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Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD

We present the first study of baryon-baryon interactions in the continuum limit of lattice QCD, finding unexpectedly large lattice artifacts. Specifically, we determine the binding energy of the <math display="inline"><mi>H</mi></math> dibaryon at a single quark-mas...

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Autores principales: Green, Jeremy R., Hanlon, Andrew D., Junnarkar, Parikshit M., Wittig, Hartmut
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevLett.127.242003
http://cds.cern.ch/record/2753574
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author Green, Jeremy R.
Hanlon, Andrew D.
Junnarkar, Parikshit M.
Wittig, Hartmut
author_facet Green, Jeremy R.
Hanlon, Andrew D.
Junnarkar, Parikshit M.
Wittig, Hartmut
author_sort Green, Jeremy R.
collection CERN
description We present the first study of baryon-baryon interactions in the continuum limit of lattice QCD, finding unexpectedly large lattice artifacts. Specifically, we determine the binding energy of the <math display="inline"><mi>H</mi></math> dibaryon at a single quark-mass point. The calculation is performed at six values of the lattice spacing <math display="inline"><mi>a</mi></math>, using <math display="inline"><mrow><mi mathvariant="normal">O</mi><mo stretchy="false">(</mo><mi>a</mi><mo stretchy="false">)</mo></mrow></math>-improved Wilson fermions at the SU(3)-symmetric point with <math display="inline"><mrow><msub><mrow><mi>m</mi></mrow><mrow><mi>π</mi></mrow></msub><mo>=</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>K</mi></mrow></msub><mo>≈</mo><mn>420</mn><mtext> </mtext><mtext> </mtext><mi>MeV</mi></mrow></math>. Energy levels are extracted by applying a variational method to correlation matrices of bilocal two-baryon interpolating operators computed using the distillation technique. Our analysis employs Lüscher’s finite-volume quantization condition to determine the scattering phase shifts from the spectrum and vice versa, both above and below the two-baryon threshold. We perform global fits to the lattice spectra using parametrizations of the phase shift, supplemented by terms describing discretization effects, then extrapolate the lattice spacing to zero. The phase shift and the binding energy determined from it are found to be strongly affected by lattice artifacts. Our estimate of the binding energy in the continuum limit of three-flavor QCD is <math display="inline"><mrow><msubsup><mrow><mi>B</mi></mrow><mrow><mi>H</mi></mrow><mrow><msub><mrow><mi>SU</mi><mo stretchy="false">(</mo><mn>3</mn><mo stretchy="false">)</mo></mrow><mrow><mi>f</mi></mrow></msub></mrow></msubsup><mo>=</mo><mn>4.56</mn><mo>±</mo><mn>1.1</mn><msub><mrow><mn>3</mn></mrow><mrow><mi>stat</mi></mrow></msub><mo>±</mo><mn>0.6</mn><msub><mrow><mn>3</mn></mrow><mrow><mi>syst</mi></mrow></msub><mtext> </mtext><mtext> </mtext><mi>MeV</mi></mrow></math>.
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publishDate 2021
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spelling cern-27535742023-09-01T04:27:08Zdoi:10.1103/PhysRevLett.127.242003http://cds.cern.ch/record/2753574engGreen, Jeremy R.Hanlon, Andrew D.Junnarkar, Parikshit M.Wittig, HartmutWeakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCDnucl-thNuclear Physics - Theoryhep-phParticle Physics - Phenomenologyhep-latParticle Physics - LatticeWe present the first study of baryon-baryon interactions in the continuum limit of lattice QCD, finding unexpectedly large lattice artifacts. Specifically, we determine the binding energy of the <math display="inline"><mi>H</mi></math> dibaryon at a single quark-mass point. The calculation is performed at six values of the lattice spacing <math display="inline"><mi>a</mi></math>, using <math display="inline"><mrow><mi mathvariant="normal">O</mi><mo stretchy="false">(</mo><mi>a</mi><mo stretchy="false">)</mo></mrow></math>-improved Wilson fermions at the SU(3)-symmetric point with <math display="inline"><mrow><msub><mrow><mi>m</mi></mrow><mrow><mi>π</mi></mrow></msub><mo>=</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>K</mi></mrow></msub><mo>≈</mo><mn>420</mn><mtext> </mtext><mtext> </mtext><mi>MeV</mi></mrow></math>. Energy levels are extracted by applying a variational method to correlation matrices of bilocal two-baryon interpolating operators computed using the distillation technique. Our analysis employs Lüscher’s finite-volume quantization condition to determine the scattering phase shifts from the spectrum and vice versa, both above and below the two-baryon threshold. We perform global fits to the lattice spectra using parametrizations of the phase shift, supplemented by terms describing discretization effects, then extrapolate the lattice spacing to zero. The phase shift and the binding energy determined from it are found to be strongly affected by lattice artifacts. Our estimate of the binding energy in the continuum limit of three-flavor QCD is <math display="inline"><mrow><msubsup><mrow><mi>B</mi></mrow><mrow><mi>H</mi></mrow><mrow><msub><mrow><mi>SU</mi><mo stretchy="false">(</mo><mn>3</mn><mo stretchy="false">)</mo></mrow><mrow><mi>f</mi></mrow></msub></mrow></msubsup><mo>=</mo><mn>4.56</mn><mo>±</mo><mn>1.1</mn><msub><mrow><mn>3</mn></mrow><mrow><mi>stat</mi></mrow></msub><mo>±</mo><mn>0.6</mn><msub><mrow><mn>3</mn></mrow><mrow><mi>syst</mi></mrow></msub><mtext> </mtext><mtext> </mtext><mi>MeV</mi></mrow></math>.We present the first study of baryon-baryon interactions in the continuum limit of lattice QCD, finding unexpectedly large lattice artifacts. Specifically, we determine the binding energy of the $H$ dibaryon at a single quark-mass point. The calculation is performed at six values of the lattice spacing $a$, using O($a$)-improved Wilson fermions at the SU(3)-symmetric point with $m_\pi=m_K\approx 420$ MeV. Energy levels are extracted by applying a variational method to correlation matrices of bilocal two-baryon interpolating operators computed using the distillation technique. Our analysis employs Lüscher's finite-volume quantization condition to determine the scattering phase shifts from the spectrum and vice versa, both above and below the two-baryon threshold. We perform global fits to the lattice spectra using parametrizations of the phase shift, supplemented by terms describing discretization effects, then extrapolate the lattice spacing to zero. The phase shift and the binding energy determined from it are found to be strongly affected by lattice artifacts. Our estimate of the binding energy in the continuum limit of three-flavor QCD is $B_H^{\text{SU(3)}_{\rm f}}=4.56\pm1.13_{\rm stat}\pm0.63_{\rm syst}$ MeV.arXiv:2103.01054MITP-21-009CERN-TH-2021-024oai:cds.cern.ch:27535742021-03-01
spellingShingle nucl-th
Nuclear Physics - Theory
hep-ph
Particle Physics - Phenomenology
hep-lat
Particle Physics - Lattice
Green, Jeremy R.
Hanlon, Andrew D.
Junnarkar, Parikshit M.
Wittig, Hartmut
Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title_full Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title_fullStr Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title_full_unstemmed Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title_short Weakly bound $H$ dibaryon from SU(3)-flavor-symmetric QCD
title_sort weakly bound $h$ dibaryon from su(3)-flavor-symmetric qcd
topic nucl-th
Nuclear Physics - Theory
hep-ph
Particle Physics - Phenomenology
hep-lat
Particle Physics - Lattice
url https://dx.doi.org/10.1103/PhysRevLett.127.242003
http://cds.cern.ch/record/2753574
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AT hanlonandrewd weaklyboundhdibaryonfromsu3flavorsymmetricqcd
AT junnarkarparikshitm weaklyboundhdibaryonfromsu3flavorsymmetricqcd
AT wittighartmut weaklyboundhdibaryonfromsu3flavorsymmetricqcd