Building Diquark Model from Lattice QCD
A novel Lattice QCD (LQCD) method to determine the quark–diquark ( q – D ) interaction potential together with the diquark mass ( m D ) is proposed. Similar to the HAL QCD method, q – D potential is determined by demanding it to reproduce the q – D equal-time Nambu–Bethe–Salpeter (NBS) wave function...
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Published in | Few-body systems Vol. 62; no. 3 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Vienna
Springer Vienna
01.09.2021
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | A novel Lattice QCD (LQCD) method to determine the quark–diquark (
q
–
D
) interaction potential together with the diquark mass (
m
D
) is proposed. Similar to the HAL QCD method,
q
–
D
potential is determined by demanding it to reproduce the
q
–
D
equal-time Nambu–Bethe–Salpeter (NBS) wave function. To do this, it is necessary to use the masses of the quark and the diquark as inputs, which however are not straightforwardly obtained because of the color confinement of QCD. In this work, masses of quark and diquark are determined by demanding that the p-wave spectrums from the two-point correlators be reproduced by the potentials for
c
c
¯
and
q
–
D
sectors determined from the NBS wave functions. Numerical calculations are performed by using 2+1 flavor QCD gauge configurations with the pion mass
m
π
≃
700
MeV generated by PACS-CS collaboration. We apply our method to the
c
–
c
¯
system and the charm-diquark system (
Λ
c
baryon) to obtain the charm quark mass, diquark mass and the
c
–
D
potential. Our preliminary analysis leads to the diquark mass
m
D
≃
1.127
GeV which is roughly consistent with a naive estimate based on the constituent quark picture, i.e.,
m
D
≃
m
ρ
≃
1.12
GeV and
m
D
≃
2
m
N
/
3
≃
1.06
GeV. |
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ISSN: | 0177-7963 1432-5411 |
DOI: | 10.1007/s00601-021-01627-y |