<p>We mathematically show an equality between the index of a Dirac operator on a flat continuum torus and the <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> invariant of a lattice Dirac operator known as the Wilson Dirac operator with a negative mass when the lattice spacing is sufficiently small. Unlike the standard approach, our formulation using <i>K</i>-theory does not require modified chiral symmetry on the lattice. We prove that a one-parameter family of continuum massive Dirac operators and the corresponding Wilson Dirac operators belong to the same equivalence class of the <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(K^1\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>K</mi> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation> group at a finite lattice spacing. Their indices, which are evaluated by the spectral flow or equivalently by the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> invariant at a finite mass, are proved to be equal.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

The index of lattice Dirac operators and K-theory

  • Shoto Aoki,
  • Hidenori Fukaya,
  • Mikio Furuta,
  • Shinichiroh Matsuo,
  • Tetsuya Onogi,
  • Satoshi Yamaguchi

摘要

We mathematically show an equality between the index of a Dirac operator on a flat continuum torus and the \(\eta \) η invariant of a lattice Dirac operator known as the Wilson Dirac operator with a negative mass when the lattice spacing is sufficiently small. Unlike the standard approach, our formulation using K-theory does not require modified chiral symmetry on the lattice. We prove that a one-parameter family of continuum massive Dirac operators and the corresponding Wilson Dirac operators belong to the same equivalence class of the \(K^1\) K 1 group at a finite lattice spacing. Their indices, which are evaluated by the spectral flow or equivalently by the \(\eta \) η invariant at a finite mass, are proved to be equal.