<p>The quantum dimer magnet, with antiferromagnetic intradimer and interdimer Heisenberg exchange between spin-1/2 moments, is known to host an <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((\left|\uparrow \downarrow \right\rangle -\left|\downarrow \uparrow \right\rangle )/\sqrt{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <mrow> <mfenced close="⟩" open="∣"> <mrow> <mi>↑</mi> <mi>↓</mi> </mrow> </mfenced> <mo>−</mo> <mfenced close="⟩" open="∣"> <mrow> <mi>↓</mi> <mi>↑</mi> </mrow> </mfenced> </mrow> <mo>)</mo> </mrow> <mo>/</mo> <msqrt> <mrow> <mn>2</mn> </mrow> </msqrt> </math></EquationSource> </InlineEquation> singlet ground state when the intradimer exchange is dominant. Rare-earth-based quantum dimer systems with strong spin-orbit coupling offer the opportunity for tuning their magnetic properties by using magnetic anisotropy as a control knob. Here, we present bulk characterization and neutron scattering measurements of the quantum dimer magnet Yb<sub>2</sub>Be<sub>2</sub>SiO<sub>7</sub>. We find that the Yb<sup>3+</sup> ions can be described by an effective spin-1/2 model at low temperatures and the system does not show signs of magnetic order down to 50 mK. The magnetization, heat capacity, and neutron spectroscopy data can be well-described by an isolated dimer model with highly anisotropic exchange that stabilizes a singlet ground state with a wavefunction <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\((\left|\uparrow \uparrow \right\rangle -\left|\downarrow \downarrow \right\rangle )/\sqrt{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <mrow> <mfenced close="⟩" open="∣"> <mrow> <mi>↑</mi> <mi>↑</mi> </mrow> </mfenced> <mo>−</mo> <mfenced close="⟩" open="∣"> <mrow> <mi>↓</mi> <mi>↓</mi> </mrow> </mfenced> </mrow> <mo>)</mo> </mrow> <mo>/</mo> <msqrt> <mrow> <mn>2</mn> </mrow> </msqrt> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((\left|\uparrow \uparrow \right\rangle+\left|\downarrow \downarrow \right\rangle )/\sqrt{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <mrow> <mfenced close="⟩" open="∣"> <mrow> <mi>↑</mi> <mi>↑</mi> </mrow> </mfenced> <mo>+</mo> <mfenced close="⟩" open="∣"> <mrow> <mi>↓</mi> <mi>↓</mi> </mrow> </mfenced> </mrow> <mo>)</mo> </mrow> <mo>/</mo> <msqrt> <mrow> <mn>2</mn> </mrow> </msqrt> </math></EquationSource> </InlineEquation>. Our results show that strong spin-orbit coupling can induce unusual entangled states of matter in quantum dimer magnets.</p>

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Unconventional bipartite entanglement in the quantum dimer magnet Yb2Be2SiO7

  • A. Brassington,
  • Q. Ma,
  • G. Duan,
  • S. Calder,
  • A. I. Kolesnikov,
  • K. M. Taddei,
  • G. Sala,
  • E. S. Choi,
  • H. Wang,
  • W. Xie,
  • B. A. Frandsen,
  • N. Li,
  • X. F. Sun,
  • C. Liu,
  • R. Yu,
  • H. D. Zhou,
  • A. A. Aczel

摘要

The quantum dimer magnet, with antiferromagnetic intradimer and interdimer Heisenberg exchange between spin-1/2 moments, is known to host an \((\left|\uparrow \downarrow \right\rangle -\left|\downarrow \uparrow \right\rangle )/\sqrt{2}\) ( ) / 2 singlet ground state when the intradimer exchange is dominant. Rare-earth-based quantum dimer systems with strong spin-orbit coupling offer the opportunity for tuning their magnetic properties by using magnetic anisotropy as a control knob. Here, we present bulk characterization and neutron scattering measurements of the quantum dimer magnet Yb2Be2SiO7. We find that the Yb3+ ions can be described by an effective spin-1/2 model at low temperatures and the system does not show signs of magnetic order down to 50 mK. The magnetization, heat capacity, and neutron spectroscopy data can be well-described by an isolated dimer model with highly anisotropic exchange that stabilizes a singlet ground state with a wavefunction \((\left|\uparrow \uparrow \right\rangle -\left|\downarrow \downarrow \right\rangle )/\sqrt{2}\) ( ) / 2 or \((\left|\uparrow \uparrow \right\rangle+\left|\downarrow \downarrow \right\rangle )/\sqrt{2}\) ( + ) / 2 . Our results show that strong spin-orbit coupling can induce unusual entangled states of matter in quantum dimer magnets.