What is Chromoelectric dipole moment?

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SUMMARY

The Chromoelectric Dipole Moment (CEDM) is analogous to the Electric Dipole Moment (EDM) but is generated from the color field associated with quarks. The interaction of a particle's dipole moment with an electric field is defined by the Hamiltonian H_{EDM} = - \vec{d}_f \cdot \vec{E}. For spin-1/2 particles, the effective Lagrangian density is expressed as \mathcal{L}_{EDM} = \frac{-i}{2} d_f F_{\mu \nu} \bar{\psi}_f \sigma^{\mu \nu} \gamma^5 \psi_f. The CEDM is represented similarly with strong interactions, leading to potential violations of parity (P) and time reversal (T), thus affecting charge-parity (CP) symmetry.

PREREQUISITES
  • Understanding of quantum field theory concepts
  • Familiarity with Lagrangian density formulations
  • Knowledge of particle physics, specifically quark interactions
  • Basic principles of CP violation in particle physics
NEXT STEPS
  • Study the implications of CP violation in the Standard Model of particle physics
  • Explore the role of color charge in quantum chromodynamics (QCD)
  • Learn about the experimental methods for measuring EDMs and CEDMs
  • Investigate the relationship between CEDM and strong CP problem
USEFUL FOR

Particle physicists, theoretical physicists, and researchers focused on CP violation and quantum chromodynamics will benefit from this discussion.

Sehwook Lee
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Basically, I wonder what Chromoelectric dipole moment is and how it is formed...
 
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It is exactly the same thing as an electric dipole moment, but it's generated from color field. Therefore you must be careful about non-commutativity of the charges
 
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The Electric Dipole Moment [itex]\vec{d}_f[/itex] of some particle [itex]f[/itex], is defined by its interaction with an electric field [itex]\vec{E}[/itex]:

[itex]H_{EDM} = - \vec{d}_f \cdot \vec{E}[/itex]

For a spin-1/2 particle, this corresponds to the effective lagrangian density:

[itex]\mathcal{L}_{EDM} = \frac{-i}{2} d_f F_{\mu \nu} \bar{\psi}_f \sigma^{\mu \nu} \gamma^5 \psi_f[/itex]

you can have a similar term if you look at quarks [itex]\mathcal{q}_r[/itex], by replacing the electromagnetism with strong ints:

[itex]\mathcal{L}_{CEDM} = \frac{-i}{2} d_r^{CEDM} G_{\mu \nu}^a \bar{\mathcal{q}}_r \sigma^{\mu \nu} \gamma^5 \frac{\lambda^a}{2} \mathcal{q}_r[/itex]

and that's how it arises... In general both EDMs and CEDMs generate P and T (so CP) violations.
 
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