"Alternating sign matrix theorem"의 두 판 사이의 차이

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11번째 줄: 11번째 줄:
 
<h5>1+1 dimensional Lorentzian quantum gravity</h5>
 
<h5>1+1 dimensional Lorentzian quantum gravity</h5>
  
exists quantities
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exists quantities \phi such that if \phi(g,a)=\phi'(g',a') then [T(a,g),T(a',g')]=0
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\phi(g,a)=\frac{1-g^2(1-a^2)}{ag}=q+q^{-1}
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<h5>DPP to l</h5>
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lattice paths (lattice fermions)
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94번째 줄: 110번째 줄:
 
** Notices of the American Mathematical Society, 46 (1999), 637-646.
 
** Notices of the American Mathematical Society, 46 (1999), 637-646.
 
*  Another proof of the alternating sign matrix conjecture<br>
 
*  Another proof of the alternating sign matrix conjecture<br>
** Kuperberg, Greg
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** G Kuperberg, International Mathematics Research Notes (1996), 139-150.
** International Mathematics Research Notes (1996), 139-150.
 
 
*  Proof of the alternating sign matrix conjecture<br>
 
*  Proof of the alternating sign matrix conjecture<br>
 
** Zeilberger, Doron
 
** Zeilberger, Doron

2010년 12월 1일 (수) 08:12 판

introduction

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descending plane partitions and alternating sign matrix

 

 

1+1 dimensional Lorentzian quantum gravity

exists quantities \phi such that if \phi(g,a)=\phi'(g',a') then [T(a,g),T(a',g')]=0

\phi(g,a)=\frac{1-g^2(1-a^2)}{ag}=q+q^{-1}

 

 

DPP to l

lattice paths (lattice fermions)

 

 

 

 

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