<p>Ising superconductors, known for their exceptionally high in-plane upper critical magnetic field (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq1.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <msub> <mrow> <mi mathvariant="normal">μ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <mi>H</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> <mn>2</mn> </mrow> <mrow> <mo>∥</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation>) beyond the Pauli limit, have so far been explored mainly in two-dimensional limit systems and molecularly intercalated bulk materials based on transition metal dichalcogenides. By exploiting the high pressure approach, we simultaneously optimize the superconducting transition temperature (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\({T}_{{\rm{c}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>) and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq1.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <msub> <mrow> <mi mathvariant="normal">μ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <mi>H</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> <mn>2</mn> </mrow> <mrow> <mo>∥</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation> in a bulk 4<i>Hb</i>-TaS<sub>2</sub> Ising superconductor. The pressure-optimized Ising superconductivity of 4<i>Hb</i>-TaS<sub>2</sub> exhibits drastically enhanced <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq1.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <msub> <mrow> <mi mathvariant="normal">μ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <mi>H</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> <mn>2</mn> </mrow> <mrow> <mo>∥</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation> that is comparable to the performance of three-layer TaS<sub>2</sub>, while also with a record-high <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\({T}_{{\rm{c}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> surpassing all the TaS<sub>2</sub>-based systems reported so far. Combined in-situ high-pressure X-ray diffraction, Hall-effect measurements, and theoretical calculations, we reveal that the dome-shaped <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\({T}_{{\rm{c}}}(P)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> </mrow> </msub> <mo>(</mo> <mi>P</mi> <mo>)</mo> </mrow> </math></EquationSource> </InlineEquation> behavior of 4<i>Hb</i>-TaS<sub>2</sub> arises from competition between superconductivity in the <i>H</i>-layers and charge density wave (CDW) orders in the <i>T</i> and <i>H</i> layers. Simultaneously, the dome-like response of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41535_2025_823_Article_IEq1.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <msub> <mrow> <mi mathvariant="normal">μ</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <mi>H</mi> </mrow> <mrow> <mi mathvariant="normal">c</mi> <mn>2</mn> </mrow> <mrow> <mo>∥</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation> on pressure is governed by synergistic effects of interlayer coupling and spin-orbital coupling. These central findings provide a practical route to achieving record-high functionalities of Ising superconductivity with superior application potentials.</p>

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Enhanced Ising superconductivity in a unicompositional bulk 4Hb-TaS2 superlattice via pressure

  • Limin Yan,
  • Jiaqing Gao,
  • Zihan Zhang,
  • Lijuan Wang,
  • Cheng Jin,
  • Tian Li,
  • Chuanying Xi,
  • Mingtao Li,
  • Nana Li,
  • Jiayi Guan,
  • Jiahao Ning,
  • Xuqiang Liu,
  • Xin Wang,
  • Ping Cui,
  • Zhenyu Zhang,
  • Wenge Yang

摘要

Ising superconductors, known for their exceptionally high in-plane upper critical magnetic field ( \({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\) μ 0 H c 2 ) beyond the Pauli limit, have so far been explored mainly in two-dimensional limit systems and molecularly intercalated bulk materials based on transition metal dichalcogenides. By exploiting the high pressure approach, we simultaneously optimize the superconducting transition temperature ( \({T}_{{\rm{c}}}\) T c ) and \({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\) μ 0 H c 2 in a bulk 4Hb-TaS2 Ising superconductor. The pressure-optimized Ising superconductivity of 4Hb-TaS2 exhibits drastically enhanced \({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\) μ 0 H c 2 that is comparable to the performance of three-layer TaS2, while also with a record-high \({T}_{{\rm{c}}}\) T c surpassing all the TaS2-based systems reported so far. Combined in-situ high-pressure X-ray diffraction, Hall-effect measurements, and theoretical calculations, we reveal that the dome-shaped \({T}_{{\rm{c}}}(P)\) T c ( P ) behavior of 4Hb-TaS2 arises from competition between superconductivity in the H-layers and charge density wave (CDW) orders in the T and H layers. Simultaneously, the dome-like response of \({{{\rm{\mu }}}_{0}H}_{{\rm{c}}2}^{\parallel }\) μ 0 H c 2 on pressure is governed by synergistic effects of interlayer coupling and spin-orbital coupling. These central findings provide a practical route to achieving record-high functionalities of Ising superconductivity with superior application potentials.