Mirror Dark Matter Interpretation of the DAMA, Cogent and CRESSTII Experiments
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Small Scale Problems of the CDM Model
galaxies Article Small Scale Problems of the LCDM Model: A Short Review Antonino Del Popolo 1,2,3,* and Morgan Le Delliou 4,5,6 1 Dipartimento di Fisica e Astronomia, University of Catania , Viale Andrea Doria 6, 95125 Catania, Italy 2 INFN Sezione di Catania, Via S. Sofia 64, I-95123 Catania, Italy 3 International Institute of Physics, Universidade Federal do Rio Grande do Norte, 59012-970 Natal, Brazil 4 Instituto de Física Teorica, Universidade Estadual de São Paulo (IFT-UNESP), Rua Dr. Bento Teobaldo Ferraz 271, Bloco 2 - Barra Funda, 01140-070 São Paulo, SP Brazil; [email protected] 5 Institute of Theoretical Physics Physics Department, Lanzhou University No. 222, South Tianshui Road, Lanzhou 730000, Gansu, China 6 Instituto de Astrofísica e Ciências do Espaço, Universidade de Lisboa, Faculdade de Ciências, Ed. C8, Campo Grande, 1769-016 Lisboa, Portugal † [email protected] Academic Editors: Jose Gaite and Antonaldo Diaferio Received: 30 May 2016; Accepted: 9 December 2016; Published: 16 February 2017 Abstract: The LCDM model, or concordance cosmology, as it is often called, is a paradigm at its maturity. It is clearly able to describe the universe at large scale, even if some issues remain open, such as the cosmological constant problem, the small-scale problems in galaxy formation, or the unexplained anomalies in the CMB. LCDM clearly shows difficulty at small scales, which could be related to our scant understanding, from the nature of dark matter to that of gravity; or to the role of baryon physics, which is not well understood and implemented in simulation codes or in semi-analytic models. -
Current Perspectives on Dark Matter
Cosmological Signatures of a Mirror Twin Higgs Zackaria Chacko University of Maryland, College Park Curtin, Geller & Tsai Introduction The Twin Higgs framework is a promising approach to the naturalness problem of the Standard Model (SM). In Mirror Twin Higgs models, the SM is extended to include a complete mirror (“twin”) copy of the SM, with its own particle content and gauge groups. The SM and its twin counterpart are related by a discrete Z2 “twin” symmetry. Z2 SMA SMB The mirror particles are completely neutral under the SM strong, weak and electromagnetic forces. Only feel gravity. In Mirror Twin Higgs models, the one loop quadratic divergences that contribute to the Higgs mass are cancelled by twin sector states that carry no charge under the SM gauge groups. Discovery of these states at LHC is therefore difficult. May explain null results. The SM and twin SM primarily interact through the Higgs portal. This interaction is needed for cancellation of quadratic divergences. After electroweak symmetry breaking, SM Higgs and twin Higgs mix. • Higgs couplings to SM states are suppressed by the mixing. • Higgs now has (mixing suppressed) couplings to twin states. A soft breaking of the Z2 symmetry ensures that 퐯B, the VEV of the twin Higgs, is greater than 퐯A, the VEV of the SM Higgs. The mixing angle ~ 퐯A/퐯B. Higgs measurements constrain 퐯A/퐯B ≤ ퟏ/ퟑ. Twin fermions are heavier than SM fermions by a factor of 퐯B/퐯A . Naturalness requires 퐯A/퐯B ≥ ퟏ/ퟓ. (Twin top should not be too heavy.) The Higgs portal interaction has implications for cosmology. -
Self-Interacting Inelastic Dark Matter: a Viable Solution to the Small Scale Structure Problems
Prepared for submission to JCAP ADP-16-48/T1004 Self-interacting inelastic dark matter: A viable solution to the small scale structure problems Mattias Blennow,a Stefan Clementz,a Juan Herrero-Garciaa; b aDepartment of physics, School of Engineering Sciences, KTH Royal Institute of Tech- nology, AlbaNova University Center, 106 91 Stockholm, Sweden bARC Center of Excellence for Particle Physics at the Terascale (CoEPP), University of Adelaide, Adelaide, SA 5005, Australia Abstract. Self-interacting dark matter has been proposed as a solution to the small- scale structure problems, such as the observed flat cores in dwarf and low surface brightness galaxies. If scattering takes place through light mediators, the scattering cross section relevant to solve these problems may fall into the non-perturbative regime leading to a non-trivial velocity dependence, which allows compatibility with limits stemming from cluster-size objects. However, these models are strongly constrained by different observations, in particular from the requirements that the decay of the light mediator is sufficiently rapid (before Big Bang Nucleosynthesis) and from direct detection. A natural solution to reconcile both requirements are inelastic endothermic interactions, such that scatterings in direct detection experiments are suppressed or even kinematically forbidden if the mass splitting between the two-states is sufficiently large. Using an exact solution when numerically solving the Schr¨odingerequation, we study such scenarios and find regions in the parameter space of dark matter and mediator masses, and the mass splitting of the states, where the small scale structure problems can be solved, the dark matter has the correct relic abundance and direct detection limits can be evaded. -
Signs of Dark Matter May Point to Mirror Matter Candidate 27 April 2010, by Lisa Zyga
Signs of dark matter may point to mirror matter candidate 27 April 2010, by Lisa Zyga (PhysOrg.com) -- Dark matter, which contains the At first, mirror matter may sound a bit like antimatter "missing mass" that's needed to explain why (which is ordinary matter with an opposite charge). galaxies stay together, could take any number of In both theories, the number of known particles forms. The main possible candidates include would double. However, while antimatter interacts MACHOS and WIMPS, but there is no shortage of very strongly with ordinary matter, annihilating itself proposals. Rather, the biggest challenge is finding into photons, mirror matter would interact very some evidence that would support one or more of weakly with ordinary matter. For this reason, some these candidates. Currently, more than 30 physicists have speculated that mirror particles experiments are underway trying to detect a sign of could be candidates for dark matter. Even though dark matter. So far, only two experiments claim to mirror matter would produce light, we would not see have found signals, with the most recent it, and it would be very difficult to detect. observations coming just a month ago. Now, physicist Robert Foot from the University of However, mirror matter would not be impossible to Melbourne has shown that the results of these two detect, and Foot thinks that the DAMA experiment experiments can be simultaneously explained by and the CoGeNT experiment may have detected an intriguing dark matter candidate called mirror mirror matter. In DAMA, scientists observed a piece matter. of sodium iodide, which should generate a photon when struck by a dark matter particle. -
Particle - Mirror Particle Oscillations: CP-Violation and Baryon Asymmetry
Particle - Mirror Particle Oscillations: CP-violation and Baryon Asymmetry Zurab Berezhiani Università di L’Aquila and LNGS, Italy 0 CPT at ICTP, Triest, 2-5 July 2008 n − n oscillations etc ... - p. 1/42 Alice & Mirror World Lewis Carroll, "Through the Looking-Glass" ‘Now, if you’ll only attend, Kitty, and not talk so much, I’ll tell you all my ideas about Looking-glass House. There’s the room you can see through the glass – that’s just the same ● Carrol’s Alice... ● Mirror World as our drawing-room, only the things go the other way... the books are something like our ● Mirror Particles ● Interactions books, only the words go the wrong way: I know that, because I’ve held up one of our books to ● B & L violation ● BBN demands the glass, and then they hold up one in the other room. I can see all of it – all but the bit just ● Present Cosmology ● Visible vs. Dark matter behind the fireplace. I do so wish I could see that bit! I want so to know whether they’ve a fire ● B vs. D – Fine Tuning demonstration ● Unification in the winter: you never can tell, you know, unless our fire smokes, and then smoke comes up ● Neutrino Mixing ● See-Saw in that room too – but that may be only pretence, just to make it look as if they had a fire... ● Leptogenesis: diagrams ● Leptogenesis: formulas ‘How would you like to leave in the Looking-glass House, Kitty? I wander if they’d give you milk ● Epochs ● Neutron mixing in there? But perhaps Looking-glass milk isn’t good to drink? Now we come to the passage: ● Neutron mixing ● Oscillation it’s very like our passage as far as you can see, only you know it may be quite on beyond. -
Prospects for Dark Matter Detection with Inelastic Transitions of Xenon
Prospects for dark matter detection with inelastic transitions of xenon Christopher McCabe GRAPPA Centre for Excellence, Institute for Theoretical Physics Amsterdam (ITFA), University of Amsterdam, Science Park 904, the Netherlands E-mail: [email protected] Abstract. Dark matter can scatter and excite a nucleus to a low-lying excitation in a direct detection experiment. This signature is distinct from the canonical elastic scattering signal because the inelastic signal also contains the energy deposited from the subsequent prompt de-excitation of the nucleus. A measurement of the elastic and inelastic signal will allow a single experiment to distinguish between a spin-independent and spin-dependent interaction. For the first time, we characterise the inelastic signal for two-phase xenon de- tectors in which dark matter inelastically scatters off the 129Xe or 131Xe isotope. We do this by implementing a realistic simulation of a typical tonne-scale two-phase xenon detector and by carefully estimating the relevant background signals. With our detector simulation, we explore whether the inelastic signal from the axial-vector interaction is detectable with upcoming tonne-scale detectors. We find that two-phase detectors allow for some discrim- ination between signal and background so that it is possible to detect dark matter that inelastically scatters off either the 129Xe or 131Xe isotope for dark matter particles that are heavier than approximately 100 GeV. If, after two years of data, the XENON1T search for elastic scattering nuclei finds no evidence for dark matter, the possibility of ever detecting arXiv:1512.00460v2 [hep-ph] 23 May 2016 an inelastic signal from the axial-vector interaction will be almost entirely excluded. -
Glossary of Terms Absorption Line a Dark Line at a Particular Wavelength Superimposed Upon a Bright, Continuous Spectrum
Glossary of terms absorption line A dark line at a particular wavelength superimposed upon a bright, continuous spectrum. Such a spectral line can be formed when electromag- netic radiation, while travelling on its way to an observer, meets a substance; if that substance can absorb energy at that particular wavelength then the observer sees an absorption line. Compare with emission line. accretion disk A disk of gas or dust orbiting a massive object such as a star, a stellar-mass black hole or an active galactic nucleus. An accretion disk plays an important role in the formation of a planetary system around a young star. An accretion disk around a supermassive black hole is thought to be the key mecha- nism powering an active galactic nucleus. active galactic nucleus (agn) A compact region at the center of a galaxy that emits vast amounts of electromagnetic radiation and fast-moving jets of particles; an agn can outshine the rest of the galaxy despite being hardly larger in volume than the Solar System. Various classes of agn exist, including quasars and Seyfert galaxies, but in each case the energy is believed to be generated as matter accretes onto a supermassive black hole. adaptive optics A technique used by large ground-based optical telescopes to remove the blurring affects caused by Earth’s atmosphere. Light from a guide star is used as a calibration source; a complicated system of software and hardware then deforms a small mirror to correct for atmospheric distortions. The mirror shape changes more quickly than the atmosphere itself fluctuates. -
Isospin Violating Dark Matter
Isospin Violating Dark Matter David Sanford Work with J.L. Feng, J. Kumar, and D. Marfatia UC Irvine Pheno 2011 - Tuesday May 10, 2011 Current State of Light Dark Matter I Great recent interest in CoGeNT light dark matter DAMA (Savage et. al.) CDMS-Si (shallow-site) I Major inconsistencies CDMS-Ge(shallow-site) CDMS-Ge (Soudan) between experimental XENON1 (! 11) XENON10 (! 11) results I DAMA and CoGeNT regions do not agree I XENON10/XENON100 rule out DAMA and CoGeNT I CDMS-Ge (Soudan) rules out much of CoGeNT and all of DAMA I Both DAMA and CoGeNT report annual modulation signals Possible Explanations of the Discrepancy Many theories have been put forward I Inelastic dark matter I Tucker-Smith and Weiner (2001) I Details of Leff in liquid xenon at low recoil energy I Collar and McKinsey (2010) I Channeling in NaI at DAMA I Bernabei et. al. [DAMA] (2007); Bozorgnia, Gelmini, Gondolo (2010) We propose to rescind the assumption of isospin conservation I Unfounded theoretical assumption I Simple resolution of several discrepancies I Also considered by Chang, Liu, Pierce, Weiner, Yavin (2010) I For fp 6= fn, this result must be altered Z I In fact, for fn=fp = − A−Z , σA vanishes from completely destructive interference Z I A−Z decreases for higher Z isotopes Isospin Conservation and Violation I DM-nucleus scattering is Dark Matter Compton Wavelength coherent I The single atom SI scattering cross-section is Nucleus 2 σA / [fpZ + fn(A − Z)] 2 2 / fp A (fp = fn) Z : atomic number A: number of nucleons 2 I Well-known A fp: coupling to protons -
Astrophysical Issues in Indirect DM Detection
Astrophysical issues in indirect DM detection Julien Lavalle CNRS Lab. Univers & Particules de Montpellier (LUPM), France Université Montpellier II – CNRS-IN2P3 (UMR 5299) Max-Planck-Institut für Kernphysik Heidelberg – 1st VII 2013 Outline * Introduction * Practical examples of astrophysical issues (at the Galactic scale) => size of the GCR diffusion zone: relevant to antiprotons, antideuterons, (diffuse gamma-rays) => positron fraction: clarifying the role of local astrophysical sources => impact of DM inhomogeneities: boost + reinterpreting current constraints => diffuse gamma-rays * Perspectives Julien Lavalle, MPIK, Heidelberg, 1st VII 2013 Indirect dark matter detection in the Milky Way Main arguments: But: ● Annihilation final states lead to: gamma-rays + antimatter ● Do we control the backgrounds? ● -rays : lines, spatial + spectral distribution of signals vs bg ● γ Antiprotons are secondaries, not necessarily positrons ● Antimatter cosmic rays: secondary, therefore low bg ● Do the natural DM particle models provide clean signatures? ● DM-induced antimatter has specific spectral properties Julien Lavalle, MPIK, Heidelberg, 1st VII 2013 Indirect dark matter detection in the Milky Way Main arguments: But: ● Annihilation final states lead to: gamma-rays + antimatter ● Do we control the backgrounds? ● -rays : lines, spatial + spectral distribution of signals vs bg ● γ Antiprotons are secondaries, not necessarily positrons ● Antimatter cosmic rays: secondary, therefore low bg ● Do the natural DM particle models provide clean signatures? -
Low-Mass Dark Matter Search with the Darkside-50 Experiment
Low-Mass Dark Matter Search with the DarkSide-50 Experiment P. Agnes,1 I. F. M. Albuquerque,2 T. Alexander,3 A. K. Alton,4 G. R. Araujo,2 D. M. Asner,5 M. Ave,2 H. O. Back,3 B. Baldin,6,a G. Batignani,7, 8 K. Biery,6 V. Bocci,9 G. Bonfini,10 W. Bonivento,11 B. Bottino,12, 13 F. Budano,14, 15 S. Bussino,14, 15 M. Cadeddu,16, 11 M. Cadoni,16, 11 F. Calaprice,17 A. Caminata,13 N. Canci,1, 10 A. Candela,10 M. Caravati,16, 11 M. Cariello,13 M. Carlini,10 M. Carpinelli,18, 19 S. Catalanotti,20, 21 V. Cataudella,20, 21 P. Cavalcante,22, 10 S. Cavuoti,20, 21 R. Cereseto,13 A. Chepurnov,23 C. Cical`o,11 L. Cifarelli,24, 25 A. G. Cocco,21 G. Covone,20, 21 D. D'Angelo,26, 27 M. D'Incecco,10 D. D'Urso,18, 19 S. Davini,13 A. De Candia,20, 21 S. De Cecco,9, 28 M. De Deo,10 G. De Filippis,20, 21 G. De Rosa,20, 21 M. De Vincenzi,14, 15 P. Demontis,18, 19, 29 A. V. Derbin,30 A. Devoto,16, 11 F. Di Eusanio,17 G. Di Pietro,10, 27 C. Dionisi,9, 28 M. Downing,31 E. Edkins,32 A. Empl,1 A. Fan,33 G. Fiorillo,20, 21 K. Fomenko,34 D. Franco,35 F. Gabriele,10 A. Gabrieli,18, 19 C. Galbiati,17, 36 P. Garcia Abia,37 C. Ghiano,10 S. Giagu,9, 28 C. -
Jianglai Liu Shanghai Jiao Tong University
Jianglai Liu Shanghai Jiao Tong University Jianglai Liu Pheno 2017 1 If DM particles have non-gravitational interaction with normal matter, can be detected in “laboratories”. DM DM Collider Search Indirect Search ? SM SM Direct Search Pheno 2017 Jianglai Liu Pheno 2017 2 Galactic halo . The solar system is cycling the center of galaxy with on average 220 km/s speed (annual modulation in earth movement) . DM local density around us: 0.3(0.1) GeV/cm3 Astrophys. J. 756:89 Inclusion of new LAMOST survey data: 0.32(0.02), arXiv:1604.01216 Jianglai Liu Pheno 2017 3 1973: discovery of neutral current Gargamelle detector in CERN neutrino beam Dieter Haidt, CERN Courier Oct 2004: “The searches for neutral currents in previous neutrino experiments resulted in discouragingly low limits (@1968), and it was somehow commonly concluded that no weak neutral currents existed.” leptonic NC hadronic NC v beam Jianglai Liu Pheno 2017 4 Direct detection A = m2/m1 . DM: velocity ~1/1500 c, mass ~100 GeV, KE ~ 20 keV . Nuclear recoil (NR, “hadronic”): recoiling energy ~10 keV . Electron recoil (ER, “leptonic”): 10-4 suppression in energy, very difficult to detect New ideas exist, e.g. Hochberg, Zhao, and Zurek, PRL 116, 011301 Jianglai Liu Pheno 2017 5 Elastic recoil spectrum . Energy threshold mass DM . SI: coherent scattering on all nucleons (A2 Ge Xe enhancement) . Note, spin-dependent Si effect can be viewed as scattering with outer unpaired nucleon. No luxury of A2 enhancement Gaitskell, Annu. Rev. Nucl. Part. Sci. 2004 Jianglai Liu Pheno 2017 6 Neutrino “floor” Goodman & Witten Ideas do exist Phys. -
Mirror Matter: Astrophysical Implications
Mirror Matter: Astrophysical implications Zurab Berezhiani Summary Mirror Matter: Astrophysical implications Introduction: Dark Matter from a Parallel World Chapter I: Neutrino - mirror neutrino mixings Zurab Berezhiani Chapter II: neutron { mirror University of L'Aquila and LNGS neutron mixing Chapter IV: n − n0 and Neutron Stars Quarks-2021 , 22-24 June 2021 Contents Mirror Matter: Astrophysical implications Zurab Berezhiani Summary Introduction: Dark Matter from 1 Introduction: Dark Matter from a Parallel World a Parallel World Chapter I: Neutrino - mirror neutrino mixings 2 Chapter I: Neutrino - mirror neutrino mixings Chapter II: neutron { mirror neutron mixing Chapter IV: n − n0 and 3 Chapter II: neutron { mirror neutron mixing Neutron Stars 4 Chapter IV: n n0 and Neutron Stars − Mirror Matter: Astrophysical implications Zurab Berezhiani Summary Introduction: Dark Matter from a Parallel World Introduction Chapter I: Neutrino - mirror neutrino mixings Chapter II: neutron { mirror neutron mixing Chapter IV: n − n0 and Everything can be explained by the Standard Model ! Neutron Stars ... but there should be more than one Standard Models Bright & Dark Sides of our Universe Mirror Matter: Ω 0 05 observable matter: electron, proton, neutron ! Astrophysical B : implications ' ΩD 0:25 dark matter: WIMP? axion? sterile ν? ... Zurab Berezhiani ' ΩΛ 0:70 dark energy: Λ-term? Quintessence? .... Summary ' 3 Introduction: ΩR < 10− relativistic fraction: relic photons and neutrinos Dark Matter from a Parallel World Matter { dark energy coincidence: Ω Ω 0 45, (Ω = Ω + Ω ) Chapter I: M = Λ : M D B Neutrino - mirror 3 ' ρΛ Const., ρM a− ; why ρM /ρΛ 1 { just Today? neutrino mixings ∼ ∼ ∼ Chapter II: Antrophic explanation: if not Today, then Yesterday or Tomorrow.