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  • Chapter 15 Symmetry violation - Theory and Simulation Group of the . . .
    We also consider the violation, or possible violation, of the product symmetry operations CP and CPT Such symmetry violations are normally thought of as being studied in fundamental particle physics, but they can lead to spectroscopically measurable consequences for atoms and molecules
  • The Strong CP Problem - Duke University
    Vvector symmetry is the symmetry corresponding to isospin times baryon number [U(2) V= SU(2) I U(1) B], and is indeed a good approximate symmetry of the strong interactions This can be evident by the appearance of nucleon and pion multiplets in the spectrum of hadrons 1
  • CP violation in electroweak interactions - Scholarpedia
    One of the important phenomena in the field of fundamental interactions presently described by the the Standard Model (SM), is the violation of CP symmetry, the combination of C-symmetry (charge conjugation symmetry) and P-symmetry (parity symmetry)
  • Phys. Rev. D 45, 466 (1992) - Strong CP violation, electroweak . . .
    We discuss the influence of strong CP-violating effects in invisible-axion models on electroweak baryogenesis We find that they can be important only if the electroweak phase transition (EPT) occurs simultaneously with the chirality-breaking phase transition in QCD
  • electromagnetism - QFT symmetry breaking and CP violation - Physics . . .
    Hence, it cannot enmesh CP violation with either the photon or the Z! Both electromagnetism and neutral current weak interactions respect CP Weak mixing has nothing to do with CP violation You might then say that EM preserves CP at all energies
  • Electroweak baryogenesis, dark matter, and dark CP-symmetry
    With the motivation of explaining the dark matter and achieving the electroweak baryogenesis via the spontaneous CP-violation at high temperature, we propose a complex singlet scalar (S = χ+iηs 2√) extension of the two-Higgs-doublet model respecting a discrete dark CP-symmetry: S → −S∗
  • Electroweak baryogenesis, dark matter, and dark $CP$ symmetry
    With the motivation of explaining the dark matter and achieving the electroweak baryogenesis via the spontaneous C P violation at high temperature, we propose a complex singlet scalar (S = χ + i η s 2) extension of the two-Higgs-doublet model respecting a discrete dark C P symmetry: S → − S *
  • CP VIOLATION - CERN
    Charge conjugation (C) and Parity (P) are drastically violated by the weak inter- actions; however, their product CP happens to be a good symmetry in nearly all observed phenomena So far, only in the decay of neutral kaons a slight violation of the CP symmetry (˘2 10−3) has been established
  • A Model of Grand Unified Theory: Suggested Solution for CP-Violation . . .
    This study demonstrates that beyond standard model (BSM) cosmic funda-mental interactions—weak, strong, and electromagnetic forces—can be uni-fied through a common basis of representation
  • Chapter 11 Electroweak interactions - ETH Z
    Some signals are also present in low energy atomic physics, e g electroweak interference and parity violation One can observe that the timescales involved in weak decays are much − larger than the ones of strong or electromagnetic decays





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