Lowering the Icecube Detection Threshold by Wavelength-Shifting Optical Modules
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The Future of High Energy Physics and China’s Role Yifang Wang Institute of High Energy Physics, Beijing HKUST, Sep. 24, 2018 A Very Active Field ILC,FCC, China-based LHC: ATLAS/CMS CEPC/SPPC High China-participated Others Energy Compositeness AMS, PAMELA Extra-dimensions Supersymmetry Antimatter Higgs CP violation Daya Bay, JUNO,T2K,Nova, SuperK,HyperK,LBNF/DUNE, Icecube/PINGU, KM3net/ORKA, Neutrinos SNO+,EXO/nEXO, KamLAND-Zen, Precision Standard COMET, tests Model Gerda,Katrin… mu2e, g-2, K-decays,… Hadron physics Cosmology & QCD Standard Model of Cosmology Rare decays Dark matter LUX, Xenon, LZ, BESIII,LHCb, Axions PandaX, CDEX, High BELLEII, Darkside, … precision PANDA,… ADMX,… Fermi, DAMPE, AMS,… 2 Roadmaps of HEP in the World • Japan (2012) – If new particles(e.g. Higgs) are discovered, build ILC – If θ13 is big enough, build HyperK and T2HK • EU (2013) – Continue LHC, upgrade its luminosity, until 2035 – Study future circular collider (FCC-hh or FCC-ee) • US (2014) – Build long baseline neutrino facility LBNF/DUNE – Study future colliders A new round of roadmap study is starting 3 Where Are We Going ? • ILC is a machine we planned for ~30 years, way before the Higgs boson was discovered. Is it still the only machine for our future ? • Shall we wait for results from LHC/HL-LHC to decide our next step ? • What if ILC could not be approved ? • What is the future of High Energy Physics ? • A new route: – Thanks to the low mass Higgs, there is a possibility to build a circular e+e- collider(Higgs factory) followed by a proton machine in the same tunnel – This idea was reported for the first time at the “Higgs Factory workshop(HF2012)” in Oct. -
Effective Neutrino Masses in KATRIN and Future Tritium Beta-Decay Experiments
PHYSICAL REVIEW D 101, 016003 (2020) Effective neutrino masses in KATRIN and future tritium beta-decay experiments † ‡ Guo-yuan Huang,1,2,* Werner Rodejohann ,3, and Shun Zhou1,2, 1Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China 2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China 3Max-Planck-Institut für Kernphysik, Postfach 103980, D-69029 Heidelberg, Germany (Received 25 October 2019; published 3 January 2020) Past and current direct neutrino mass experiments set limits on the so-called effective neutrino mass, which is an incoherent sum of neutrino masses and lepton mixing matrix elements. The electron energy spectrum which neglects the relativistic and nuclear recoil effects is often assumed. Alternative definitions of effective masses exist, and an exact relativistic spectrum is calculable. We quantitatively compare the validity of those different approximations as function of energy resolution and exposure in view of tritium beta decays in the KATRIN, Project 8, and PTOLEMY experiments. Furthermore, adopting the Bayesian approach, we present the posterior distributions of the effective neutrino mass by including current experimental information from neutrino oscillations, beta decay, neutrinoless double-beta decay, and cosmological observations. Both linear and logarithmic priors for the smallest neutrino mass are assumed. DOI: 10.1103/PhysRevD.101.016003 I. INTRODUCTION region close to its end point will be distorted in com- parisontothatinthelimitofzeroneutrinomasses.This Neutrino oscillation experiments have measured with kinematic effect is usually described by the effective very good precision the three leptonic flavor mixing neutrino mass [7] angles fθ12; θ13; θ23g and two independent neutrino 2 2 2 2 mass-squared differences Δm21 ≡ m2 − m1 and jΔm31j≡ qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi 2 − 2 2 2 2 2 2 2 jm3 m1j. -
Neutrino Mass Analysis with KATRIN
Technical University Munich Max Planck Institute for Physics Physics Department Werner Heisenberg Institute Advanced Lab Course Neutrino Mass Analysis with KATRIN Christian Karl, Susanne Mertens, Martin Slezák Last edited: September 2, 2020 Contents 1 Introduction 3 2 The KATRIN Experiment5 2.1 Neutrino Mass Determination from Beta-Decay............................5 2.2 Molecular Tritium as Beta-Decay Source................................6 2.3 Measuring Principle: MAC-E Filter Electron Spectroscopy.....................7 2.4 Experimental Setup.............................................8 2.4.1 Rear Section.............................................8 2.4.2 Windowless Gaseous Tritium Source..............................8 2.4.3 Pumping Sections.........................................9 2.4.4 Pre- and Main-Spectrometer...................................9 2.4.5 Focal Plane Detector........................................ 10 2.5 Modelling of the Integrated Beta-Decay Spectrum.......................... 10 2.5.1 Final State Distribution...................................... 10 2.5.2 Doppler Effect........................................... 11 2.5.3 Response Function......................................... 12 2.5.4 Model of the Rate Expectation................................. 13 3 Basic Principles of Data Analysis 15 3.1 Maximum Likelihood Analysis...................................... 15 3.2 Interval Estimation............................................. 16 4 Tasks 18 4.1 Understanding the Model........................................ -
Search for Neutrinos from TANAMI Observed AGN Using Fermi
Search for neutrinos from TANAMI observed AGN using Fermi lightcurves with ANTARES Suche nach Neutrinos von TANAMI-AGN unter Verwendung von Fermi-Lichtkurven mit ANTARES Der Naturwissenschaftlichen Fakultät der Friedrich-Alexander-Universität Erlangen-Nürnberg zur Erlangung des Doktorgrads Dr. rer. nat. vorgelegt von Kerstin Fehn Als Dissertation genehmigt von der Naturwissenschaftlichen Fakultät der Friedrich-Alexander Universität Erlangen-Nürnberg Tag der mündlichen Prüfung: 24.03.2015 Vorsitzender des Promotionsorgans: Prof. Dr. Jörn Wilms Gutachter/in: Prof. Dr. Gisela Anton Prof. Dr. Ulrich Katz ν Abstract Active galactic nuclei (AGN) are promising candidates for hadronic acceleration. The combination of radio, gamma ray and neutrino data should give information on their properties, especially concerning the sources of the high-energetic cosmic rays. Assuming a temporal correlation of gamma and neutrino emission in AGN the background of neutrino telescopes can be reduced using gamma ray lightcurves. Thereby the sensitivity for discovering cosmic neutrino sources is enhanced. In the present work a stacked search for a group of AGN with the ANTARES neutrino telescope in the Mediterranean is presented. The selection of AGN is based on the source sample of TANAMI, a multiwavelength observation program (radio to gamma rays) of extragalactic jets southerly of −30◦ declination. In the analysis lightcurves of the gamma satellite Fermi are used. In an unbinned maximum likelihood approach the test statistic in the background only case and in the signal and background case is determined. For the investigated 10% of data of ANTARES within the measurement time between 01.09.2008 and 30.07.2012 no significant excess is observed. -
Nuclear Physics
Nuclear Physics Overview One of the enduring mysteries of the universe is the nature of matter—what are its basic constituents and how do they interact to form the properties we observe? The largest contribution by far to the mass of the visible matter we are familiar with comes from protons and heavier nuclei. The mission of the Nuclear Physics (NP) program is to discover, explore, and understand all forms of nuclear matter. Although the fundamental particles that compose nuclear matter—quarks and gluons—are themselves relatively well understood, exactly how they interact and combine to form the different types of matter observed in the universe today and during its evolution remains largely unknown. Nuclear physicists seek to understand not just the familiar forms of matter we see around us, but also exotic forms such as those that existed in the first moments after the Big Bang and that exist today inside neutron stars, and to understand why matter takes on the specific forms now observed in nature. Nuclear physics addresses three broad, yet tightly interrelated, scientific thrusts: Quantum Chromodynamics (QCD); Nuclei and Nuclear Astrophysics; and Fundamental Symmetries: . QCD seeks to develop a complete understanding of how the fundamental particles that compose nuclear matter, the quarks and gluons, assemble themselves into composite nuclear particles such as protons and neutrons, how nuclear forces arise between these composite particles that lead to nuclei, and how novel forms of bulk, strongly interacting matter behave, such as the quark-gluon plasma that formed in the early universe. Nuclei and Nuclear Astrophysics seeks to understand how protons and neutrons combine to form atomic nuclei, including some now being observed for the first time, and how these nuclei have arisen during the 13.8 billion years since the birth of the cosmos. -
Dissertation Imaging Single Barium Atoms in Solid Xenon for Barium
Dissertation Imaging Single Barium Atoms in Solid Xenon for Barium Tagging in the nEXO Neutrinoless Double Beta Decay Experiment Submitted by Timothy Walton Department of Physics In partial fulfillment of the requirements For the Degree of Doctor of Philosophy Colorado State University Fort Collins, Colorado Spring 2016 Doctoral Committee: Advisor: William M. Fairbank, Jr. Bruce Berger Alan Van Orden Robert Wilson Copyright by Timothy Walton 2016 All Rights Reserved Abstract Imaging Single Barium Atoms in Solid Xenon for Barium Tagging in the nEXO Neutrinoless Double Beta Decay Experiment The nEXO experiment will search for neutrinoless double beta decay of the isotope 136Xe in a ton-scale liquid xenon time projection chamber, in order to probe the Majorana nature of neutrinos. Detecting the daughter 136Ba of double beta decay events, called barium tagging, is a technique under investigation which would provide a veto for a background-free measurement. This would involve detecting a single barium ion from within a macroscopic volume of liquid xenon. One proposed barium tagging method is to trap the barium ion in solid xenon at the end of a cold probe, and then detect it by its fluorescence in the solid xenon. In this thesis, new studies on the spectroscopy of deposits of Ba and Ba+ in solid xenon are presented. Imaging of barium atoms in solid xenon is demonstrated with sensitivity down to the single atom level. Achievement of this level of sensitivity is a major step toward barium tagging by this method. ii Acknowledgements I thank my adviser William M. Fairbank, Jr. with inadequate words for his inspiring courage, foresight, and intuition as a physicist. -
Neurychlovacová Fyzika Elementárních Cástic
Czech contribution to neutrino experiments V. Vorobel Charles University in Prague, FMP • Direct neutrino mass measurement – KATRIN • Accelerator neutrino NOvA • Reactor neutrino – Daya Bay, JUNO • Sterile neutrino DANCE • Doublel beta decay – NEMO3, SuperNEMO • Small scale experiments TGV 27.3.2015 RECFA - Vít Vorobel 1 KATRIN experiment - model independent search for the neutrino mass Czech participant: Nuclear Physics Institute of the Czech Acad. Sci., Řež near Prague Local and KATRIN websites: http://ojs.ujf.cas.cz/katrin/ http://www.katrin.kit.edu/ 2 KATRIN - Karlsruhe Tritium Neutrino Experiment: direct β-spectroscopic search for mν Measured quantity : 2 2 2 mνe = Σ|Uei| · mi i Mass eigenstates Neutrino mixing matrix elements theoretical decay amplitude: 2 1/2 dN/dE = K × F(Ee, Z+1) × pe × (Ee+me) × (E0-Ee) × [ (E0-Ee)2 – mνe ] Sensitiviy after 1000 measuring days: mν < 0.2 eV at 90 % C.L. if no effect is observed 3 mν = 0.35 eV would be seen as 5σ effect KATRIN setup - with MAC-E filter spectrometers For sensitivity of 200 meV: -high resolution: 0.9 eV -high luminosity: 19% of 4p -low detector back.: 10 mHz -T2 injection of 40 g/day, 4.7 Ci/s -1000 measurement days -high stability of key parameters e.g.: ± 3 ppm for retar. HV calibration & monitoring electron sources are developed at NPI 4 KATRIN – NPI: relations, manpower, funding, tasks With institutions from Germany, Russia, USA NPI is a founder of KATRIN Solid O. Dragoun and D. Vénos are members of the KATRIN Collaboration Board Electron D. Venos is co-leader of the task Calibration and Monitoring source Collaborators in 2014 . -
Letter of Interest Direct Neutrino-Mass Measurements with KATRIN
Snowmass2021 - Letter of Interest Direct Neutrino-Mass Measurements with KATRIN NF Topical Groups: (check all that apply /) (NF1) Neutrino oscillations (NF2) Sterile neutrinos (NF3) Beyond the Standard Model (NF4) Neutrinos from natural sources (NF5) Neutrino properties (NF6) Neutrino cross sections (NF7) Applications (TF11) Theory of neutrino physics (NF9) Artificial neutrino sources (NF10) Neutrino detectors (Other) [Please specify frontier/topical group(s)] Contact Information: Diana Parno (Carnegie Mellon University) [email protected] Collaboration: KATRIN Authors: The full author list follows the text and references. Abstract: (maximum 200 words) The Karlsruhe Tritium Neutrino-Mass (KATRIN) experiment has re- cently set the world’s best direct limit on the neutrino mass, from the measurement of the electron energy spectrum of tritium β-decay near its endpoint. This first result is based on the equivalent of only 9 days of data-taking in the experiment’s design configuration. Here, we discuss KATRIN’s plans for further ex- ploring the neutrino mass in the next 1000 days of data-taking, including research and development toward still-greater sensitivities. 1 The neutrino-mass scale is one of the most pressing open questions in particle physics, affecting not only neutrino theory within the Standard Model, but also the possible rates of neutrinoless double-beta decay and structure formation in the early universe. Cosmological observations have set extremely tight constraints P on the sum of neutrino-mass values mi, recently reporting mi < 0.26 eV (95% confidence level, CL) from cosmic-microwave-background power spectra alone [1]. However, the interpretation of these limits implicitly relies upon the paradigm of the cosmological standard model. -
Session: Neutrino Astronomy
Session: Neutrino Astronomy Chair: Takaaki Kajita, Institute for Cosmic Ray Research, Univ. of Tokyo Basic natures of neutrinos Neutrino was introduced in 1930 by W. Pauli in order to save the energy conservation law in nuclear beta decay processes, in which the emitted electron exhibits a continuous energy spectrum. It was assumed that the penetration power of neutrinos is much higher than that of the gamma rays. More than 20 years later, the existence of neutrinos was experimentally confirmed by an experiment that measured neutrinos produced by a nuclear power reactor. Since then, the basic nature of neutrinos has been understood through various theoretical and experimental studies: Neutrinos interact with matter extremely weakly. The number of neutrino species is three. They are called electron-neutrino, muon-neutrino and tau-neutrino. In addition, recent neutrino experiments discovered that neutrinos have very small masses. Observing the Universe by neutrinos (1) Because of the extremely high penetration power of neutrinos, neutrinos produced at the center of a star easily penetrate to the outer space. Theories of astrophysics predict that there are various processes that neutrinos play an essential role at the center of stars. For example, the Sun is generating its energy by nuclear fusion processes in the central region. In these processes, low energy electron neutrinos with various energy spectra are generated. Thus the observation of solar neutrinos directly probes the nuclear fusion reactions in the Sun. Another example is the supernova explosion. While the optical measurements observe an exploding star, what is happening in the central region of the star is the collapse of the core of a massive star. -
Carsten Rott Curriculum Vitae Feb 2018
Carsten Rott Curriculum Vitae Feb 2018 Department of Physics, Sungkyunkwan University, Suwon 16419, Korea Tel: +82-31-290-5902 E-mail:[email protected] Experimental astro-particle physics, particle physics, geophysics, neutri- Research nos physics Focus Languages German, English; Elementary: French, Japanese, and Korean Employment 2017 { 2018 Honorary Fellow at Wisconsin IceCube Particle Astrophysics Center (WIPAC) (Sabbatical), University of Wisconsin Madison, USA 2017 { now Associate Professor, Sungkyunkwan University, Korea 2013 { 2017 Assistant Professor, Sungkyunkwan University, Korea 2016 Visiting Researcher (3-month), University of Tokyo, Japan 2009 { 2013 Senior Fellow of the Center for Cosmology and AstroParticle Physics (CCAPP) (5-year term), The Ohio State University, USA 2008 { 2009 CCAPP Fellow (3-year term), The Ohio State University, USA 2005 { 2008 Postdoctoral Fellow, Pennsylvania State University, USA Education 1998 { 2004 Purdue University, Indiana, USA Ph.D in Experimental Particle Physics (December 2004) Title : \Search for Scalar Bottom Quarks from Gluino Decays" at CDF Thesis Adviser : Prof. Daniela Bortoletto 1995 { 1998 Universit¨atHannover, Hannover, Germany Honors and Awards 2011 Recipient of NSF Antarctica Service Medal 2005 \Fermilab's Result of the Week" (FermiNews, August 11, 2005) 2004 George W. Tautfest Award, Purdue University 1998 { 1999 University of Hannover { Purdue University direct exchange fellowship Funds and Grants 2017 { present NRF Midscale Research Fund (PI), Korea { NRF-2017R1A2B2003666 2017 { present Foreign Facility Fund (PI of 7 sub-PIs) { NRF-2017K1A3A7A09015973 2016 { present NRF SRC Korea Neutrino Research Center (KNRC) (Co-I), Korea 2016 { 2017 NRF Individual Researcher (PI), Korea { NRF-2016R1D1A1B03931688 2013 { present BrainKorea (BK21plus) participant, Korea 2013 { 2016 NRF Individual Researcher (PI), Korea { NRF-2013R1A1A1007068 2013 { 2014 SKKU Intramural Faculty Fund Award, Korea 2013 { 2014 Fermi GI Cycle 6 (Co-I with Prof. -
Strengthening Global Coordination on Large Neutrino Infrastructures”
July 8, 2016 Press Release concerning the 3rd International Neutrino Meeting on Large Neutrino Infrastructures hosted by KEK on the 30-31st of May 2016 “Strengthening global coordination on large neutrino infrastructures” Funding-agency1 and laboratory representatives2 gathered at the 3rd International Meeting on Large Neutrino Infrastructures3 on May 30-31, 2016 at KEK in Tsukuba, Japan to gauge the progress in the global coordination of projects that had been launched during the first and second international meetings4 and to discuss the next steps in the global coordination. The meeting was opened by the 2015 Nobel Prize winner Takaaki Kajita who commented that “Very large-scale experiments will be needed to fully explore neutrino properties. These large-scale experiments will also naturally have astrophysics potential and increase the sensitivity of searches for proton disintegration.” He went on to note that to realise the necessary very large-scale facilities would require “… international coordination and collaboration” and defined the goals of the meeting to be to “… discuss the physics cases and global strategy, including astrophysics and proton decays, which are the part of the aim of this series of meetings; have follow-up discussions of the ICFA Neutrino Panel’s5 roadmap discussion document”6 and to discuss “… the various neutrino experiments, including Hyper- Kamiokande7, toward the realization of an efficient and productive global neutrino program.” In this meeting, the funding-agency and laboratory representatives welcomed the important steps that had been made towards the realisation of the Hyper-Kamiokande (Hyper-K) experiment7. The international proto-collaboration has developed new, high- sensitivity, large-aperture photomultiplier tubes that substantially reduce the total project cost without unduly compromising its potential to address important questions in particle and astroparticle physics and in nucleon decay. -
Optimization of a KATRIN Source Analysis Tool and Investigations of the Potential to Constrain the Relic Neutrino Background
Optimization of a KATRIN source analysis tool and investigations of the potential to constrain the relic neutrino background Master Thesis of Florian Heizmann At the Department of Physics Institute of Experimental Nuclear Physics Reviewer: Prof. G. Drexlin Second reviewer: Prof. U. Husemann Advisor: Dr. K. Valerius Second advisor: Dr. M. Babutzka January 2015 KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association www.kit.edu ABSTRACT The KArlsruhe TRItium Neutrino (KATRIN) experiment { currently under con- struction at KIT { will determine the neutrino mass with an unprecedented sensi- tivity of 200 meV at 90 % C.L. by high-precision tritium β-decay spectroscopy. In order to reach this new level of neutrino mass sensitivity it is very important to understand the tritium source properties and the related systematic measurement uncertainties. Therefore, in the scope of this thesis, the electromagnetic design of a source analysis tool is optimized. Furthermore, the unique tritium source opens up the possibility to search for the elusive relic neutrinos, at least to set limits on the local relic neutrino overdensity, in a laboratory experiment. The potential of KATRIN to set those limits is also explored in this thesis. Das KArlsruhe TRItium Neutrino (KATRIN) Experiment { welches sich momen- tan im Aufbau am KIT befindet { ist konstruiert, um mittels hochaufl¨osender β- Zerfall Spektroskopie die Neutrinomasse mit einer bisher unerreichten Sensitivit¨at von 200 meV zu 90 % C.L. zu bestimmen. Das Erreichen dieses Sensitivit¨atsziels erfordert ein detailliertes Verst¨andnis der Eigenschaften der Quelle und der damit verbundenen systematischen Messunsicher- heiten.