Search for New Particles at LEP

Total Page:16

File Type:pdf, Size:1020Kb

Search for New Particles at LEP Search for New Particles at LEP S. Rosier-Lees LAPP (INPPS-CNRS) Annecy-Le-Vieux - France Abstract The LEP energy upgrade up to fi =189 GeV has allowed us to extend substantially the potential of searches for new physics. Results on searches for Higgs bosoms and supersymmetric particles obtained by the ALEPH, DELPHI, L3, and OPAL exper- iments are reported. No evidence of any signal is observed. Therefore, new limits on the Higgs boson masses as well as on the masses of the various supersymmetric particles are derived. They significantly improve those obtained either at LEPl or LEP1.5. The LEPBOO discovery potential for the neutral Higgs bosons is also shown. @ 1998 by S. Rosier-Lees. -409- . be discovered at LEP200 when running at &=200 GeV and assuming an integrated luminosity of 200 pb-’ collected by each experiment. LEP PRELIMINARY Individual Limit LEP Combined 11 Table 1: Individual and LEP combined observed and expected mass limits for the Stan- dard Model Higgs boson [3], up to fi = 183 GeV. 4 _?I: 80 82 84 86 88 90 92 94 10 80 82 84 86 88 90 92 mH(GeV/ z5 k --- HZ-Signal(mn=85GeV) 2 1.5 1 0.5 0 0 20 40 60 80 loo 0 mF(GeV) Figure 1: Mass distribution for the candidate events selected by the OPAL experiment in the searches for e+e- + HZ at center-of-mass energies up to 183 GeV [3]. I,,,I,,,,,,/,I lo 80 82 84 86 88 90 92 94. 80 82 84 86 88 90 92 94 mH(GeV/c’) mH(Ge V/c2) 2.2 The MSSM Higgs Bosons Figure 2: Average expected (dashed lines) and observed (solid lines) confidence levels, CL,, obtained In the MSSM, all SUSY particle masses, their couplings, and their production cross sec- from combining the results of the four LEP Collaborations using the four statistical methods. The tions and decay widths are predicted in terms of only six free independent parameters: intersections of the curves with the horizontal lines at 0.05 define the 95% confidence level lower rnilz (the common gaugino mass parameter at the GUT scale), me (the common mass for bounds, ezpected and observed, for the mass of the 5X4 Higgs boson. scalar fermions at the GUT scale), p (the higgsino mixing parameter), tan/3 (the ratio of the vacuum expectation values of the two Higgs doublets), mA (the mass of the neutral CP-odd Higgs boson A), and A (the trilinear coupling in the Higgs sector at the GUT scale); the renormalization group equations are used to determine the parameters at low -411- h ] Mh.a Lower Limit (GeV/c2) ] PRELIMINARY Range of ~ Lower ’ Individual Limit LEP Combined (ADLO) y#p#p h (Obs.) 70.7-74.4 78.8 (Exp.) 67.4-70.3 76.3 A (Obs.) 71.0-76.1 79.1 (ExP.) 68.4-72.0 76.3 Table 4: Individual and LEP combined mass limits for the neutral h and A bosons [3]. background contamination. The 95% C.L. individual limits on the charged Higgs boson Mu*=60 GeV/c’ r-o,r+u, T+V,SC cssi: Efficiency 24% 42% 40% Expected events 9.2 30.1 99.4 Observed events ] 6 1 28 1 93 0 100 200 300 400 500 mA (GeV/c2) Table 5: Typical efficiencies and number of expected and observed events obtained by the L3 experiment in the charged Higgs boson searches at a c.m. energy of 183 GeV (141. Individual Limit (ADLO) LEP Combmed 10 11 Table 6: Individual and LEP combined mass limits for the charged Higgs bosons. mass is shown as a function of the branching ratio Br(H* + r*vT) in Fig. 4. Combining all LEP results, a lower limit on the charged Higgs boson mass of 68 GeV is established at the 95% C.L., assuming that the sum BR(H+ + r’+uT) + Br(H+ + cS) is equal to one. It represents a gain of almost 10 GeV with respect to the individual limits, Table 6. 0 20 40 60 80 loo 120 140 3 Other SUSY Particles mh (GeV/c2) The supersymmetric particles searched for at LEP2, not counting the Higgs bosons, are Figure 3: LEP combined exclusion domains (method D) in the plane (MA, tan,@ (top) or sleptons, stops, sbottoms, charginos, and neutralinos as detailed in Refs. [17] and [18]. (Mh, tan,@ (bottom) by the LEP direct searches for e+e- + hZ and hA at center-of-mass The most popular SUSY breaking mechanisms are the gravity and the gauge mediated energies up to 183 GeV assuming either a maximal mixing or no mixing [3] and [IS]. SUSY breaking models (GMSB). The results of SUSY searches at LEP are interpreted in the framework of these two models. In general, to avoid lepton and baryon number -413- -PIP- ‘cd37 $?? pa!pnls a1s s[auueqD Lwap ay$30 lsour ‘[w@s aql 03 palvduroa suo!$3as 55013 uo!pnpold a[qeuos%zal ~J!M sassaao1d a~qepyw-~[aM 0% anp are sa31nos punoL?yLnzq pea1 quamF1adxa tjasa 103 r-qd ()P-OE 30 hpOU!unl pa$%?18a$u! ue qp~ Aafj 6531~9 $8 aq$[[e azm!s .uo!pnpo1d Il’ed-M 30 asoq$ 0% .IVI!UI!S haA a1’l? sa1nlou$s 1w18!s aq$ ‘sanpzA dlluaaal pauyqo sl!unI Impw!pu! aql lsql ospz uoyam plnoqs a~ ‘8 alqvA u! u~oqs se (Aafj ()g - 09 =)~v a%%?[ 10~ ‘suo!KRJa$u! uoloqd-oM$ iEq paqwI!uIop SF pUnOI8~Xq uoymqruo~ aq$ IIF pauyqo s! ‘IOAV~ uoldal 1~pm aql uo Bmpuadap ‘Aa 01 0% z 11~023 aq+ pus ‘Ehaua aIq!s!A ~01 ‘I? pue .Qyd!~~ntu ~01 B Lq paz!1al9weqz a1e s~w@s aql 103 8uyBue1 II@ ‘I? pm sdlay &sou!umI a1otu ‘~!ur!l pz3ymau!y aql 1110131~3 a1v aa acms sa@oIodo$ palzadxa aq$ ‘a8uw (Aa=) 01 - 9 =)mv MOI aql UI .W1aua a[q!s!a aql ~101) ‘Aa ogz- = rl 103 pwe ‘z 01 p.1 -uo3 ga!q~ (6’~ - =snsw = NV) azma1agLp SS\?UI ds? ayl pue a[zysd ~sfls aql Lq moq Su@ue~ sanpzn @mu Iualagtp ~03 panFlap am sl!unf pmpFA!pu! aq~ ‘2 +!A u! UMO~S papagE acyawd u! a.nz suo!$!puo~ puno&?!yavq aql pu’e GfoIodo$ ~euB!s aq& ‘&T aq$ Aq am Aafj ~$31 0% dn [SC] sasdpm? d37 up 30 s1noquo:, uoyq3xa pamquxoa aqL .s1alammd $no pa;11w Gi1aua BU!SS!UI puz suo%daI puv/~o slaf 30 uo!+vu!quro:, awes 30 $s!suoa sam$ asaql uo spuadap a%eq~xa Iauusy>$ :X aql u! uoyDas ssom uoFmpo1d aq+ ‘“2 JOJ -WI@ Asps ‘s&7 pw saIa!$n?d J@S 09 keaap saIcnl.rvd Asps pampo1d-1!sd sno!1%t aqA ‘uo!$anpo1d-1!sd 103 uoyaas SSOJCI “!aql q>agv lou op tnq (saya1eas :X aq$ Lq LEM~UTZ pa1aAoa uo@al ayl u! :X 30 sasSem MOI 103 b~uo luvAaIa1) EX 0% &uydnoa l!ayq aSueq3 lsnf 1Ewu sla$awwvd asaql am!s ‘+ pus Wj ~03 @IB$ 10 71 uo .L~~gS~~sQuo puadap s~!ux!~ asaqL .( %U ‘ A’uL) areid aql IIF paA!Jap art? s$!uu[ 11~ saShpe 631 11” 103 pa$zw~qns ‘(Aa I N %V WP’ ‘2) s! uoFympo1d 1!‘ed-M uroq pnno&yzq papadxa aqA L@O uo!$anpo1d XT~? IunoaDa o)u~ ouyAw% aql s! y slapour 8sw3 u! aI!qti ‘(:X) ouy21~nau Isa@!1 aql s! dsq aql ‘s[apotu Bu!yv~ qIn*ejap Lq ua@ ale sasswu uo s)!ur!~ ‘71 103 uar[~~ 1aIIsurs s! xf 30 %pnpo1d 1!ed Puyea1q Asps L~!AEI~ II! reIncy.nzd III 9uycm1ary &eaM pw p1lnau aq 0% pasoddns ayl 103 uoyaas SSOJD aql ‘IwauaP u! acm!s .[pz] +JZ] Aa ggr=sJ 07 Idn d37 1~ paa1asqo s! y acm!s uo!pa)ap sadwsa puv aIqv$s SI (ds?) al3!$1vd Asps qsa)q%y aql ‘uoydurnssv S&?M sassaaold ws u10q palaadxa sluaaa 30 1aqumu aql 03 qaadsa1 I#!M ssa3xa ON sq$ u!q$!~ .salayed Asfls 103 I- = pwe sal3!$1ed prepuv~s 103 1 = ‘rz+as+7(~-) = g :payonu! s! 1aqurnu urnluenb Mau ‘t?30 uoyeAnlasuo3 aq$ ‘sdoo1 nsns bq pacmpu! suoyqo!~ +j Aa ggl o) dn sa!%aua sswu-jo-1a$ua~ ye -H+H t -a+a ~03 saqweas panp 631 ay% Aq [(“CZL t &.LH ‘FH,wJ] aweId aq$ u! su~wuop uo!snIzxa pawquro3 d3q :p aIn&J - - y..---+ i ,.“.........‘... i i... t ..- z’o .; i ,cqv luala3pp ~03 sassaao1d ms uroq sluaaa palaadxa puv sayxaygfa Iw!dQ ‘:X aql PUB :: : ;: : uolda[ yecw aql uaaM+aq ‘JV\TV ‘aaua1agtp sswu aq$ uo h1%01)s puadap saqanzas asaql.103 :: / sa!$!arl!suas aq!$ ‘uoympo1$u! aql u! pau!ydxa dpvaqs sv Gl1aua Bu~ss~ur sn[d suo$daI “’ ““- p’o 1sueIdocm Qansn uaql aw uoympo1d uo$daI 1yeas 111013Bu!spe sa@olodo) aye .alq!ssod a~anm& . aq hur (ou!Zhvq~ ad&ou@nS a1nd ‘t! 103 d~uo 71.103) 2X ou!81erl:, $sa@!I aql via 10 :X ya Sh3ap apKww ‘(dS?N) apyvd nsns $sa@+o$-$xau aq$ lou SF uo2dal 1~?1ws aq$31 ‘:X ... .. .. .. i - 9’0 ouyz1)nau $sa@!I aq$ pus s.wr+red KS 1!aq$ o$u! Kemp b~~uw~~u~op suolda1 rye~s ayL .lauuvq3-? aql u! sou!Iw~nau Bu!Suvq3xa Lq paanpo1d aq ospz uw _a suollya 1eyez~s wa1aqM ‘LIUO lauueqa-s aql u! a%eqaxa z .IO A~~&.r~oEr~r~ 8’0 L v!a spaaDo1d 4 sne$ .IS~~~S puw g suonm 1yez~ 30 uo!pnpo1d aql ‘suoy~~o~ -a+a III ‘[CT] suo!p$Dadxa ns aql q$y sq$p!~ 2 pamseacu aql30 uos! E -xedwo3 aq$ 111013 ‘Aa EP 07 dn SBSSBUI q!p~ sou!l$nau .K?IKW papnlaxa sluar.u!ladxa 6x7 2 I I .I I ..,.
Recommended publications
  • Arxiv:2001.07837V2 [Hep-Ex] 4 Jul 2020 Scale Funding Will Be Requested at Different Stages Across the Globe
    Brazilian Participation in the Next-Generation Collider Experiments W. L. Aldá Júniora C. A. Bernardesb D. De Jesus Damiãoa M. Donadellic D. E. Martinsd G. Gil da Silveirae;a C. Henself H. Malbouissona A. Massafferrif E. M. da Costaa C. Mora Herreraa I. Nastevad M. Rangeld P. Rebello Telesa T. R. F. P. Tomeib A. Vilela Pereiraa aDepartamento de Física Nuclear e Altas Energias, Universidade do Estado do Rio de Janeiro (UERJ), Rua São Francisco Xavier, 524, CEP 20550-900, Rio de Janeiro, Brazil bUniversidade Estadual Paulista (Unesp), Núcleo de Computação Científica Rua Dr. Bento Teobaldo Ferraz, 271, 01140-070, Sao Paulo, Brazil cInstituto de Física, Universidade de São Paulo (USP), Rua do Matão, 1371, CEP 05508-090, São Paulo, Brazil dUniversidade Federal do Rio de Janeiro (UFRJ), Instituto de Física, Caixa Postal 68528, 21941-972 Rio de Janeiro, Brazil eInstituto de Física, Universidade Federal do Rio Grande do Sul , Av. Bento Gonçalves, 9550, CEP 91501-970, Caixa Postal 15051, Porto Alegre, Brazil f Centro Brasileiro de Pesquisas Físicas (CBPF), Rua Dr. Xavier Sigaud, 150, CEP 22290-180 Rio de Janeiro, RJ, Brazil E-mail: [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: This proposal concerns the participation of the Brazilian High-Energy Physics community in the next-generation collider experiments.
    [Show full text]
  • HERA Collisions CERN LHC Magnets
    The Gallex (gallium-based) solar neutrino experiment in the Gran Sasso underground Laboratory in Italy has seen evidence for neutrinos from the proton-proton fusion reaction deep inside the sun. A detailed report will be published in our next edition. again, with particles taken to 26.5 aperture models are also foreseen to GeV and initial evidence for electron- CERN test coil and collar assemblies and a proton collisions being seen. new conductor distribution will further Earlier this year, the big Zeus and LHC magnets improve multipole components. H1 detectors were moved into A number of other models and position to intercept the first HERA With test magnets for CERN's LHC prototypes are being built elsewhere collisions, and initial results from this proton-proton collider regularly including a twin-aperture model at new physics frontier are eagerly attaining field strengths which show the Japanese KEK Laboratory and awaited. that 10 Tesla is not forbidden terri­ another in the Netherlands (FOM-UT- tory, attention turns to why and NIHKEF). The latter will use niobium- where quenches happen. If 'training' tin conductor, reaching for an even can be reduced, superconducting higher field of 11.5 T. At KEK, a magnets become easier to commis­ single aperture configuration was sion. Tests have shown that successfully tested at 4.3 K, reaching quenches occur mainly at the ends of the short sample limit of the cable the LHC magnets. This should be (8 T) in three quenches. This magnet rectifiable, and models incorporating was then shipped to CERN for HERA collisions improvements will soon be reassem­ testing at the superfluid helium bled by the industrial suppliers.
    [Show full text]
  • The ATLAS Pixel Detector
    The ATLAS Pixel Detector Maurice Garcia-Sciveres Lawrence Berkeley National Laboratory DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 1 ATLAS Pixel Collaboration • ~100 collaborators • 17 institutions • 8 countries DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 2 The Large Hadron Colloder will be the world’s most powerful microscope Camera goes here p p 14TeV ~10-19m resolution but… ¾Need high intensity ¾At design intensity LHC beam has 330MJ stored energy Iron yoke ¾1% will blow up dipole ¾Driving factor in vertex detector design 2 beam pipes Channels for superconducting wire DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 3 ATLAS 45m DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 4 ATLAS Pixel Detector p p Along axis 80M pixels (2m2 active area) 1744 parallel modules covering 3 barrels + 6 disks 1.3 m DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 5 Top Quark Photo Zoom in x10 Zoom in again x10 Actual Top Quark Decay Recorded by the CDF experiment with a silicon strip detector DEC 9, 2005 SRI Workshop --- the ATLAS pixel detector --- M. Garcia-Sciveres 6 Hybrid pixel detectors in particle physics • Silicon strip detectors have been used in particle physics for some 20 years (and are here to stay). This is a type of hybrid imager with resolution in only 1 dimension. ISL detector of CDF experiment • A hybrid pixel detector is a conceptually trivial (but technically difficult) generalization of a strip detector to 2 dimensions.
    [Show full text]
  • Information for Guides
    DRAFT 27 February 2014 Information for guides for Underground Visits Document prepared by Gloria Corti 1. Introduction This document is intended to provide you with material on which you can base your discussion with the visitors, along with more detailed background information for those not familiar with LHCb. It is not be intended to provide a word-by-word account of what an ideal visit underground to LHCb (and Delphi) should contain, nor what you should say on the surface. Everyone is specialized in different fields and the best is to convey the key messages from a personal and enthusiastic angle, and react to the response from your group. The main idea while underground is to explain what the visitors can see, at each stopping point of the itinerary. Discussions of more abstract concepts such as particle physics, the Standard Model, etc, should be done on the surface, either before or after the visit underground. Guides at the Exhibit are also encouraged to explain the various detectors on display. Pages 1 to 2 may be useful to all guides, while 2 to 5 are mostly intended for underground guides. The rest gives some general background for the LHCb experiment and detector and on the DELPHI experiment. Some summary facts and numbers are listed at the end. 2. When you first meet the visitors The first thing you should do is to introduce yourself, then check they are all present and they wear closed shoes and don’t have big bags with them. You may have to wait before going underground and you can use this time and that on the lift going underground to give visitors some general information.
    [Show full text]
  • Jan/Feb 2015
    I NTERNATIONAL J OURNAL OF H IGH -E NERGY P HYSICS CERNCOURIER WELCOME V OLUME 5 5 N UMBER 1 J ANUARY /F EBRUARY 2 0 1 5 CERN Courier – digital edition Welcome to the digital edition of the January/February 2015 issue of CERN Courier. CMS and the The coming year at CERN will see the restart of the LHC for Run 2. As the meticulous preparations for running the machine at a new high energy near their end on all fronts, the LHC experiment collaborations continue LHC Run 1 legacy to glean as much new knowledge as possible from the Run 1 data. Other labs are also working towards a bright future, for example at TRIUMF in Canada, where a new flagship facility for research with rare isotopes is taking shape. To sign up to the new-issue alert, please visit: http://cerncourier.com/cws/sign-up. To subscribe to the magazine, the e-mail new-issue alert, please visit: http://cerncourier.com/cws/how-to-subscribe. TRIUMF TRIBUTE CERN & Canada’s new Emilio Picasso and research facility his enthusiasm SOCIETY EDITOR: CHRISTINE SUTTON, CERN for rare isotopes for physics The thinking behind DIGITAL EDITION CREATED BY JESSE KARJALAINEN/IOP PUBLISHING, UK p26 p19 a new foundation p50 CERNCOURIER www. V OLUME 5 5 N UMBER 1 J AARYN U /F EBRUARY 2 0 1 5 CERN Courier January/February 2015 Contents 4 COMPLETE SOLUTIONS Covering current developments in high-energy Which do you want to engage? physics and related fi elds worldwide CERN Courier is distributed to member-state governments, institutes and laboratories affi liated with CERN, and to their personnel.
    [Show full text]
  • Vertex Detector
    FACHBEREICH PHYSIK BERGISCHE UNIVERSITAT¨ GESAMTHOCHSCHULE WUPPERTAL Johann M. Heuser Construction, Operation and Application of the DELPHI Pixel Detector at LEP2 Dissertation zur Erlangung des Doktorgrades des Fachbereichs Naturwissenschaften I { Physik der Bergischen Universit¨at-Gesamthochschule Wuppertal WUB-DIS 99-1 Januar 1999 Kurzub¨ ersicht Die vorliegende Arbeit diskutiert das Projekt des DELPHI Pixeldetektors, die erste Anwendung eines hybriden Silizium-Pixeldetektors in einem Collider-Experiment. Der Pixeldetektor ist Teil des \Very Forward Tracker", einer der neuen und erweiterten Detektorkomponenten des DELPHI Experiments zur optimierten Spurrekonstruktion bei LEP2, der Hochenergieperiode von CERN's \Large Electron Positron"-Collider mit angestrebten e+e−{Schwerpunktenergien von bis zu 200 GeV. Der DELPHI Pixeldetektor wird in Pixeldetektor-Entwicklungen eingeordnet, die ge- genw¨artig bei CERN fur¨ die zukunftigen¨ Experimente am \Large Hadron Collider" durchgefuhrt¨ werden. Die physikalische Motivation fur¨ die Anwendung eines Pixel- detektors bei DELPHI wird dargestellt. Die Entwicklung und Konstruktion des Sili- ziumdetektors werden behandelt und Erfahrungen zusammengefaßt, die w¨ahrend der ersten drei Betriebsjahre gewonnen wurden. Die Leistungsf¨ahigkeit des Pixeldetektors und sein Beitrag zur Spurrekonstruktion in den Endkappen des DELPHI Experiments werden charakterisiert und diskutiert. Die Untersuchung der Produktion von W-Bosonen z¨ahlt zu den wichtigen physikali- schen Forschungszielen bei LEP2. Der Very Forward
    [Show full text]
  • Electroweak Measurements in Electron-Positron Collisions at W
    EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CERN-PH-EP/2013-022 arXiv:1302.3415 [hep-ex] February 14th, 2013 Electroweak Measurements in Electron-Positron Collisions at W-Boson-Pair Energies at LEP The ALEPH Collaboration The DELPHI Collaboration The L3 Collaboration The OPAL Collaboration 1 arXiv:1302.3415v4 [hep-ex] 19 Sep 2013 The LEP Electroweak Working Group Submitted to PHYSICS REPORTS February 14th, 2013 1 Web access at http://www.cern.ch/LEPEWWG Abstract Electroweak measurements performed with data taken at the electron-positron collider LEP at CERN from 1995 to 2000 are reported. The combined data set considered in this report 1 corresponds to a total luminosity of about 3 fb− collected by the four LEP experiments ALEPH, DELPHI, L3 and OPAL, at centre-of-mass energies ranging from 130 GeV to 209 GeV. Combining the published results of the four LEP experiments, the measurements include total and differential cross-sections in photon-pair, fermion-pair and four-fermion production, the latter resulting from both double-resonant WW and ZZ production as well as singly resonant production. Total and differential cross-sections are measured precisely, providing a stringent test of the Standard Model at centre-of-mass energies never explored before in electron-positron collisions. Final-state interaction effects in four-fermion production, such as those arising from colour reconnection and Bose-Einstein correlations between the two W decay systems arising in WW production, are searched for and upper limits on the strength of possible effects are obtained. The data are used to determine fundamental properties of the W boson and the electroweak theory.
    [Show full text]
  • The Collaboration in Photos
    LHCb the collaboration in photos 3 Foreword 5 1 45 4 The experiment Operation 7 The Large Hadron Collider 46 Piloting the experiment 7 LHCb 50 Taking data 9 Looking for new particles 52 Storage solutions 54 Reconstructing the particle puzzle 11 2 Turning ideas into reality 12 The LHCb cavern 57 5 The adventure begins 13 The big build 58 Starting up the Large Hadron Collider 15 An efficient operation 60 First high energy collisions 62 A resounding success 63 The first beauty particle 17 3 Detective work The Vertex Locator 19 The Ring Imaging Cherenkov detectors 65 6 23 Your LHCb 66 Join the adventure 27 The Magnet 67 Colliding ideas, advancing technology 31 The Trackers 68 An invitation to visit 35 The Calorimeters 70 Find out more 39 The Muon Detector The Beam-pipe 43 75 Credits 76 The LHCb collaboration 1 2 Foreword Flavour physics, or the study of relationships between different kinds of quarks, has an excellent track record for making discoveries. New physics has been deduced on several occasions by precise observations of the behaviour of known particles, before any direct measurements of the new phenomena, such as detection of a new particle. Already in 1992, several ideas were under discussion to explore flavour physics at CERN’s Large Hadron Collider. By 1995, these ideas had evolved into a design for a single fully-optimized detector: the LHCb experiment. It then took almost 15 years of effort by over 730 people from many universities and institutes across 15 countries, to complete the construction of LHCb.
    [Show full text]
  • Arxiv:1909.00679V1 [Physics.Hist-Ph] 2 Sep 2019 1Cresti M., Loria A
    Oral History Interview with Marcello Cresti by Alessandro De Angelis, August 2019 Born in Grosseto, 26 April 1928, Marcello Cresti graduated in Physics in 1950 at the University of Pisa by attending the Scuola Normale Superiore, and became professor of Experimental Physics in Padua in 1965. His research focused on the physics of cosmic rays and elementary particles. In 1951, working at the mountain observatory built by the Padua research group at Pian di Fedaia, close to the Marmolada mountain, at an altitude of 2000 m a.s.l., he developed and used a system of overlapping Wilson chambers that allowed an analysis of particles produced by cosmic rays. With this device, in collaboration with Arturo Loria and Guido Zago, he obtained results on the extended air showers of cosmic radiation and on the production of pions and strange particles.1 As other mountain observatories, the Fedaia Laboratory had an important role in establishing international collaborations with other cosmic ray groups in Europe. In 1955 he worked at the Max Planck Institute for Physics in G¨ottingen,directed by Werner Heisenberg, to analyze the data obtained, developing a technique for reconstructing events that used one of the first electronic computers, built in that Institute by Heinz Billing in the early 1950s. During his stay in G¨ottingen, he collaborated with Martin Deutschmann who brought to the Fedaia observatory a multiplate cloud chamber2 and also established a relationship with Klaus Gottstein, who later led the Max Planck cosmic ray group and with whom he later collaborated in Berkeley. In 1956/57 he worked at the UCRL (University of California Radiation Laboratory) in Berkeley under the direction of Luis W.
    [Show full text]
  • Autoreferat Presentation of Research Achievements Piotr Zalewski
    Attachment 2b to the Wniosek o wszcz eciepost epowania habilitacyjnego (Application for initiation of habilitation proceeding) (le: PZannex2bEngAutoref.pdf) Autoreferat Presentation of research achievements Piotr Zalewski National Centre for Nuclear Research High Energy Physics Department 00-681 Warszawa, ul. Ho»a 69, POLAND Warszawa, Korze«, July-August 2013 Table of contents Table of contents 1 1 Personal data 2 2 Education 2 3 Scientic biography 2 3.1 Towards Ph.D. and short after . .2 3.2 Searching for a new particles . .3 4 Presentation of the scientic achievement 6 4.1 Introduction . .6 4.2 Search for the Higgs bosons at the LEP and the LHC . .7 4.2.1 The nal result of searching for the Higgs boson of the SM at the LEP collider . .8 4.2.2 Search for the Higgs bosons beyond the SM using LEP 1 and LEP 2 data . .9 4.2.3 The discovery of a new particle during the search for the Higgs boson . 13 4.2.4 Study of the properties of the new particle . 15 4.2.5 Summary of the Higgs boson searches . 17 4.3 A use of the CMS muon system for a search for new particles . 18 4.3.1 PAC Trigger subsystem based on the RPC . 19 4.3.2 GhostBuster replicating PACT signals removal . 20 4.3.3 Time of ight measurement using Drift Tubes . 21 4.3.4 PAC comparator version sensitive to delayed particles . 24 4.3.5 Summary of the author participation in the development of the CMS muon system 26 4.4 Search for massive long-lived particles in the CMS experiment .
    [Show full text]
  • Reconstruction of B Hadron Decays at DELPHI
    Helsinki Institute of Physics Internal Report Series HIP-2006-1 Reconstruction of B Hadron Decays at DELPHI Laura Salmi Helsinki Institute of Physics P.O. BOX 64, FI-00014 University of Helsinki, Finland Dissertation for the degree of Doctor of Science in Technology to be presented with due permission of the Department of Engineering Physics and Mathematics, Helsinki University of Technology, for public examination and debate in Auditorium F1 at Helsinki University of Technology (Espoo, Finland) on the 24th of March, 2006, at 12 o’clock noon. Helsinki 2006 ISBN 952-10-1697-3 (printed) ISBN 952-10-1698-1 (PDF) ISSN 1455-0563 Helsinki 2006 Yliopistopaino Abstract This thesis describes three analyses related to heavy quarks. The analysis with the largest impact is the extraction of parameters of heavy quark decays using the lepton energy spectrum and the hadronic mass spec- trum in semileptonic B decays. The extraction of the parameters allows to test the framework used to theoretically describe the decay of heavy mesons, and more accurate knowledge of the parameter values results in greater accuracy in the determination of the element Vcb of the Cabibbo-Kobayashi-Maskawa (CKM) quark mixing matrix. The| determination| described in this thesis is important, since it is so far the only one where the full lepton energy spec- trum has been used. The other determinations are based on using only a part of the spectrum. The first extraction of the parameters in the kinetic mass scheme was based on the statistical moments of the lepton energy spectrum and hadronic mass spectrum measured using the data collected at delphi.
    [Show full text]
  • A “LHC Premium” for Early Career Researchers? Perceptions from Within
    A “LHC Premium” for Early Career Researchers? Perceptions from within Tiziano Camporesi1,Gelsomina Catalano2,3, Massimo Florio2, Francesco Giffoni3 1 CERN European Organization for Nuclear Research 2 Department of Economics, Management and Quantitative Methods, University of Milan 3 CSIL Centre for Industrial Studies This version: 04.07.2016 Abstract More than 36,000 students and post-docs will be involved in experiments at the Large Hadron Collider (LHC) until 2025. Do they expect that their learning experience will have an impact on their professional future? By drawing from earlier salary expectations literature, this paper proposes a framework aiming at explaining the professional expectations of early career researchers (ECR) at the LHC. The model is tested by data from a survey involving 318 current and former students (now employed in different jobs) at LHC. Results from different ordered logistic models suggest that experiential learning at LHC positively correlates with both current and former students’ salary expectations. At least two not mutually exclusive explanations underlie such a relationship. First, the training at LHC gives early career researchers valuable expertise, which in turn affects salary expectations; secondly, respondents recognise that the LHC research experience per se may act as signal in the labour market. Respondents put a price tag on their experience at LHC, a ‘salary premium’ ranging from 5% to 12% in terms of their future salaries compared with what they would have expected without such experience. Keywords: Research infrastructures, Cost-Benefit Analysis, Human Capital, Expectations, Salary Premium, Large Hadron Collider JEL Codes: C83, D31, D61, D81, I23, O32 Acknowledgments: An earlier version of this paper has been produced in the frame of the research project ‘Cost/Benefit Analysis in the Research, Development and Innovation Sector’ sponsored by the EIB University Research Sponsorship programme (EIBURS), whose financial support is gratefully acknowledged.
    [Show full text]