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Related papers: CPT Tests: Kaon vs Neutrinos

200 papers

I present several preliminary measurements from KTeV of the fundamental neutral kaon parameters, and their implications for CPT violation. A new limit is given on the sidereal time dependence of $\phi_{+-}$. The results are based on data…

High Energy Physics - Experiment · Physics 2017-08-23 Hogan Nguyen

CP violation in the neutral kaon system is known to be dominated by the mixing of K0 and anti-K0. Direct CP violation in the 2 pion decays of neutral kaons has been a controversial subject over the last decade. A strong experimental effort…

High Energy Physics - Experiment · Physics 2007-05-23 M. Cirilli

On 2010 MINOS experiment was showing an hint of possible different mass splitting and mixing angles for neutrinos and anti-neutrinos, suggesting a charge-parity-time (CPT) violation in the lepton sector; last year 2012 a second result from…

High Energy Physics - Phenomenology · Physics 2013-03-13 D. Fargion , D. D Armiento

We show that under gravity the effective masses for neutrino and antineutrino are different which opens a possible window of neutrino-antineutrino oscillation even if the rest masses of the corresponding eigenstates are same. This is due to…

General Relativity and Quantum Cosmology · Physics 2016-11-15 Banibrata Mukhopadhyay

As limits improve on the neutrino mixing angles and mass-squared differences, the focus of T2K has shifted towards studying antineutrino oscillation. This will give an insight into CP violation (if P($\bar{\nu}_{\mu} \rightarrow…

High Energy Physics - Experiment · Physics 2016-05-06 Kirsty Duffy

Neutral kaons provide one of the most sensitive system to CP and CPT violation. Tests on CP, CPT and quantum mechanics have been performed at KLOE operating at the DAFNE e+e- collider. Results on the quantum interference in the channel…

High Energy Physics - Experiment · Physics 2012-08-27 KLOE Collaboration

We point out that a background torsion field will produce an effective potential to the $K$ and $\bar{K}$ with opposite signs. This allows us to constrain the background torsion field from the $K_L$ and $K_S$ mass difference, CPT violating…

High Energy Physics - Phenomenology · Physics 2016-09-06 Subhendra Mohanty , Utpal Sarkar

Recent measurements by the T2K neutrino oscillation experiment indicate that CP violation in neutrino mixing may be observed in the future by long-baseline neutrino oscillation experiments. We propose an extension to the currently approved…

High Energy Physics - Experiment · Physics 2016-09-15 K. Abe , H. Aihara , A. Amji , J. Amey , C. Andreopoulos , M. Antonova , S. Aoki , A. Atherton , S. Ban , F. C. T. Barbato , M. Barbi , F. C. T. Barbato , G. J. Barker , G. Barr , P. Bartet-Friburg , M. Batkiewicz , V. Berardi , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , S. Bordoni , S. B. Boyd , D. Brailsford , A. Bravar , C. Bronner , M. Buizza Avanzini , J. Calcutt , R. G. Calland , D. Calvet , T. Campbell , S. Cao , S. L. Cartwright , R. Castillo , M. G. Catanesi , A. Cervera , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , A. Clifton , J. Coleman , G. Collazuol , D. Coplowe , L. Cremonesi , A. Cudd , A. Dabrowska , A. Delbart , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , D. Dewhurst , F. Di Lodovico , S. Dolan , O. Drapier , K. E. Duffy , J. Dumarchez , M. Dunkman , M. Dziewiecki , S. Emery-Schrenk , P. Fernanddez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , M. Fitton , M. Friend , Y. Fujii , D. Fukuda , Y. Fukuda , A. Garcia , C. Giganti , F. Gizzarelli , M. Gonin , N. Grant , D. R. Hadley , L. Haegel , M. D. Haigh , D. Hansen , J. Harada , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , T. Hiraki , A. Hiramoto , S. Hirota , M. Hogan , J. Holeczek , F. Hosomi , K. Huang , A. K. Ichikawa , M. Ikeda , J. Imber , J. Insler , R. A. Intonti , T. Ishida , T. Ishii , E. Iwai , K. Iwamoto , A. Izmaylov , B. Jamieson , M. Jiang , S. Johnson , J. H. Jo , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , H. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , A. Konaka , K. Kondo , L. L. Kormos , A. Korzenev , Y. Koshio , K. L. Kowalik , W. Kropp , Y. Kudenko , R. Kurjata , T. Kutter , L. Labarga , J. Lagoda , I. Lamont , M. Lamoureux , E. Larkin , P. Lasorak , M. Laveder , M. Lawe , T. Lindner , Z. J. Liptak , R. P. Litchfield , X. Li , A. Longhin , J. P. Lopez , T. Lou , L. Ludovici , X. Lu , L. Magaletti , K. Mahn , M. Malek , S. Manly , A. D. Marino , J. F. Martin , P. Martins , S. Martynenko , T. Maruyama , V. Matveev , K. Mavrokoridis , W. Y. Ma , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , P. Mijakowski , A. Minamino , O. Mineev , S. Mine , A. Missert , M. Miura , S. Moriyama , Th. A. Mueller , Y. Nagai , T. Nakadaira , M. Nakahata , K. G. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakanishi , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , K. Nishikawa , Y. Nishimura , P. Novella , J. Nowak , H. M. O'Keeffe , R. Ohta , K. Okumura , T. Okusawa , T. Ovsyannikova , R. A. Owen , Y. Oyama , V. Palladino , J. L. Palomino , V. Paolone , W. Parker , N. D. Patel , M. Pavin , D. Payne , J. D. Perkin , L. Pickard , L. Pickering , E. S. Pinzon Guerra , B. Popov , M. Posiadala-Zezula , J. -M. Poutissou , R. Poutissou , P. Przewlocki , B. Quilain , T. Radermacher , E. Radicioni , P. N. Ratoff , M. Ravonel , M. A. Rayner , E. Reinherz-Aronis , C. Riccio , P. Rojas , E. Rondio , B. Rossi , S. Roth , A. C. Ruggeri , A. Rychter , R. Sacco , K. Sakashita , F. Sánchez , E. Scantamburlo , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , D. Shaw , M. Shiozawa , T. Shirahige , S. Short , M. Smy , J. T. Sobczyk , H. Sobel , L. Southwell , J. Steinmann , T. Stewart , P. Stowell , Y. Suda , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , M. Szeptycka , R. Tacik , M. Tada , A. Takeda , Y. Takeuchi , R. Tamura , H. K. Tanaka , H. A. Tanaka , D. Terhorst , R. Terri , T. Thakore , L. F. Thompson , W. Toki , T. Tomura , C. Touramanis , T. Tsukamoto , M. Tzanov , M. A. Uchida , Y. Uchida , M. Vagins , A. Vacheret , Z. Vallari , G. Vasseur , T. Wachala , C. W. Walter , D. Wark , M. O. Wascko , A. Weber , R. Wendell , R. J. Wilkes , M. J. Wilking , J. R. Wilson , R. J. Wilson , C. Wret , Y. Yamada , K. Yamamoto , M. Yamamoto , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , J. Yoo , K. Yoshida , T. Yuan , M. Yu , A. Zalewska , J. Zalipska , L. Zambelli , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito

A search for sidereal variations in the frequency difference between co-located 129-Xe and 3-He Zeeman masers sets the most stringent limit to date on leading-order Lorentz and CPT violation involving the neutron, consistent with no effect…

Atomic Physics · Physics 2009-09-25 D. Bear , R. E. Stoner , R. L. Walsworth , V. Alan Kostelecky , Charles D. Lane

A breakdown of the Local Lorentz Invariance and hence the special theory of relativity in the Kaon system can, in principle, induce oscillations between the $K^0$ and $\bar{K}^0$ states. We construct a general formulation in which…

High Energy Physics - Phenomenology · Physics 2009-10-30 T. Hambye , R. B. Mann , U. Sarkar

Some extensions of the Standard Model of Particle Physics allow for Lorentz invariance and Charge-Parity-Time (CPT)-invariance violations. In the neutrino sector strong constraints have been set by neutrino-oscillation and time-of-flight…

Nuclear Experiment · Physics 2023-05-10 M. Aker , D. Batzler , A. Beglarian , J. Behrens , A. Berlev , U. Besserer , B. Bieringer , F. Block , S. Bobien , B. Bornschein , L. Bornschein , M. Böttcher , T. Brunst , T. S. Caldwell , R. M. D. Carney , S. Chilingaryan , W. Choi , K. Debowski , M. Deffert , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , F. Edzards , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , A. Felden , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , K. Gauda , A. S. Gavin , W. Gil , F. Glück , R. Grössle , R. Gumbsheimer , V. Hannen , N. Haußmann , K. Helbing , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , T. Houdy , A. Huber , A. Jansen , C. Karl , J. Kellerer , M. Kleifges , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , H. Krause , L. La Cascio , T. Lasserre , T. L. Le , O. Lebeda , B. Lehnert , A. Lokhov , M. Machatschek , E. Malcherek , M. Mark , A. Marsteller , E. L. Martin , C. Melzer , S. Mertens , J. Mostafa , K. Müller , H. Neumann , S. Niemes , P. Oelpmann , D. S. Parno , A. W. P. Poon , J. M. L. Poyato , F. Priester , J. Ráliš , S. Ramachandran , R. G. H. Robertson , W. Rodejohann , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , R. Salomon , P. Schäfer , L. Schimpf , M. Schlösser , K. Schlösser , L. Schlüter , S. Schneidewind , M. Schrank , A. Schwemmer , M. Šefčík , V. Sibille , D. Siegmann , M. Slezák , F. Spanier , M. Steidl , M. Sturm , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , K. Urban , K. Valerius , D. Vénos , A. P. Vizcaya Hernández , C. Weinheimer , S. Welte , J. Wendel , M. Wetter , J. Wickles , C. Wiesinger , J. F. Wilkerson , J. Wolf , S. Wüstling , J. Wydra , W. Xu , S. Zadoroghny , G. Zeller

This talk summarizes some theoretical features and experimental implications of a general Lorentz-violating extension of the minimal SU(3) x SU(2) x U(1) standard model that allows for both CPT-even and CPT-odd effects. The theory would…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alan Kostelecky

A general formalism is presented for violations of Lorentz and CPT symmetry in the neutrino sector. The effective hamiltonian for neutrino propagation in the presence of Lorentz and CPT violation is derived, and its properties are studied.…

High Energy Physics - Phenomenology · Physics 2009-09-25 Alan Kostelecky , Matthew Mewes

The situation connected with a possibility of CPT violation in neutrino sector is considered.

High Energy Physics - Phenomenology · Physics 2015-03-17 V. P. Efrosinin

The ideal neutrino detector at the neutrino factory should have a mass in the range of 10 kton, provide particle identification to tag the flavor of the incoming neutrino, lepton charge measurement to select the incoming neutrino helicity,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Andre Rubbia

In the minimal Left-Right model the choice of left-right symmetry is twofold: either generalized parity $\mathcal P$ or charge conjugation $\mathcal C$. In the minimal model with spontaneously broken strict $\mathcal P$, a large tree-level…

High Energy Physics - Phenomenology · Physics 2014-11-11 Alessio Maiezza , Miha Nemevšek

We investigate matter-induced (or extrinsic) CPT violation effects in neutrino oscillations in matter. Especially, we present approximate analytical formulas for the CPT-violating probability differences for three flavor neutrino…

High Energy Physics - Phenomenology · Physics 2009-05-20 Magnus Jacobson , Tommy Ohlsson

Parameters describing CPT violation are extracted from a variety of rate asymmetries in the neutral-$D$ system. The precision to which these parameters could be measured in present and planned machines is examined.

High Energy Physics - Phenomenology · Physics 2007-05-23 Don Colladay , Alan Kostelecky

Diagnosing core of supernova requires favor-dependent reconstruction of three species of neutrino spectra, \nu_e, \bar{\nu}_{e} and \nu_x (a collective notation for \nu_{\mu}, \bar{\nu}_{\mu}, \nu_{\tau}, and \bar{\nu}_{\tau}). We point out…

High Energy Physics - Phenomenology · Physics 2013-05-29 Hisakazu Minakata , Shoichi Uchinami

In this talk, we investigate extrinsic CPT violation in neutrino oscillations in matter with three flavors. Note that extrinsic CPT violation is different from intrinsic CPT violation. Extrinsic CPT violation is one way of quantifying…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tommy Ohlsson