Possibilities of Detecting Light Dark Matter Produced Via Drell-Yan Channel in a Fixed Target Experiment
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Arxiv:1712.01768V1 [Hep-Ex] 5 Dec 2017
Prospects of the SHiP and NA62 experiments at CERN for hidden sector searches Philippe Mermod∗, on behalf of the SHiP Collaboration Particle Physics Department, Faculty of Science, University of Geneva, Geneva, Switzerland E-mail: [email protected] High-intensity proton beams impinging on a fixed target or beam dump allow to probe new physics via the production of new weakly-coupled particles in hadron decays. The CERN SPS provides opportunities to do so with the running NA62 experiment and the planned SHiP ex- periment. Reconstruction of kaon decay kinematics (beam mode) allows NA62 to probe for the existence of right-handed neutrinos and dark photons with masses below 0.45 GeV. Direct recon- struction of displaced vertices from the decays of new neutral particles (dump mode) will allow NA62 and SHiP to probe right-handed neutrinos with masses up to 5 GeV and mixings down to several orders of magnitude smaller than current constraints, in regions favoured in models which explain at once neutrino masses, matter-antimatter asymmetry and dark matter. arXiv:1712.01768v1 [hep-ex] 5 Dec 2017 The 19th International Workshop on Neutrinos from Accelerators-NUFACT2017 25-30 September, 2017 Uppsala University, Uppsala, Sweden ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0). https://pos.sissa.it/ Hidden sector searches with SHiP and NA62 Philippe Mermod 1. Introduction The LHC experiments have been running for several years without finding new physics at the TeV scale. A complementary approach is to probe the presence of new particles at lower energy scales with couplings to the Standard Model so weak that they have escaped detection in previous searches. -
Dark Matter and the Early Universe: a Review Arxiv:2104.11488V1 [Hep-Ph
Dark matter and the early Universe: a review A. Arbey and F. Mahmoudi Univ Lyon, Univ Claude Bernard Lyon 1, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, UMR 5822, 69622 Villeurbanne, France Theoretical Physics Department, CERN, CH-1211 Geneva 23, Switzerland Institut Universitaire de France, 103 boulevard Saint-Michel, 75005 Paris, France Abstract Dark matter represents currently an outstanding problem in both cosmology and particle physics. In this review we discuss the possible explanations for dark matter and the experimental observables which can eventually lead to the discovery of dark matter and its nature, and demonstrate the close interplay between the cosmological properties of the early Universe and the observables used to constrain dark matter models in the context of new physics beyond the Standard Model. arXiv:2104.11488v1 [hep-ph] 23 Apr 2021 1 Contents 1 Introduction 3 2 Standard Cosmological Model 3 2.1 Friedmann-Lema^ıtre-Robertson-Walker model . 4 2.2 A quick story of the Universe . 5 2.3 Big-Bang nucleosynthesis . 8 3 Dark matter(s) 9 3.1 Observational evidences . 9 3.1.1 Galaxies . 9 3.1.2 Galaxy clusters . 10 3.1.3 Large and cosmological scales . 12 3.2 Generic types of dark matter . 14 4 Beyond the standard cosmological model 16 4.1 Dark energy . 17 4.2 Inflation and reheating . 19 4.3 Other models . 20 4.4 Phase transitions . 21 5 Dark matter in particle physics 21 5.1 Dark matter and new physics . 22 5.1.1 Thermal relics . 22 5.1.2 Non-thermal relics . -
Letter of Interest Cosmic Probes of Ultra-Light Axion Dark Matter
Snowmass2021 - Letter of Interest Cosmic probes of ultra-light axion dark matter Thematic Areas: (check all that apply /) (CF1) Dark Matter: Particle Like (CF2) Dark Matter: Wavelike (CF3) Dark Matter: Cosmic Probes (CF4) Dark Energy and Cosmic Acceleration: The Modern Universe (CF5) Dark Energy and Cosmic Acceleration: Cosmic Dawn and Before (CF6) Dark Energy and Cosmic Acceleration: Complementarity of Probes and New Facilities (CF7) Cosmic Probes of Fundamental Physics (TF09) Astro-particle physics and cosmology Contact Information: Name (Institution) [email]: Keir K. Rogers (Oskar Klein Centre for Cosmoparticle Physics, Stockholm University; Dunlap Institute, University of Toronto) [ [email protected]] Authors: Simeon Bird (UC Riverside), Simon Birrer (Stanford University), Djuna Croon (TRIUMF), Alex Drlica-Wagner (Fermilab, University of Chicago), Jeff A. Dror (UC Berkeley, Lawrence Berkeley National Laboratory), Daniel Grin (Haverford College), David J. E. Marsh (Georg-August University Goettingen), Philip Mocz (Princeton), Ethan Nadler (Stanford), Chanda Prescod-Weinstein (University of New Hamp- shire), Keir K. Rogers (Oskar Klein Centre for Cosmoparticle Physics, Stockholm University; Dunlap Insti- tute, University of Toronto), Katelin Schutz (MIT), Neelima Sehgal (Stony Brook University), Yu-Dai Tsai (Fermilab), Tien-Tien Yu (University of Oregon), Yimin Zhong (University of Chicago). Abstract: Ultra-light axions are a compelling dark matter candidate, motivated by the string axiverse, the strong CP problem in QCD, and possible tensions in the CDM model. They are hard to probe experimentally, and so cosmological/astrophysical observations are very sensitive to the distinctive gravitational phenomena of ULA dark matter. There is the prospect of probing fifteen orders of magnitude in mass, often down to sub-percent contributions to the DM in the next ten to twenty years. -
Pandax-II ! 2015.4.9 Sino-French PPL, Hefei Pandax Dark Matter Search Program
Jinping Mountain WIMPs PandaX Dark Matter Search with Liquid Xenon at Jinping Kaixuan Ni! (on behalf of the PandaX Collaboration)! Shanghai Jiao Tong University! from PandaX-I to PandaX-II ! 2015.4.9 Sino-French PPL, Hefei PandaX dark matter search program ❖ 2009.3 SJTU group visited Jinping for the first time! ❖ 2009.4 Proposals submitted for dark matter search with liquid xenon at Jinping! ❖ 2010.1 PandaX collaboration formed, funding supported by SJTU/MOST/NSFC, started to develop the PandaX-I detector at SJTU! ❖ 2012.8 PandaX-I detector moved to CJPL! ❖ 2012.9-2013.9 Two engineering runs carried out for system integration! ❖ 2014.3 Detector fully functional for data taking! ❖ 2014.8 PandaX-I first results (17 days) published! ❖ 2014.11 Another 63 days dark matter data were collected! ❖ 2015 Upgrading from PandaX-I (125-kg) to PandaX-II (500-kg) PandaX Collaboration for Dark Matter Search Shanghai Jiao Tong University! Shanghai Institute of Applied Physics, CAS! Shandong University! University of Maryland! University of Michigan! Peking University! http://pandax.org/ Yalong River Hydropower Development Co.! China Institute of Atomic Energy (new group joined 2015) Why Liquid Xenon? • Ultra-low background: using self-shielding with 3D fiducialization and ER/NR discrimination • Sensitive to both heavy and light dark matter • Sensitive to both Spin-independent and Spin-dependent (129Xe,131Xe) • Ultra-pure Xe target: xenon gas can be purified with sub-ppb (O2 etc.) and sub-ppt (Kr) impurities • Multi-ton target achievable: with reasonable cost ($1.5M/ton) and relative simple cryogenics (165K) Two-phase xenon for dark matter searches WIMPs/Neutrons. -
Review of Dark Matter
Review of Dark Matter Leonard S. Kisslinger Department of Physics, Carnegie Mellon University, Pittsburgh PA 15213 USA. Debasish Das Saha Institute of Nuclear Physics,1/AF, Bidhan Nagar, Kolkata 700064, INDIA. PACS Indices:11.30.Er,14.60.Lm,13.15.+g Keywords: dark matter, sterile neutrinos, dark photons Abstract In this review of Dark Matter we review dark matter as sterile neutrinos, fermions, with their present and possibly future detection via neutrino Oscillations. We review the creation of Dark Matter via interactions with the Dark Energy (quintesence) field. We also review bosons as dark matter, discussing a proposed search for dark photons. Since photons are vector bosons, if dark photons exist at least part of dark matter are vector bosons. Ongoing experimental detection of Dark Matter is reviewed. 1 Introduction The most important experiments which have estimated the amount of Dark Matter in the present universe are Cosmic Microwave Background Radiation (CMBR) experiments, discussed in the section 2. There have been a number of theoretical models for the creation of Dark Matter, which is reviewed in section 3. It is almost certain that sterile nuetrinos are part of Dark Matter. Experiments detecting sterile nuetrinos via neutrino oscillation and a theoretical study of neutrino oscil- lations with 3 active and 3 sterile neutrinos with the present results are discussed in section 4. Also a recent search for sub-Gev Dark Matter by the MiniBooNE-DM Collaboration is briefly discussed in section 4. Neutrinos are fermions with quantum spin 1/2. It is possible that some Dark Matter particle are vector bosons with quantum spin 1, like the photon. -
Light Dark Matter Searches with Positrons
Eur. Phys. J. A manuscript No. (will be inserted by the editor) Light dark matter searches with positrons M. Battaglieri1,2, A. Bianconi3,4, P. Bisio5, M. Bondì1, A. Celentano1, G. Costantini3,4, P.L. Cole6, L. Darmé7, R. De Vita1, A. D’Angelo8,9, M. De Napoli10, L. El Fassi11, V. Kozhuharov7,12, A. Italiano10, G. Krnjaic13,14, L. Lanza8, M. Leali3,4, L. Marsicano1,a, V. Mascagna4,15, S. Migliorati3,4, E. Nardi7, M. Raggi16,17,a, N. Randazzo10, E. Santopinto1, E. Smith2, M. Spreafico5, S. Stepanyan2, M. Ungaro2, P. Valente17, L. Venturelli3,4, M.H. Wood18 1Istituto Nazionale di Fisica Nucleare, Sezione di Genova, 16146 Genova, Italy 2Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606 3Università degli Studi di Brescia, 25123 Brescia, Italy 4INFN, Sezione di Pavia, 27100 Pavia, Italy 5Università degli Studi di Genova, 16146 Genova, Italy 6Lamar University, 4400 MLK Blvd, PO Box 10046, Beaumont, Texas 77710 7Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati, Via E. Fermi 54, Frascati, Italy 8INFN, Sezione di Roma Tor Vergata, 00133 Rome, Italy 9Università di Roma Tor Vergata, 00133 Rome Italy 10Istituto Nazionale di Fisica Nucleare, Sezione di Catania, 95125 Catania, Italy 11Mississippi State University, Mississippi State, Mississippi 39762-5167, USA 12Faculty of physics, University of Sofia, 5 J. Bourchier Blvd., 1164 Sofia, Bulgaria 13Fermi National Accelerator Laboratory, Batavia, Illinois 60510, USA 14Kavli Institute for Cosmological Physics, University of Chicago, Chicago, Illinois 60637, USA 15Università degli Studi dell’Insubria, 22100 Como, Italy 16Sapienza Università di Roma, piazzale Aldo Moro 5 Roma, Italy 17Istituto Nazionale di Fisica Nucleare, Sezione di Roma, piazzale Aldo Moro 5 Roma, Italy 18Canisius College, Buffalo, NY 14208, USA Draft : May 27, 2021 Abstract We discuss two complementary strategies to 1 Introduction and motivations search for light dark matter (LDM) exploiting the posi- tron beam possibly available in the future at Jefferson One of the most compelling arguments motivating the Laboratory. -
Lectures on BSM and Dark Matter Theory (2Nd Class)
Lectures on BSM and Dark Matter theory (2nd class) Stefania Gori UC Santa Cruz 15th annual Fermilab - CERN Hadron Collider Physics Summer School August 10-21, 2020 Twin Higgs models & the hierarchy problem SMA x SMB x Z2 Global symmetry of the scalar potential (e.g. SU(4)) The SM Higgs is a (massless) Nambu-Goldstone boson ~SM Higgs doublet Twin Higgs doublet S.Gori 23 Twin Higgs models & the hierarchy problem SMA x SMB x Z2 Global symmetry of the scalar potential (e.g. SU(4)) The SM Higgs is a (massless) Nambu-Goldstone boson ~SM Higgs doublet Twin Higgs doublet Loop corrections to the Higgs mass: HA HA HB HB yA yA yB yB top twin-top Loop corrections to mass are SU(4) symmetric no quadratically divergent corrections! S.Gori 23 Twin Higgs models & the hierarchy problem SMA x SMB x Z2 Global symmetry of the scalar potential (e.g. SU(4)) The SM Higgs is a (massless) Nambu-Goldstone boson ~SM Higgs doublet Twin Higgs doublet Loop corrections to the Higgs mass: HA HA HB HB SU(4) and Z2 are (softly) broken: yA yA yB yB top twin-top Loop corrections to mass are SU(4) symmetric no quadratically divergent corrections! S.Gori 23 Phenomenology of the twin Higgs A typical spectrum: Htwin Twin tops Twin W, Z SM Higgs Twin bottoms Twin taus Glueballs S.Gori 24 Phenomenology of the twin Higgs 1. Production of the twin Higgs The twin Higgs will mix with the 125 GeV Higgs with a mixing angle ~ v2 / f2 Because of this mixing, it can be produced as a SM Higgs boson (reduced rates!) A typical spectrum: Htwin Twin tops Twin W, Z SM Higgs Twin bottoms Twin taus Glueballs S.Gori 24 Phenomenology of the twin Higgs 1. -
Arxiv:2107.07524V1 [Hep-Ph] 15 Jul 2021
Sterile neutrino dark matter catalyzed by a very light dark photon Gonzalo Alonso-Alvarez´ ∗ and James M. Cliney McGill University, Department of Physics, 3600 University St., Montr´eal,QC H3A2T8 Canada Sterile neutrinos (νs) that mix with active neutrinos (νa) are interesting dark matter candidates with a rich cosmological and astrophysical phenomenology. In their simplest incarnation, their production is severely constrained by a combination of structure formation observations and X-ray searches. We show that if active neutrinos couple to an oscillating condensate of a very light Lµ Lτ − gauge field, resonant νa-νs oscillations can occur in the early universe, consistent with νs constituting all of the dark matter, while respecting X-ray constraints on νs νaγ decays. Interesting deviations from standard solar and atmospheric neutrino oscillations can! persist to the present. I. INTRODUCTION the expansion of the universe eventually shuts off the resonance at late times. 1 The possibility that sterile neutrinos νs constitute the The formation of bosonic condensates is conjectured dark matter (DM) of the universe has attracted steady to be possible in the early universe. The most well-known interest since its inception long ago. Supposing that the examples are those of the QCD axion [30{32] and ul- νs abundance is initially negligible, its relic density can tralight scalar dark matter [33], but an analogous phe- be generated by nonresonant oscillations with an active nomenon is possible for light vector bosons [34]. The con- neutrino species νa though mass mixing [1], with a mixing densate can be described in terms of the classical bosonic −6 angle as small as θ 10 for mνs 100 keV [2]. -
Supersymmetric Dark Matter Candidates in Light of Constraints from Collider and Astroparticle Observables
THESE` Pour obtenir le grade de DOCTEUR DE L’UNIVERSITE´ DE GRENOBLE Specialit´ e´ : Physique Theorique´ Arretˆ e´ ministeriel´ : 7 aoutˆ 2006 Present´ ee´ par Jonathan DA SILVA These` dirigee´ par Genevieve` BELANGER´ prepar´ ee´ au sein du Laboratoire d’Annecy-le-Vieux de Physique Theorique´ (LAPTh) et de l’Ecole´ Doctorale de Physique de Grenoble Supersymmetric Dark Matter candidates in light of constraints from collider and astroparticle observables These` soutenue publiquement le 3 juillet 2013, devant le jury compose´ de : arXiv:1312.0257v1 [hep-ph] 1 Dec 2013 Dr. Rohini GODBOLE Professeur, CHEP Bangalore, Inde, Presidente´ Dr. Farvah Nazila MAHMOUDI Maˆıtre de Conferences,´ LPC Clermont, Rapporteur Dr. Ulrich ELLWANGER Professeur, LPT Orsay, Rapporteur Dr. Celine´ BŒHM Charge´ de recherche, Durham University, Royaume-Uni, Examinatrice Dr. Anupam MAZUMDAR Professeur, Lancaster University, Royaume-Uni, Examinateur Dr. Genevieve` BELANGER´ Directeur de Recherche, LAPTh, Directeur de these` A meus av´os. Contents Acknowledgements - Remerciements vii List of Figures xi List of Tables xvii List of Abbreviations xix List of Publications xxiii Introduction1 I Status of particle physics and cosmology ... and beyond5 1 From the infinitely small : the Standard Model of particle physics ...7 1.1 Building of the model : gauge sector . .8 1.2 Matter sector . 10 1.2.1 Leptons . 10 1.2.2 Quarks . 12 1.3 The Higgs mechanism . 13 1.4 Full standard picture . 16 1.5 Successes of the SM . 18 1.6 SM issues . 19 1.6.1 Theoretical problems . 19 1.6.2 Experimental discrepancies . 20 1.6.3 Cosmological connexion . 22 2 ... To the infinitely large : the Lambda Cold Dark Matter model 23 2.1 Theoretical framework . -
Theory and Visible Dark Photons Primer
Dark Sectors 2016 ! Theory and Visible Dark Photons Primer Natalia Toro ! Prepared with Rouven Essig & Philip Schuster Welcome! 2 Looking Back In 2009, SLAC held a “Dark Forces” workshop. At that time… • Astrophysics data spurred renewed theoretical interest Dark Forces Workshop 2009 • Re-analysis of data from multi- purpose detectors opened window to the dark sector • First-generation experiments were starting to take shape. 3 Searching in Dumps Now is a greatdiscoverable with new, low- time! power beam dump 0.01 0.1 1 106 seconds @ 100 nA, 6 GeV 0.01 0.01 10-4 Scalar Thermal Relic DM Broad, one signal event per hour KLOE -3 10 LHC HADES KLOE -5 BaBar -4 3 3 10 a,5 APEX 10 10 10 PHENIX Test -5 LEP favored A1 10 * a,±2 NA48/2 E774 -6 10-6 10 ae international 4 4 4 E774 CRESST II 10 10 ) 10-7 BaBar E141(10cm, A' -7 m -8 10 / 10 XENON 10 5 .3 mC) 5 2 -9 ⇥ ⇥ 10 10 10 m activity ( -8 E141 -10 E137 10 D 10 E137 -11 Density 6 6 2 10 Relic (200m, 30 C) 10 10 -9 -12 LSND 10 = 10 +CERN, milli- y searching for -13 MegaWatt x Year 10 7 7 -10 x SIDM 10 charge 10 10 10-14 LSND lower limit Orsay U70 10-15 -11 dark sectors! 8 8 10 10-16 10 10 -3 -2 -1 (dump10 experiments10 also constrain10 1 1 10 102 103 0.01 0.1 1 longer-lived decaym modes,A' [GeV ] m (MeV) mA' GeV see Schuster, NT, Yavin to appear) *E774: 20cm, .3 mC 8 Many of the first-generation dedicated experiments are still ongoing. -
27. Dark Matter
1 27. Dark Matter 27. Dark Matter Written August 2019 by L. Baudis (Zurich U.) and S. Profumo (UC Santa Cruz). 27.1 The case for dark matter Modern cosmological models invariably include an electromagnetically close-to-neutral, non- baryonic matter species with negligible velocity from the standpoint of structure formation, gener- ically referred to as “cold dark matter” (CDM; see The Big-Bang Cosmology—Sec. 22 of this Re- view). For the benchmark ΛCDM cosmology adopted in the Cosmological Parameters—Sec. 25.1 of this Review, the DM accounts for 26.4% of the critical density in the universe, or 84.4% of the total matter density. The nature of only a small fraction, between at least 0.5% (given neutrino os- cillations) and at most 1.6% (from combined cosmological constraints), of the non-baryonic matter content of the universe is known: the three Standard Model neutrinos (see the Neutrino Masses, Mixing, and Oscillations—Sec. 14 of this Review) ). The fundamental makeup of the large majority of the DM is, as of yet, unknown. Assuming the validity of General Relativity, DM is observed to be ubiquitous in gravitation- ally collapsed structures of size ranging from the smallest known galaxies [1] to galaxies of size comparable to the Milky Way [2], to groups and clusters of galaxies [3]. The mass-to-light ratio is observed to saturate at the largest collapsed scales to a value indicative, and close to, what inferred from other cosmological observations for the universe as a whole [4]. In such collapsed structures, the existence of DM is inferred directly using tracers of mass enclosed within a certain radius such as stellar velocity dispersion, rotation curves in axisymmetric systems, the virial theorem, gravitational lensing, and measures of the amount of non-dark, i.e. -
Search for Dark Photons from Supersymmetric Hidden Valleys
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Kenneth Bloom Publications Research Papers in Physics and Astronomy 2009 Search for Dark Photons from Supersymmetric Hidden Valleys V. M. Abazov Joint Institute for Nuclear Research, Dubna, Russia Kenneth A. Bloom University of Nebraska-Lincoln, [email protected] Gregory Snow University of Nebraska-Lincoln, [email protected] D0 Collaboration Follow this and additional works at: https://digitalcommons.unl.edu/physicsbloom Part of the Physics Commons Abazov, V. M.; Bloom, Kenneth A.; Snow, Gregory; and Collaboration, D0, "Search for Dark Photons from Supersymmetric Hidden Valleys" (2009). Kenneth Bloom Publications. 310. https://digitalcommons.unl.edu/physicsbloom/310 This Article is brought to you for free and open access by the Research Papers in Physics and Astronomy at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Kenneth Bloom Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. week ending PRL 103, 081802 (2009) PHYSICAL REVIEW LETTERS 21 AUGUST 2009 Search for Dark Photons from Supersymmetric Hidden Valleys V.M. Abazov,37 B. Abbott,75 M. Abolins,65 B. S. Acharya,30 M. Adams,51 T. Adams,49 E. Aguilo,6 M. Ahsan,59 G. D. Alexeev,37 G. Alkhazov,41 A. Alton,64,* G. Alverson,63 G. A. Alves,2 L. S. Ancu,36 T. Andeen,53 M. S. Anzelc,53 M. Aoki,50 Y. Arnoud,14 M. Arov,60 M. Arthaud,18 A. Askew,49,† B. A˚ sman,42 O. Atramentov,49,† C. Avila,8 J. BackusMayes,82 F. Badaud,13 L. Bagby,50 B. Baldin,50 D.