<p>This paper tackles the long-standing problem of quantizing the rational spin Ruijsenaars–Schneider model originating in the work of Krichever and Zabrodin (Russ Math Surv 50:1101, 1995. <a href="http://arxiv.org/abs/hep-th/9505039">arXiv:hep-th/9505039</a>). We make use of the technique of quantum Hamiltonian reduction to construct a quantized quiver variety <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathfrak {A}_{N,\ell }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">A</mi> <mrow> <mi>N</mi> <mo>,</mo> <mi>ℓ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>, which is simultaneously the algebra of quantum observables of the rational spin Ruijsenaars–Schneider model of <i>N</i> particles with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation> spin polarizations. Inside this algebra, we find a loop algebra and Yangian of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathfrak {gl}_\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">gl</mi> <mi>ℓ</mi> </msub> </math></EquationSource> </InlineEquation> and conjecture that the algebra <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathfrak {A}_{N,\ell }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">A</mi> <mrow> <mi>N</mi> <mo>,</mo> <mi>ℓ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> can be identified with a truncated Yangian of affine type <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(A_{\ell -1}^{(1)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>ℓ</mi> <mo>-</mo> <mn>1</mn> </mrow> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation>. Finally, we use the commutation relations inside <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathfrak {A}_{N,\ell }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">A</mi> <mrow> <mi>N</mi> <mo>,</mo> <mi>ℓ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> to derive a difference equation for eigenstates of the lowest Hamiltonian that reproduces the known quantization of the spinless case when <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\ell =1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ℓ</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Quantized Quiver Varieties and the Quantum Spin Ruijsenaars–Schneider Model

  • Gleb Arutyunov,
  • Lukas Hardi

摘要

This paper tackles the long-standing problem of quantizing the rational spin Ruijsenaars–Schneider model originating in the work of Krichever and Zabrodin (Russ Math Surv 50:1101, 1995. arXiv:hep-th/9505039). We make use of the technique of quantum Hamiltonian reduction to construct a quantized quiver variety \(\mathfrak {A}_{N,\ell }\) A N , , which is simultaneously the algebra of quantum observables of the rational spin Ruijsenaars–Schneider model of N particles with \(\ell \) spin polarizations. Inside this algebra, we find a loop algebra and Yangian of \(\mathfrak {gl}_\ell \) gl and conjecture that the algebra \(\mathfrak {A}_{N,\ell }\) A N , can be identified with a truncated Yangian of affine type \(A_{\ell -1}^{(1)}\) A - 1 ( 1 ) . Finally, we use the commutation relations inside \(\mathfrak {A}_{N,\ell }\) A N , to derive a difference equation for eigenstates of the lowest Hamiltonian that reproduces the known quantization of the spinless case when \(\ell =1\) = 1 .