Pure states of $M_n(Bbb C)$












0












$begingroup$


I saw a reference book,there is a statement:the pure states of $M_n(Bbb C)$ are the rank 1 projections of $M_n(Bbb C)$.



By definition of states,they should be the positive linear functional of norm 1.So the pure states should be positive linear functional of $M_n(Bbb C)$.How to interpret the statement.










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$endgroup$












  • $begingroup$
    As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 16:45












  • $begingroup$
    That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 20:36


















0












$begingroup$


I saw a reference book,there is a statement:the pure states of $M_n(Bbb C)$ are the rank 1 projections of $M_n(Bbb C)$.



By definition of states,they should be the positive linear functional of norm 1.So the pure states should be positive linear functional of $M_n(Bbb C)$.How to interpret the statement.










share|cite|improve this question











$endgroup$












  • $begingroup$
    As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 16:45












  • $begingroup$
    That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 20:36
















0












0








0





$begingroup$


I saw a reference book,there is a statement:the pure states of $M_n(Bbb C)$ are the rank 1 projections of $M_n(Bbb C)$.



By definition of states,they should be the positive linear functional of norm 1.So the pure states should be positive linear functional of $M_n(Bbb C)$.How to interpret the statement.










share|cite|improve this question











$endgroup$




I saw a reference book,there is a statement:the pure states of $M_n(Bbb C)$ are the rank 1 projections of $M_n(Bbb C)$.



By definition of states,they should be the positive linear functional of norm 1.So the pure states should be positive linear functional of $M_n(Bbb C)$.How to interpret the statement.







operator-theory operator-algebras c-star-algebras






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share|cite|improve this question













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share|cite|improve this question








edited Jan 2 at 19:33









Martin Argerami

124k1177176




124k1177176










asked Jan 2 at 16:20









mathrookiemathrookie

832512




832512












  • $begingroup$
    As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 16:45












  • $begingroup$
    That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 20:36




















  • $begingroup$
    As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 16:45












  • $begingroup$
    That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
    $endgroup$
    – Frederik vom Ende
    Jan 2 at 20:36


















$begingroup$
As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
$endgroup$
– Frederik vom Ende
Jan 2 at 16:45






$begingroup$
As every linear functional on $M_n(mathbb C)$ is of the form $Amapstooperatorname{tr}(AB)$ for some matrix $B$, states and density matrices have a one-to-one correspondence (and thus the pure states correspond exactly to rank-1 projections). For a more detailed answer, check out this link.
$endgroup$
– Frederik vom Ende
Jan 2 at 16:45














$begingroup$
That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
$endgroup$
– Frederik vom Ende
Jan 2 at 20:36






$begingroup$
That is indeed true. Assume that $B,B'in M_n(mathbb C)$ generate the same state $phi$ (via the trace). Define $A_{xy}:zmapstolangle x,zrangle y$ for arbitrary $x,yinmathbb C^n$, then $langle x,Byrangle=operatorname{tr}(A_{xy}B)=phi(A_{xy})=operatorname{tr}(A_{xy}B')=langle x,B'yrangle$, so all matrix elements of $B,B'$ coincide (and thus $B=B'$).
$endgroup$
– Frederik vom Ende
Jan 2 at 20:36












1 Answer
1






active

oldest

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$begingroup$

It is easy to check that any linear functional on $M_n(mathbb C)$ is of the form $Xlongmapsto operatorname{Tr}(AX)$ for some $Ain M_n(mathbb C)$. Under this correspondence positive functional correspond with positive matrices, and so states correspond with positive matrices of trace 1. Among these, one can check that the pure states are precisely those given by the rank-one projections.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
    $endgroup$
    – Martin Argerami
    Jan 2 at 18:49











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1 Answer
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active

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1 Answer
1






active

oldest

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active

oldest

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active

oldest

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3












$begingroup$

It is easy to check that any linear functional on $M_n(mathbb C)$ is of the form $Xlongmapsto operatorname{Tr}(AX)$ for some $Ain M_n(mathbb C)$. Under this correspondence positive functional correspond with positive matrices, and so states correspond with positive matrices of trace 1. Among these, one can check that the pure states are precisely those given by the rank-one projections.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
    $endgroup$
    – Martin Argerami
    Jan 2 at 18:49
















3












$begingroup$

It is easy to check that any linear functional on $M_n(mathbb C)$ is of the form $Xlongmapsto operatorname{Tr}(AX)$ for some $Ain M_n(mathbb C)$. Under this correspondence positive functional correspond with positive matrices, and so states correspond with positive matrices of trace 1. Among these, one can check that the pure states are precisely those given by the rank-one projections.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
    $endgroup$
    – Martin Argerami
    Jan 2 at 18:49














3












3








3





$begingroup$

It is easy to check that any linear functional on $M_n(mathbb C)$ is of the form $Xlongmapsto operatorname{Tr}(AX)$ for some $Ain M_n(mathbb C)$. Under this correspondence positive functional correspond with positive matrices, and so states correspond with positive matrices of trace 1. Among these, one can check that the pure states are precisely those given by the rank-one projections.






share|cite|improve this answer









$endgroup$



It is easy to check that any linear functional on $M_n(mathbb C)$ is of the form $Xlongmapsto operatorname{Tr}(AX)$ for some $Ain M_n(mathbb C)$. Under this correspondence positive functional correspond with positive matrices, and so states correspond with positive matrices of trace 1. Among these, one can check that the pure states are precisely those given by the rank-one projections.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Jan 2 at 17:42









Martin ArgeramiMartin Argerami

124k1177176




124k1177176












  • $begingroup$
    Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
    $endgroup$
    – Martin Argerami
    Jan 2 at 18:49


















  • $begingroup$
    Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
    $endgroup$
    – Martin Argerami
    Jan 2 at 18:49
















$begingroup$
Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
$endgroup$
– Martin Argerami
Jan 2 at 18:49




$begingroup$
Yes, you use the same definition: you take them to be the extreme points of the state space. The states on an operator system $S$ are exactly the same as the states on $C^*(S)$, so there is nothing new or different.
$endgroup$
– Martin Argerami
Jan 2 at 18:49


















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