Detection Scenarios for Preon Stars Detection Scenarios for Preon Stars
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International Centre for Theoretical Physics
IC/80/62 INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS QUANTUM CHROMODYNAMICS A THEORY OF THE NUCLEAR FORCE U.S. Craigie INTERNATIONAL ATOMIC ENERGY AGENCY UNITED NATIONS EDUCATIONAL, SCIENTIFIC AND CULTURAL ORGANIZATION 1980 MIRAMARE-TRIESTE IC/8O/6E International Atomic Energy Agency sad United Rations Educational Scientific and Cultural Organization IBTEHHATIOHAL CEHTHB FOR THEORETICAL PHYSICS QUAHTUM CHROMODIHAMICS A THBORT OF TIffl KUCLEAK FORCE • H.S. Craigie tnterna.ttgp«l Centre for Theoretical Phyaics, Trieste, Italy, and Ietltuto IFuiotude dl Fisiea Kucleare, Sezlone dl Trieste, Italy. MHUHHB- TRIESTE June l?60 aliven at tJse Int#rM*iotial SuB»er College on Physics ana Seeds, Nathiagali,Pakistan, 1&-28 Jtm« 1980, EARLY ID"Ad ON T'KK NVCLrAR F'JRCK AiO Tire uMEKOENCE OF1 THE tJCD LAGRANGIAN Let us recap a little of the early ideas on the nuclear force. [n the AIMS s, nuclear structure was thought to be described in terms of elementary protons and neutrons, which formed an isospin doublet 5 =| P\ vith I, = -^ In these lectures I hope to give a brief outline of a possible theory for the proton aiui T = -rz for the neutron, where isospiti, i.e. SU{2) of the nuclear force and the strong interactions between elementary particles, invariance, vas the recognised symmetry of nuclear interactions at ttvit time. which ve suppose is responsible for nuclear matter. The theory I will be Further, the nuclear force between these nucleons was thought to be mediated by describing is known as quantum chromodynamics because of its association vith an elementary meson, which was seen to form an isotriplet (IT ,tt ,n ) because i new kind of nuclear charge called colour and its resemblance to quantum of its three charged states- If all these particles were elementary, then in electrodynamics. -
Astro-Ph/0410417V1 18 Oct 2004 Nwihteeaen Tbeconfigurations
Preon stars: a new class of cosmic compact objects J. Hansson∗ & F. Sandin† Department of Physics, Lule˚aUniversity of Technology, SE-971 87 Lule˚a, Sweden In the context of the standard model of particle physics, there is a definite upper limit to the density of stable compact stars. However, if a more fundamental level of elementary particles exists, in the form of preons, stability may be re-established beyond this limiting density. We show that a degenerate gas of interacting fermionic preons does allow for stable compact stars, with densities far beyond that in neutron stars and quark stars. In keeping with tradition, we call these objects “preon stars”, even though they are small and light compared to white dwarfs and neutron stars. We briefly note the potential importance of preon stars in astrophysics, e.g., as a candidate for cold dark matter and sources of ultra-high energy cosmic rays, and a means for observing them. PACS numbers: 12.60.Rc - 04.40.Dg - 97.60.-s - 95.35.+d I. INTRODUCTION The three different types of compact objects traditionally considered in astrophysics are white dwarfs, neutron stars (including quark and hybrid stars), and black holes. The first two classes are supported by Fermi pressure from their constituent particles. For white dwarfs, electrons provide the pressure counterbalancing gravity. In neutron stars, the neutrons play this role. For black holes, the degeneracy pressure is overcome by gravity and the object collapses indefinitely, or at least to the Planck density. arXiv:astro-ph/0410417v1 18 Oct 2004 The distinct classes of degenerate compact stars originate directly from the properties of gravity, as was made clear by a theorem of Wheeler and collaborators in the mid 1960s [1]. -
The Structure of Quarks and Leptons
The Structure of Quarks and Leptons They have been , considered the elementary particles ofmatter, but instead they may consist of still smaller entities confjned within a volume less than a thousandth the size of a proton by Haim Harari n the past 100 years the search for the the quark model that brought relief. In imagination: they suggest a way of I ultimate constituents of matter has the initial formulation of the model all building a complex world out of a few penetrated four layers of structure. hadrons could be explained as combina simple parts. All matter has been shown to consist of tions of just three kinds of quarks. atoms. The atom itself has been found Now it is the quarks and leptons Any theory of the elementary particles to have a dense nucleus surrounded by a themselves whose proliferation is begin fl. of matter must also take into ac cloud of electrons. The nucleus in turn ning to stir interest in the possibility of a count the forces that act between them has been broken down into its compo simpler-scheme. Whereas the original and the laws of nature that govern the nent protons and neutrons. More recent model had three quarks, there are now forces. Little would be gained in simpli ly it has become apparent that the pro thought to be at least 18, as well as six fying the spectrum of particles if the ton and the neutron are also composite leptons and a dozen other particles that number of forces and laws were thereby particles; they are made up of the small act as carriers of forces. -
Quark-Lepton Unification and Proton Decay
\\£ IC/80/72 INTERNATIONAL CENTRE FOR •2t i / -Tr/ THEORETICAL PHYSICS QUARK-LEPTON UNIFICATION AND PROTON DECAY Jogesh C. Pati and Abdus Salam INTERNATIONAL ATOMIC ENERGY AGENCY UNITED NATIONS EDUCATIONAL, SCIENTIFIC AND CULTURAL ORGANIZATION 1980 MIRAMARE-TRIESTE IC/60/72 QUABK-LEFTON UNIFICATION AND PROTON DECAY I. INTRODUCTION Jogesh C. Pati The hypothesis of prnncS unification servinR to unify all basic particles - quarks and leptons - and their force:; - weak, International Centre for Theoretical Physics, Trieste, Italy, electromagnetic as well as strong - stands at present primarily and on its aesthetic merits. It gives the flavour of synthesis in that it provides a rationale for the existence of quarks and Department of Physics, University of Maryland, College Park, leptons by assigning the two sets of particles to one multiplet + Maryland, USA, of a gauge symmetry G. It derives their forces through one principle-gauge unification. and With quarks and leptons in one multiplet of a local sponta- neously broken gauge symmetry G, baryon and lepton number conserv- ation cannot be absolute. This line of reasoning had led us to Abdiis Salam suggest in 1973 that the lightest baryon - the proton - must ultimately decay into leptons 2. Theoretical considerations International Centre for Theoretical Physics, Trieste, Italy, suggest a lifetime for the proton in the ran^e of 102° to 1033 a and years "5. Its decay modes and corresponding branching ratios depend In general upon the details of the structure of the symmetry Imperial College, London, England. Kroup and its breaking Dattern. What is worth noticing »t this Junction Is that studies of (i) proton decay modes, (il) n-n oscillation (iii) neutrinoless double 6-deeay and (iv) the weak angle T sin26y are perhaps the only effective tools we would have for sometiae to probe into the underlying design of grand unification. -
The Maxwell-Cassano Equations of an Electromagnetic-Nuclear Field Yields the Fermion & Hadron Architecture
ISSN: 2639-0108 Research Article Advances in Theoretical & Computational Physics The Maxwell-Cassano Equations of an Electromagnetic-nuclear Field Yields the Fermion & Hadron Architecture Claude Michael Cassano *Corresponding author Claude Michael Cassano, Santa Clara, California, USA; E-mail: cloudmichael@ Santa Clara, California, USA hotmail.com Submitted: 16 July 2019; Accepted: 23 July 2019; Published: 05 Aug 2019 Abstract The Helmholtzian operator and factorization, via the Maxwell-Cassano equations yields a fermion architecture table equivalent to that of the standard model and lead to linear transformation groups of the mesons and baryons, respectively; plus a straightforward elementary description of quark colour based on integral indices: 1,0,1, rather than the subjective, correlative explanation using: {R,G,B;Y} indexes. keywords: Helmholtzian, Klein-Gordon equation, electromag- where: netism, preon, elementary particles, standard model, elementary (2) particle, particle interactions, fermions, leptons, quarks, hadrons, mesons, baryons, Pauli matrices, Gell-Mann matrices, Hermitian (3) matrices, Lie algebra, su(2), Yukawa potential Similarly, mass-generalized electric and magnetic potentials for the Introduction Helmholtzian operator factorization : Using the principles of the analysis of a linear function of a linear variable [1], constuctive algebras developed using the weighted matrix product [2] leads to the d’Alembertian operator and it’s factorization [3], and a space with all smooth functions satisfying Maxwell’s equations [4] [5] [6] [7]. This leads to the Helmholtzian operator and factorization[8], and a space in which all smooth functions satisfy the Maxwell-Cassano equations[9] (which generalizes both Maxwell’s equations and the Dirac equation [10] [11] [12]) - a linearization of the Klein-Gordon equations [13] [14] [12]. -
Pages from C13-03-02 3.Pdf
The GIM Mechanism: origin, predictions and recent uses Luciano Maiani CERN, Geneva, Switzerland Dipartimento di Fisica, Universita di Roma La Sapienza, Roma, Italy The GIM Mechanism was introduced by Sheldon L. Glashow, John Iliopoulos and Luciano Maiani in 1970) to explain the suppression of Delta S=l, 2 neutral current processes and is an important element of the unified theories of the weak and electromagnetic interactions. Origin, predictions and uses of the GIM Mechanism are illustrated. Flavor changing neutral current processes (FCNC) represent today an important benchmark for the Standard Theory and give strong limitations to theories that go beyond ST in the fewTe V region. Ideas on the ways constraints on FCNC may be imposed are briefly described. 1 Setting the scene The final years of the sixties marked an important transition period for the physics of elementary particles. Two important discoveries made in the early sixties, quarks and Cabibbo theory, had been consolidated by a wealth of new data and there was the feeling that a more complete picture of the strong and of the electro-weak interactions could be at hand. The quark model of hadrons introduced by M. Gell-Mann 1 and G. Zweig2 explained neatly the spectrum of the lowest lying mesons and baryons as qij and qqq states, respectively, with: (1) and electric charges Q 2/3 1/3 /3 respectively. 1 Doubts persisted on= quarks, - being, - real, physical entities or rather a simple mathematical tool to describe hadrons. This was due to the symmetry puzzle, namely the fact that one had to assume an overall symmetric configuration of the three quarks to describe the spin-charge structure of the baryons, rather than the antisymmetric configuration required by the fermion nature of physical, spin 1/2, quark$'. -
Combinatorial Preon Model for Matter and Unification
Open Access Library Journal 2016, Volume 3, e3032 ISSN Online: 2333-9721 ISSN Print: 2333-9705 Combinatorial Preon Model for Matter and Unification Risto Raitio Espoo, Finland How to cite this paper: Raitio, R. (2016) Abstract Combinatorial Preon Model for Matter and Unification. Open Access Library Journal, 3: I consider a preon model for quarks and leptons based on constituents defined by e3032. mass, spin and charge. The preons form a finite combinatorial system for the stan- http://dx.doi.org/10.4236/oalib.1103032 dard model fermions. The color and weak interaction gauge structures can be de- Received: September 2, 2016 duced from the preon bound states. By applying the area eigenvalues of loop quan- Accepted: October 8, 2016 tum gravity to black hole preons, one gets a preon mass spectrum starting from zero. Published: October 11, 2016 Gravitational baryon number non-conservation mechanism is obtained. Argument is given for unified field theory is based only on gravitational and electromagnetic in- Copyright © 2016 by author and Open Access Library Inc. teractions of preons. This work is licensed under the Creative Commons Attribution International Subject Areas License (CC BY 4.0). http://creativecommons.org/licenses/by/4.0/ Particle Physics Open Access Keywords Preons, Standard Model, Quantum Black Hole, Statistical Mechanics, General Relativity, Loop Quantum Gravity 1. Introduction The purpose of this note is to reinforce a draft model for particles, their interactions and spacetime [1]-[3]. The difficulty of constructing a unified picture of “everything” is realized. It has been questioned whether such popular elements, like grand unified theories (GUT) of gauge interactions, supersymmetry or, most intriguingly, superstring theory, do occur in nature. -
Preon Trinity
Preon Trinity Jean-Jacques Dugne,1 Sverker Fredriksson,2 Johan Hansson,2 and Enrico Predazzi3 1Laboratoire de Physique Corpusculaire, Universit´eBlaise Pascal, Clermont-Ferrand II, FR-63177 Aubi`ere, France 2Department of Physics, Lule˚aUniversity of Technology, SE-97187 Lule˚a, Sweden 3Department of Theoretical Physics, Universit´adi Torino, IT-10125 Torino, Italy We present a new minimal model for the substructure of all known quarks, leptons and weak gauge bosons, based on only three fundamental and stable spin-1/2 preons. As a consequence, we predict three new quarks, three new leptons, and six new vector bosons. One of the new quarks has charge −4e/3. The model explains the apparent conservation of three lepton numbers, as well as the so- called Cabibbo-mixing of the d and s quarks, and predicts electromagnetic decays or oscillations between the neutrinosν ¯µ (νµ) and νe (¯νe). Other neutrino oscillations, as well as rarer quark mixings and CP violation can come about due to a small quantum-mechanical mixing of two of the preons in the quark and lepton wave functions. PACS numbers: 12.60.Rc, 13.35.-r, 14.60.-z, 14.65.-q The arguments in favor of a substructure of quarks and Kobayashi-Maskawa formalism [6] (quantified by the so- leptons in terms of more fundamental preons have been called CKM matrix), and the CP violation in neutral K discussed for two decades (a review is given in [1]). The meson decays. most compelling ones are that there exist so many quarks A classical problem with all preon models (including and leptons, and that they seemingly form a pattern of ours) is that neutrinos are so much lighter than the three “families”. -
Neutrino Masses and the Structure of the Weak Gauge Boson
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Neutrino masses and the structure of the weak gauge boson V.N.Yershov University College London, Mullard Space Science Laboratory, Holmbury St.Mary, Dorking RH5 6NT, United Kingdom E-mail: [email protected] Abstract. The problem of neutrino masses is discussed. It is assumed that the electron 0 neutrino mass is related to the structures and masses of the W ± and Z bosons. Using a composite model of fermions (described by the author elsewhere), it is shown that the massless 0 neutrino is not consistent with the high values of the experimental masses of W ± and Z . Consistency can be achieved on the assumption that the electron-neutrino has a mass of about 4.5 meV. Masses of the muon- and tau-neutrinos are also estimated. PACS numbers: 11.30.Na, 12.60.Rc, 14.60.St, 14.70.Fm, 14.70.Hp 1. Introduction The results of recent observations of atmospheric and solar neutrinos aimed at testing the hypothesis of the neutrino flavour oscillations [1, 2] indicate that neutrinos are massive. Although a very small, but non-zero neutrino mass, can be a key to new physics underlying the Standard Model of particle physics [3]. The Standard Model consider all three neutrinos (νe, νµ,andντ ) to be massless. Thus, observations show that the Standard Model needs some corrections or extensions. So far, many models have been proposed in order to explain possible mechanisms for the neutrino mass generation [4]-[9], and many experiments have been carried out for measuring this mass. -
Israel Prize
Year Winner Discipline 1953 Gedaliah Alon Jewish studies 1953 Haim Hazaz literature 1953 Ya'akov Cohen literature 1953 Dina Feitelson-Schur education 1953 Mark Dvorzhetski social science 1953 Lipman Heilprin medical science 1953 Zeev Ben-Zvi sculpture 1953 Shimshon Amitsur exact sciences 1953 Jacob Levitzki exact sciences 1954 Moshe Zvi Segal Jewish studies 1954 Schmuel Hugo Bergmann humanities 1954 David Shimoni literature 1954 Shmuel Yosef Agnon literature 1954 Arthur Biram education 1954 Gad Tedeschi jurisprudence 1954 Franz Ollendorff exact sciences 1954 Michael Zohary life sciences 1954 Shimon Fritz Bodenheimer agriculture 1955 Ödön Pártos music 1955 Ephraim Urbach Jewish studies 1955 Isaac Heinemann Jewish studies 1955 Zalman Shneur literature 1955 Yitzhak Lamdan literature 1955 Michael Fekete exact sciences 1955 Israel Reichart life sciences 1955 Yaakov Ben-Tor life sciences 1955 Akiva Vroman life sciences 1955 Benjamin Shapira medical science 1955 Sara Hestrin-Lerner medical science 1955 Netanel Hochberg agriculture 1956 Zahara Schatz painting and sculpture 1956 Naftali Herz Tur-Sinai Jewish studies 1956 Yigael Yadin Jewish studies 1956 Yehezkel Abramsky Rabbinical literature 1956 Gershon Shufman literature 1956 Miriam Yalan-Shteklis children's literature 1956 Nechama Leibowitz education 1956 Yaakov Talmon social sciences 1956 Avraham HaLevi Frankel exact sciences 1956 Manfred Aschner life sciences 1956 Haim Ernst Wertheimer medicine 1957 Hanna Rovina theatre 1957 Haim Shirman Jewish studies 1957 Yohanan Levi humanities 1957 Yaakov -
Braided Fermions from Hurwitz Algebras
Braided fermions from Hurwitz algebras Niels G Gresnigt Xi'an Jiaotong-Liverpool University, Department of Mathematical Sciences. 111 Ren'ai Road, Dushu Lake Science and Education Innovation District, Suzhou Industrial Park, Suzhou, 215123, P.R. China E-mail: [email protected] Abstract. Some curious structural similarities between a recent braid- and Hurwitz algebraic description of the unbroken internal symmetries for a single generations of Standard Model fermions were recently identified. The non-trivial braid groups that can be represented using c the four normed division algebras are B2 and B3, exactly those required to represent a single generation of fermions in terms of simple three strand ribbon braids. These braided fermion states can be identified with the basis states of the minimal left ideals of the Clifford algebra C`(6), generated from the nested left actions of the complex octonions C ⊗ O on itself. That is, the ribbon spectrum can be related to octonion algebras. Some speculative ideas relating to ongoing research that attempts to construct a unified theory based on braid groups and Hurwitz algebras are discussed. 1. Introduction Leptons and quarks are identified with representations of the gauge group U(1)Y × SU(2)L × SU(3)C in the Standard Model (SM) of particle physics. Despite its success in accurately describing and predicting experimental observations, this gauge group lacks a theoretical basis. Why has Nature chosen these gauge groups from an infinite set of Lie groups, and why do only some representations correspond to physical states? A second shortcoming of the SM is the lack of gravity, or equivalently, its unification with General Relativity (GR). -
A Conjectural Preon Theory and Its Implications
A Conjectural Preon Theory and its Implications Rupert Gerritsen Copyright © - Rupert Gerritsen Batavia Online Publishing A Conjectural Preon Theory and its Implications Batavia Online Publishing Canberra, Australia Published by Batavia Online Publishing 2012 Copyright © Rupert Gerritsen National Library of Australia Cataloguing-in-Publication Data Author: Gerritsen, Rupert, 1953- Title: A Conjectural Preon Theory ISBN: 978-0-9872141-5-7 (pbk.) Notes: Includes bibliographic references Subjects: Particles (Nuclear physics) Dewey Number: 539.72 Copyright © - Rupert Gerritsen 1 A Conjectural Preon Theory and its Implications At present the dominant paradigm in particle physics is the Standard Model. This theory has taken hold over the last 30 years as its predictions of new particles have been dramatically borne out in increasingly sophisticated experiments. Despite this it would seem that the Standard Model has some shortcomings and leaves a number of questions unanswered. The number of arbitrary constants and parameters incorporated in the Model is one unsatisfactory aspect, as is its inability to explain the masses of the quarks and leptons. Another problematic area often cited is the Model’s failure to account for the number of generations of quarks and leptons. The plethora of “fundamental” particles also appears to represent a major weakness in the Standard Model. There are 16 “fundamental” or “elementary” particles, as well as their anti-particles, engendered in the Standard Model, along with 8 types of gluons. This difficulty may be further compounded by theorizing based on supersymmetry, as an extension of the Standard Model, because it requires heavier twins for the known particles. Furthermore the Higgs mechanism, postulated to generate mass in particles, has not as yet been validated experimentally.