Physics Beyond Colliders at CERN: Beyond the Standard Model
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Freeze-In Dark Matter from a Minimal B-L Model and Possible Grand
PHYSICAL REVIEW D 101, 115022 (2020) Freeze-in dark matter from a minimal B − L model and possible grand unification Rabindra N. Mohapatra1 and Nobuchika Okada 2 1Maryland Center for Fundamental Physics and Department of Physics, University of Maryland, College Park, Maryland 20742, USA 2Department of Physics and Astronomy, University of Alabama, Tuscaloosa, Alabama 35487, USA (Received 5 May 2020; accepted 5 June 2020; published 17 June 2020) We show that a minimal local B − L symmetry extension of the standard model can provide a unified description of both neutrino mass and dark matter. In our model, B − L breaking is responsible for neutrino masses via the seesaw mechanism, whereas the real part of the B − L breaking Higgs field (called σ here) plays the role of a freeze-in dark matter candidate for a wide parameter range. Since the σ particle is unstable, for it to qualify as dark matter, its lifetime must be longer than 1025 seconds implying that the B − L gauge coupling must be very small. This in turn implies that the dark matter relic density must arise from the freeze-in mechanism. The dark matter lifetime bound combined with dark matter relic density gives a lower bound on the B − L gauge boson mass in terms of the dark matter mass. We point out parameter domains where the dark matter mass can be both in the keV to MeV range as well as in the PeV range. We discuss ways to test some parameter ranges of this scenario in collider experiments. Finally, we show that if instead of B − L, we consider the extra Uð1Þ generator to be −4I3R þ 3ðB − LÞ, the basic phenomenology remains unaltered and for certain gauge coupling ranges, the model can be embedded into a five-dimensional SOð10Þ grand unified theory. -
1 Standard Model: Successes and Problems
Searching for new particles at the Large Hadron Collider James Hirschauer (Fermi National Accelerator Laboratory) Sambamurti Memorial Lecture : August 7, 2017 Our current theory of the most fundamental laws of physics, known as the standard model (SM), works very well to explain many aspects of nature. Most recently, the Higgs boson, predicted to exist in the late 1960s, was discovered by the CMS and ATLAS collaborations at the Large Hadron Collider at CERN in 2012 [1] marking the first observation of the full spectrum of predicted SM particles. Despite the great success of this theory, there are several aspects of nature for which the SM description is completely lacking or unsatisfactory, including the identity of the astronomically observed dark matter and the mass of newly discovered Higgs boson. These and other apparent limitations of the SM motivate the search for new phenomena beyond the SM either directly at the LHC or indirectly with lower energy, high precision experiments. In these proceedings, the successes and some of the shortcomings of the SM are described, followed by a description of the methods and status of the search for new phenomena at the LHC, with some focus on supersymmetry (SUSY) [2], a specific theory of physics beyond the standard model (BSM). 1 Standard model: successes and problems The standard model of particle physics describes the interactions of fundamental matter particles (quarks and leptons) via the fundamental forces (mediated by the force carrying particles: the photon, gluon, and weak bosons). The Higgs boson, also a fundamental SM particle, plays a central role in the mechanism that determines the masses of the photon and weak bosons, as well as the rest of the standard model particles. -
Gpus for the Realtime Low-Level Trigger of the NA62 Experiment at CERN
GPUs for the realtime low-level trigger of the NA62 experiment at CERN R. Ammendola4, M. Bauce3,7, A. Biagioni3, S. Chiozzi1,5, A. Cotta Ramusino1,5, R. Fantechi2, 1,5, 1,5 2,6 2,8 3 3,7 M. Fiorini ∗, A. Gianoli , E. Graverini , G. Lamanna , A. Lonardo , A. Messina , I. Neri1,5, F. Pantaleo2,6, P. S. Paolucci3, R. Piandani2,6, L. Pontisso2, F. Simula3, M. Sozzi2,6, P. Vicini3 1INFN Sezione di Ferrara, Via Saragat 1, 44122 Ferrara, Italy 2INFN Sezione di Pisa, Largo B. Pontecorvo 3, 56127 Pisa, Italy 3INFN Sezione di Roma“La Sapienza”, P.le A. Moro 2, 00185 Roma, Italy 4INFN Sezione di Roma “Tor Vergata”, Via della Ricerca Scientifica 1, 00133 Roma, Italy 5University of Ferrara, Via Saragat 1, 44122 Ferrara, Italy 6University of Pisa, Largo B. Pontecorvo 3, 56127 Pisa, Italy 7University of Rome “La Sapienza”, P.le A.Moro 2, 00185 Roma, Italy 8INFN Sezione di Frascati, Via E.Fermi 40, 00044 Frascati (Roma), Italy ∗ Corresponding author. E-mail: fi[email protected] DOI: http://dx.doi.org/10.3204/DESY-PROC-2014-05/15 A pilot project for the use of GPUs (Graphics processing units) in online triggering ap- plications for high energy physics experiments (HEP) is presented. GPUs offer a highly parallel architecture and the fact that most of the chip resources are devoted to computa- tion. Moreover, they allow to achieve a large computing power using a limited amount of space and power. The application of online parallel computing on GPUs is shown for the synchronous low level trigger of NA62 experiment at CERN. -
Electron Ion Collider Conceptual Design Report Experimental Equipment Contributors: W
November 18, 2020 Electron Ion Collider Conceptual Design Report Experimental Equipment Contributors: W. Akers2, E-C. Aschenauer1, F. Barbosa2, A. Bressan3, C.M. Camacho4, K. Chen1, S. Dalla Torre3 L. Elouadhriri2, R. Ent2, O. Evdokimov5, Y. Furletova2, D. Gaskell2, T. Horn6, J. Huang1, A. Jentsch1, A. Kiselev1, W. Schmidke1, R. Seidl7, T. Ullrich1, 1Brookhaven National Laboratory, USA 2Thomas Jefferson National Accelerator Facility, USA 3University of Trieste and INFN at Trieste, Italy 4Institut de Physique Nucleaire´ at Orsay, France 5University of Illinois at Chicago, USA 6Catholic University of America, Washington DC, USA 7RIKEN Nishina Center for Accelerator-Based Science, Japan Contents 2 The Science of EIC 1 2.1 Introduction . .1 2.1.1 EIC Physics and Accelerator Requirements . .1 2.1.2 Interaction Region and Detector Requirements . .2 2.2 EIC Context and History . .5 2.3 The Science Goals of the EIC and the Machine Parameters . .6 2.3.1 Nucleon Spin and Imaging . .9 2.3.2 Physics with High-Energy Nuclear Beams at the EIC . 17 2.3.3 Passage of Color Charge Through Cold QCD Matter . 25 2.4 Summary of Machine Design Parameters for the EIC Physics . 27 2.5 Scientific Requirements for the Detectors and IRs . 30 2.5.1 Scientific Requirements for the Detectors . 31 2.5.2 Scientific Requirements for the Interaction Regions . 38 8 The EIC Experimental Equipment 49 8.1 Realization of the Experimental Equipment in the National and Interna- tional Context . 49 8.2 Experimental Equipment Requirements Summary . 51 8.3 Operational Requirements for an EIC Detector . 54 8.3.1 EIC Collision Rates and Multiplicities . -
Tests of the Do Calorimeter Response in 2-150 Gev Beams*
TESTS OF THE DO CALORIMETER RESPONSE IN 2-150 GEV BEAMS* Kaushik De t Department of Physics University of Michigan Ann Arbor, MI 48109 Abstract At the heart of the DO detector, which recently started its maiden data run at the Fermilab Tevatron p~ collider, is a finely segmented hermetic large angle liquid argon calorimeter. We present here results from the latest test beam studies of the calorimeter in 1991. Modules from the central calorimeter, end calorimeter and the inter-cryostat detector were included in this run. New results on resolution, uniformity and linearity will be presented with electron and pion beams of various energies. Special emphasis will be placed on first results from the innovative technique of using scintillator sampling in the in- termediate rapidity region to improve uniformity and hermeticity. INTRODUCTION study pp collisions at 1.8 TeV. The three ma- jor components of the detector include a cen- The DO experiment at the Fermilab Teva- tral tracking detector surrounded by a liquid tron uses a large angle hermetic detector to argon calorimeter, which in turn is enclosed in a magnetic tracking muon detector. A cut-out *Presented for the DO Collaboration: Universi- view of the calorimeter and central detector is dad de los Andes (Colombia), University of Aft- shown in Figure 1. sons, Brookhaven National Laboratory, Brown Uni- versity, University of California at Riverside, CBPF (Brasil), CINVESTAV (Mexico), Columbia Univer- sity, Delhi University (India), Fermilab, Florida State University, University of Hawaii, -
Supersymmetric Particle Searches
Citation: K.A. Olive et al. (Particle Data Group), Chin. Phys. C38, 090001 (2014) (URL: http://pdg.lbl.gov) Supersymmetric Particle Searches A REVIEW GOES HERE – Check our WWW List of Reviews A REVIEW GOES HERE – Check our WWW List of Reviews SUPERSYMMETRIC MODEL ASSUMPTIONS The exclusion of particle masses within a mass range (m1, m2) will be denoted with the notation “none m m ” in the VALUE column of the 1− 2 following Listings. The latest unpublished results are described in the “Supersymmetry: Experiment” review. A REVIEW GOES HERE – Check our WWW List of Reviews CONTENTS: χ0 (Lightest Neutralino) Mass Limit 1 e Accelerator limits for stable χ0 − 1 Bounds on χ0 from dark mattere searches − 1 χ0-p elastice cross section − 1 eSpin-dependent interactions Spin-independent interactions Other bounds on χ0 from astrophysics and cosmology − 1 Unstable χ0 (Lighteste Neutralino) Mass Limit − 1 χ0, χ0, χ0 (Neutralinos)e Mass Limits 2 3 4 χe ,eχ e(Charginos) Mass Limits 1± 2± Long-livede e χ± (Chargino) Mass Limits ν (Sneutrino)e Mass Limit Chargede Sleptons e (Selectron) Mass Limit − µ (Smuon) Mass Limit − e τ (Stau) Mass Limit − e Degenerate Charged Sleptons − e ℓ (Slepton) Mass Limit − q (Squark)e Mass Limit Long-livede q (Squark) Mass Limit b (Sbottom)e Mass Limit te (Stop) Mass Limit eHeavy g (Gluino) Mass Limit Long-lived/lighte g (Gluino) Mass Limit Light G (Gravitino)e Mass Limits from Collider Experiments Supersymmetrye Miscellaneous Results HTTP://PDG.LBL.GOV Page1 Created: 8/21/2014 12:57 Citation: K.A. Olive et al. -
Search for Long-Lived Stopped R-Hadrons Decaying out of Time with Pp Collisions Using the ATLAS Detector
PHYSICAL REVIEW D 88, 112003 (2013) Search for long-lived stopped R-hadrons decaying out of time with pp collisions using the ATLAS detector G. Aad et al.* (ATLAS Collaboration) (Received 24 October 2013; published 3 December 2013) An updated search is performed for gluino, top squark, or bottom squark R-hadrons that have come to rest within the ATLAS calorimeter, and decay at some later time to hadronic jets and a neutralino, using 5.0 and 22:9fbÀ1 of pp collisions at 7 and 8 TeV, respectively. Candidate decay events are triggered in selected empty bunch crossings of the LHC in order to remove pp collision backgrounds. Selections based on jet shape and muon system activity are applied to discriminate signal events from cosmic ray and beam-halo muon backgrounds. In the absence of an excess of events, improved limits are set on gluino, stop, and sbottom masses for different decays, lifetimes, and neutralino masses. With a neutralino of mass 100 GeV, the analysis excludes gluinos with mass below 832 GeV (with an expected lower limit of 731 GeV), for a gluino lifetime between 10 s and 1000 s in the generic R-hadron model with equal branching ratios for decays to qq~0 and g~0. Under the same assumptions for the neutralino mass and squark lifetime, top squarks and bottom squarks in the Regge R-hadron model are excluded with masses below 379 and 344 GeV, respectively. DOI: 10.1103/PhysRevD.88.112003 PACS numbers: 14.80.Ly R-hadrons may change their properties through strong I. -
Introduction to Supersymmetry
Introduction to Supersymmetry Pre-SUSY Summer School Corpus Christi, Texas May 15-18, 2019 Stephen P. Martin Northern Illinois University [email protected] 1 Topics: Why: Motivation for supersymmetry (SUSY) • What: SUSY Lagrangians, SUSY breaking and the Minimal • Supersymmetric Standard Model, superpartner decays Who: Sorry, not covered. • For some more details and a slightly better attempt at proper referencing: A supersymmetry primer, hep-ph/9709356, version 7, January 2016 • TASI 2011 lectures notes: two-component fermion notation and • supersymmetry, arXiv:1205.4076. If you find corrections, please do let me know! 2 Lecture 1: Motivation and Introduction to Supersymmetry Motivation: The Hierarchy Problem • Supermultiplets • Particle content of the Minimal Supersymmetric Standard Model • (MSSM) Need for “soft” breaking of supersymmetry • The Wess-Zumino Model • 3 People have cited many reasons why extensions of the Standard Model might involve supersymmetry (SUSY). Some of them are: A possible cold dark matter particle • A light Higgs boson, M = 125 GeV • h Unification of gauge couplings • Mathematical elegance, beauty • ⋆ “What does that even mean? No such thing!” – Some modern pundits ⋆ “We beg to differ.” – Einstein, Dirac, . However, for me, the single compelling reason is: The Hierarchy Problem • 4 An analogy: Coulomb self-energy correction to the electron’s mass A point-like electron would have an infinite classical electrostatic energy. Instead, suppose the electron is a solid sphere of uniform charge density and radius R. An undergraduate problem gives: 3e2 ∆ECoulomb = 20πǫ0R 2 Interpreting this as a correction ∆me = ∆ECoulomb/c to the electron mass: 15 0.86 10− meters m = m + (1 MeV/c2) × . -
Elementary Particle Physics from Theory to Experiment
Elementary Particle Physics From Theory to Experiment Carlos Wagner Physics Department, EFI and KICP, Univ. of Chicago HEP Division, Argonne National Laboratory Society of Physics Students, Univ. of Chicago, Nov. 10, 2014 Particle Physics studies the smallest pieces of matter, 1 1/10.000 1/100.000 1/100.000.000 and their interactions. Friday, November 2, 2012 Forces and Particles in Nature Gravitational Force Electromagnetic Force Attractive force between 2 massive objects: Attracts particles of opposite charge k e e F = 1 2 d2 1 G = 2 MPl Forces within atoms and between atoms Proportional to product of masses + and - charges bind together Strong Force and screen each other Assumes interaction over a distance d ==> comes from properties of spaceAtoms and timeare made fromElectrons protons, interact with protons via quantum neutrons and electrons. Strong nuclear forceof binds e.m. energy together : the photons protons and neutrons to form atoms nuclei Strong nuclear force binds! togethers! =1 m! = 0 protons and neutrons to form nuclei protonD. I. S. of uuelectronsd formedwith Modeled protons by threeor by neutrons a theoryquarks, based bound on together Is very weak unless one ofneutron theat masses high energies is huge,udd shows by thatthe U(1)gluons gauge of thesymmetry strong interactions like the earth protons and neutrons SU (3) c are not fundamental Friday,p November! u u d 2, 2012 formed by three quarks, bound together by n ! u d d the gluons of the strong interactions Modeled by a theory based on SU ( 3 ) C gauge symmetry we see no free quarks Very strong at large distances confinement " in nature ! Weak Force Force Mediating particle transformations Observation of Beta decay demands a novel interaction Weak Force Short range forces exist only inside the protons 2 and neutrons, with massive force carriers: gauge bosons ! W and Z " MW d FW ! e / d Similar transformations explain the non-observation of heavier elementary particles in our everyday experience. -
NEWSLETTER 45 Istituto Nazionale Di Fisica Nucleare MARCH 2018
NEWSLETTER 45 Istituto Nazionale di Fisica Nucleare MARCH 2018 RESEARCH NA62 RESEARCH AND THE RARE DECAYS OF THE K-MESON The NA62 experiment at CERN has recently presented its latest results concerning a very rare event: the decay of the charged K-meson into a pion and two neutrinos. The interest in extremely rare or even "forbidden" decays is motivated by the fact that these processes allow energy scales even much higher than those directly accessible to the most powerful particle colliders, such as the Large Hadron Collider (LHC) at CERN, to be indirectly probed. The study of these decays could therefore open a window in the near future on physics beyond the Standard Model. Moreover, the results just presented by NA62 are also interesting because they demonstrate the effectiveness of the new technique, called "in flight", used by the experiment to investigate these K-meson decays. In the coming years, this will allow the elusive process to be studied with a precision never achieved before. According to theoretical predictions, the charged K-meson decays into a pion and two neutrinos only in a very small fraction of cases. To understand the extreme rarity of this process, the Standard Model foresees, with considerable precision, that only eight decays of this type must occur every one hundred billion decays of the K-meson. In numerous theories that aim to overcome the Standard Model, the fraction of events expected for this decay is instead significantly different: therefore, a sufficiently precise measure could highlight the presence of what physicists call New Physics. The results obtained so far, at this level of statistical precision, are compatible with the Standard Model predictions. -
The NA62 Experiment at CERN
126 EPJ Web of Conferences , 04036 (2016) DOI: 10.1051/epjconf/201612604036 ICNFP 2015 The NA62 experiment at CERN Mauro Piccini1,a 1INFN - Sezione di Perugia Abstract. The rare decays K → πνν¯ are excellent processes to make tests of new physics at the highest scale complementary to LHC thanks to their theoretically cleanness. The NA62 experiment at CERN SPS aims to collect of the order of 100 events in two years of data taking for the decay K+ → π+νν¯, keeping the background at the level of 10%. Part of the experimental apparatus has been commissioned during a technical run in 2012. The diverse and innovative experimental techniques will be explained and some preliminary results obtained during the 2014 pilot run will be reviewed. 1 Introduction NA62 is the last generation kaon experiment at CERN SPS aiming to study the decay K+ → π+νν¯. The goal of the experiment is to measure the decay branching ratio (O(10−10)) with 10% accuracy, collecting about 100 events in two years of data taking and assuming a 10% signal acceptance. The proton beam extracted from the SPS in the north area at CERN fulfills such demanding request in aOn behalf of the NA62 Collaboration: G. Aglieri Rinella, R. Aliberti, F. Ambrosino, B. Angelucci, A. Antonelli, G. Anzivino, R. Arcidiacono, I. Azhinenko, S. Balev, M. Barbanera, J. Bendotti, A. Biagioni, L. Bician, C. Biino, A. Bizzeti, T. Blazek, A. Blik, B. Bloch-Devaux, V. Bolotov, V. Bonaiuto, M. Bragadireanu, D. Britton, G. Britvich, M.B. Brunetti, D. Bry- man, F. Bucci, F. Butin, E. -
The ATLAS Experiment at The
High School Teacher Programme 2016 https://indico.cern.ch/e/HST2016 • Particle Detectors • Mar Capeans CERN EP-DT July 8th 2016 • Particle Detectors• OUTLINE 1. Particle Detector Challenges at LHC 2. Interactions of Particles with Matter 3. Detector Technologies 4. How HEP Experiments Work Mar Capeans 8/7/2016 2 • Particle Physics Tools• • Accelerators . Luminosity, energy… • Detectors . Efficiency, granularity, resolution… • Trigger/DAQ (Online) . Efficiency, filters, through-put… • Data Analysis (Offline) . Large scale computing, physics results… Mar Capeans 8/7/2016 3 • Imaging Events• 50’s – 70’s LEP: 88 - 2000 LHC Mar Capeans 8/7/2016 4 • ATLAS Event • Mar Capeans 8/7/2016 5 • LHC• p-p Beam Energy Luminosity Nb of bunches Nb p/bunch Bunch collisions 40 million/s ~25 interactions / Bunch crossing overlapping in time and space 1000 x 106 events/s > 1000 particle signals in the detector at 40MHz rate 1 interesting collision in 1013 Mar Capeans 8/7/2016 6 • Past VS LHC• Dozens of 109 collisions/s particles/s No event selection VS Registering 1/1012 events ‘Eye’ analysis GRID computing At each bunch crossing ~1000 individual particles to be identified every 25 ns …. High density of particles imply high granularity in the detection system … Large quantity of readout services (100 M channels/active components) Large neutron fluxes, large photon fluxes capable of compromising the mechanical properties of materials and electronics components. Induced radioactivity in high Z materials (activation) which will add complexity to the maintenance