Tau Leptons New Measurements of the Tau Mass
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
People and Things
People and things On 15 April, Haim Harari of the Weizmann Institute, Israel, was guest speaker at a symposium to mark 20 years of accelerator operation at the Paul Scherrer Institute, Maurice Jacob's roving camera caught Murray Villigen, Switzerland. Gell Mann in a London pub with the manu (Photo Armin Muller) script of his book 'The Quark and the Jaguar'. 20 years of PSI In April the Swiss Paul Scherrer Institute celebrated 20 years of accelerator operations. Originally built for particle research, these facilities now extend over a wide spectrum of applications, from molecular structure to cancer therapy. Each year over 400 visiting researchers make use of PSI particle beams. Meetings An international symposium on strangeness and quark matter will be held from 1-5 September in Crete, covering 1. strangeness and quark- gluon plasma, 2. strangeness con LAPP, Annecy, well known authority French Academy of Sciences densation, 3. strange astrophysics, 4. on non-Abelian gauge theories, and strangelets, 5. dedicated instrumen Michel Davier, long-time specialist in tation for strangeness and quark Among the new corresponding electron-positron collision physics matter. Information from the Secre members of the French Academy of and former Director of the Orsay tariat, University of Athens, Physics Sciences (Academie des Sciences Linear Accelerator Laboratory. Other Dept., Nuclear & Particle Physics de Paris) are Raymond Stora of new members are Alain Aspect, Division, Panepistimioupolis, Greece- 15771 Athens, tel. (30-1)7247502, 7243362, 7243143, fax (30- 1)7235089, email gvassils ©atlas, uoa.ariadne-t.gr At a special colloquium held at CERN on 20 April to mark Carlo Rubbia's 60th birthday and the tenth anniversary of his Nobel Prize award with Simon van der Meer, left to right - Canadian TRIUMF Laboratory Director and former UA1 co-spokesman Alan Astbury, LHC Project Director Lyn Evans, Carlo Rubbia, Director General Chris Llewellyn Smith, and former UA 1 co-spokesman John Dowel I. -
Probing Light Gauge Bosons in Tau Neutrino Experiments
Probing Light Gauge Bosons in Tau Neutrino Experiments Felix Kling∗ SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA The tau neutrino is probably the least studied particle in the SM, with only a handful of interaction events being identified so far. This can in part be attributed to their small production rate in the SM, which occurs mainly through Ds meson decay. However, this also makes the tau neutrino flux measurement an interesting laboratory for additional new physics production modes. In this study, we investigate the possibility of tau neutrino production in the decay of light vector bosons. We consider four scenarios of anomaly-free U(1) gauge groups corresponding to the B−L, B−Lµ−2Lτ , B − Le − 2Lτ and B − 3Lτ numbers, analyze current constraints on their parameter spaces and explore the sensitivity of DONuT and as well as the future emulsion detector experiments FASERν, SND@LHC and SND@SHiP. We find that these experiments provide the leading direct constraints in parts of the parameter space, especially when the vector boson's mass is close to the mass of the ! meson. I. INTRODUCTION other neutrino flavors. This small SM production rate makes the tau neutrino flux measurement an interesting The standard model (SM) consist of 17 particles, out laboratory for additional beyond the SM (BSM) produc- tion modes. of which the tau neutrino ντ is the least experimentally constrained one. To detect the rare tau neutrino interac- One example of such new physics are light vector tions, an intense neutrino beam with a sufficiently large bosons V associated with additional gauge groups. -
Hadronic R Decays and QCD
FR0005562 LAL 99-78 December 1999 Hadronic r decays and QCD M. Davier Laboratoire de l'Accelerateur Lineaire IN2P3-CNRS et Universite de Paris-Sud, BP 34, F-91898 Orsay Cedex Invited talk given at the &h International Symposium on Heavy Flavour Physics University of Southampton, England, 25-29 July 1999 U.E.R Institut National de de Physique Nucleaire PUniversite Paris-Sud et de Physique des Particules 32/ 05 B.P. 34 ~ Bailment 200 - 91898 ORSAY CEDEX Gestion IH\S Doc. Enreg. I© .iU4/. N* TRN &&.O.O.OSS LAL 99-78 December 1999 Hadronic r decays and QCD Michel Davier Laboratoire de VAccel6rateur Lineaire IN2P3/CNRS et University de Paris-Sud 91898 Orsay, France E-mail: davierQlal.in2p3.fr ABSTRACT: Hadronic decays of the r lepton provide a clean source to study hadron dynamics in an energy regime dominated by resonances, with the interesting information captured in the spectral functions. Recent results on exclusive channels are reviewed. Inclusive spectral functions are the basis for QCD analyses, delivering an accurate determination of the strong coupling constant and quantitative information on nonperturbative contributions. Strange decays yield a determination of the strange quark mass. 1. Introduction Radiative corrections violate CVC, as contained in the SEW factor which is dominated by short- Hadrons produced in T decays are borne out of distance effects and thus expected to be essen- the charged weak current, i.e. out of the QCD tially final-state independent. vacuum. This property garantees that hadronic Hadronic r decays are then a clean probe of physics factorizes in these processes which are hadron dynamics in an interesting energy region then completely characterized for each decay chan- dominated by resonances. -
Prix Andr Lagarrigue 2010
2010 André Lagarrigue Prize Under the sponsorship of the French Physical Society (SFP) and on the occasion of the 50th birthday of the Orsay Linear Accelerator Laboratory (LAL) in 2006, a prestigious Prize, awarded every second year, was created in honor of Professor André Lagarrigue. Director of LAL from 1969 until his untimely death in 1975. André Lagarrigue discovered, together with an European team, the weak interaction neutral currents in 1973, a crucial step in establishing the present theory of particle physics. The André Lagarrigue Prize rewards a senior physicist who has lead a large experimental project including conceptual design and realisation of a complex apparatus and has extracted the best of it with a strong team spirit and has carried out his work in a French laboratory or in close collaboration with French teams. This prize is co-financed by CEA, CERN, Ecole Polytechnique, IN2P3, LAL and the University Paris Sud 11. The international jury of the Andre Lagarrigue Prize1 met under the chairmanship of IN2P3 director Jacques Martino, and reviewed the nominees proposed by the French community of particles physics following a call for proposal sent to all French lab directors. The winner of the 2010 Andre Lagarrigue Prize is Michel Davier, Professor of Physics at the University Paris Sud 11 and a member of the French Academy of Science. Michel Davier's worldwide authority in the field of particle physics is undisputed and his prominent role is in every way worthy of that of André Lagarrigue. They share the same qualities of deep understanding of physics and of experimental devices of great complexity, of tenacity and pedagogy with the same passion for training young people. -
PDF Version for Printing
Friday, Jan. 30, 2009 Calendar Feature From ISGTW Friday, Jan. 30 ANL, Fermilab and UChicago Beauty to unlock the mystery of 3:30 p.m. come together for fifth meeting asymmetry DIRECTOR'S COFFEE BREAK - 2nd Flr X-Over In an ongoing effort to keep Illinois a science 4:00 p.m. powerhouse, Fermilab, Argonne and Joint Experimental-Theoretical University of Chicago scientists continue to Physics Seminar - One West look for future collaborative opportunities. Speaker: Michel Davier, LAL, More than 70 scientists from the three Orsay institutions will meet Monday at Argonne for + - → Title: BaBar Results on e e the fifth joint meeting organized to to share π+ π- and the Muon g-2 ideas about future projects and institutions' Prediction strategic plans. Monday, Feb. 2 The meetings, started in 2006 by Fermilab and 2:30 p.m. Argonne, initially focused on accelerator R&D. Particle Astrophysics Seminar While this is still a large focus of the - Curia II collaboration, particularly in regards to Project Speaker: Leanne Duffy, Los X, a series of research grants provided by the Alamos National Laboratory University of Chicago has led to joint projects Title: Phase-Space Structure in other research areas as well. of the Milky Way's Dark Halo The LHCb electomagnetic calorimeter, a device to 3:30 p.m. Proposals for joint projects include the detect electrons, their antiparticles (called DIRECTOR'S COFFEE production of better superconducting cavities, positrons) and photons, particles of light. This BREAK - 2nd Flr X-Over detector R&D, work on the LHC experiments immense array will collect immense amounts of 4 p.m. -
Dstau: Study of Tau Neutrino Production with 400 Gev Protons from the CERN-SPS
Prepared for submission to JHEP DsTau: Study of tau neutrino production with 400 GeV protons from the CERN-SPS Shigeki Aoki,a Akitaka Ariga,b;1 Tomoko Ariga,b;c Sergey Dmitrievsky,d Elena Firu,e Dean Forshaw,b Tsutomu Fukuda,f Yuri Gornushkin,d Ali Murat Guler,g Maria Haiduc,e Koichi Kodama,h Masahiro Komatsu,f Muhtesem Akif Korkmaz,g Umut Kose,i Madalina Miloi,e Antonio Miucci,b Motoaki Miyanishi,f Mitsuhiro Nakamura,f Toshiyuki Nakano,f Alina Neagu,e Hiroki Rokujo,f Osamu Sato,f Elizaveta Sitnikova,d Yosuke Suzuki,f Tomoki Takao,f Svetlana Vasina,d Mykhailo Vladymyrov,b Thomas Weston,b Junya Yoshida,j Masahiro Yoshimoto.k The DsTau Collaboration aKobe University, Kobe, Japan bAlbert Einstein Center for Fundamental Physics, Laboratory for High Energy Physics, University of Bern, Bern, Switzerland cKyushu University, Fukuoka, Japan dJoint Institute for Nuclear Research, Dubna, Russia eInstitute of Space Science, Bucharest, Romania f Nagoya University, Nagoya, Japan gMiddle East Technical University, Ankara, Turkey hAichi University of Education, Kariya, Japan iCERN, Geneva, Switzerland jAdvanced Science Research Center, Japan Atomic Energy Agency, Tokai, Japan kGifu University, Gifu, Japan E-mail: [email protected] Abstract: In the DsTau experiment at the CERN SPS, an independent and direct way to measure tau neutrino production following high energy proton interactions was proposed. As the main source of tau neutrinos is a decay of Ds mesons, produced in proton-nucleus arXiv:1906.03487v1 [hep-ex] 8 Jun 2019 interactions, the project aims at measuring a differential cross section of this reaction. The experimental method is based on a use of high resolution emulsion detectors for effective registration of events with short lived particle decays. -
Detection of the Tau-Neutrino at The
DETECTION OF THE TAIPNEIITRINO AT me LI·IC* Klaus Winter CERN. Geneva. Switzerland I. Introduction Following the discovery of the tau-lepton in e+e` collisions by M. Perl and collabo rators [1 ], all evidence today favours the hypothesis that it is a sequential heavy lepton belonging to a third lepton Family [2]. From measurements of the forward-bacl< ward angular asymmetry of tau produced in e+e` annihilations [3], [4] e+e* +* ft a value of the axial-vector neutral current coupling constant of ga = — 0.—l5 1 0.05 was deduced in agreement with ga = -1 /2 for the assignment of lel’t—handed tau leptons as the "down" state (I3 = -1 /2) of a weak isospin doublet. Hence, the most natural assignment of the "up" state (I3 = +1/2) would be to a neutrino with the same lepton flavour. the tau-neutrino. Further indirect evidence about the tau—neutrino can be obtained from leptonic tau decays [4]. e.g. 1:- Q u_v,,X. The muon energy spectrum has the familiar [2] Michel shape suggesting that the par ticle X is a spin l /2 particle. Its mass has been constrained to less than 35 MeV by analysing semi-leptonic tau—deca)s with multipion final states [5]. Hence, the particle Xmay be a neutrino. Is it a sequential neutrino, with a flavour property which distin guishes it from the electron- and the muon-neutrino? The possibility of a complete identity with we or uu can indeed be excluded. Searches for charged current neutrino reactions which produce a tau-lepton UN ·=* T_X have given negative results. -
Neutrino Physics
0 Neutrino Physics Zhi-zhong Xing ★ Neutrino’s history & lepton families (IHEP, Beijing) ★ Dirac & Majorana neutrino masses ★ Lepton flavor mixing & CP violation ★ Neutrino oscillation phenomenology ★ Seesaw & leptogenesis mechanisms ★ Extreme corners in the neutrino sky Lecture A @ the 2nd Asia-Europe-Pacific School of HEP, 11/2014, Puri, India Neutrinos everywhere 1 SM Properties: charge = 0 spin = ½ mass = 0 Big Bang speed = c neutrinos Galaxy Human Supernova Sun Earth Reactor Accelerator Neutrinos: witness and participant 1 in the evolution of the Universe 3 2 < 1% Some open questions 3 . the absolute mass scale? . the mass hierarchy? . the flavor desert? . leptonic CP violation? . the Majorana nature? . How many species? . cosmic background? . supernova & stellar ’s? . UHE cosmic ’s? . warm dark matter? . matter-antimatter asymmetry… Lecture A1 ★ Neutrinos from new physics ★ Interactions and discoveries ★ Flavors / families of leptons Beta decays in 1930 5 2-body Energy crisis = New physics ? decays J. Chadwick 1914/C. Ellis 1920-1927 What to do? Two ways out? 6 . giving up sth . adding in sth Niels Bohr Wolfgang Pauli (1930) Pauli put forward this idea in a letter instead of a paper….. Solvay 1933 7 Pauli gave a talk on his neutrino proposal in this congress. Fermi’s theory 8 Enrico Fermi assumed a new force for I will be remembered decay by combining 3 new concepts: for this paper. ------ Fermi in Italian ★ Pauli’s idea: neutrinos Alps, Christmas 1933 ★ Dirac’s idea: creation of particles ★ Heisenberg’s idea: isospin symmetry Fermi’s paper 9 This is Fermi’s best theoretical work! ---- C.N. Yang Published first in this journal and later in Z. -
Masses of the Sub-Nuclear Particles Fit Into One Equation
Masses of the Sub-Nuclear Particles Theodore M. Lach The masses of the quarks and leptons are for the most part a mystery to particle physicists. Currently there seems to be no correlation between the masses of the elementary particles. This paper is an attempt to formulate a theory that would begin to explain the relationship between the sub-nuclear particle masses. A key premise of the Standard Model is that there are 3 and only 3 generations of quarks and leptons. The currently accepted masses of these elementary particles are: (1) Table 1. Generation # 1 Generation # 2 Generation # 3 Up quark = 3 MeV, (1-5) Charmed quark = 1.25+0.1 GeV Top quark = 175 +5 GeV Down quark = 6 MeV Strange quark = 100 MeV Bottom quark = 4.2 GeV (3-9 MeV) (75-170 MeV) + 0.2 GeV Electron = 0.5109989MeV Muon = 105.6583 MeV Tau = 1777.1 MeV The neutrino masses in the standard model are still a hotly debated issue, yet arXiv:nucl-th/0008026 14 Aug 2000 most current references put the upper bound of the three neutrinos at: Table 2. Electron neutrino = 10 ev (5 – 17 ev) Muon neutrino = 270 KeV (200 – 270 KeV) Tau neutrino = 31 MeV (20 – 35 MeV) In an attempt to determine why the quark masses predicted in the CBM (2), Checker Board Model of the nucleus, do not fit into the standard model, I will deviate from the S.M. and assume that my quark masses in table 3 are correct and that there are more than 3 generations. -
The Tau and Beyond: Future Research on Heavy Leptons*
SLAC-PUB-4819 January 1988 Pm) THE TAU AND BEYOND: FUTURE RESEARCH ON HEAVY LEPTONS* MARTIN L. PERL Stanford Linear Accelerator Center Stanford University, Stanford, California 94309 . ABSTRACT: This paper outlines directions for future experimental research on the tau and tau neutrino. Present limits on the existence of heavier charged leptons are re- viewed, with emphasis on the close-mass lepton pair con- cept. *Work supported by the Department of Energy, contract DE-AC03-76SF00515. Presented at the 8th International Conference on Physics in Collision, Capri, Italy, October 19-21, 1988. Table of Contents I. Introduction II. The Tau A. The Decay Mode Problem B. Better Measurements of Conventional Properties C. Tau Lepton Number Conservation D. Deviations From a Dirac Point Particle E. The Concept of Lepton-Specific Forces and the Tau III. The Tau Neutrino A. Tau Neutrino Mass B. Tau Neutrino Mixing C. Interactions of the Tau Neutrino D. Variations on the Tau Neutrino IV. Limits on the Existence of Heavier Charged Leptons A. Present Limits B. Future Searches for Charged Leptons I. Introduction In 1981, at the first Physics In Collision Conference, I reviewed the status of the tau and of the search for heavier leptons. Now, seven years later, I have the pleasure of presenting another such review. Those seven years demonstrate the perversity of nature, or more precisely, demonstrate the obstinacy of nature with respect to the desires and expectations of the physicist. By 1981 the tau was established and the particle physicist looked forward to the discovery of more and heavier leptons. Two new electron-positron colliders PETRA and PEP were in operation, and the CERN pp collider was under construction. -
Discoverers of the Neutrino and Tau Recognised
RESEARCH I NEWS Discoverers of the Neutrino the turn of two of the six leptons of today's and Tau Recognised particle physics, the electron-neutrino ve and the T lepton, tau, to acquire 'Nobelity'. Particles that Acq ui red 'hlobei ity' K V L Sarma Frederick Reines (University of California, Irvine), now 77,with Clyde L Cowan Jr. (who The 1995 Nobel Prize in Physics is shared by died in 1974) reported the first direct evidence the American physicists Frederick J Reines of the existence of the 'neutrino' in 1956. The and Martin L Perl for their pioneering experi neutrino is a tiny neutral particle hypoth mental contributions to 'lepton' physics. Lep esized by Wolfgang Pauli Jr. in 1930. Twenty tons, such as the electron, do not feel the five years later and with the invention of the nuclear force but only the electromagnetic nuclear reactor it was possible to verify its and the weak beta decay force. This year it is existence. This year's Nobel award in Physics is in recognition belong. A summary of the discoveries made in the of two landmark experiments in elementary par world of leptons is given in the table below. The ticle physics. One provided the confirmation of the third generation has now started getting Nobel neutrino, as envisaged by Pauli more than two prizes. It should be noted that v T still needs to be decades earlier. The second discovered the heavy identified experimentally land hence the question charged lepton "t which heralded the third, and marks in the last row of the table!. -
Recent Progress on Isospin Breaking Corrections and Their Impact on the Muon G −2 Value *
CPC(HEP & NP), 2010, 34(6): 1{6 Chinese Physics C Vol. 34, No. 6, Jun., 2010 Recent progress on isospin breaking corrections and their impact on the muon g −2 value * Gabriel L´opez Castro1) Departamento de F´ısica, Cinvestav, Apartado Postal 14-740, 07000 M´exico, D.F M´exico Abstract We describe some recent results on isospin breaking corrections which are of relevance for predictions had;LO of the leading order hadronic contribution to the muon anomalous magnetic moment aµ when using τ lepton data. When these corrections are applied to the new combined data on the ππ0 spectral function, the had;LO + − prediction for aµ based on τ lepton data gets closer to the one obtained using e e data. Key words isospin breaking, tau decays, muon magnetic moment, radiative corrections PACS 12.40.Bv, 13.35.Dx, 13.40.Em, 13.40.Ks 1 Introduction τ ππν predicted from e+e− data corrected by IB ! effects was underestimated by more than 4σ with re- Currently, the accuracy of the Standard Model spect to the average of direct measurements [4, 6]. prediction of the muon anomalous magnetic moment Given this `e+e− vs τ discrepancy'2), it is believed aµ = (g 2)=2 is limited by the uncertainties of that τ decay data does not provide at present a re- − had;LO hadronic contributions [1, 2]. The dominant term in liable determination of aµ (currently, other use- had;LO the leading order hadronic contribution aµ and ful contributions from τ decay data involve only the an important part of its associated uncertainty is pro- 2π and 4π channels [2]).