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The Standard Model of the electroweak and strong interactions of particle physics is a quantum field theory. Elementary particles are not indivisible `pieces' of matter but energy bundles of fields, whose properties and interactions are a…

High Energy Physics - Phenomenology · Physics 2022-11-29 José Ignacio Illana , Alejandro Jiménez Cano

We investigate the weak-interaction emission of spin-1/2 fermions from decaying (and non-decaying) particles endowed with uniform circular motion. The decay of swirling protons and the neutrino- antineutrino emission from circularly moving…

High Energy Physics - Theory · Physics 2007-05-23 George E. A. Matsas , Daniel A. T. Vanzella

Are black holes elementary particles? Are they fermions or bosons? We investigate the remarkable possibility that quantum black holes are the smallest and heaviest elementary particles. We are able to construct various fundamental quantum…

General Relativity and Quantum Cosmology · Physics 2009-01-02 Yuan K. Ha

We examine a recent argument that ``identical'' quantum particles with an anti-symmetric state (fermions) are weakly discernible objects, just like irreflexively related ordinary objects in situations with perfect symmetry (Black's spheres,…

Quantum Physics · Physics 2009-11-13 Dennis Dieks , Marijn Versteegh

Quarks and leptons, the fundamental building blocks of the subatomic world, manifest in three families - replicas with identical quantum numbers that differ only in their masses. After revisiting the key milestones that led to the discovery…

High Energy Physics - Phenomenology · Physics 2025-01-14 Ferruccio Feruglio

This is a conference mostly devoted to diquarks. Although an exotic meson can in principle be composed of a diquark and an antidiquark, such an exotic is unlikely to be experimentally observable in the near future. The reason, according to…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg , R. Roncaglia , E. Predazzi

The Proceedings of the 2011 workshop on Fundamental Physics at the Intensity Frontier. Science opportunities at the intensity frontier are identified and described in the areas of heavy quarks, charged leptons, neutrinos, proton decay, new…

High Energy Physics - Experiment · Physics 2012-05-14 J. L. Hewett , H. Weerts , R. Brock , J. N. Butler , B. C. K. Casey , J. Collar , A. de Gouvea , R. Essig , Y. Grossman , W. Haxton , J. A. Jaros , C. K. Jung , Z. T. Lu , K. Pitts , Z. Ligeti , J. R. Patterson , M. Ramsey-Musolf , J. L. Ritchie , A. Roodman , K. Scholberg , C. E. M. Wagner , G. P. Zeller , S. Aefsky , A. Afanasev , K. Agashe , C. Albright , J. Alonso , C. Ankenbrandt , M. Aoki , C. A. Arguelles , N. Arkani-Hamed , J. R. Armendariz , C. Armendariz-Picon , E. Arrieta Diaz , J. Asaadi , D. M. Asner , K. S. Babu , K. Bailey , O. Baker , B. Balantekin , B. Baller , M. Bass , B. Batell , J. Beacham , J. Behr , N. Berger , M. Bergevin , E. Berman , R. Bernstein , A. J. Bevan , M. Bishai , M. Blanke , S. Blessing , A. Blondel , T. Blum , G. Bock , A. Bodek , G. Bonvicini , F. Bossi , J. Boyce , R. Breedon , M. Breidenbach , S. J. Brice , R. A. Briere , S. Brodsky , C. Bromberg , A. Bross , T. E. Browder , D. A. Bryman , M. Buckley , R. Burnstein , E. Caden , P. Campana , R. Carlini , G. Carosi , C. Castromonte , R. Cenci , I. Chakaberia , M. C. Chen , C. H. Cheng , B. Choudhary , N. H. Christ , E. Christensen , M. E. Christy , T. E. Chupp , E. Church , D. B. Cline , T. E. Coan , P. Coloma , J. Comfort , L. Coney , J. Cooper , R. J. Cooper , R. Cowan , D. F. Cowen , D. Cronin-Hennessy , A. Datta , G. S. Davies , M. Demarteau , D. P. DeMille , A. Denig , R. Dermisek , A. Deshpande , M. S. Dewey , R. Dharmapalan , J. Dhooghe , M. R. Dietrich , M. Diwan , Z. Djurcic , S. Dobbs , M. Duraisamy , B. Dutta , H. Duyang , D. A. Dwyer , M. Eads , B. Echenard , S. R. Elliott , C. Escobar , J. Fajans , S. Farooq , C. Faroughy , J. E. Fast , B. Feinberg , J. Felde , G. Feldman , P. Fierlinger , P. Fileviez Perez , B. Filippone , P. Fisher , B. T. Flemming , K. T. Flood , R. Forty , M. J. Frank , A. Freyberger , A. Friedland , R. Gandhi , K. S. Ganezer , A. Garcia , F. G. Garcia , S. Gardner , L. Garrison , A. Gasparian , S. Geer , V. M. Gehman , T. Gershon , M. Gilchriese , C. Ginsberg , I. Gogoladze , M. Gonderinger , M. Goodman , H. Gould , M. Graham , P. W. Graham , R. Gran , J. Grange , G. Gratta , J. P. Green , H. Greenlee , R. C. Group , E. Guardincerri , V. Gudkov , R. Guenette , A. Haas , A. Hahn , T. Han , T. Handler , J. C. Hardy , R. Harnik , D. A. Harris , F. A. Harris , P. G. Harris , J. Hartnett , B. He , B. R. Heckel , K. M. Heeger , S. Henderson , D. Hertzog , R. Hill , E. A Hinds , D. G. Hitlin , R. J. Holt , N. Holtkamp , G. Horton-Smith , P. Huber , W. Huelsnitz , J. Imber , I. Irastorza , J. Jaeckel , I. Jaegle , C. James , A. Jawahery , D. Jensen , C. P. Jessop , B. Jones , H. Jostlein , T. Junk , A. L. Kagan , M. Kalita , Y. Kamyshkov , D. M. Kaplan , G. Karagiorgi , A. Karle , T. Katori , B. Kayser , R. Kephart , S. Kettell , Y. K. Kim , M. Kirby , K. Kirch , J. Klein , J. Kneller , A. Kobach , M. Kohl , J. Kopp , M. Kordosky , W. Korsch , I. Kourbanis , A. D. Krisch , P. Krizan , A. S. Kronfeld , S. Kulkarni , K. S. Kumar , Y. Kuno , T. Kutter , T. Lachenmaier , M. Lamm , J. Lancaster , M. Lancaster , C. Lane , K. Lang , P. Langacker , S. Lazarevic , T. Le , K. Lee , K. T. Lesko , Y. Li , M. Lindgren , A. Lindner , J. Link , D. Lissauer , L. S. Littenberg , B. Littlejohn , C. Y. Liu , W. Loinaz , W. Lorenzon , W. C. Louis , J. Lozier , L. Ludovici , L. Lueking , C. Lunardini , D. B. MacFarlane , P. A. N. Machado , P. B. Mackenzie , J. Maloney , W. J. Marciano , W. Marsh , M. Marshak , J. W. Martin , C. Mauger , K. S. McFarland , C. McGrew , G. McLaughlin , D. McKeen , R. McKeown , B. T. Meadows , R. Mehdiyev , D. Melconian , H. Merkel , M. Messier , J. P. Miller , G. Mills , U. K. Minamisono , S. R. Mishra , I. Mocioiu , S. Moed Sher , R. N. Mohapatra , B. Monreal , C. D. Moore , J. G. Morfin , J. Mousseau , L. A. Moustakas , G. Mueller , P. Mueller , M. Muether , H. P. Mumm , C. Munger , H. Murayama , P. Nath , O. Naviliat-Cuncin , J. K. Nelson , D. Neuffer , J. S. Nico , A. Norman , D. Nygren , Y. Obayashi , T. P. O'Connor , Y. Okada , J. Olsen , L. Orozco , J. L. Orrell , J. Osta , B. Pahlka , J. Paley , V. Papadimitriou , M. Papucci , S. Parke , R. H. Parker , Z. Parsa , K. Partyka , A. Patch , J. C. Pati , R. B. Patterson , Z. Pavlovic , G. Paz , G. N. Perdue , D. Perevalov , G. Perez , R. Petti , W. Pettus , A. Piepke , M. Pivovaroff , R. Plunkett , C. C. Polly , M. Pospelov , R. Povey , A. Prakesh , M. V. Purohit , S. Raby , J. L. Raaf , R. Rajendran , S. Rajendran , G. Rameika , R. Ramsey , A. Rashed , B. N. Ratcliff , B. Rebel , J. Redondo , P. Reimer , D. Reitzner , F. Ringer , A. Ringwald , S. Riordan , B. L. Roberts , D. A. Roberts , R. Robertson , F. Robicheaux , M. Rominsky , R. Roser , J. L. Rosner , C. Rott , P. Rubin , N. Saito , M. Sanchez , S. Sarkar , H. Schellman , B. Schmidt , M. Schmitt , D. W. Schmitz , J. Schneps , A. Schopper , P. Schuster , A. J. Schwartz , M. Schwarz , J. Seeman , Y. K. Semertzidis , K. K. Seth , Q. Shafi , P. Shanahan , R. Sharma , S. R. Sharpe , M. Shiozawa , V. Shiltsev , K. Sigurdson , P. Sikivie , J. Singh , D. Sivers , T. Skwarnicki , N. Smith , J. Sobczyk , H. Sobel , M. Soderberg , Y. H. Song , A. Soni , P. Souder , A. Sousa , J. Spitz , M. Stancari , G. C. Stavenga , J. H. Steffen , S. Stepanyan , D. Stoeckinger , S. Stone , J. Strait , M. Strassler , I. A. Sulai , R. Sundrum , R. Svoboda , B. Szczerbinska , A. Szelc , T. Takeuchi , P. Tanedo , S. Taneja , J. Tang , D. B. Tanner , R. Tayloe , I. Taylor , J. Thomas , C. Thorn , X. Tian , B. G. Tice , M. Tobar , N. Tolich , N. Toro , I. S. Towner , Y. Tsai , R. Tschirhart , C. D. Tunnell , M. Tzanov , A. Upadhye , J. Urheim , S. Vahsen , A. Vainshtein , E. Valencia , R. G. Van de Water , R. S. Van de Water , M. Velasco , J. Vogel , P. Vogel , W. Vogelsang , Y. W. Wah , D. Walker , N. Weiner , A. Weltman , R. Wendell , W. Wester , M. Wetstein , C. White , L. Whitehead , J. Whitmore , E. Widmann , G. Wiedemann , J. Wilkerson , G. Wilkinson , P. Wilson , R. J. Wilson , W. Winter , M. B. Wise , J. Wodin , S. Wojcicki , B. Wojtsekhowski , T. Wongjirad , E. Worcester , J. Wurtele , T. Xin , J. Xu , T. Yamanaka , Y. Yamazaki , I. Yavin , J. Yeck , M. Yeh , M. Yokoyama , J. Yoo , A. Young , E. Zimmerman , K. Zioutas , M. Zisman , J. Zupan , R. Zwaska

We consider the possibility that the particles in the Ultra High Energy Cosmic Rays arriving to Earth might be neutrons instead of protons. We stress that in such case the argument for the GZK cutoff is weaker and that it is conceivable…

High Energy Physics - Phenomenology · Physics 2008-11-26 Adolfo De Unánue , Sarira Sahu , Daniel Sudarsky

We argue that fundamental objects in particle theory are not elementary particles and antiparticles but objects described by irreducible representations (IRs) of the de Sitter (dS) algebra. One might ask why, then, experimental data give…

General Physics · Physics 2024-03-13 Felix Lev

We show that neutrinos and electrons share the same theoretical structure, and satisfy parallel relations particularly of the Large Number kind. We then argue that the neutrino can be described as a ``cold'' electron in a sense that is…

General Physics · Physics 2007-05-23 B G Sidharth

Since quarks are regarded as the most fundamental particles which constitute hadrons that we observe in the real world, there are many theories about how many of them are needed and what quantum numbers they carry. Another important…

High Energy Physics - Phenomenology · Physics 2008-03-19 Y. S. Kim , Marilyn E. Noz

The quark and gluon structure of the proton has been under intense experimental and theoretical investigation for five decades. Even for the distributions of the well-studied valence quarks, challenges such as the value of the down quark to…

Nuclear Experiment · Physics 2019-03-27 D. F. Geesaman , P. E. Reimer

We explain why it is so hard to determine whether neutrinos are Majorana or Dirac particles as long as the only neutrinos we study are ultra-relativistic. We then show how non-relativistic neutrinos could help, and focus on the angular…

High Energy Physics - Phenomenology · Physics 2018-05-22 Boris Kayser

Weak radiative hyperon decays present us with a long-standing puzzle, namely the question of validity of a hadron-level theorem proved by Hara. We briefly discuss the conflict between expectations based on Hara's theorem and experiment as…

High Energy Physics - Phenomenology · Physics 2009-10-28 Piotr Zenczykowski

Even though neutrinos and antineutrinos are everywhere in the Universe, their critical importance might be overlooked, especially because that at least one species of neutrinos has the mass 0.058 eV, far larger than the cosmic…

High Energy Physics - Phenomenology · Physics 2016-01-14 W-Y. Pauchy Hwang

A new model for the substructure of quarks, leptons and weak gauge bosons is discussed. It is based on three fundamental and absolutely stable spin-1/2 preons. Its preon flavour SU(3) symmetry leads to a prediction of nine quarks, nine…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jean-Jacques Dugne , Sverker Fredriksson , Johan Hansson , Enrico Predazzi

We emphasize that the composite structure of the nucleon may play quite an important role in nuclear physics. It is shown that the momentum-dependent repulsive force of second order in the scalar field, which plays an important role in…

Nuclear Theory · Physics 2009-09-25 Koichi Saito , Anthony W. Thomas

We review the insufficiencies of the hypothesis that neutrinos and quarks are physical particles in our spacetime; we introduce the hypothesis that the energy and spin needed for the synthesis of the neutron inside stars originate either…

General Physics · Physics 2016-12-21 Ruggero Maria Santilli

The masses of the quarks and leptons are for the most part a mystery to particle physicists. Currently there seems to be no correlation between the masses of the elementary particles. This paper is an attempt to formulate a theory that…

Nuclear Theory · Physics 2007-05-23 Theodore M. Lach

In the chiral $SU(15)$ gauge theory presented here, the quarks and leptons are bound states ("prebaryons") of massless preons. The Standard Model charges of the preons imply 3 generations of quarks and leptons, plus some vectorlike fermions…

High Energy Physics - Phenomenology · Physics 2022-01-03 Bogdan A. Dobrescu
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