eta invariant
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2021 ◽  
Vol 2021 (12) ◽  
Author(s):  
Tetsuya Onogi ◽  
Takuya Yoda

Abstract It is known that the Atiyah-Patodi-Singer index can be reformulated as the eta invariant of the Dirac operators with a domain wall mass which plays a key role in the anomaly inflow of the topological insulator with boundary. In this paper, we give a conjecture that the reformulated version of the Atiyah-Patodi-Singer index can be given simply from the Berry phase associated with domain wall Dirac operators when adiabatic approximation is valid. We explicitly confirm this conjecture for a special case in two dimensions where an analytic calculation is possible. The Berry phase is divided into the bulk and the boundary contributions, each of which gives the bulk integration of the Chern character and the eta-invariant.


Author(s):  
Pierre Albin ◽  
Hadrian Quan

Abstract We study the behavior of the heat kernel of the Hodge Laplacian on a contact manifold endowed with a family of Riemannian metrics that blow-up the directions transverse to the contact distribution. We apply this to analyze the behavior of global spectral invariants such as the $\eta $-invariant and the determinant of the Laplacian. In particular, we prove that contact versions of the relative $\eta $-invariant and the relative analytic torsion are equal to their Riemannian analogues and hence topological.


2020 ◽  
Vol 2020 (4) ◽  
Author(s):  
Hidenori Fukaya ◽  
Naoki Kawai ◽  
Yoshiyuki Matsuki ◽  
Makito Mori ◽  
Katsumasa Nakayama ◽  
...  

Abstract We propose a nonperturbative formulation of the Atiyah–Patodi–Singer (APS) index in lattice gauge theory in four dimensions, in which the index is given by the $\eta$ invariant of the domain-wall Dirac operator. Our definition of the index is always an integer with a finite lattice spacing. To verify this proposal, using the eigenmode set of the free domain-wall fermion we perturbatively show in the continuum limit that the curvature term in the APS theorem appears as the contribution from the massive bulk extended modes, while the boundary $\eta$ invariant comes entirely from the massless edge-localized modes.


2019 ◽  
Vol 2019 (11) ◽  
Author(s):  
Aoyama Tatsumi ◽  
Yoshio Kikukawa

Abstract We consider a lattice implementation of the $\eta$-invariant, using the complex phase of the determinant of the simplified domain-wall fermion, which couples to an interpolating 5D gauge field. We clarify the relation to the effective action for chiral Ginsparg–Wilson fermions. The integrability, which holds true for anomaly-free theories in the classical continuum limit, is not assured on a lattice with finite spacing. A lattice expression for the 5D Chern–Simons term is obtained.


Author(s):  
Zhizhang Xie ◽  
Guoliang Yu

Abstract In this paper, we establish a precise connection between higher rho invariants and delocalized eta invariants. Given an element in a discrete group, if its conjugacy class has polynomial growth, then there is a natural trace map on the $K_0$-group of its group $C^\ast$-algebra. For each such trace map, we construct a determinant map on secondary higher invariants. We show that, under the evaluation of this determinant map, the image of a higher rho invariant is precisely the corresponding delocalized eta invariant of Lott. As a consequence, we show that if the Baum–Connes conjecture holds for a group, then Lott’s delocalized eta invariants take values in algebraic numbers. We also generalize Lott’s delocalized eta invariant to the case where the corresponding conjugacy class does not have polynomial growth, provided that the strong Novikov conjecture holds for the group.


2018 ◽  
Vol 26 (2) ◽  
pp. 271-346
Author(s):  
Ruth Gornet ◽  
Ken Richardson
Keyword(s):  

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