Unparticle Physics
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B2.IV Nuclear and Particle Physics
B2.IV Nuclear and Particle Physics A.J. Barr February 13, 2014 ii Contents 1 Introduction 1 2 Nuclear 3 2.1 Structure of matter and energy scales . 3 2.2 Binding Energy . 4 2.2.1 Semi-empirical mass formula . 4 2.3 Decays and reactions . 8 2.3.1 Alpha Decays . 10 2.3.2 Beta decays . 13 2.4 Nuclear Scattering . 18 2.4.1 Cross sections . 18 2.4.2 Resonances and the Breit-Wigner formula . 19 2.4.3 Nuclear scattering and form factors . 22 2.5 Key points . 24 Appendices 25 2.A Natural units . 25 2.B Tools . 26 2.B.1 Decays and the Fermi Golden Rule . 26 2.B.2 Density of states . 26 2.B.3 Fermi G.R. example . 27 2.B.4 Lifetimes and decays . 27 2.B.5 The flux factor . 28 2.B.6 Luminosity . 28 2.C Shell Model § ............................. 29 2.D Gamma decays § ............................ 29 3 Hadrons 33 3.1 Introduction . 33 3.1.1 Pions . 33 3.1.2 Baryon number conservation . 34 3.1.3 Delta baryons . 35 3.2 Linear Accelerators . 36 iii CONTENTS CONTENTS 3.3 Symmetries . 36 3.3.1 Baryons . 37 3.3.2 Mesons . 37 3.3.3 Quark flow diagrams . 38 3.3.4 Strangeness . 39 3.3.5 Pseudoscalar octet . 40 3.3.6 Baryon octet . 40 3.4 Colour . 41 3.5 Heavier quarks . 43 3.6 Charmonium . 45 3.7 Hadron decays . 47 Appendices 48 3.A Isospin § ................................ 49 3.B Discovery of the Omega § ...................... -
Bounds on Unparticles from the Higgs Sector
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by UNT Digital Library Preprint typeset in JHEP style - HYPER VERSION Bounds on Unparticles from the Higgs Sector Patrick J. Foxa, Arvind Rajaramanb and Yuri Shirmanb a Theoretical Physics Group, Lawrence Berkeley National Laboratory, Berkeley, CA 94720 b Department of Physics, University of California, Irvine, CA92697 Abstract: We study supersymmetric QCD in the conformal window as a laboratory for unparticle physics, and analyze couplings between the unparticle sector and the Higgs sector. These couplings can lead to the unparticle sector being pushed away from its scale invariant fixed point. We show that this implies that low energy experiments will not be able to see unparticle physics, and the best hope of seeing unparticles is in high energy collider experiments such as the Tevatron and the LHC. We also demonstrate how the breaking of scale invariance could be observed at these experiments. Contents 1. Introduction and Conclusions 1 2. Supersymmetric QCD as a model of unparticle physics 2 3. Operator analysis and experimental constraints 3 4. New effects in non-unparticle physics 5 1. Introduction and Conclusions Recently there has been a lot of interest [1–8] in unparticle theories [9, 10] in which the Standard Model (SM) is coupled to a conformal sector (called the unparticle sector). As shown in [9, 10], the conformal sector can have interesting and unexpected consequences. In this note, we shall investigate the effects on the conformal sector from the Higgs sector, and we will show that this leads to surprising new bounds on unparticle physics. -
When the Disorder Is Just Right
VIEWPOINT When the Disorder is Just Right A new model suggests that disorder can be a crucial ingredient for producing non-Fermi-liquid behavior in a system of interacting fermions. By Philip W. Phillips n 1956, physicist Lev Landau developed a theory describing devilishly difficult. Only a handful of solvable non-Fermi-liquid the low-temperature properties of helium-3 as those of a models exist for simplified cases. Building on one of these Iliquid of interacting fermions. Landau’s Fermi-liquid theory models, called the Sachdev–Ye–Kitaev (SYK) model [1], a team turned out to be widely applicable. It successfully describes, for led by Subir Sachdev of Harvard University has developed a new instance, the low-temperature properties of most metals. There theory that addresses an important, unresolved question: how are, however, numerous fermionic systems that aren’t Fermi does non-Fermi-liquid behavior arise in a condensed-matter liquids, including one-dimensional “Luttinger” liquids, Mott system—for instance, one where fermions (such as electrons) insulators, and heavy fermion materials. Understanding these are coupled to massless bosons (such as phonons)? The team’s exotic systems is an important research direction in modern results show that in a 2D system, non-Fermi liquid behavior can condensed-matter physics, but their theoretical description is emerge if there is a sufficient degree of disorder in the coupling between the bosons and the fermions [2]. To understand what might destroy Fermi-liquid behavior, it is helpful to recall an important property of Fermi liquids—they admit a purely local description in momentum space. -
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. -
Lecture 2 - Energy and Momentum
Lecture 2 - Energy and Momentum E. Daw February 16, 2012 1 Energy In discussing energy in a relativistic course, we start by consid- ering the behaviour of energy in the three regimes we worked with last time. In the first regime, the particle velocity v is much less than c, or more precisely β < 0:3. In this regime, the rest energy ER that the particle has by virtue of its non{zero rest mass is much greater than the kinetic energy T which it has by virtue of its kinetic energy. The rest energy is given by Einstein's famous equation, 2 ER = m0c (1) So, here is an example. An electron has a rest mass of 0:511 MeV=c2. What is it's rest energy?. The important thing here is to realise that there is no need to insert a factor of (3×108)2 to convert from rest mass in MeV=c2 to rest energy in MeV. The units are such that 0.511 is already an energy in MeV, and to get to a mass you would need to divide by c2, so the rest mass is (0:511 MeV)=c2, and all that is left to do is remove the brackets. If you divide by 9 × 1016 the answer is indeed a mass, but the units are eV m−2s2, and I'm sure you will appreciate why these units are horrible. Enough said about that. Now, what about kinetic energy? In the non{relativistic regime β < 0:3, the kinetic energy is significantly smaller than the rest 1 energy. -
The Standard Model and Beyond Maxim Perelstein, LEPP/Cornell U
The Standard Model and Beyond Maxim Perelstein, LEPP/Cornell U. NYSS APS/AAPT Conference, April 19, 2008 The basic question of particle physics: What is the world made of? What is the smallest indivisible building block of matter? Is there such a thing? In the 20th century, we made tremendous progress in observing smaller and smaller objects Today’s accelerators allow us to study matter on length scales as short as 10^(-18) m The world’s largest particle accelerator/collider: the Tevatron (located at Fermilab in suburban Chicago) 4 miles long, accelerates protons and antiprotons to 99.9999% of speed of light and collides them head-on, 2 The CDF million collisions/sec. detector The control room Particle Collider is a Giant Microscope! • Optics: diffraction limit, ∆min ≈ λ • Quantum mechanics: particles waves, λ ≈ h¯/p • Higher energies shorter distances: ∆ ∼ 10−13 cm M c2 ∼ 1 GeV • Nucleus: proton mass p • Colliders today: E ∼ 100 GeV ∆ ∼ 10−16 cm • Colliders in near future: E ∼ 1000 GeV ∼ 1 TeV ∆ ∼ 10−17 cm Particle Colliders Can Create New Particles! • All naturally occuring matter consists of particles of just a few types: protons, neutrons, electrons, photons, neutrinos • Most other known particles are highly unstable (lifetimes << 1 sec) do not occur naturally In Special Relativity, energy and momentum are conserved, • 2 but mass is not: energy-mass transfer is possible! E = mc • So, a collision of 2 protons moving relativistically can result in production of particles that are much heavier than the protons, “made out of” their kinetic -
3/2/15 -3/4/15 Week, Ken Intriligator's Phys 4D Lecture Outline • the Principle of Special Relativity Is That All of Physics
3/2/15 -3/4/15 week, Ken Intriligator’s Phys 4D Lecture outline The principle of special relativity is that all of physics must transform between • different inertial frames such that all are equally valid. No experiment can tell Alice or Bob which one is moving, as long as both are in inertial frames (so vrel = constant). As we discussed, if aµ = (a0,~a) and bµ = (b0,~b) are any 4-vectors, they transform • with the usual Lorentz transformation between the lab and rocket frames, and a b · ≡ a0b0 ~a ~b is a Lorentz invariant quantity, called a 4-scalar. We’ve so far met two examples − · of 4-vectors: xµ (or dxµ) and kµ. Some other examples of 4-scalars, besides ∆s2: mass m, electric charge q. All inertial • observers can agree on the values of these quantities. Also proper time, dτ ds2/c2. ≡ Next example: 4-velocity uµ = dxµ/dτ = (γ, γ~v). Note d = γ d . Thep addition of • dτ dt velocities formula becomes the usual Lorentz transformation for 4-velocity. In a particle’s own rest frame, uµ = (1,~0). Note that u u = 1, in any frame of reference. uµ can · be physically interpreted as the unit tangent vector to a particle’s world-line. All ~v’s in physics should be replaced with uµ. In particular, ~p = m~v should be replaced with pµ = muµ. Argue pµ = (E/c, ~p) • from their relation to xµ. So E = γmc2 and ~p = γm~v. For non-relativistic case, E ≈ 2 1 2 mc + 2 m~v , so rest-mass energy and kinetic energy. -
Search for Dark Matter and Unparticles Produced in Association with a Z Boson in Proton-Proton Collisions at √S = 8 Tev
Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at √s = 8 TeV The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Khachatryan, V. et al. “Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at √s = 8 TeV.” Physical Review D 93, 5 (March 2016): 052011 © 2016 CERN, for the CMS Collaboration As Published http://dx.doi.org/10.1103/PhysRevD.93.052011 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/110705 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. PHYSICAL REVIEW D 93, 052011 (2016) Search for dark matter and unparticles producedp inffiffi association with a Z boson in proton-proton collisions at s ¼ 8 TeV V. Khachatryan et al.* (CMS Collaboration) (Received 30 November 2015; published 22 March 2016) A search for evidence of particle dark matter (DM) and unparticle production at the LHC has been performed using events containing two charged leptons, consistent with the decay of a Z boson, and large missing transverse momentum. This study is based on data collected with the CMS detector corresponding to an integrated luminosity of 19.7 fb−1 of pp collisions at the LHC at a center-of-mass energy of 8 TeV. No significant excess of events is observed above the number expected from the standard model contributions. -
INTELLIGENCE, the FOUNDATION of MATTER Albert Hoffmann
INTELLIGENCE, THE FOUNDATION OF MATTER Albert Hoffmann To cite this version: Albert Hoffmann. INTELLIGENCE, THE FOUNDATION OF MATTER. 2020. halshs-02458460 HAL Id: halshs-02458460 https://halshs.archives-ouvertes.fr/halshs-02458460 Submitted on 28 Jan 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. INTELLIGENCE, THE FOUNDATION OF MATTER (by Albert Hoffmann – 2019) [01] All the ideas presented in this article are based on the writings of Jakob Lorber who between 1840 until his death in 1864 wrote 25 volumes under divine inspiration. This monumental work is referred to as the New Revelation (NR) and the books can be read for free online at the Internet Archive at https://archive.org/details/BeyondTheThreshold. It contains the most extraordinary deepest of wisdom ever brought to paper and touches on every conceivable subject of life. Internationally renowned statistician, economist and philosopher E.F. Schumacher who became famous for his best-seller “Small is Beautiful”, commented about the NR in his book “A Guide for the Perplexed” as follows: "They (the books of the NR) contain many strange things which are unacceptable to modern mentality, but at the same time contain such plethora of high wisdom and insight that it would be difficult to find anything more impressive in the whole of world literature." (1977). -
Vector Unparticle Enhanced Black Holes: Exact Solutions and Thermodynamics
Physics Faculty Works Seaver College of Science and Engineering 9-2010 Vector unparticle enhanced black holes: exact solutions and thermodynamics Jonas R. Mureika Loyola Marymount University, [email protected] Euro Spallucci Universit`a di Trieste & INFN Follow this and additional works at: https://digitalcommons.lmu.edu/phys_fac Part of the Physics Commons Recommended Citation Mureika, J.R. and E. Spallucci, "Vector unparticle enhanced black holes: Exact solutions and thermodynamics," Physics Letters B 693, 129-133 (2010). http://dx.doi.org/10.1016/ j.physletb.2010.08.025. This Article - post-print is brought to you for free and open access by the Seaver College of Science and Engineering at Digital Commons @ Loyola Marymount University and Loyola Law School. It has been accepted for inclusion in Physics Faculty Works by an authorized administrator of Digital Commons@Loyola Marymount University and Loyola Law School. For more information, please contact [email protected]. Vector unparticle enhanced black holes: exact solutions and thermodynamics J. R. Mureika 1 Department of Physics, Loyola Marymount University, Los Angeles, CA 90045-2659 Euro Spallucci 2 Dipartimento di Fisica Teorica, Universit`adi Trieste and INFN, Sezione di Trieste, Italy Abstract Tensor and scalar unparticle couplings to matter have been shown to enhance gravitational interactions and provide corrections to the Schwarzschild metric and associated black hole structure. We derive an exact solution to the Einstein equations for vector unparticles, and conclusively demonstrate that these induce Riessner-Nordstr¨om (RN)-like solutions where the role of the “charge” is defined by a composite of unparticle phase space parameters. These black holes admit double-horizon structure, although unlike the RN metric these solutions have a minimum inner horizon value. -
The Question of Charge and of Mass
The question of charge and of mass. Voicu Dolocan Faculty of Physics, University of Bucharest, Bucharest, Romania Abstract. There are two long –range forces in the Universe, electromagnetism and gravity. We have found a general expression for the energy of interaction in these cases, αћc/r, where α is the fine structure constant and r is the distance between the two particles. In the case of electromagnetic interaction we have 2 αћc = e /4πεo, where e is the gauge charge, which is the elementary electron charge. In the case of the gravitational interaction we have αћc = GM2, where M = 1.85×10-9 kg is the gauge mass of the particle. This is a giant particle. A system of like charged giant particles, would be a charged superfluid. By spontaneous breaking of a gauge symmetry are generated the Higgs massive bosons. The unitary gauge assure generation of the neutral massive particles. The perturbation from the unitary gauge generates charged massive particles. Also, the Higgs boson decays into charged and neutral particles. The Tesla coil is the user of the excitations of the vacuum. 1. What is electric charge, and what is mass? According to the Standard Model “ The electric charge is a fundamental conserved property of certain subatomic particles that determines the electromagnetic interactions”. Electrically charged particles are influenced by and create electromagnetic fields. The elementary unit of charge is carried by a single proton and the equivalent negative charge is carried by a single electron. Also, there are up quarks with (2/3)e charge and there are down quarks with (1/3)e- charge. -
Strange Metals
SciPost Phys. 6, 061 (2019) Planckian dissipation, minimal viscosity and the transport in cuprate strange metals Jan Zaanen The Institute Lorentz for Theoretical Physics, Leiden University, Leiden, The Netherlands [email protected] Abstract Could it be that the matter formed from the electrons in high Tc superconductors is of a radically new kind that may be called "many body entangled compressible quantum matter"? Much of this text is intended as an easy to read tutorial, explaining recent theoretical advances that have been unfolding at the cross roads of condensed matter- and string theory, black hole physics as well as quantum information theory. These de- velopments suggest that the physics of such matter may be governed by surprisingly simple principles. My real objective is to present an experimental strategy to test criti- cally whether these principles are actually at work, revolving around the famous linear resistivity characterizing the strange metal phase. The theory suggests a very simple explanation of this "unreasonably simple" behavior that is actually directly linked to re- markable results from the study of the quark gluon plasma formed at the heavy ion colliders: the "fast hydrodynamization" and the "minimal viscosity". This leads to high quality predictions for experiment: the momentum relaxation rate governing the resis- tivity relates directly to the electronic entropy, while at low temperatures the electron fluid should become unviscous to a degree that turbulent flows can develop even on the nanometre scale. Copyright J. Zaanen. Received 05-09-2018 This work is licensed under the Creative Commons Accepted 14-05-2019 Check for Attribution 4.0 International License.