Ⅰ = 2ππ potential in the HAL QCD method with all-to-all propagators
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DOI[10.1093/ptep/ptz078]to the data of the same series
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- Material Type
- 記事
- Author/Editor
- Yutaro AkahoshiSinya AokiTatsumi Aoyama
- Publication, Distribution, etc.
- Publication Date
- 2019-08-11
- Publication Date (W3CDTF)
- 2019-08-11
- Periodical title
- Progress of Theoretical and Experimental Physics : PTEP
- No. or year of volume/issue
- 2019(8)
- Volume
- 2019(8)
- ISSN (Periodical Title)
- 2050-3911
- Text Language Code
- eng
- DOI
- 10.1093/ptep/ptz078
- Persistent ID (NDL)
- info:ndljp/pid/11661812
- Collection
- Collection (Materials For Handicapped People:1)
- Collection (particular)
- 国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > その他
- Acquisition Basis
- オンライン資料収集制度
- Date Accepted (W3CDTF)
- 2021-04-08T08:04:22+09:00
- Date Captured (W3CDTF)
- 2021-04-02
- Format (IMT)
- application/pdf
- Access Restrictions
- 国立国会図書館内限定公開
- Service for the Digitized Contents Transmission Service
- 図書館・個人送信対象外
- Availability of remote photoduplication service
- 可
- Periodical Title (URI)
- Periodical Title (Persistent ID (NDL))
- info:ndljp/pid/11661810
- Data Provider (Database)
- 国立国会図書館 : 国立国会図書館デジタルコレクション
- Summary, etc.
- In this paper, we perform the first application of the hybrid method (exact low modes plus stochastically estimated high modes) for all-to-all propagators to the HAL QCD method. We calculate the HAL QCD potentials in the I=2ππ scattering in order to see how statistical fluctuations of the potential behave under the hybrid method. All of the calculations are performed with the 2+1 flavor gauge configurations on a 163×32 lattice at the lattice spacing a≈0.12 fm and mπ≈870 MeV. It is revealed that statistical errors for the potential are enhanced by stochastic noises introduced by the hybrid method, which, however, are shown to be reduced by increasing the level of dilutions, in particular, that of space dilutions. From systematic studies, we obtain a guiding principle for a choice of dilution types/levels and a number of eigenvectors to reduce noise contamination to the potential while keeping numerical costs reasonable. We also confirm that we can obtain the scattering phase shifts for the I=2ππ system by the hybrid method within a reasonable numerical cost; these phase shifts are consistent with the result obtained with the conventional method. The knowledge that we obtain in this study will become useful for the investigation of hadron resonances that require quark annihilation diagrams such as the ρ meson by the HAL QCD potential with the hybrid method.
- DOI
- 10.1093/ptep/ptz07810.48550/arxiv.1904.09549
- Access Restrictions
- インターネット公開
- Rights (production)
- © The Author(s) 2019. Published by Oxford University Press on behalf of the Physical Society of Japan. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.Funded by SCOAP3
- Related Material (URI)
- Is Referenced By
- Emergence of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ρ</mml:mi></mml:math> resonance from the HAL QCD potential in lattice QCDInteraction potentials for two-particle states with nonzero total momenta in lattice QCDChemical potential (in)dependence of hadron scatterings in the hadronic phase of QCD-like theories and its applicationsScale setting and hadronic properties in the light quark sector with ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mn>2</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:math> )-flavor Wilson fermions at the physical pointThe HAL QCD potential in the I = 1ππ system with the ρ meson bound stateS-wave kaon-nucleon potentials with all-to-all propagators in the HAL QCD method
- References
- Polynomial hybrid Monte Carlo algorithm for lattice QCD with an odd number of flavorsTwo-baryonpotentials and H-dibaryon from 3-flavor lattice QCD simulationsOmega-Omega interaction from 2+1-flavor lattice quantum chromodynamicsNΩ dibaryon from lattice QCD near the physical pointFate of the Tetraquark Candidate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>Z</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mn>3900</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math> from Lattice QCDSpin-2 NΩ dibaryon from lattice QCDHyperon?nucleon force from lattice QCDHadron?hadron interactions from imaginary-time Nambu?Bethe?Salpeter wave function on the latticeBound dibaryon in flavor SU(3) limit of lattice QCDMirage in temporal correlation functions for baryon-baryon interactions in lattice QCDSystematics of the HAL QCD potential at low energies in lattice QCDConsistency between Lüscher’s finite volume method and HAL QCD method for two-baryon systems in lattice QCDCoupled-channel approach to strangeness S = -2 baryon-bayron interactions in lattice QCDAre two nucleons bound in lattice QCD for heavy quark masses? Consistency check with Lüscher’s finite volume formulaMost Strange Dibaryon from Lattice QCDCharmed tetraquarks <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.gif" overflow="scroll"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si2.gif" overflow="scroll"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math> from dynamical lattice QCD simulationsSpin–orbit force from lattice QCD<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>P</mml:mi></mml:math> -wave <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>π</mml:mi><mml:mi>π</mml:mi></mml:math> scattering and the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ρ</mml:mi></mml:math> resonance from lattice QCDAsymptotic behavior of Nambu-Bethe-Salpeter wave functions for multiparticles in quantum field theoriesTwo-particle states on a torus and their relation to the scattering matrixΛN interaction from lattice QCD and its application to Λ hypernucleiThe tetraquark candidate ${Z}_{{c}}(3900)$ from dynamical lattice QCD simulationsIsoscalar <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>π</mml:mi><mml:mi>π</mml:mi><mml:mo>,</mml:mo><mml:mtext> </mml:mtext><mml:mi>K</mml:mi><mml:mover accent="true"><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">¯</mml:mo></mml:mrow></mml:mover><mml:mo>,</mml:mo><mml:mtext> </mml:mtext><mml:mi>η</mml:mi><mml:mi>η</mml:mi></mml:mrow></mml:math> scattering and the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>σ</mml:mi><mml:mo>,</mml:mo><mml:mtext> </mml:mtext><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mtext> </mml:mtext><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math> mesons from QCDResonance scattering phase shifts on a non-rest-frame latticeHadron interactions in lattice QCDRenormalization group analysis of lattice theories and improved lattice action: Two-dimensional non-linear O(N) sigma modelPractical all-to-all propagators for lattice QCDCoupled<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>π</mml:mi><mml:mi>π</mml:mi></mml:mrow></mml:math>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mover accent="true"><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math>scattering in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>P</mml:mi></mml:math>-wave and the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ρ</mml:mi></mml:math>resonance from lattice QCDObservation of a Narrow Pentaquark State, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mn>4312</mml:mn><mml:msup><mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math> , and of the Two-Peak Structure of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>P</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mn>4450</mml:mn><mml:msup><mml:mo stretchy="false">)</mml:mo><mml:mo>+</mml:mo></mml:msup></mml:math>Heavy-quark QCD exoticaObservation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>J</mml:mi><mml:mo stretchy="false">/</mml:mo><mml:mi>ψ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math>Resonances Consistent with Pentaquark States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msubsup><mml:mrow><mml:mi mathvariant="normal">Λ</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msubsup><mml:mo stretchy="false">→</mml:mo><mml:mi>J</mml:mi><mml:mo stretchy="false">/</mml:mo><mml:mi>ψ</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>p</mml:mi></mml:mrow></mml:math>DecaysNovel quark-field creation operator construction for hadronic physics in lattice QCDNuclear Force from Lattice QCDLattice QCD calculation of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ρ</mml:mi></mml:math>meson decay widthMultiple-channel generalization of Lellouch-Lüscher formulaIsoscalar <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>π</mml:mi><mml:mi>π</mml:mi></mml:math> Scattering and the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>σ</mml:mi></mml:math> Meson Resonance from QCDScattering processes and resonances from lattice QCDImproved continuum limit lattice action for QCD with wilson fermionsExploring Three-Nucleon Forces in Lattice QCDTheoretical foundation of the nuclear force in QCD and its applications to central and tenser forces in quenched lattice QCD simulationsNucleon-nucleon potential and its non-locality in lattice QCD
- Data Provider (Database)
- 国立情報学研究所 : CiNii Research
- Original Data Provider (Database)
- 学術機関リポジトリデータベース雑誌記事索引データベースCrossrefCiNii Articles科学研究費助成事業データベース科学研究費助成事業データベース科学研究費助成事業データベースCrossrefCrossrefCrossrefCrossrefCrossrefCrossref
- Bibliographic ID (NDL)
- 11661812
- NAID
- 120006878537