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![Page 1: 4-quark operator contributions to neutron electric dipole moment Haipeng An, University of Maryland; PHENO 2009 In collaboration with Xiangdong Ji, Fanrong.](https://reader036.fdocuments.us/reader036/viewer/2022081418/5697bf941a28abf838c90746/html5/thumbnails/1.jpg)
4-quark operator contributions to neutron electric dipole moment
Haipeng An,
University of Maryland;
PHENO 2009
In collaboration with Xiangdong Ji, Fanrong Xu
![Page 2: 4-quark operator contributions to neutron electric dipole moment Haipeng An, University of Maryland; PHENO 2009 In collaboration with Xiangdong Ji, Fanrong.](https://reader036.fdocuments.us/reader036/viewer/2022081418/5697bf941a28abf838c90746/html5/thumbnails/2.jpg)
Intrinsic EDM interacting with the electric field
, E E s s
T-transformation:
P-transformation: , E E s s
So if a particle has an intrinsic EDM, its interaction with the photon is odd under parity and time reversal (CP) transformations.
A system in an external electric field the potential energy generated by the EDM is
Therefore, for elementary particles
The effective vertex of the electric dipole moment for spin-1/2 particle
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Experimental upper bound
The current upper bound is
|den| < 2.9 x 10-26 e cm (Institut Laue Langevin)
C. A. Baker et al., Phys. Rev. Lett. 97, 131801 (2006)
Current experiment at the Oak Ridge National Lab will give two orders of magnitude improvement.
Takeyasu M. Ito, J.Phys.Conf.Ser, 69:012037, (2007)
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Motivations
Neutron EDM is flavor conserving; It is difficult for electroweak theory to generate flavor-
conserving CP-violations;
New sources of the CP violations are needed for the sake of baryogenesis;
The new sources of CP violations may generate larger flavor-conserving CP-violation sources.
Quark EDM from the electroweak sector is about 10-34 e cm.
E.P. Shabalin, Sov. J. Nucl. Phys. 28, 75 (1978)
A. Czarnecki, B. Krause, Phys. Rev. Lett. 78, 4339(1997)
Two-body interaction contribution
den≈10-32-10-31 e cm Nanopoulos et al., Phys. Lett. B87, 53 (1979)
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P-odd, CP-odd, Flavor neutral operators
Dim-3 and 4, related by U (1)A transformation
Dim-5 QEDM and QCDM
Dim-6 three-gluon operator
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Method
Matching the CP-odd operators to the hadronic operators in the chiral perturbation theory
1. Decompose 4-quark operators into irreducible representations of SU(3)L x SU(3)R chiral symmetry;
2. Find all the leading order corresponding hadronic operators. 3. Use hadronic models to calculate the Wilson coefficients of
hadronic operators by calculating some simple matrix elements.
Calculate the chiral loop diagrams to get the Neutron EDM 1. Get the CP-odd nucleon-pion couplings and CP-odd neutron
mass from the hadronic operators; 2. Calculate the chiral loop diagrams to get the Neutron EDM; 3. CP-odd neutron mass transforms the neutron magnetic
moment to neutron EDM.
Meson condensate effects
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Meson-condensate contribution
Flavor neutral, P-odd, CP-odd operators have the same quantum numbers as the neutral meson fields π0, η, η’. For example, we can use factorization method
C4 is the wilson coefficient of the 4-quark operator
The meson condensates are proportional inversely to the quark masses.
B0=1.3 GeV
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Meson-condensate contribution
In the chiral perturbation theory, the chiral Lagrangian is constructed by
Mesons condensate
Redefine meson and baryon fields
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Meson condensate contribution
Baryon fields in the chiral perturbation theory are collected as
It transforms nonlinearly under the chiral transformation; is introduced to make it transforms linearly
Baryon fields also need to be redefined in the presence of the meson condensates.
The redefinition is equivalent to a chiral transformation, so it only bothers the terms explicitly breaking chiral symmetry.
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Meson-condensate contribution
Corrections of Baryon masses due to the nonzero light quark masses (σ-term)
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Meson-condensate contribution
Corrections of Goldberger-Treiman relation
CP odd mass of neutron
Transform the magnetic dipole to electric dipole
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Direct contribution
Decompose the 4-quark operators into irreducible representations of the SU(3)LxSU(3)R chiral group,
Collect all the leading order hadronic operators in the same representations, take the case as an example
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P-odd, CP-odd hadronic operators
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Direct contribution Match the quark operators to the hadronic operators and get the
wilson coefficients
Leading terms
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Direct contribution
Calculate the simplest matrix elements and determine the wilson coefficients
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Direct contribution
We used nonrelativistic quark model and the MIT bag model to do the matching;
The weakness of using quark models is that it is difficult to calculate the scale dependence, so they can only be used as an order estimate;
The operators without tilde can generate CP-odd pion-nucleon vertices,
The operators with a tilde can give neutron CP-odd mass,
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Induced Strong CP The θ-term in QCD violates CP and contributes to neutron EDM,
Peccei-Quinn symmetry was invented to cure this problem;
1010 Strong CP problem!!
Axion field
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Contributions to neutron EDM
Direct matching
Photopion-production
counter term of NEDM
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Numerical upper bound for Wilson coefficients of four-quark operators
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Conclusion
All the leading order P-odd, CP-odd, flavor-conserving chiral operators are collected;
Meson condensate contributions and direct matching contributions are estimated;
The contribution from the induced theta-term can be added in the result if the Peccei-Quinn symmetry is used to cure the strong CP-problem.