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Related papers: Breaking CPT by mixed non-commutativity

200 papers

In our past experiments on a single electron and positron we measured the cyclotron and spin-cyclotron difference frequencies omega_c and omega_a and the ratios a = omega_a/ omega_c at omega_c = 141 Ghz for e^- and e^+ and later, only for…

High Energy Physics - Phenomenology · Physics 2012-08-27 H. Dehmelt , R. Mittleman , R. S. Van Dyck, , P. Schwinberg

The radiatively induced Lorentz and CPT violating Chern-Simons terms in QED is calculated based on the recently developed loop regularization method [Y.L. Wu, Int.J.Mod.Phys.A18 (2003) 5363, hep-th/0209021; Y.L. Wu, Mod.Phys.Lett.A19 (2004)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yong-Liang Ma , Yue-Liang Wu

The Lorentz invariant $CPT$ violation by using non-local interactions is naturally incorporated in the Higgs coupling to neutrinos in the Standard Model, without spoiling the basic $SU(2)_{L}\times U(1)$ gauge symmetry. The…

High Energy Physics - Phenomenology · Physics 2015-06-11 Masud Chaichian , Kazuo Fujikawa , Anca Tureanu

What do we know about CPT symmetry? We conclude that the direcrt measurement of CPT violation leads to a result that CPT violation force is limited to about 30% of CP violating forces. The best test of CPT symmetry is to see if theoretical…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. I. Sanda

We calculate the induced Lorentz- and CPT-violating Chern-Simons term arising from the Lorentz- and CPT-violating sector of quantum electrodynamics with a $b_\mu\bar{\psi}\gamma^\mu\gamma_5\psi$ term. The result to all orders in $b$…

High Energy Physics - Theory · Physics 2008-11-26 J. -M. Chung

We show that the strength of non-commutativity could play a role in determining the boundary condition of a physical problem. As a toy model we consider the inverse square problem in non-commutative space. The scale invariance of the system…

High Energy Physics - Theory · Physics 2009-08-17 Pulak Ranjan Giri

Interplay between axial anomaly and quark-hadron duality in the presence of strong mixing is considered. The anomaly sum rule for meson transition form factors based on the dispersive representation of axial anomaly and quark-hadron duality…

High Energy Physics - Phenomenology · Physics 2012-02-01 Yaroslav Klopot , Armen Oganesian , Oleg Teryaev

Using primarily experimental inputs for S(B -> psi Ks), Delta M_Bs, Delta M_Bd, BR(B -> tau nu) and epsilon_K along with necessary inputs from the lattice, we find that the measured value of sin(2 beta) is smaller than expectations of the…

High Energy Physics - Phenomenology · Physics 2011-06-27 E. Lunghi , A. Soni

In this paper we study the invariance of the noncmmutative gauge theories under C, P and T transformations. For the noncommutative space (when only the spatial part of $\theta$ is non-zero) we show that NCQED is Parity invariant. In…

High Energy Physics - Theory · Physics 2009-10-07 M. M. Sheikh-Jabbari

Charge Parity asymmetry in charmless B meson decays is a key issue to be understood. Many theoretical calculations have been performed using short distance factorization approaches which, in general, do not take into account the CPT…

High Energy Physics - Phenomenology · Physics 2016-11-02 J. H. Alvarenga Nogueira , I. Bediaga , T. Frederico , P. C. Magalhães , J. Molina Rodriguez

Entangled pseudoscalar neutral meson pairs have been used in studying CP violation and searching CPT violation, but almost all the previous works concern $C=-1$ entangled state. Here we consider $C=+1$ entangled state of pseudoscalar…

High Energy Physics - Phenomenology · Physics 2015-06-16 Zhijie Huang , Yu Shi

CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or…

High Energy Physics - Phenomenology · Physics 2010-04-05 Thomas Dent , Joaquim Silva-Marcos

In this work, we derive the conditions that assure gauge invariance of a non-minimal dimension-5 Lorentz-violating QED. The two and three point functions at one-loop are computed. The gauge Ward identities are checked and the conditions to…

High Energy Physics - Theory · Physics 2025-08-04 A. P. B. Scarpelli , A. R. Vieira

An interesting framework to achieve gauge coupling unification consists in adding to the Standard Model Lagrangian non-renormalizable operators of $d \geq 5$, which affect the kinetic term of gauge fields. We first review the phenomenology…

High Energy Physics - Phenomenology · Physics 2026-04-08 Isabella Masina , Mariano Quiros

We consider CP-violating effects in tau->K pi pi nu_tau, assuming that a charged Higgs boson provides a new amplitude that can interfere with the usual Standard Model amplitude. We consider four CP-odd observables -- the regular rate…

High Energy Physics - Phenomenology · Physics 2009-01-08 Ken Kiers , Kevin Little , Alakabha Datta , David London , Makiko Nagashima , Alejandro Szynkman

Recent evidence for anomalous CP violation in B-meson oscillations can be interpreted as resulting from CPT violation. This yields the first sensitivity to CPT violation in the B_s^0 system, with the relevant coefficient for CPT violation…

High Energy Physics - Phenomenology · Physics 2010-12-09 Alan Kostelecky , R. Van Kooten

The status of CP violation and the CKM matrix is reviewed. Direct CP violation in B decay has been established and the measurement of sin(2beta) in \psi K modes reached 5% accuracy. I discuss the implications of these, and of the possible…

High Energy Physics - Phenomenology · Physics 2014-11-17 Zoltan Ligeti

A modified Dirac equation with general Lorentz- and CPT-violating operators in the electromagnetic field is studied. Constraints on and possible sensitivities to Lorentz-violating coefficients in the nonminimal sector up to mass-dimension…

High Energy Physics - Phenomenology · Physics 2016-10-31 Yunhua Ding

We consider the possibility of several different mechanisms contributing to the $\betabeta$-decay amplitude in the general case of CP nonconservation: light Majorana neutrino exchange, heavy left-handed (LH) and heavy right-handed (RH)…

High Energy Physics - Phenomenology · Physics 2011-06-24 Amand Faessler , Aurora Meroni , Serguey T. Petcov , Fedor Simkovic , John Vergados

We propose a diagnostic tool for detecting non-trivial symmetry protected topological (SPT) phases protected by a symmetry group $G$ in 2+1 dimensions. Our method is based on directly studying the 1+1-dimensional anomalous edge conformal…

Strongly Correlated Electrons · Physics 2017-09-13 Bo Han , Apoorv Tiwari , Chang-Tse Hsieh , Shinsei Ryu
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