scholarly journals Atiyah-Patodi-Singer index theorem for domain-wall fermion Dirac operator

2018 ◽  
Vol 175 ◽  
pp. 11009 ◽  
Author(s):  
Hidenori Fukaya ◽  
Tetsuya Onogi ◽  
Satoshi Yamaguchi

Recently, the Atiyah-Patodi-Singer(APS) index theorem attracts attention for understanding physics on the surface of materials in topological phases. Although it is widely applied to physics, the mathematical set-up in the original APS index theorem is too abstract and general (allowing non-trivial metric and so on) and also the connection between the APS boundary condition and the physical boundary condition on the surface of topological material is unclear. For this reason, in contrast to the Atiyah-Singer index theorem, derivation of the APS index theorem in physics language is still missing. In this talk, we attempt to reformulate the APS index in a "physicist-friendly" way, similar to the Fujikawa method on closed manifolds, for our familiar domain-wall fermion Dirac operator in a flat Euclidean space. We find that the APS index is naturally embedded in the determinant of domain-wall fermions, representing the so-called anomaly descent equations.

2007 ◽  
Vol 22 (07n10) ◽  
pp. 499-513
Author(s):  
YUSUKE TANIGUCHI

In this proceeding we propose a new procedure to impose the Schrödinger functional Dirichlet boundary condition on the overlap Dirac operator and the domain-wall fermion using an orbifolding projection. With this procedure the zero mode problem with Dirichlet boundary condition can easily be avoided.


2016 ◽  
Author(s):  
Shoji Hashimoto ◽  
Guido Cossu ◽  
Hidenori Fukaya ◽  
Takashi Kaneko ◽  
Jun Noaki

2018 ◽  
Vol 175 ◽  
pp. 13013
Author(s):  
Peter A Boyle ◽  
Luigi Del Debbio ◽  
Andreas Jüttner ◽  
Ava Khamseh ◽  
Justus Tobias Tsang ◽  
...  

We review the domain wall charm physics program of the RBC and UKQCD collaborations based on simulations including ensembles with physical pion mass. We summarise our current set-up and present a status update on the decay constants fD, fDs, the charm quark mass, heavy-light and heavy-strange bag parameters and the ratio ξ


2017 ◽  
Vol 96 (12) ◽  
Author(s):  
Hidenori Fukaya ◽  
Tetsuya Onogi ◽  
Satoshi Yamaguchi

2002 ◽  
Vol 106-107 ◽  
pp. 718-720 ◽  
Author(s):  
S. Aoki ◽  
Y. Aoki ◽  
R. Burkhalter ◽  
S. Ejiri ◽  
M. Fukugita ◽  
...  

2016 ◽  
Author(s):  
Meifeng Lin ◽  
Eric Papenhausen ◽  
M. Harper Langston ◽  
Benoit Meister ◽  
Muthu Baskaran ◽  
...  

2020 ◽  
Vol 6 (1) ◽  
pp. 1-15 ◽  
Author(s):  
Chongsheng Cao ◽  
Edriss S. Titi

AbstractIt is well known, by now, that the three-dimensional non-viscous planetary geostrophic model, with vertical hydrostatic balance and horizontal Rayleigh friction/damping, coupled to the heat diffusion and transport, is mathematically ill-posed. This is because the no-normal flow physical boundary condition implicitly produces an additional boundary condition for the temperature at the lateral boundary. This additional boundary condition is different, because of the Coriolis forcing term, than the no-heat-flux physical boundary condition. Consequently, the second order parabolic heat equation is over-determined with two different boundary conditions. In a previous work we proposed one remedy to this problem by introducing a fourth-order artificial hyper-diffusion to the heat transport equation and proved global regularity for the proposed model. A shortcoming of this higher-oder diffusion is the loss of the maximum/minimum principle for the heat equation. Another remedy for this problem was suggested by R. Salmon by introducing an additional Rayleigh-like friction/damping term for the vertical component of the velocity in the hydrostatic balance equation. In this paper we prove the global, for all time and all initial data, well-posedness of strong solutions to the three-dimensional Salmon’s planetary geostrophic model of ocean dynamics. That is, we show global existence, uniqueness and continuous dependence of the strong solutions on initial data for this model. Unlike the 3D viscous PG model, we are still unable to show the uniqueness of the weak solution. Notably, we also demonstrate in what sense the additional damping term, suggested by Salmon, annihilate the ill-posedness in the original system; consequently, it can be viewed as “regularizing” term that can possibly be used to regularize other related systems.


2001 ◽  
Vol 94 (1-3) ◽  
pp. 725-728 ◽  
Author(s):  
A. Ali Khan ◽  
S. Aoki ◽  
Y. Aoki ◽  
R. Burkhalter ◽  
S. Ejiri ◽  
...  

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