<p>We construct a topological space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation> consisting of translation invariant injective matrix product states (MPS) of all physical and bond dimensions and show that it has the weak homotopy type <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(K(\mathbb {Z}, 2) \times K(\mathbb {Z}, 3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>K</mi> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">Z</mi> <mo>,</mo> <mn>2</mn> <mo stretchy="false">)</mo> <mo>×</mo> <mi>K</mi> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">Z</mi> <mo>,</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. The implication is that the phase of a family of such states parametrized by a space <i>X</i> is completely determined by two invariants: a class in <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(H^2(X;\mathbb {Z})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>;</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> corresponding to the Chern number per unit cell and a class in <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(H^3(X;\mathbb {Z})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>3</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>;</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, the so-called Kapustin–Spodyneiko (KS) number. The space <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation> is defined as the quotient of a contractible space <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathcal {E}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">E</mi> </math></EquationSource> </InlineEquation> of MPS tensors by an equivalence relation describing gauge transformations of the tensors. We prove that the projection map <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(p:\mathcal {E}\rightarrow \mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>:</mo> <mi mathvariant="script">E</mi> <mo stretchy="false">→</mo> <mi mathvariant="script">B</mi> </mrow> </math></EquationSource> </InlineEquation> is a quasifibration, and this allows us to determine the weak homotopy type of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation>. As an example, we review the Chern number pump—a family of MPS parametrized by <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(S^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>S</mi> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>—and prove that it generates <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\pi _3(\mathcal {B})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>π</mi> <mn>3</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">B</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

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A Classifying Space for Phases of Matrix Product States

  • Daniel D. Spiegel,
  • Marvin Qi,
  • David T. Stephen,
  • Michael Hermele,
  • Markus J. Pflaum,
  • Agnès Beaudry

摘要

We construct a topological space \(\mathcal {B}\) B consisting of translation invariant injective matrix product states (MPS) of all physical and bond dimensions and show that it has the weak homotopy type \(K(\mathbb {Z}, 2) \times K(\mathbb {Z}, 3)\) K ( Z , 2 ) × K ( Z , 3 ) . The implication is that the phase of a family of such states parametrized by a space X is completely determined by two invariants: a class in \(H^2(X;\mathbb {Z})\) H 2 ( X ; Z ) corresponding to the Chern number per unit cell and a class in \(H^3(X;\mathbb {Z})\) H 3 ( X ; Z ) , the so-called Kapustin–Spodyneiko (KS) number. The space \(\mathcal {B}\) B is defined as the quotient of a contractible space \(\mathcal {E}\) E of MPS tensors by an equivalence relation describing gauge transformations of the tensors. We prove that the projection map \(p:\mathcal {E}\rightarrow \mathcal {B}\) p : E B is a quasifibration, and this allows us to determine the weak homotopy type of \(\mathcal {B}\) B . As an example, we review the Chern number pump—a family of MPS parametrized by \(S^3\) S 3 —and prove that it generates \(\pi _3(\mathcal {B})\) π 3 ( B ) .