism $V simeq W$ and consider $T$ as a map $V to V$, but my point is that this is much more than we really need.



    In the same spirit, in order to define the singular values of a map, we need to choose inner products on both spaces. (Which is again less information then choosing isomorphisms of $V,W$ to $mathbbR^d$).




    The question is whether there is an "analogous" piece of extra structure which naturally fits into the definition of the trace. Of course, when $V=W$ (or when we are given some isomorphism between $V$ and $W$) we can define the trace of $T$ as a map $V to V$.




    (A coordinate-free version would be using the natural identification $V^* otimes V cong textHom(V,V)$, and the contraction map $V^* otimes V to F$. Alternatively we can choose a basis, and use the fact the trace of a matrix is invariant under conjugation).



    I am aware that it's not entirely clear whether the trace can be given a purely "geometric meaning" (in the sense that it's not invariant under isometries for instance). This is different than the situation with the determinant, or the singular values.



    Edit:



    In a slight contrast to the last contrast, here is some evidence that the trace is at least "partially" a geometric creature: The space of trace-free matrices is the tangent space at the identity to $SL_d$ (the group of volume preserving matrices). Thus, I am guessing that we shall need at least something like an isomorphism $bigwedge^d V simeq bigwedge^d W$ (in order to define a notion of volume preservation for maps). Using this isomorphism, we can now identify $bigwedge^d T$ as a map $bigwedge^d V to bigwedge^d V$, and define
    $$
    "SL"= , bigwedge^d T=textId_bigwedge^d V .
    $$



    The problem is that I am not sure if we can "single out" which element is the analog of the "identity map" among all these elements of our $"SL"$. Thus, I am not sure that a choice of an isomorphism $bigwedge^d V simeq bigwedge^d W$ would suffice to even define what is "trace=$0$"...







    share|cite|improve this question
























      up vote
      11
      down vote

      favorite
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      up vote
      11
      down vote

      favorite
      4






      4





      Let $V,W$ be real vector spaces of dimension $d$, and let $T in textHom(V,W)$.




      Is there a "natural piece of additional information" required in order to give a meaningful interpretation of the trace of $T$? (which is "less than" choosing an isomorphism $V cong W$).




      Let me explain a bit what do I mean by "additional information" through other examples:



      Suppose we want to define the determinant of $T$. Then sufficient additional information is a choice of preferred volume forms on $V,W$. Assuming we are given such forms, we can then define $det T$ by requiring
      $$T^*(textVol_W)=det T cdot textVol_V.$$



      Perhaps an even more economical option would be to provide an isomorphism $bigwedge^d V simeq bigwedge^d W$. Since $bigwedge^d T:bigwedge^d V to bigwedge^d W
      $, by composing it with the given isomorphism we can identify $bigwedge^d T$ with a map $bigwedge^d V to bigwedge^d V$ which can then be naturally identified with a scalar.



      (Choosing a volume form is equivalent to choosing an isomorphism $bigwedge^d V cong mathbbR$).



      Of course, we could be given an isomorphism $V simeq W$ and consider $T$ as a map $V to V$, but my point is that this is much more than we really need.



      In the same spirit, in order to define the singular values of a map, we need to choose inner products on both spaces. (Which is again less information then choosing isomorphisms of $V,W$ to $mathbbR^d$).




      The question is whether there is an "analogous" piece of extra structure which naturally fits into the definition of the trace. Of course, when $V=W$ (or when we are given some isomorphism between $V$ and $W$) we can define the trace of $T$ as a map $V to V$.




      (A coordinate-free version would be using the natural identification $V^* otimes V cong textHom(V,V)$, and the contraction map $V^* otimes V to F$. Alternatively we can choose a basis, and use the fact the trace of a matrix is invariant under conjugation).



      I am aware that it's not entirely clear whether the trace can be given a purely "geometric meaning" (in the sense that it's not invariant under isometries for instance). This is different than the situation with the determinant, or the singular values.



      Edit:



      In a slight contrast to the last contrast, here is some evidence that the trace is at least "partially" a geometric creature: The space of trace-free matrices is the tangent space at the identity to $SL_d$ (the group of volume preserving matrices). Thus, I am guessing that we shall need at least something like an isomorphism $bigwedge^d V simeq bigwedge^d W$ (in order to define a notion of volume preservation for maps). Using this isomorphism, we can now identify $bigwedge^d T$ as a map $bigwedge^d V to bigwedge^d V$, and define
      $$
      "SL"= , bigwedge^d T=textId_bigwedge^d V .
      $$



      The problem is that I am not sure if we can "single out" which element is the analog of the "identity map" among all these elements of our $"SL"$. Thus, I am not sure that a choice of an isomorphism $bigwedge^d V simeq bigwedge^d W$ would suffice to even define what is "trace=$0$"...







      share|cite|improve this question














      Let $V,W$ be real vector spaces of dimension $d$, and let $T in textHom(V,W)$.




      Is there a "natural piece of additional information" required in order to give a meaningful interpretation of the trace of $T$? (which is "less than" choosing an isomorphism $V cong W$).




      Let me explain a bit what do I mean by "additional information" through other examples:



      Suppose we want to define the determinant of $T$. Then sufficient additional information is a choice of preferred volume forms on $V,W$. Assuming we are given such forms, we can then define $det T$ by requiring
      $$T^*(textVol_W)=det T cdot textVol_V.$$



      Perhaps an even more economical option would be to provide an isomorphism $bigwedge^d V simeq bigwedge^d W$. Since $bigwedge^d T:bigwedge^d V to bigwedge^d W
      $, by composing it with the given isomorphism we can identify $bigwedge^d T$ with a map $bigwedge^d V to bigwedge^d V$ which can then be naturally identified with a scalar.



      (Choosing a volume form is equivalent to choosing an isomorphism $bigwedge^d V cong mathbbR$).



      Of course, we could be given an isomorphism $V simeq W$ and consider $T$ as a map $V to V$, but my point is that this is much more than we really need.



      In the same spirit, in order to define the singular values of a map, we need to choose inner products on both spaces. (Which is again less information then choosing isomorphisms of $V,W$ to $mathbbR^d$).




      The question is whether there is an "analogous" piece of extra structure which naturally fits into the definition of the trace. Of course, when $V=W$ (or when we are given some isomorphism between $V$ and $W$) we can define the trace of $T$ as a map $V to V$.




      (A coordinate-free version would be using the natural identification $V^* otimes V cong textHom(V,V)$, and the contraction map $V^* otimes V to F$. Alternatively we can choose a basis, and use the fact the trace of a matrix is invariant under conjugation).



      I am aware that it's not entirely clear whether the trace can be given a purely "geometric meaning" (in the sense that it's not invariant under isometries for instance). This is different than the situation with the determinant, or the singular values.



      Edit:



      In a slight contrast to the last contrast, here is some evidence that the trace is at least "partially" a geometric creature: The space of trace-free matrices is the tangent space at the identity to $SL_d$ (the group of volume preserving matrices). Thus, I am guessing that we shall need at least something like an isomorphism $bigwedge^d V simeq bigwedge^d W$ (in order to define a notion of volume preservation for maps). Using this isomorphism, we can now identify $bigwedge^d T$ as a map $bigwedge^d V to bigwedge^d V$, and define
      $$
      "SL"= , bigwedge^d T=textId_bigwedge^d V .
      $$



      The problem is that I am not sure if we can "single out" which element is the analog of the "identity map" among all these elements of our $"SL"$. Thus, I am not sure that a choice of an isomorphism $bigwedge^d V simeq bigwedge^d W$ would suffice to even define what is "trace=$0$"...









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      edited Aug 24 at 15:27

























      asked Aug 24 at 13:13









      Asaf Shachar

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          As you observe, if we choose an isomorphism $A:Wto V$, we can define the trace of $f:Vto W$ to be
          $$mathrmTr_A(f):=mathrmTr(fA)=mathrmTr(A f).$$
          If $B:Wto V$ is another isomorphism, then $B=MA$ for some $Min GL(V)$, and
          $$
          mathrmTr_B(f)=mathrmTr(MA f).$$
          If $mathrmTr_A=mathrmTr_B$, then $mathrmTr(MC)=mathrmTr(C)$ for every $CinmathrmEnd(V)$. This implies $mathrmTr((M-mathrmId_V)C)=0$ for all $C$, which implies $M=mathrmId_V$. So the trace function determines the isomorphism from $W$ to $V$.



          By contrast, $det(MA)=det(A)$ for all $A$ if and only if $det(M)=1$. So knowing the determinant function only defines an isomorphism of $W$ with $V$ modulo determinant $1$ maps. The orbit space $mathrmIso(W,V)/SL(V)$ can be identified with $mathrmIso(bigwedge^d W,bigwedge^d V)$.






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            1 Answer
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            active

            oldest

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            up vote
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            down vote



            accepted










            As you observe, if we choose an isomorphism $A:Wto V$, we can define the trace of $f:Vto W$ to be
            $$mathrmTr_A(f):=mathrmTr(fA)=mathrmTr(A f).$$
            If $B:Wto V$ is another isomorphism, then $B=MA$ for some $Min GL(V)$, and
            $$
            mathrmTr_B(f)=mathrmTr(MA f).$$
            If $mathrmTr_A=mathrmTr_B$, then $mathrmTr(MC)=mathrmTr(C)$ for every $CinmathrmEnd(V)$. This implies $mathrmTr((M-mathrmId_V)C)=0$ for all $C$, which implies $M=mathrmId_V$. So the trace function determines the isomorphism from $W$ to $V$.



            By contrast, $det(MA)=det(A)$ for all $A$ if and only if $det(M)=1$. So knowing the determinant function only defines an isomorphism of $W$ with $V$ modulo determinant $1$ maps. The orbit space $mathrmIso(W,V)/SL(V)$ can be identified with $mathrmIso(bigwedge^d W,bigwedge^d V)$.






            share|cite|improve this answer
























              up vote
              5
              down vote



              accepted










              As you observe, if we choose an isomorphism $A:Wto V$, we can define the trace of $f:Vto W$ to be
              $$mathrmTr_A(f):=mathrmTr(fA)=mathrmTr(A f).$$
              If $B:Wto V$ is another isomorphism, then $B=MA$ for some $Min GL(V)$, and
              $$
              mathrmTr_B(f)=mathrmTr(MA f).$$
              If $mathrmTr_A=mathrmTr_B$, then $mathrmTr(MC)=mathrmTr(C)$ for every $CinmathrmEnd(V)$. This implies $mathrmTr((M-mathrmId_V)C)=0$ for all $C$, which implies $M=mathrmId_V$. So the trace function determines the isomorphism from $W$ to $V$.



              By contrast, $det(MA)=det(A)$ for all $A$ if and only if $det(M)=1$. So knowing the determinant function only defines an isomorphism of $W$ with $V$ modulo determinant $1$ maps. The orbit space $mathrmIso(W,V)/SL(V)$ can be identified with $mathrmIso(bigwedge^d W,bigwedge^d V)$.






              share|cite|improve this answer






















                up vote
                5
                down vote



                accepted







                up vote
                5
                down vote



                accepted






                As you observe, if we choose an isomorphism $A:Wto V$, we can define the trace of $f:Vto W$ to be
                $$mathrmTr_A(f):=mathrmTr(fA)=mathrmTr(A f).$$
                If $B:Wto V$ is another isomorphism, then $B=MA$ for some $Min GL(V)$, and
                $$
                mathrmTr_B(f)=mathrmTr(MA f).$$
                If $mathrmTr_A=mathrmTr_B$, then $mathrmTr(MC)=mathrmTr(C)$ for every $CinmathrmEnd(V)$. This implies $mathrmTr((M-mathrmId_V)C)=0$ for all $C$, which implies $M=mathrmId_V$. So the trace function determines the isomorphism from $W$ to $V$.



                By contrast, $det(MA)=det(A)$ for all $A$ if and only if $det(M)=1$. So knowing the determinant function only defines an isomorphism of $W$ with $V$ modulo determinant $1$ maps. The orbit space $mathrmIso(W,V)/SL(V)$ can be identified with $mathrmIso(bigwedge^d W,bigwedge^d V)$.






                share|cite|improve this answer












                As you observe, if we choose an isomorphism $A:Wto V$, we can define the trace of $f:Vto W$ to be
                $$mathrmTr_A(f):=mathrmTr(fA)=mathrmTr(A f).$$
                If $B:Wto V$ is another isomorphism, then $B=MA$ for some $Min GL(V)$, and
                $$
                mathrmTr_B(f)=mathrmTr(MA f).$$
                If $mathrmTr_A=mathrmTr_B$, then $mathrmTr(MC)=mathrmTr(C)$ for every $CinmathrmEnd(V)$. This implies $mathrmTr((M-mathrmId_V)C)=0$ for all $C$, which implies $M=mathrmId_V$. So the trace function determines the isomorphism from $W$ to $V$.



                By contrast, $det(MA)=det(A)$ for all $A$ if and only if $det(M)=1$. So knowing the determinant function only defines an isomorphism of $W$ with $V$ modulo determinant $1$ maps. The orbit space $mathrmIso(W,V)/SL(V)$ can be identified with $mathrmIso(bigwedge^d W,bigwedge^d V)$.







                share|cite|improve this answer












                share|cite|improve this answer



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                answered Aug 24 at 16:12









                Julian Rosen

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