IUPAP Report 41A
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Parallel Sessions
Identification of Dark Matter July 23-27, 2012 9th International Conference Chicago, IL http://kicp-workshops.uchicago.edu/IDM2012/ PARALLEL SESSIONS http://kicp.uchicago.edu/ http://www.nsf.gov/ http://www.uchicago.edu/ http://www.fnal.gov/ International Advisory Committee Daniel Akerib Elena Aprile Rita Bernabei Case Western Reserve University, Columbia University, USA Universita degli Studi di Roma, Italy Cleveland, USA Gianfranco Bertone Joakim Edsjo Katherine Freese University of Amsterdam Oskar Klein Centre / Stockholm University of Michigan, USA University Richard Gaitskell Gilles Gerbier Anne Green Brown University, USA IRFU/ CEA Saclay, France University of Nottingham, UK Karsten Jedamzik Xiangdong Ji Lawrence Krauss Universite de Montpellier, France University of Maryland, USA Arizona State University, USA Vitaly Kudryavtsev Reina Maruyama Leszek Roszkowski University of Sheffield University of Wisconsin-Madison University of Sheffield, UK Bernard Sadoulet Pierre Salati Daniel Santos University of California, Berkeley, USA University of California, Berkeley, USA LPSC/UJF/CNRS Pierre Sikivie Daniel Snowden-Ifft Neil Spooner University of Florida, USA Occidental College University of Sheffield, UK Max Tegmark Karl van Bibber Kavli Institute for Astrophysics & Space Naval Postgraduate School Monterey, Research at MIT, USA USA Local Organizing Committee Daniel Bauer Matthew Buckley Juan Collar Fermi National Accelerator Laboratory Fermi National Accelerator Laboratory Kavli Institute for Cosmological Physics Scott Dodelson Aimee -
Deep Science at Boulby Underground Laboratory
Sean Paling STFC Boulby Underground Science Facility Hartlepool Nuclear Power Station Astroparticle Physics: the search for Dark Matter & beyond Earth and environmental science, Astrobiology and planetary exploration CYGNUS Directional Dark Matter search Deep Science at Boulby Underground Laboratory: Subterranean studies at the UK’s deep underground science facility Underground lab @ Boulby World antineutrino flux levels A WATer CHerenkov Monitor of ANtineutrinos Design, excavation, installation & operation 2019 to 2026(+) A 6kT Gd- loaded water detector looking at ~20 m anti-neutrinos from Hartlepool nuclear reactor • 3500 tons of gadoliniumVertices doped water within 50cm • 3000 photomultiplier tubes Funding: US (>$70M), UK (~£10M) • Signal: ~11 events/month/core confirmed in 2017 & 2018 respectively • ΔTBackground: ~30μs ~20 events/month NEW 6kT prototype detector: R&D for anti-neutrino monitoring of nuclear reactors for global nuclear non-proliferation purposes & more Deep Science @ Boulby Underground Laboratory… 1) About Boulby Mine and Boulby Underground Lab 2) Boulby Science Overview: • Astroparticle Physics & Low Background Science • Earth & Environmental Science • Astrobiology & Planetary Exploration Studies 3) The future: inc. AIT-NEO (WATCHMAN) Boulby Underground Laboratory The UK’s deep underground science facility operating in a working polyhalite & salt mine. 1.1km depth (2805 mwe). With low background surrounding rock-salt Operated by the UK’s Science & Technology Facilities Council (STFC) in partnership with the mine operators ICL Polyhalite Deepest mine in Britain Permian Evaporites Factor ~106 reduction in cosmic ray flux vs. surface A QUIET place in the Universe Boulby Geology & Mining Major local employer. Open since 1968. Originally mining potash (KCl) for fertiliser. Now first and only producers of polyhalite Excavations are in Salt (NaCl) & Potash (KCl) Permian evaporite layers left over from the Zechstein Sea. -
The PICASSO Dark Matter Physics Program at SNOLAB
33RD INTERNATIONAL COSMIC RAY CONFERENCE,RIO DE JANEIRO 2013 THE ASTROPARTICLE PHYSICS CONFERENCE The PICASSO Dark Matter Physics Program at SNOLAB A.J. NOBLE1 FOR THE PICASSO COLLABORATION: S. ARCHAMBAULT2, E. BEHNKE3, P. BHATTACHARJEE4, S. BHATTACHARYA4, X. DAI1, M. DAS4, A. DAVOUR1, F. DEBRIS2, N. DHUNGANA5, J. FARINE5, S. GAGNEBIN6, G. GIROUX2, E. GRACE3, C. M. JACKSON2, A. KAMAHA1, C. KRAUSS6, S. KUMARATUNGA2, M. LAFRENIRE2, M. LAURIN2, I. LAWSON7, L. LESSARD2, I. LEVINE3, C. LEVY1, R. P. MACDONALD6, D. MARLISOV6, J.-P. MARTIN2, P. MITRA6, A. J. NOBLE1, M.-C. PIRO2, R. PODVIYANUK5, S. POSPISIL8, S. SAHA4, O. SCALLON2, S. SETH4, N. STARINSKI2, I. STEKL8, U. WICHOSKI5, T. XIE1, V. ZACEK2 1 Department of Physics, Queens University, Kingston, K7L 3N6, Canada 2 Departement´ de Physique, Universite´ de Montreal,´ Montreal,´ H3C 3J7, Canada 3 Department of Physics & Astronomy, Indiana University South Bend, South Bend, IN 46634, USA 4 Saha Institute of Nuclear Physics, Centre for AstroParticle Physics (CAPP), Kolkata, 700064, India 5 Department of Physics, Laurentian University, Sudbury, P3E 2C6, Canada 6 Department of Physics, University of Alberta, Edmonton, T6G 2G7, Canada 7 SNOLAB, 1039 Regional Road 24, Lively ON, P3Y 1N2, Canada 8 Institute of Experimental and Applied Physics, Czech Technical University in Prague, Prague, Cz-12800, Czech Republic [email protected] Abstract: PICASSO is a dark matter search experiment currently operational at the SNOLAB International Facility for Astroparticle Physics, located 2 km underground in Sudbury, Canada. PICASSO is based on the superheated bubble technique. With good control of radiological backgrounds and a detector design that stabilizes the superheated liquid even when very close to the critical temperature, PICASSO has achieved very low nuclear recoil thresholds. -
Dark Matter the Invisible Material
Dark matter The invisible material Our universe holds everything we know and everything we are still figuring out. For years, physicists around the world have studied our universe to better understand its nature and its future. They have found that we only understand about 4% of the matter and energy in our universe (including stars, planets, and hot gas). The other 96% is invisible to us and 23% of this invisible material is named dark matter. If dark matter is invisible, how do we know it exists? To answer this, we go back to the 1930s when physicist Fritz Zwicky Galaxy cluster* coined the term dark matter while studying galaxy clusters. Galaxy clusters have up to thousands of galaxies (like our Milky Way for example) held together by gravity. When Dr. Zwicky calculated the total visible mass of galaxies in the Coma cluster, he found that it was not enough to create the gravity needed to hold the cluster together (mass causes gravity). He concluded that there must be an invisible material causing the extra gravity: dark matter. Now fast forward to the 1970s when Vera Rubin studied galaxy rotation curves. According to Newton’s laws, when objects rotate around a common centre, the ones furthest from the centre move more slowly Gravitational lens – than those near it. Otherwise, the furthest objects would fly off. Dr. Rubin galaxies look long found that stars in galaxies do not follow this rule. In fact, stars at the and distorted* outer edges of galaxies move at about the same rate as those near the centre. -
Required Sensitivity to Search the Neutrinoless Double Beta Decay in 124Sn
Required sensitivity to search the neutrinoless double beta decay in 124Sn Manoj Kumar Singh,1;2∗ Lakhwinder Singh,1;2 Vivek Sharma,1;2 Manoj Kumar Singh,1 Abhishek Kumar,1 Akash Pandey,1 Venktesh Singh,1∗ Henry Tsz-King Wong2 1 Department of Physics, Institute of Science, Banaras Hindu University, Varanasi 221005, India. 2 Institute of Physics, Academia Sinica, Taipei 11529, Taiwan. E-mail: ∗ [email protected] E-mail: ∗ [email protected] Abstract. The INdias TIN (TIN.TIN) detector is under development in the search for neutrinoless double-β decay (0νββ) using 90% enriched 124Sn isotope as the target mass. This detector will be housed in the upcoming underground facility of the India based Neutrino Observatory. We present the most important experimental parameters that would be used in the study of required sensitivity for the TIN.TIN experiment to probe the neutrino mass hierarchy. The sensitivity of the TIN.TIN detector in the presence of sole two neutrino double-β decay (2νββ) decay background is studied at various energy resolutions. The most optimistic and pessimistic scenario to probe the neutrino mass hierarchy at 3σ sensitivity level and 90% C.L. is also discussed. Keywords: Double Beta Decay, Nuclear Matrix Element, Neutrino Mass Hierarchy. arXiv:1802.04484v2 [hep-ph] 25 Oct 2018 PACS numbers: 12.60.Fr, 11.15.Ex, 23.40-s, 14.60.Pq Required sensitivity to search the neutrinoless double beta decay in 124Sn 2 1. Introduction Neutrinoless double-β decay (0νββ) is an interesting venue to look for the most important question whether neutrinos have Majorana or Dirac nature. -
The Germanium Detector Array for the Search of Neutrinoless Double Beta Decay of 76Ge
Colloquium on particle physics, astrophysics and cosmology 22 November 2004 GERDA The GERmanium Detector Array for the search of neutrinoless double beta decay of 76Ge Bernhard Schwingenheuer, Max-Planck-Insitut Kernphysik, Heidelberg Outline o Physics Motivation o Nuclear Matrix Elements oPast 76Ge Experiments o The GERDA Approach o Our Friends: the Competition oSummary GERDA Collaboration INFN LNGS, Assergi, Italy INR, Moscow, Russia A.Di Vacri, M. Junker, M. Laubenstein, C. Tomei, L. Pandola I. Barabanov, L. Bezrukov, A. Gangapshev, V. Gurentsov, V. Kusminov, E. Yanovich JINR Dubna, Russia ITEP Physics, Moscow, Russia S. Belogurov,V. Brudanin, V. Egorov, K. Gusev, S. Katulina, V.P. Bolotsky, E. Demidova, I.V. Kirpichnikov, A.A. A. Klimenko, O. Kochetov, I. Nemchenok, V. Vasenko, V.N. Kornoukhov Sandukovsky, A. Smolnikov, J. Yurkowski, S. Vasiliev, Kurchatov Institute, Moscow, Russia MPIK, Heidelberg, Germany A.M. Bakalyarov, S.T. Belyaev, M.V. Chirchenko, G.Y. C. Bauer, O. Chkvorets, W. Hampel, G. Heusser, W. Grigoriev, L.V. Inzhechik, V.I. Lebedev, A.V. Tikhomirov, Hofmann, J. Kiko, K.T. Knöpfle, P. Peiffer, S. S.V. Zhukov Schönert, J. Schreiner, B. Schwingenheuer, H. Simgen, G. Zuzel MPI Physik, München, Germany I. Abt, M. Altmann, C. Bűttner. A. Caldwell, R. Kotthaus, X. Univ. Köln, Germany Liu, H.-G. Moser, R.H. Richter J. Eberth, D. Weisshaar Univ. di Padova e INFN, Padova, Italy Jagiellonian University, Krakow, Poland A. Bettini, E. Farnea, C. Rossi Alvarez, C.A. Ur M.Wojcik Univ. Tübingen, Germany Univ. di Milano Bicocca e INFN, Milano, Italy M. Bauer, H. Clement, J. Jochum, S. Scholl, K. -
Particle Dark Matter an Introduction Into Evidence, Models, and Direct Searches
Particle Dark Matter An Introduction into Evidence, Models, and Direct Searches Lecture for ESIPAP 2016 European School of Instrumentation in Particle & Astroparticle Physics Archamps Technopole XENON1T January 25th, 2016 Uwe Oberlack Institute of Physics & PRISMA Cluster of Excellence Johannes Gutenberg University Mainz http://xenon.physik.uni-mainz.de Outline ● Evidence for Dark Matter: ▸ The Problem of Missing Mass ▸ In galaxies ▸ In galaxy clusters ▸ In the universe as a whole ● DM Candidates: ▸ The DM particle zoo ▸ WIMPs ● DM Direct Searches: ▸ Detection principle, physics inputs ▸ Example experiments & results ▸ Outlook Uwe Oberlack ESIPAP 2016 2 Types of Evidences for Dark Matter ● Kinematic studies use luminous astrophysical objects to probe the gravitational potential of a massive environment, e.g.: ▸ Stars or gas clouds probing the gravitational potential of galaxies ▸ Galaxies or intergalactic gas probing the gravitational potential of galaxy clusters ● Gravitational lensing is an independent way to measure the total mass (profle) of a foreground object using the light of background sources (galaxies, active galactic nuclei). ● Comparison of mass profles with observed luminosity profles lead to a problem of missing mass, usually interpreted as evidence for Dark Matter. ● Measuring the geometry (curvature) of the universe, indicates a ”fat” universe with close to critical density. Comparison with luminous mass: → a major accounting problem! Including observations of the expansion history lead to the Standard Model of Cosmology: accounting defcit solved by ~68% Dark Energy, ~27% Dark Matter and <5% “regular” (baryonic) matter. ● Other lines of evidence probe properties of matter under the infuence of gravity: ▸ the equation of state of oscillating matter as observed through fuctuations of the Cosmic Microwave Background (acoustic peaks). -
Dark Matter, Oscillations, Exotics Subgroup
Dark matter from ZeV to aeV: 3rd IBS-MultiDark-IPPP Workshop Durham, November 2016 Juande ZZornozaornoza (IFIC, UV-CSIC) Introduction X-rays and sterile neutrinos Neutrino telescopes Results . Sun . Earth . Milky Way . Extra-galactic Future Summary The evidence for the existence Virial theorem of dark matter is very solid and, which is very important, at many different scales Rotation curves Comma Cluster Cosmic Microwave Background Bullet Cluster Gravitational Lensing + BNN, N-body simulations… We do not know what is dark matter, so it is hard to say which is the winning strategy: multi-front attack! PAMELA, AMS FERMI, MAGIC ANTARES, IceCube… Indirect detection XENON χ q, W+, Z… CDMS In any case: CoGENT -we want more than one DAMA “detection” +astrophysical ANAIS -results (constraints) of each … probes ( self- strategy are input for the others interaction of χ Directdetection q, W-, Z… DM affecting dark matter densities in Accelerators LHC galaxies…) Credit: Sky & Telescope / Gregg Dinderman X-ray astronomy (1-100 keV) differs from gamma ray astronomy in the detection strategy Atmosphere absorbs X-rays and fluxes are high, so observation is based on balloons and satellites X-rays cannot be focused by lenses, so focusing is based on total reflection (Wolter telescope) Projects: Chandra, XMM-Newton, Suzaku XMM-Newton: Large collecting area Simultaneous imaging and high resolution spectroscopy Monochromatic 3.5 keV photon line observed in data of XMM-Newton from 73 galaxy clusters Located within 50-100 eV of several known faint lines Interpreted as decay from sterile Bulbul, arxiv:1402.2301 neutrinos with ms=7.1 keV, which would be dark matter Boyarsky, arxiv:1402.4119 Also observed in Andromeda and Perseus Interpretation as sterile neutrino (sin2 (2θ)∼7x10-11) consistent with present constraints However, significant astrophysical unknowns involved (for instance, potassium XVIII line) Bulbul, arxiv:1402.2301 Boyarsky, arxiv:1402.4119 Astro-H Chandra Astro-H satellite (aka Hitomi), equipped with a X-ray spectrometer, was launched in Feb 2016. -
GERDA: Germanium Detector Array Searching for 0Νββ Decay Gedet: Germanium Detector R&D
GERDA: GERmanium Detector Array searching for 0νββ decay GeDet: Germanium Detector R&D Director: Allen Caldwell Projector leaders: Béla Majorovits (GERDA), Iris Abt (GeDet) Postdoc: Josef Janicsko, Xiang Liu, Jens Schubert Ph.D.: Manuela Jelen, Kevin Kröninger(graduated 07/07), Daniel Lenz, Jing Liu Group engineer: Franz Stelzer Diplomand: Markus Kästle Werkstudenten/in: Golam Dastagir, Westa Domanova, Maximilian Empl, Daniel Greenwald, Andreas Kaiser Construction: Karlheinz Ackermann, Stefan Mayer, Sven Voggt Many thanks to colleagues from electronic & mechanic departments! Project Review 17/12/2007 Neutrino masses & mixing parameters 2 ν ν3 2 ν1 Mass 2 e Δm 32 μ ν τ 2 2 Δm 21 ν1 ν3 normal (NH) inverted (IH) 0 2 -3 2 atmospheric accelerator Æ Δm 32 = 2.2•10 eV 2 -5 2 solar reactor Æ Δm 21 = 8.1•10 eV absolute mass NH or IH Dirac or Majorana(ν=ν) page 2 0νββ decay Æ effective Majorana neutrino mass mββ np W- (A,Z) Æ (A, Z+2) + 2e- e- νL ΔL ≠0 e- νR happens, if ν=ν& mν>0 W- n p 2 2 −1 2 GT gV F half life []T1/2 = G( Q,Z)⋅ M − 2 M ⋅ mββ gA Phase space nuclear matrix element effective mass mββ 2 2 2 2 i(α2 −α1) i(−α1−2δ) mββ = ∑mjUej = m1 ⋅ Ue1 +m2 ⋅ Ue2 e +m3 ⋅ Ue3 e j page 3 Measure T1/2 of 0νββ decay npnp W- - e- e ν L ν - e- νR e W- ν n p n p 0νββ 2νββ: (A,Z) Æ (A,Z+2) +2e-+2ν search for energy peak at Q value (Ge76: 2039keV) page 4 0νββ experiments 21 Experiment Underground Isotope T1/2 [10 y] <mee> [eV] (selected) Laboratory Elegant VI Oto (Japan) 48Ca > 95 < 7.2 - 44.7 Heidelberg- Gran Sasso 76Ge >19000 < 0.35 - 1.2 Moscow (Italy) -
José Ángel Villar Rivacoba Was ANAIS Spokesperson and Chair Professor of Atomic, Molecular and Nuclear Physics at the Theo
24/10/2017 Direct Detection of Dark Matter and present status of ANAIS-112 experiment J. Amaré, I. Coarasa, S. Cebrián, C. Cuesta, E. García, M. Martínez, M.A. Oliván, Y. Ortigoza, A. Ortiz de Solórzano, J. Puimedón, A. Salinas, M.L. Sarsa, J.A. Villar✝, P. Villar In Memoriam In Memoriam • José Ángel Villar Rivacoba was ANAIS spokesperson and chair professor of Atomic, Molecular and Nuclear Physics at the Theoretical Physics Department of the University of Zaragoza • He passed away last August and we are deeply in sorrow 1 24/10/2017 In Memoriam In Memoriam • He was Bachelor and Doctor in Physics (Thesis supervised by Julio Morales) by the University of Zaragoza • He was always deeply involved in academic and research management activities in his University: • Dean of the Science Faculty at the University of Zaragoza (1992-2001) • Research Vice-Probost of the University of Zaragoza (2004-2008) • President of the Research Commission of the University of Zaragoza (2004-2008) • He was also strongly involved in scientific management at national and In Memoriam international level: • He was the coordinator of the national network of astroparticles (RENATA) • Member of the Executive Committee of the National Center for Physics of Astroparticles and Nuclear (CPAN) • Member of the general assembly and Joint Secretariat of the ApPEC Consortium • Organizer of numerous national and international congresses • Member of the Board and Science Assembly of ILIAS • Adviser to the successive Ministries responsible for Science and Technology, the Government -
Astrophysical Uncertainties of Direct Dark Matter Searches
Technische Universit¨atM¨unchen Astrophysical uncertainties of direct dark matter searches Dissertation by Andreas G¨unter Rappelt Physik Department, T30d & Collaborative Research Center SFB 1258 “Neutrinos and Dark Matter in Astro- and Particlephysics” Technische Universit¨atM¨unchen Physik Department T30d Astrophysical uncertainties of direct dark matter searches Andreas G¨unter Rappelt Vollst¨andigerAbdruck der von der Fakult¨atf¨urPhysik der Technischen Universit¨at M¨unchen zur Erlangung des akademischen Grades eines Doktors der Naturwissenschaften genehmigten Dissertation. Vorsitzender: Prof. Dr. Lothar Oberauer Pr¨uferder Dissertation: 1. Prof. Dr. Alejandro Ibarra 2. Prof. Dr. Bj¨ornGarbrecht Die Dissertation wurde am 12.11.2019 bei der Technischen Universit¨at M¨unchen eingereicht und durch die Fakult¨atf¨urPhysik am 24.01.2020 angenommen. Abstract Although the first hints towards dark matter were discovered almost 100 years ago, little is known today about its properties. Also, dark matter has so far only been inferred through astronomical and cosmological observations. In this work, we therefore investi- gate the influence of astrophysical assumptions on the interpretation of direct searches for dark matter. For this, we assume that dark matter is a weakly interacting massive particle. First, we discuss the development of a new analysis method for direct dark matter searches. Starting from the decomposition of the dark matter velocity distribu- tion into streams, we present a method that is completely independent of astrophysical assumptions. We extend this by using an effective theory for the interaction of dark matter with nucleons. This allows to analyze experiments with minimal assumptions on the particle physics of dark matter. Finally, we improve our method so that arbitrarily strong deviations from a reference velocity distribution can be considered. -
In-Situ Gamma-Ray Background Measurements for Next Generation CDEX Experiment in the China Jinping Underground Laboratory a a a a ∗ a a A,B a H
In-situ gamma-ray background measurements for next generation CDEX experiment in the China Jinping Underground Laboratory a a a a < a a a,b a H. Ma , Z. She , W. H. Zeng , Z. Zeng , , M. K. Jing , Q. Yue , J. P. Cheng , J. L. Li and a H. Zhang aKey Laboratory of Particle and Radiation Imaging (Ministry of Education) and Department of Engineering Physics, Tsinghua University, Beijing 100084 bCollege of Nuclear Science and Technology, Beijing Normal University, Beijing 100875 ARTICLEINFO ABSTRACT Keywords: In-situ -ray measurements were performed using a portable high purity germanium spectrometer in In-situ -ray measurements Hall-C at the second phase of the China Jinping Underground Laboratory (CJPL-II) to characterise Environmental radioactivity the environmental radioactivity background below 3 MeV and provide ambient -ray background Underground laboratory parameters for next generation of China Dark Matter Experiment (CDEX). The integral count rate Rare event physics of the spectrum was 46.8 cps in the energy range of 60 to 2700 keV. Detection efficiencies of the CJPL spectrometer corresponding to concrete walls and surrounding air were obtained from numerical calculation and Monte Carlo simulation, respectively. The radioactivity concentrations of the walls 238 232 in the Hall-C were calculated to be 6:8 , 1:5 Bq/kg for U, 5:4 , 0:6 Bq/kg for Th, 81:9 , 14:3 40 Bq/kg for K. Based on the measurement results, the expected background rates from these primordial radionuclides of future CDEX experiment were simulated in unit of counts per keV per ton per year (cpkty) for the energy ranges of 2 to 4 keV and around 2 MeV.