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Ⅰ = 2ππ po...

Ⅰ = 2ππ potential in the HAL QCD method with all-to-all propagators

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Ⅰ = 2ππ potential in the HAL QCD method with all-to-all propagators

Persistent ID (NDL)
info:ndljp/pid/11661812
Material type
記事
Author
Yutaro Akahoshiほか
Publisher
Oxford University Press
Publication date
2019-08-11
Material Format
Digital
Journal name
Progress of Theoretical and Experimental Physics : PTEP 2019(8)
Publication Page
-
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In this paper, we perform the first application of the hybrid method (exact low modes plus stochastically estimated high modes) for all-to-all propaga...

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Digital

Material Type
記事
Author/Editor
Yutaro Akahoshi
Sinya Aoki
Tatsumi 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
Persistent ID (NDL)
info:ndljp/pid/11661812
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
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

Digital

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.
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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
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 QCD
Interaction potentials for two-particle states with nonzero total momenta in lattice QCD
Chemical potential (in)dependence of hadron scatterings in the hadronic phase of QCD-like theories and its applications
Scale 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 point
The HAL QCD potential in the I = 1ππ system with the ρ meson bound state
S-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 flavors
Two-baryonpotentials and H-dibaryon from 3-flavor lattice QCD simulations
Omega-Omega interaction from 2+1-flavor lattice quantum chromodynamics
NΩ dibaryon from lattice QCD near the physical point
Fate 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 QCD
Spin-2 NΩ dibaryon from lattice QCD
Hyperon?nucleon force from lattice QCD
Hadron?hadron interactions from imaginary-time Nambu?Bethe?Salpeter wave function on the lattice
Bound dibaryon in flavor SU(3) limit of lattice QCD
Mirage in temporal correlation functions for baryon-baryon interactions in lattice QCD
Systematics of the HAL QCD potential at low energies in lattice QCD
Consistency between Lüscher’s finite volume method and HAL QCD method for two-baryon systems in lattice QCD
Coupled-channel approach to strangeness S = -2 baryon-bayron interactions in lattice QCD
Are two nucleons bound in lattice QCD for heavy quark masses? Consistency check with Lüscher’s finite volume formula
Most Strange Dibaryon from Lattice QCD
Charmed 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 simulations
Spin–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 QCD
Asymptotic behavior of Nambu-Bethe-Salpeter wave functions for multiparticles in quantum field theories
Two-particle states on a torus and their relation to the scattering matrix
ΛN interaction from lattice QCD and its application to Λ hypernuclei
The tetraquark candidate ${Z}_{{c}}(3900)$ from dynamical lattice QCD simulations
Isoscalar <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 QCD
Resonance scattering phase shifts on a non-rest-frame lattice
Hadron interactions in lattice QCD
Renormalization group analysis of lattice theories and improved lattice action: Two-dimensional non-linear O(N) sigma model
Practical all-to-all propagators for lattice QCD
Coupled<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 QCD
Observation 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 exotica
Observation 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>Decays
Novel quark-field creation operator construction for hadronic physics in lattice QCD
Nuclear Force from Lattice QCD
Lattice 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 width
Multiple-channel generalization of Lellouch-Lüscher formula
Isoscalar <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 QCD
Scattering processes and resonances from lattice QCD
Improved continuum limit lattice action for QCD with wilson fermions
Exploring Three-Nucleon Forces in Lattice QCD
Theoretical foundation of the nuclear force in QCD and its applications to central and tenser forces in quenched lattice QCD simulations
Nucleon-nucleon potential and its non-locality in lattice QCD
Data Provider (Database)
国立情報学研究所 : CiNii Research
Bibliographic ID (NDL)
11661812
NAID
120006878537