P. de Forcrand and O. Philipsen, Nucl. Phys. B 642
2003
Cited alongside, same era.
C. R. Allton et al
2003
Cited alongside, same era.
J. Ambjorn, K. N. Anagnostopoulos, J. Nishimura and J. J. M. Verbaarschot, JHEP 10
2004
Cited alongside, same era.
Z. Fodor and S. D. Katz, Phys. Lett. B 534
2004
Cited alongside, same era.
J. Ambjorn, K. N. Anagnostopoulos, W. Bietenholz, T. Hotta and J. Nishimura, JHEP 07
2005
Cited alongside, same era.
J. Nishimura, T. Okubo and F. Sugino, Prog. Theor. Phys. 114
2005
Cited alongside, same era.
H. Kawai, S. Kawamoto, T. Kuroki, T. Matsuo and S. Shinohara, Nucl. Phys. B 647
2006
Cited alongside, same era.
This is the case in the models studied in Refs. 0108041 and Fodor:2007vv . See Ref. Ambjorn:2003rr for an analysis in the case where w w can flip its sign
Cited in the paper.
Numerical simulations of matrix models of the IKKT type have provided a wealth of information on the large- N N limit and the nonperturbative dynamics of their degrees of freedom that are, in particular, related to the emergent space-time geometry Ambjorn:2000bf ; 0108041 . Such simulations have been extended recently to shed light on important problems such as demonstrating the gauge/gravity duality from first principles and understanding the microscopic description of black hole thermodynamics in terms of string degrees of freedom Hanada:2007ti
Cited in the paper.
K.N. Anagnostopoulos, T. Azuma, J. Nishimura, work in progress. Details of our calculations for all k k and for the SO(3) ansatz will be presented there
Cited in the paper.
As x x decreases, the dominant configurations have the property [ A μ , A ν ] ≈ 0 [A_{\mu},A_{\nu}]\approx 0 , meaning that A μ A_{\mu} are simultaneously diagonalizable, e.g. as A μ = diag ( α μ ( 1 ) , ⋯ , α μ ( N ) ) A_{\mu}=\mbox{diag}(\alpha_{\mu}^{(1)},\cdots,\alpha_{\mu}^{(N)}) . For such configurations, the determinant becomes det 𝒟 = ∏ i = 1 N { ∑ μ ( α μ ( i ) ) 2 } ≥ 0 \det{\cal D}=\prod_{i=1}^{N}\{\sum_{\mu}(\alpha_{\mu}^{(i)})^{2}\}\geq 0
Original
Cited in the paper.