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CERN Celebrates Discoveries
INTERNATIONAL JOURNAL OF HIGH-ENERGY PHYSICS CERN COURIER VOLUME 43 NUMBER 10 DECEMBER 2003 CERN celebrates discoveries NEW PARTICLES NETWORKS SPAIN Protons make pentaquarks p5 Measuring the digital divide pl7 Particle physics thrives p30 16 KPH impact 113 KPH impact series VISyN High Voltage Power Supplies When the objective is to measure the almost immeasurable, the VISyN-Series is the detector power supply of choice. These multi-output, card based high voltage power supplies are stable, predictable, and versatile. VISyN is now manufactured by Universal High Voltage, a world leader in high voltage power supplies, whose products are in use in every national laboratory. For worldwide sales and service, contact the VISyN product group at Universal High Voltage. Universal High Voltage Your High Voltage Power Partner 57 Commerce Drive, Brookfield CT 06804 USA « (203) 740-8555 • Fax (203) 740-9555 www.universalhv.com Covering current developments in high- energy physics and related fields worldwide CERN Courier (ISSN 0304-288X) is distributed to member state governments, institutes and laboratories affiliated with CERN, and to their personnel. It is published monthly, except for January and August, in English and French editions. The views expressed are CERN not necessarily those of the CERN management. Editor Christine Sutton CERN, 1211 Geneva 23, Switzerland E-mail: [email protected] Fax:+41 (22) 782 1906 Web: cerncourier.com COURIER Advisory Board R Landua (Chairman), P Sphicas, K Potter, E Lillest0l, C Detraz, H Hoffmann, R Bailey -
About Testing Nu Mu Oscillation with Dm2 Smaller Than 0.001 Ev2 With
2 About testing νµ oscillation with ∆m smaller than 0.001 eV2 with the CERN Proton Synchrotron P. F. Loverre, R. Santacesaria, F. R. Spada Universit`a“La Sapienza” and Istituto Nazionale di Fisica Nucleare (INFN) Rome, Italy – Submitted to The European Physical Journal C Abstract We study the feasibility of a long–baseline neutrino experiment from CERN to Gran Sasso LNGS Laboratories using the CERN PS accelerator. Baseline and neutrino energy spectrum are suitable to explore a region of the (∆m2, sin2 2θ) parameters space which is not reached by K2K, the first experiment that will test at accelerator the atmospheric neutrino anomaly put in evidence by Super–Kamiokande. The recent Super–Kamiokande measurements of atmospheric neutrino arXiv:hep-ex/9911043v1 29 Nov 1999 fluxes [1] favour νµ → ντ (or νµ → νx) oscillations, with almost maximal mixing and ∆m2 in the range (5 ÷ 60) · 10−4 eV2. The first test of this atmospheric neutrino anomaly at accelerator will be performed in Japan by the K2K [2] experiment. K2K has recently started taking data using a neutrino beam generated by the KEK 12–GeV Pro- ton Synchrotron directed toward the Super–Kamiokande detector, which is placed about 250 Km away from KEK. The K2K experiment, owing to an L/E ratio of order 250/1 (Km/GeV), explores via disappearance νµ oscilla- tions down to ∆m2 ∼ 2 · 10−3 eV2. The same ∆m2 region can be explored with higher sensitivity with the high energy neutrino beams of FNAL (NuMI – MINOS experiment [3,4]) and 1 CERN (CERN – Gran Sasso LNGS beam [5]). -
K2K Cross Section Studies
K2K Cross Section Studies Rik Gran U. Minnesota Duluth 0. K2K experiment and NEUT interaction code 1. NC single p0/(All CC) in 1KT Cherenkov detector 2. CC-Coherent Pion Production in SciBar detector 3. MA-QE from shape fit to SciFi detector data Motivations Improve Neutrino Cross Sections knowledge of Cross Sections (Lipari 1995) En (GeV) Cross Sections and Nuclear Effects are important for extracting oscillation parameters from nu-mu disappearance nu-e appearance experiments. K2K oscillation result K2K beamline at KEK in Tsukuba, Japan OperK2Kated frneutom ri1999no osci to 2004llation experiment Al target 12 GeV PS 200m fast extraction every 2.2sec beam spill width 1.1s ( 9 bunches ) ~6x1012 protons/spill K2K beam and near detectors 98% pure n beam target materials: H2O, HC, Fe n energies SciFi Water Target at the K2K near detectors En (GeV) The NEUT neutrino interaction model Charged current quasi-elastic n + N -> l + N' Neutral current elastic n + N -> n + N CC/NC single p (h,K) resonance n + N -> l(n) + N' + p NC coherent pion (not CC !) n + A -> n + A + p0 CC/NC deep inelastic scattering n + q -> l(n) + had Cross-sections Total (NC+CC) n = neutrino (e, or t) ) V CC Total e l = lepton (e, or t) G / 2 m c CC quasi-elastic 8 3 - 0 1 From 100 MeV to 10 TeV ( DIS E / CC single π (cosmic ray induced neutrinos too!) σ NC single π0 Eν (GeV) More about the interaction models Quasi-elastic follows Llewelyn-Smith using dipole form factors and MAQE = 1.1 GeV (For neutrino beam, target is always neutron) Resonance production from Rein and Sehgal 18 resonances, MA1p = 1.1 GeV (Coherent pion production also from Rein and Sehgal) Deep inelastic Scattering from GRV94 PYTHIA/JETSET for hadron final states Bodek-Yang correction in Resonance-DIS overlap region Description and references available in Ch. -
April 2003 $4.95
SOLVING THE NEUTRINO MYSTERY • RECOGNIZING ANCIENT LIFE APRIL 2003 $4.95 WWW.SCIAM.COM James D.Watson discusses DNA, the brain, designer babies and more as he reflects on Grid Computing’s Unbounded Potential Ginkgo Biloba Will Mount Etna and Memory Explode Tomorrow? Delivering Drugs with Implanted Chips COPYRIGHT 2003 SCIENTIFIC AMERICAN, INC. april 2003 contentsSCIENTIFIC AMERICAN Volume 288 Number 4 features ASTROPHYSICS 40 Solving the Solar Neutrino Problem BY ARTHUR B. MCDONALD, JOSHUA R. KLEIN AND DAVID L. WARK After 30 years, physicists fathom the mystery of the missing neutrinos: the phantom particles change en route from the sun. BIOTECHNOLOGY 50 Where a Pill Won’t Reach BY ROBERT LANGER Implanted microchips, embedded polymers and ultrasonic blasts of proteins will deliver next-generation medicines. 66 James D. Watson VOLCANOLOGY 58 Mount Etna’s Ferocious Future BY TOM PFEIFFER Europe’s most active volcano grows more dangerous, but slowly. CELEBRATING THE GENETIC JUBILEE 66 A Conversation with James D. Watson The co-discoverer of DNA’s double helix reflects on the molecular model that changed both science and society. LIFE SCIENCE 70 Questioning the Oldest Signs of Life BY SARAH SIMPSON Researchers are reevaluating how they identify traces left by life in ancient rocks on earth—and elsewhere in the solar system. INFORMATION TECHNOLOGY 78 The Grid: Computing without Bounds BY IAN FOSTER Powerful global networks of processors and storage may end the era of self-contained computing. MEDICINE 86 The Lowdown on Ginkgo Biloba BY PAUL E. GOLD, LARRY CAHILL AND GARY L. WENK This herbal supplement may slightly improve your memory—but so can eating a candy bar. -
Search for the Process E+E−→Η′(958) with the CMD-3 Detector
Physics Letters B 740 (2015) 273–277 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb + − Search for the process e e → η (958) with the CMD-3 detector R.R. Akhmetshin a,b, A.V. Anisenkov a,b, V.M. Aulchenko a,b, V.Sh. Banzarov a, N.S. Bashtovoy a, D.E. Berkaev a,b, A.E. Bondar a,b, A.V. Bragin a, S.I. Eidelman a,b, D.A. Epifanov a,e, L.B. Epshteyn a,c, A.L. Erofeev a, G.V. Fedotovich a,b, S.E. Gayazov a,b, A.A. Grebenuk a,b, D.N. Grigoriev a,b,c, E.N. Gromov a, F.V. Ignatov a,b, S.V. Karpov a, V.F. Kazanin a,b, B.I. Khazin a,b,1, I.A. Koop a,b, O.A. Kovalenko a,b, A.N. Kozyrev a, E.A. Kozyrev a,b, P.P. Krokovny a,b, A.E. Kuzmenko a,b, A.S. Kuzmin a,b, I.B. Logashenko a,b, P.A. Lukin a,b, K.Yu. Mikhailov a, N.Yu. Muchnoi a,b, V.S. Okhapkin a, Yu.N. Pestov a, E.A. Perevedentsev a,b, A.S. Popov a,b, G.P. Razuvaev a,b, Yu.A. Rogovsky a, A.L. Romanov a, A.A. Ruban a, N.M. Ryskulov a, A.E. Ryzhenenkov a,b, V.E. Shebalin a,b, D.N. Shemyakin a,b, B.A. Shwartz a,b, D.B. Shwartz a,b, A.L. Sibidanov a,d, P.Yu. Shatunov a, Yu.M. -
The History of Neutrinos, 1930 − 1985
The History of Neutrinos, 1930 − 1985. What have we Learned About Neutrinos? What have we Learned Using Neutrinos? J. Steinberger Prepared for “25th International Conference On Neutrino Physics and Astrophysics”, Kyoto (Japan), June 2012 1 2 3 4 The detector of the experiment of Conversi, Pancini and Piccioni, 1946, 5 which showed that the mesotron is not the Yukawa particle. Detector with 80 Geiger counters. The muon decay spectrum is continuous. My thesis experiment, under Fermi, which showed that the muon decays into two neutral particles, plus the electron. Fermi, myself and others, in 1954, at a summer school in Varenna, lake Como, a few months before Fermi’s untimely disappearance. 6 Demonstration of the Neutrino In 1956 Cowan and Reines detected antineutrinos from a nuclear reactor, reacting with protons in liquid scintillator which also contained cadmium, observing the positron as well as the scattering of the neutron on cadmium. 7 The Electron and Muon Neutrinos are Different. 1. G. Feinberg, 1958. 2. B. Pontecorvo, 1959. 3. M. Schwartz (T.D. Lee), 1959 4. Higher energy accelerators, Courant, Livingston and Snyder. Pontecorvo 8 9 A C B D Spark chamber and counter arrangement. A are triggering counters, Energy spectra of neutrinos B, C and D are anticoincidence counters from pion and kaon decays. 10 Event with penetrating muon and hadron shower 11 The group of the 2nd neutrino experiment in 1962: J.S., Goulianos, Gaillard, Mistry, Danby, technician whose name I have forgotten, Lederman and Schwartz. 12 Same group, 26 years later, at Nobel ceremony in Stockholm. 13 Discovery of partons, nucleon structure, scaling, in deep inelastic scattering of electrons on protons at SLAC in 1969. -
Summary of the Second Workshop on Liquid Argon Time Projection Chamber Research and Development in the United States
FERMILAB-CONF-15-149-ND Preprint typeset in JINST style - HYPER VERSION Summary of the Second Workshop on Liquid Argon Time Projection Chamber Research and Development in the United States R. Acciarria, M. Adamowskia, D. Artripb, B. Ballera, C. Brombergc, F. Cavannaa;d, B. Carlsa, H. Chene, G. Deptucha, L. Epprecht f , R. Dharmapalang W. Foremanh A. Hahna, M. Johnsona, B. J. P. Jones i, T. Junka, K. Lang j, S. Lockwitza, A. Marchionnia, C. Maugerk, C. Montanaril, S. Mufsonm, M. Nessin, H. Olling Backo, G. Petrillop, S. Pordesa, J. Raafa, B. Rebela, G. Sininsk, M. Soderberga;q, N. Spoonerr, M. Stancaria, T. Strausss, K. Teraot , C. Thorne, T. Topea, M. Toupsi, J. Urheimm, R. Van de Waterk, H. Wangu, R. Wassermanv, M. Webers, D. Whittingtonm, T. Yanga aFermi National Accelerator Laboratory, Batavia, IL 60510, USA bResearch Catalytics, USA cMichigan State University, East Lansing, MI 48824, USA dYale University, New Haven, CT 06520, USA eBrookhaven National Laboratory, Upton, NY 11973, USA f ETH Zürich, 8092 Zürich, Switzerland gArgonne National Laboratory, Argonne, IL, 60439, USA hUniversity of Chicago, Chicago, IL 60637, USA iMassachusetts Institute of Technology, Cambridge, MA 02139, USA jUniversity of Texas at Austin, TX 78712, USA kLos Alamos National Laboratory, Los Alamos, NM 87545, USA lIstituto Nazionale di Fisica Nucleare, Pavia 6-27100, Italy mIndiana University, Bloomington, IN 47405, USA nCERN, 1217 Meyrin, Switzerland oPrinceton University, Princeton, NJ 08544, USA pUniversity of Rochester, Rochester, NY 14627, USA qSyracuse University, NY 13210, USA rUniversity of Sheffield, Sheffield, South Yorkshire S10 2TN, UK sUniversity of Bern, 3012 Bern, Switzerland t Columbia University, New York, NY 10027, USA uUniversity of California Los Angeles, Los Angeles, CA 90095, USA vColorado State University, Fort Collins, CO 80523, USA – 1 – Operated by Fermi Research Alliance, LLC under Contract No. -
CERN Courier Is Distributed to Member-State Governments, Institutes and Laboratories Affiliated with CERN, and to Their Personnel
I n t e r n at I o n a l J o u r n a l o f H I g H - e n e r g y P H y s I c s CERN COURIERV o l u m e 4 6 n u m b e r 9 n o V e m b e r 2 0 0 6 OPERA makes its grand debut ACCELERATORS COMPUTING NEWS INTERVIEW Laser-wakefield device Business signs up to Stephen Hawking pays reaches 1 GeV p5 work with EGEE p12 a visit to CERN p28 CCENovCover1.indd 1 18/10/06 08:53:59 CERN & ProCurve Networking 15 petabytes of data And a network that can handle it “CERN uses ProCurve Switches because we generate a colossal amount of data, making dependability a top priority.” —David Foster, Communication Systems Group Leader, CERN CERN has joined with ProCurve to build their network based on high-performance security, reliability and flexibility, along with a lifetime warranty.* From the world’s largest applications, to a company-wide email, just think what ProCurve could do for your network. Get a closer look at CERN and the world’s biggest physics experiment. Visit www.hp.com/eur/procurvecern1 *For as long as you own the product, with next-business-day advance replacement (available in most countries). For details, refer to the ProCurve Software License, Warranty and Support booklet at www.hp.com/rnd/support/warranty/index.htm The ProCurve Routing Switch 9300m series, ProCurve Routing Switch 9408sl, ProCurve Switch 8100fl series, and the ProCurve Access Control Server 745wl have a one-year- warranty with extensions available. -
Long Baseline Neutrino Oscillation Experiments 1 Introduction 2
Long Baseline Neutrino Oscillation Experiments Mark Thomson Cavendish Laboratory Department of Physics JJ Thomson Avenue Cambridge, CB3 0HE United Kingdom 1 Introduction In the last ten years the study of the quantum mechanical e®ect of neutrino os- cillations, which arises due to the mixing of the weak eigenstates fºe; º¹; º¿ g and the mass eigenstates fº1; º2; º3g, has revolutionised our understanding of neutrinos. Until recently, this understanding was dominated by experimental observations of at- mospheric [1, 2, 3] and solar neutrino [4, 5, 6] oscillations. These measurements have been of great importance. However, the use of naturally occuring neutrino sources is not su±cient to determine fully the flavour mixing parameters in the neutrino sector. For this reason, many of the current and next generation of neutrino experiments are based on high intensity accelerator generated neutrino beams. The ¯rst generation of these long-baseline (LBL) neutrino oscillation experiments, K2K, MINOS and CNGS, are the main subject of this review. The next generation of LBL experiments, T2K and NOºA, are also discussed. 2 Theoretical Background For two neutrino weak eigenstates fº®; º¯g related to two mass eigenstates fºi; ºjg, by a single mixing angle θij, it is simple to show that the survival probability of a neutrino of energy Eº and flavour ® after propagating a distance L through the vacuum is à ! 2 2 2 2 1:27¢mji(eV )L(km) P (º® ! º®) = 1 ¡ sin 2θij sin ; (1) Eº(GeV) 2 2 2 where ¢mji is the di®erence of the squares of the neutrino masses, mj ¡ mi . -
Iw F'tf- 1 -I ÛG 0 Zi
w^. m.-m?^iw f'tf- 1 -I ÛG 0 Zi Tt;: ANOMALOUS KAGNETiC i-'.OMEKT OF THE MUOM : A REVIEW DF THE THEORETICAL CONTRIBUTIONS j. CUV.ET*, S. NARISON**, H. PERROTTET* and E. de RAFAEL14 ABSTRACT : we review the possible contributions to the muon g-factor anomaly, o^ = — t^ -Z) which arc potentially significant for a comparison between theory .^nd experiment at present. This includes purely ÇF.D perturbation theory effects up to eighth-order ; hadronic effects at fourth end sixth-order ; and weak interaction effects. From these sources we'get a total theoretical contribution O-.JTheory) = (1 155 920.6 ± 12.9) x 10"9 , to be cc.'pared with the latest CERK expc-rinental result £l] , a- (Experiment) <= (1 !G5 895 ± 27) x 10"9 . J'JNE 1«6 76/P.333 K Zïr.*.rz de Pnysique Théorique, CNRS Marseille. *" Boursier de la CEE (Coir.r.unautè Economique Européenne) Postal Address : Centre de r'nysique Théorique - uiRS 31, C'.OT.ir, -'cseph Aiguicr P-Wfc- i - INTRODUCTION The latest published value of the anomalous magnetic cornent of the rcuon ir&ccured by the CCRN \-\uor. Storage Ring Collaboration [ll is The accuracy of this rce a s urcr.G nt represents an improvement by an order of magnitude with respect to tne previous result '. Since then, the Ci'\\ tfuon Storage Ring has been in operation for a certain time and o still further improvement in the accuracy is soon expected. At this level of precision there are contributions to <*• ^ , other than those gevernce uy the quantum electrodynamics of nuons ar.d electrons (Gr-D), like hadronic effects and possibly weak interaction effects, 21 which play an important role '. -
Neutron-Deuteron Scattering and Three-Body Interactions
Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 163 Neutron-Deuteron Scattering and Three-Body Interactions PHILIPPE MERMOD ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 UPPSALA ISBN 91-554-6514-5 2006 urn:nbn:se:uu:diva-6739 ! " #$ #%%& '( ) * * * + , - . / , " +, #%%&, 0 1 2 -13 4 , 50 1 -6 6 7, 8 , &', 9 $# , , 4230 : 1))$1&) $1), 1 ** * 1 :) "; , - 1 ** . * . < * 1 , -. 1 . "//= 2>808 * - 2 , - ** * * . * , - * * . "//= . , 4 1 . 6. 2>808 . ?, @ . * . 2>808 . ? . . . 1 6 , / * 1 . * ** . * ** . ** < * , - . @ 1 . 1 , - ** * 1 * ** '%A * , - . * 1 * ** , 1 * @ ? ! " # $" % & '('" " )*+',(- " B + " #%%& 4220 &) 1&# $ 4230 : 1))$1&) $1) ( ((( 1&C': 5 (DD ,6,D E F ( ((( 1&C':7 To Kristina List of Papers This thesis is based on the following papers, which are referred to in the text by their Roman numerals. I J. Klug, J. Blomgren, A. Ataç, B. Bergenwall, A. Hildebrand, C. Johansson, P. Mermod, L. Nilsson, S. Pomp, U. Tippawan, K. Elmgren, N. Olsson, O. Jonsson, A.V. Prokofiev, P.-U. Renberg, P. Nadel-Turonski, -
Neutrino Physics
Neutrino Physics Steve Boyd University of Warwick Course Map 1. History and properties of the neutrino, neutrino interactions, beams and detectors 2. Neutrino mass, direct mass measurements, double beta decay, flavour oscillations 3. Unravelling neutrino oscillations experimentally 4. Where we are and where we're going References K. Zuber, “Neutrino Physics”, IoP Publishing 2004 C. Giunti and C.W.Kim, “Fundamentals of Neutrino Physics and Astrophysics”, Oxford University Press, 2007. R. N. Mohaptara and P. B. Pal, “Massive Neutrinos in Physics and Astrophysics”, World Scientific (2nd Edition), 1998 H.V. Klapdor-Kleingrothaus & K. Zuber, “Particle Astrophysics”,IoP Publishing, 1997. Two Scientific American articles: “Detecting Massive Neutrinos”, E. Kearns, T. Kajita, Y. Totsuka, Scientific American, August 1999. “Solving the Solar Neutrino Problem”, A.B. McDonald, J.R. Klein, D.L. Wark, Scientific American, April 2003. Plus other Handouts Lecture 1 In which history is unravelled, desperation is answered, and the art of neutrino generation and detection explained Crisis It is 1914 – the new study of atomic physics is in trouble (Z+1,A) Spin 1/2 (Z,A) Spin 1/2 Spin 1/2 electron Spin ½ ≠ spin ½ + spin ½ E ≠ E +e Ra Bi “At the present stage of atomic “Desperate remedy.....” theory we have no arguments “I do not dare publish this idea....” for upholding the concept of “I admit my way out may look energy balance in the case of improbable....” b-ray disintegrations.” “Weigh it and pass sentence....” “You tell them. I'm off to a party” Detection of the Neutrino 1950 – Reines and Cowan set out to detect n 1951 1951 1951 I.