<p>A quantum cellular automaton (QCA) or a causal unitary is by definition an automorphism of a local operator algebra, by which local operators are mapped to nearby local operators. Quantum circuits of small depth, local Hamiltonian evolutions for short time, and translations (shifts) are examples. A Clifford QCA is one that maps any Pauli operator to a finite tensor product of Pauli operators. Here, we obtain a complete table of groups&#xa0;<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {C}}({\textsf{d}},p)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">C</mi> <mo stretchy="false">(</mo> <mi mathvariant="sans-serif">d</mi> <mo>,</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of translation invariant Clifford QCA in any spatial dimension&#xa0;<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textsf{d}}\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="sans-serif">d</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> modulo Clifford quantum circuits and shifts over prime&#xa0;<i>p</i>-dimensional qudits, where the circuits and shifts are allowed to obey only coarser translation invariance. The group <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {C}}({\textsf{d}},p)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">C</mi> <mo stretchy="false">(</mo> <mi mathvariant="sans-serif">d</mi> <mo>,</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is nonzero only for <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textsf{d}}= 2k+3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="sans-serif">d</mi> <mo>=</mo> <mn>2</mn> <mi>k</mi> <mo>+</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> if <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(p=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq6.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textsf{d}}= 4k+3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="sans-serif">d</mi> <mo>=</mo> <mn>4</mn> <mi>k</mi> <mo>+</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> if <i>p</i> is odd where&#xa0;<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(k \ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is any integer, in which case <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq8.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="118" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {C}}({\textsf{d}},p) \cong {\widetilde{\mathfrak {W}}}({\mathbb {F}}_p)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">C</mi> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="sans-serif">d</mi> <mo>,</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mo>≅</mo> <mover accent="true"> <mi mathvariant="fraktur">W</mi> <mo stretchy="true">~</mo> </mover> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="double-struck">F</mi> <mi>p</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, the classical Witt group of nonsingular quadratic forms over the finite field&#xa0;<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {F}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">F</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>. It is well known that <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq10.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="109" /> </InlineMediaObject> <EquationSource Format="TEX">\({\widetilde{\mathfrak {W}}}({\mathbb {F}}_2) \cong {\mathbb {Z}}/2{\mathbb {Z}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi mathvariant="fraktur">W</mi> <mo stretchy="true">~</mo> </mover> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="double-struck">F</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>≅</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq11.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="109" /> </InlineMediaObject> <EquationSource Format="TEX">\({\widetilde{\mathfrak {W}}}({\mathbb {F}}_p) \cong {\mathbb {Z}}/4{\mathbb {Z}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi mathvariant="fraktur">W</mi> <mo stretchy="true">~</mo> </mover> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="double-struck">F</mi> <mi>p</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo>≅</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">/</mo> <mn>4</mn> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation> if <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq12.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="89" /> </InlineMediaObject> <EquationSource Format="TEX">\(p = 3 \bmod 4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>3</mn> <mspace width="0.277778em" /> <mo>mod</mo> <mspace width="0.277778em" /> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq13.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="168" /> </InlineMediaObject> <EquationSource Format="TEX">\({\widetilde{\mathfrak {W}}}({\mathbb {F}}_p)\cong {\mathbb {Z}}/2{\mathbb {Z}}\oplus {\mathbb {Z}}/2{\mathbb {Z}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi mathvariant="fraktur">W</mi> <mo stretchy="true">~</mo> </mover> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="double-struck">F</mi> <mi>p</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo>≅</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> <mo>⊕</mo> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation> if <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5239_Article_IEq14.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="89" /> </InlineMediaObject> <EquationSource Format="TEX">\(p = 1 \bmod 4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>1</mn> <mspace width="0.277778em" /> <mo>mod</mo> <mspace width="0.277778em" /> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>. The classification is achieved by a dimensional descent, which is a reduction of Laurent extension theorems for algebraic <i>L</i>-groups of surgery theory in topology.</p>

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Topological Phases of Unitary Dynamics: Classification in Clifford Category

  • Jeongwan Haah

摘要

A quantum cellular automaton (QCA) or a causal unitary is by definition an automorphism of a local operator algebra, by which local operators are mapped to nearby local operators. Quantum circuits of small depth, local Hamiltonian evolutions for short time, and translations (shifts) are examples. A Clifford QCA is one that maps any Pauli operator to a finite tensor product of Pauli operators. Here, we obtain a complete table of groups  \({\mathfrak {C}}({\textsf{d}},p)\) C ( d , p ) of translation invariant Clifford QCA in any spatial dimension  \({\textsf{d}}\ge 0\) d 0 modulo Clifford quantum circuits and shifts over prime p-dimensional qudits, where the circuits and shifts are allowed to obey only coarser translation invariance. The group \({\mathfrak {C}}({\textsf{d}},p)\) C ( d , p ) is nonzero only for \({\textsf{d}}= 2k+3\) d = 2 k + 3 if \(p=2\) p = 2 and \({\textsf{d}}= 4k+3\) d = 4 k + 3 if p is odd where  \(k \ge 0\) k 0 is any integer, in which case \({\mathfrak {C}}({\textsf{d}},p) \cong {\widetilde{\mathfrak {W}}}({\mathbb {F}}_p)\) C ( d , p ) W ~ ( F p ) , the classical Witt group of nonsingular quadratic forms over the finite field  \({\mathbb {F}}_p\) F p . It is well known that \({\widetilde{\mathfrak {W}}}({\mathbb {F}}_2) \cong {\mathbb {Z}}/2{\mathbb {Z}}\) W ~ ( F 2 ) Z / 2 Z , \({\widetilde{\mathfrak {W}}}({\mathbb {F}}_p) \cong {\mathbb {Z}}/4{\mathbb {Z}}\) W ~ ( F p ) Z / 4 Z if \(p = 3 \bmod 4\) p = 3 mod 4 , and \({\widetilde{\mathfrak {W}}}({\mathbb {F}}_p)\cong {\mathbb {Z}}/2{\mathbb {Z}}\oplus {\mathbb {Z}}/2{\mathbb {Z}}\) W ~ ( F p ) Z / 2 Z Z / 2 Z if \(p = 1 \bmod 4\) p = 1 mod 4 . The classification is achieved by a dimensional descent, which is a reduction of Laurent extension theorems for algebraic L-groups of surgery theory in topology.