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Lattice approaches to the neutron electric dipole moment with dynamical clover fermions

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Title: Lattice approaches to the neutron electric dipole moment with dynamical clover fermions


1
Lattice approaches to the neutron electric dipole
moment with dynamical clover fermions
  • Eigo Shintani (Univ. of Tsukuba)
  • In collaboration with
  • Sinya Aoki (Univ. of Tsukuba)
  • Yoshinobu Kuramashi (Univ. of Tsukuba)
  • ???????2007?????, 2007/3/28

2
Introduction
  • P, T violation
  • Ratio of direct and indirect CP violation in K0
    (e/e)
  • Kobayashi-Masukawa mechanism
  • ? term, strong CP problem (NEDM, axion model)
  • Baryon number asymmetry,
  • Neutron electric dipole moment (NEDM)
  • Its sensitive object to T violation in
    strong interaction, and if ? term is present, it
    has a finite value in proportional to ?.
  • Now its value is known as much small order
    by experiment
  • dN lt 6.310-13 efm
  • ? is estimated to be O(10-10) by effective
    models.

Harris, et al. (1999)
3
Lattice works
  • Lattice QCD
  • first principle calculation, model independent
  • rigorous evaluation of dN
  • ? theoretical range of ? with precise
    experiment in future
  • Recent lattice works
  • Quench approximation (focus on methodology)
  • NEDM form factor with domain-wall (DW) fermion
    ES (2005)
  • External electric field method with clover and DW
    ES (2006)
  • Full QCD simulation
  • RBC groupNEDM form factor, Nf2 dynamical DW
    T.Blum (2006)
  • External electric field (direct method) with Nf2
    dynamical clover

  • ES
    (2006)

4
Contents
  • Introduction
  • Recent results with external electric field
  • New challenge NEDM form factor with clover
    fermion
  • Formulation
  • Results in Quench QCD
  • Momentum extrapolation ? NEDM
  • Disconnected diagram
  • Summary

5
External electric field method
  • Spin dependent energy difference
  • In presence of static and uniform electric field
    and ? term,
  • ms(E) -m-s(E) dN (sE)? O(?2)
  • ms spin dependent nucleon energy, s nucleon
    spin
  • Ratio of different spinor components with E,?
  • Sensitive to the discontinuity of Minkovski E
    field ES (2006)
  • Chirality of lattice fermion is not so important.
  • ? possibility in clover fermion action

6
Full QCD results (1)
  • Nf 2 dynamical clover fermion
  • 24348, a0.1 fm (CP-PACS), best configs. for
    topology
  • Huge statistics O(104)

mp760 MeV
mp760 MeV
7
Full QCD results (2)
  • Nf 2 dynamical clover fermion
  • mp5001100 MeV
  • topological susceptibility ?t17042204 MeV4
  • finite value of NEDM in full QCD at heavier quark
    mass

8
NEDM form factor with clover fermion
  • Challenging task
  • Chiral extrapolation, lighter quark mass
  • Nf3 dynamical simulation, continuum limit,
  • but, it seems to be difficult to do these
    tasks in external electric field method due to
    large statistical error.
  • Another possibility
  • NEDM form factor using clover fermion action
  • ? reduce the computational cost in comparison
    with DW
  • ? reduce the lattice momentum (p2p/L)
  • violation of chiral symmetry will not become
    large effect (that is prediction in the previous
    works)

9
Results in quench QCD (1)
  • Formulation ES (2005)
  • Extraction from next leading 3-pt function
  • After calculation of F1,2 and fN we can obtain
    F3.
  • Connected diagram
  • 24332 lattice
  • 1/a1.8 GeV
  • Same configs. in
  • E field method.
  • lightest quark mass

p1
tEM6
source
sink
10
Results in quench QCD (2)
  • Momentum extrapolation
  • Linear fit
  • cf. E field method
  • -0.0391(125) efm
  • Consistent with a result
  • in E field method
  • Error 60 reduction !
  • Applicable to full QCD

11
Results in quench QCD (3)
  • Disconnected diagram

tEM6
  • flavor SU(3) limit (mu,dms)
  • eu ed es0 ? ignore the disc. part
  • In fact, mu,d/ms 1/30 then that is not
  • good approximation.
  • computation of disc. part using
  • U(1) noise method

u,d,s
  • noise60
  • mu,d/ms1/3
  • its contribution will
  • be small.
  • fit -0.0230(69) efm
  • (con. -0.0239(30) efm)

12
Summary
  • Full QCD calculation in E field method
  • Dynamical clover fermion (Nf2)
  • obtain the finite value (inconsistent with zero)
    at mp5001100 MeV
  • Its hard to do the chiral extrapolation due to
    large error.
  • ? heavy sea-quark mass range (topological
    susceptibility is also large)
  • Form factor approach in clover fermion action
  • Computational cost is much smaller than DW.
  • Large size, then small momentum ? zero momentum
    extrapolation
  • In quenched study, we can obtain consistent
    results in E field method.
  • Moreover error is reduced by 60 .
  • Disconnected part is small, it means that
    connected part is dominant.
  • Applicable to full QCD ? possibility of obtaining
    the physical NEDM.
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