<p>We study the local quantum Fisher information (LQFI) of arbitrary two-qubit states for the anisotropic XY spin-1/2 chain in a transverse field <i>h</i> at finite temperature <i>T.</i> The results show that LQFI for the states of the nearest-neighbor and the next-nearest-neighbor spin pairs can clearly spotlight the critical point (CP)<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> = 0 of a quantum phase transition (QPT) in this model even at finite<i> T</i>, due to the discontinuity of the first derivative of LQFI at <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> = 0 (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> is the anisotropy parameter). Moreover, LQFI can successfully detect another QPT point <i>h</i> = 1 at <i>T</i> = 0, due to the divergence of the first derivative of LQFI at <i>h</i> = 1 if <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left| \gamma \right| \ne 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close="|" open="|"> <mi>γ</mi> </mfenced> <mo>≠</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. When <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left| \gamma \right| = 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close="|" open="|"> <mi>γ</mi> </mfenced> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, the CP <i>h</i> = 1 can be also clearly detected by LQFI at <i>T</i> &gt; 0. Besides, LQFI can pick out the special points (not the CPs), where LQFI always displays a cusp-like behavior. At some proper values of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4726_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> and <i> h</i>, LQFI can increase with increasing <i>T</i> as well. These remarkable properties suggest that LQFI could serve as an useful tool for experimentally detecting the CPs of QPTs in spin systems at finite <i>T</i>.</p>

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Local quantum fisher information and quantum phase transitions in the XY spin-1/2 chain

  • Xiao-Dong Tan,
  • Yu Shi,
  • Ru Hou

摘要

We study the local quantum Fisher information (LQFI) of arbitrary two-qubit states for the anisotropic XY spin-1/2 chain in a transverse field h at finite temperature T. The results show that LQFI for the states of the nearest-neighbor and the next-nearest-neighbor spin pairs can clearly spotlight the critical point (CP) \(\gamma\) γ  = 0 of a quantum phase transition (QPT) in this model even at finite T, due to the discontinuity of the first derivative of LQFI at \(\gamma\) γ  = 0 ( \(\gamma\) γ is the anisotropy parameter). Moreover, LQFI can successfully detect another QPT point h = 1 at T = 0, due to the divergence of the first derivative of LQFI at h = 1 if \(\left| \gamma \right| \ne 1\) γ 1 . When \(\left| \gamma \right| = 1\) γ = 1 , the CP h = 1 can be also clearly detected by LQFI at T > 0. Besides, LQFI can pick out the special points (not the CPs), where LQFI always displays a cusp-like behavior. At some proper values of \(\gamma\) γ and h, LQFI can increase with increasing T as well. These remarkable properties suggest that LQFI could serve as an useful tool for experimentally detecting the CPs of QPTs in spin systems at finite T.