Studying B S Γ at Babar Using a Fully Inclusive Method
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BABAR Studies Matter-Antimatter Asymmetry in Τ Lepton Decays
BABAR studies matter-antimatter asymmetry in τττ lepton decays Humans have wondered about the origin of matter since the dawn of history. Physicists address this age-old question by using particle accelerators to recreate the conditions that existed shortly after the Big Bang. At an accelerator, energy is converted into matter according to Einstein’s famous energy-mass relation, E = mc 2 , which offers an explanation for the origin of matter. However, matter is always created in conjunction with the same amount of antimatter. Therefore, the existence of matter – and no antimatter – in the universe indicates that there must be some difference, or asymmetry, between the properties of matter and antimatter. Since 1999, physicists from the BABAR experiment at SLAC National Accelerator Laboratory have been studying such asymmetries. Their results have solidified our understanding of the underlying micro-world theory known as the Standard Model. Despite its great success in correctly predicting the results of laboratory experiments, the Standard Model is not the ultimate theory. One indication for this is that the matter-antimatter asymmetry allowed by the Standard Model is about a billion times too small to account for the amount of matter seen in the universe. Therefore, a primary quest in particle physics is to search for hard evidence for “new physics”, evidence that will point the way to the more complete theory beyond the Standard Model. As part of this quest, BABAR physicists also search for cracks in the Standard Model. In particular, they study matter-antimatter asymmetries in processes where the Standard Model predicts that asymmetries should be very small or nonexistent. -
Reconstruction of Semileptonic K0 Decays at Babar
Reconstruction of Semileptonic K0 Decays at BaBar Henry Hinnefeld 2010 NSF/REU Program Physics Department, University of Notre Dame Advisor: Dr. John LoSecco Abstract The oscillations observed in a pion composed of a superposition of energy states can provide a valuable tool with which to examine recoiling particles produced along with the pion in a two body decay. By characterizing these oscillation in the D+ ! π+ K0 decay we develop a technique that can be applied to other similar decays. The neutral kaons produced in the D+ ! π+ K0 decay are generated in flavor eigenstates due to their production via the weak force. Kaon flavor eigenstates differ from kaon mass eigenstates so the K0 can be equally represented as a superposition of mass 0 0 eigenstates, labelled KS and KL. Conservation of energy and momentum require that the recoiling π also be in an entangled superposition of energy states. The K0 flavor can be determined by 0 measuring the lepton charge in a KL ! π l ν decay. A central difficulty with this method is the 0 accurate reconstruction of KLs in experimental data without the missing information carried off by the (undetected) neutrino. Using data generated at the Stanford Linear Accelerator (SLAC) and software created as part of the BaBar experiment I developed a set of kinematic, geometric, 0 and statistical filters that extract lists of KL candidates from experimental data. The cuts were first developed by examining simulated Monte Carlo data, and were later refined by examining 0 + − 0 trends in data from the KL ! π π π decay. -
A Successful Start to Preparations for the Babar Experiment
In June this year, the first part of new collider A successful called PEP-II was commissioned. It will be used in an experiment to observe a rare effect start to in particle physics that could explain why there appears to be only matter and not antimatter in the Universe. The effect is preparations called CP violation, and the experiment will measure for the first time subtle differences in for the BaBar the way fundamental particles called B mesons and their antiparticles decay. experiment According to theory, particles and their antimatter partners should behave like exact mirror images of each other. However, the B by Professor Mike Green mesons and their antiparticles are predicted Royal Holloway, University of London to break this mirror symmetry by a tiny amount. Extract taken from the PPARC Annual Report 1996-97 The so-called BaBar experiment (so named because the symbol for the anti-B meson is a letter 'B' with a bar across the top, and permission was obtained from the author of Babar the Elephant for the use of his name!) takes advantage of the 3-kilometre-long Stanford Linear Accelerator in California which creates and accelerates beams of electrons and their antiparticles, positrons. The beams are then injected into PEP-II. This consists of two concentric rings, 2 kilometres across, which will store the separate beams of electrons and positrons. In the rings, the beams travel close to the speed of light under the influence of electric and magnetic fields which accelerate, guide and focus the beams. The ring being used to store electrons was already in existence, and that is the one which has just been commissioned. -
Review of Lepton Universality Tests in B Decays
January 4, 2019 Review of Lepton Universality tests in B decays Simone Bifani∗, S´ebastienDescotes-Genony, Antonio Romero Vidalz, Marie-H´el`ene Schunex Abstract Several measurements of tree- and loop-level b-hadron decays performed in the recent years hint at a possible violation of Lepton Universality. This article presents an experimental and theoretical overview of the current status of the field. arXiv:1809.06229v2 [hep-ex] 3 Jan 2019 Published in Journal of Physics G: Nuclear and Particle Physics, Volume 46, Number 2 ∗University of Birmingham, School of Physics and Astronomy Edgbaston, Birmingham B15 2TT, United Kingdom yLaboratoire de Physique Th´eorique(UMR 8627), CNRS, Universit´eParis-Sud, Universit´eParis-Saclay, 91405 Orsay, France zInstituto Galego de F´ısicade Altas Enerx´ıas(IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain xLaboratoire de l'Acc´el´erateurLin´eaire,CNRS/IN2P3, Universit´eParis-Sud, Universit´eParis-Saclay, 91440 Orsay, France Contents 1 Introduction 1 2 Lepton Universality in the Standard Model 2 3 Overview of Lepton Universality tests beyond the B sector 3 3.1 Electroweak sector . .4 3.2 Decays of pseudoscalar mesons . .5 3.3 Purely leptonic decays . .7 3.4 Quarkonia decays . .7 3.5 Summary . .7 4 Theoretical treatment of b-quark decays probing Lepton Universality 8 4.1 Effective Hamiltonian . .8 4.2 Hadronic quantities . 10 4.3 Lepton Universality observables . 13 5 Experiments at the B-factories and at the Large Hadron Collider 13 5.1 B-factories . 13 5.2 Large Hadron Collider . 16 5.3 Complementarity between the B-factories and the LHC . -
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II on behalf of the U.S. Belle II Collaboration D. M. Asner1, Sw. Banerjee2, J. V. Bennett3, G. Bonvicini4, R. A. Briere5, T. E. Browder6, D. N. Brown2, C. Chen7, D. Cinabro4, J. Cochran7, L. M. Cremaldi3, A. Di Canto1, K. Flood6, B. G. Fulsom8, R. Godang9, W. W. Jacobs10, D. E. Jaffe1, K. Kinoshita11, R. Kroeger3, R. Kulasiri12, P. J. Laycock1, K. A. Nishimura6, T. K. Pedlar13, L. E. Piilonen14, S. Prell7, C. Rosenfeld15, D. A. Sanders3, V. Savinov16, A. J. Schwartz11, J. Strube8, D. J. Summers3, S. E. Vahsen6, G. S. Varner6, A. Vossen17, L. Wood8, and J. Yelton18 1Brookhaven National Laboratory, Upton, New York 11973 2University of Louisville, Louisville, Kentucky 40292 3University of Mississippi, University, Mississippi 38677 4Wayne State University, Detroit, Michigan 48202 5Carnegie Mellon University, Pittsburgh, Pennsylvania 15213 6University of Hawaii, Honolulu, Hawaii 96822 7Iowa State University, Ames, Iowa 50011 8Pacific Northwest National Laboratory, Richland, Washington 99352 9University of South Alabama, Mobile, Alabama 36688 10Indiana University, Bloomington, Indiana 47408 11University of Cincinnati, Cincinnati, Ohio 45221 12Kennesaw State University, Kennesaw, Georgia 30144 13Luther College, Decorah, Iowa 52101 14Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061 15University of South Carolina, Columbia, South Carolina 29208 16University of Pittsburgh, Pittsburgh, Pennsylvania 15260 17Duke University, Durham, North Carolina 27708 18University of Florida, Gainesville, Florida 32611 Corresponding Author: B. G. Fulsom (Pacific Northwest National Laboratory), [email protected] Thematic Area(s): (RF07) Hadron Spectroscopy 1 Abstract: The Belle II experiment at the SuperKEKB energy-asymmetric e+e− collider is a substantial upgrade of the B factory facility at KEK in Tsukuba, Japan. -
Detectors for Extreme Luminosity: Belle II
Nuclear Inst. and Methods in Physics Research, A 907 (2018) 46–59 Contents lists available at ScienceDirect Nuclear Inst. and Methods in Physics Research, A journal homepage: www.elsevier.com/locate/nima Detectors for extreme luminosity: Belle II I. Adachi a,b , T.E. Browder c, P. Kriºan d,e, *, S. Tanaka a,b , Y. Ushiroda a,b,f , (on behalf of the Belle II Collaboration) a High Energy Accelerator Research Organization (KEK), Tsukuba, Japan b SOKENDAI (The Graduate University for Advanced Studies), Hayama 240-0193, Japan c University of Hawaii, Honolulu, HI, United States d Faculty of Mathematics and Physics, University of Ljubljana, Slovenia e Joºef Stefan Institute, Ljubljana, Slovenia f Department of Physics, Graduate School of Science, University of Tokyo, Japan ARTICLEINFO ABSTRACT Keywords: We describe the Belle II detector at the SuperKEKB electron–positron accelerator. SuperKEKB operates at the Belle II energy of the 훶 .4S/ resonance where pairs of B mesons are produced in a coherent quantum mechanical state Super B Factory with no additional particles. Belle II, the first Super B factory detector, aims to achieve performance comparable SuperKEKB to the original Belle and BaBar B factory experiments, which first measured the large CP violating effects in the Magnetic spectrometer B meson system, with much higher luminosity collisions and larger beam-induced backgrounds. Flavor physics Contents 1. Introduction ..................................................................................................................................................................................................... -
The Babar Experiment at SLAC the Babar Detector Is Located at the PEP-II Electron-Positron Collider at the SLAC Laboratory in California
The BaBar Experiment at SLAC The BaBar detector is located at the PEP-II electron-positron collider at the SLAC laboratory in California. The BaBar collaboration is studying CP violation using B mesons. CP violation allows a difference between particles and antiparticles and hence is thought to explain the matter-antimatter asymmetry of the Universe. In 2001 BaBar made the world’s first observation of this phenomenon in B decays through the measurement of the parameter sin2β of the CKM matrix. The measurement of CP violation in sin2β is done by looking for a difference between B and anti-B meson decays. These can only be different if matter and antimatter are not exactly “equal- but-opposite” and this is one of the consequences of CP violation. The figure below shows the rate of B decays to a particular final state (here J/Ψ KS) compared to anti-B decays as a function of their lifetime. This shows a very clear difference between the two and was the first measurement to demonstrate “indirect” CP violation in B meson decays. The BaBar detector was completed and started data-taking in 1999. Since that time, it has recorded around 600 million B meson decays. The detector (shown above) consists of tracking, particle identification and calorimeter subdetectors. In particular, the novel particle identification device is based on observation of Cherenkov radiation from charged particles passing through quartz bars. The Cherenkov light is detected in the large prominent ring (above) at the end of the detector. BaBar has a wide physics programme other than CP violation, for example searches for new particles. -
A Measurement of Neutral B Meson Mixing Using Dilepton Events with the BABAR Detector
A measurement of neutral B meson mixing using dilepton events with the BABAR detector Naveen Jeevaka Wickramasinghe Gunawardane Imperial College, London A thesis submitted for the degree of Doctor of Philosophy of the University of London and the Diploma of Imperial College December, 2000 A measurement of neutral B meson mixing using dilepton events with the BABAR detector Naveen Gunawardane Blackett Laboratory Imperial College of Science, Technology and Medicine Prince Consort Road London SW7 2BW December, 2000 ABSTRACT This thesis reports on a measurement of the neutral B meson mixing parameter, ∆md, at the BABAR experiment and the work carried out on the electromagnetic calorimeter (EMC) data acquisition (DAQ) system and simulation software. The BABAR experiment, built at the Stanford Linear Accelerator Centre, uses the PEP-II asymmetric storage ring to make precise measurements in the B meson system. Due to the high beam crossing rates at PEP-II, the DAQ system employed by BABAR plays a very crucial role in the physics potential of the experiment. The inclusion of machine backgrounds noise is an important consideration within the simulation environment. The BABAR event mixing software written for this purpose have the functionality to mix both simulated and real detector backgrounds. Due to the high energy resolution expected from the EMC, a matched digital filter is used. The performance of the filter algorithms could be improved upon by means of a polynomial fit. Application of the fit resulted in a 4-40% improvement in the energy resolution and a 90% improvement in the timing resolution. A dilepton approach was used in the measurement of ∆md where the flavour of the B was tagged using the charge of the lepton. -
Front-End Electronic Readout System for the Belle II Imaging Time-Of- Propagation Detector
Front-end electronic readout system for the Belle II imaging Time-Of- Propagation detector Dmitri Kotchetkova, Oskar Hartbricha,*, Matthew Andrewa, Matthew Barretta,1, Martin Bessnera, Vishal Bhardwajb,2, Thomas Browdera, Julien Cercillieuxa, Ryan Conradc, Istvan Dankod, Shawn Dubeya, James Fastc, Bryan Fulsomc, Christopher Kettera, Brian Kirbya,3, Alyssa Loosb, Luca Macchiaruloa, Boštjan Mačeka,4, Kurtis Nishimuraa, Milind Purohitb, Carl Rosenfeldb, Ziru Sanga, Vladimir Savinovd, Gary Varnera, Gerard Vissere, Tobias Webera,5, Lynn Woodc a. Department of Physics and Astronomy, University of Hawaii at Manoa, 2505 Correa Road, Honolulu, HI 96822, USA b. Department of Physics and Astronomy, University of South Carolina, 712 Main Street, Columbia, SC 29208, USA c. Pacific Northwest National Laboratory, 902 Battelle Boulevard, Richland, WA 99354, USA d. Department of Physics and Astronomy, University of Pittsburgh, 3941 O’Hara Street, Pittsburgh, PA 15260, USA e. Center for Exploration of Energy and Matter, Indiana University, 2401 North Milo B. Sampson Lane, Bloomington, IN 47408, USA * Corresponding author. Phone: 1-808-956-4097. Fax: 1-808-956-2930 E-mail address: [email protected] 1Present address: Department of Physics and Astronomy, Wayne State University, 666 W Hancock St, Detroit, MI 48201, USA 2Present address: Indian Institute of Science Education and Research Mohali, Knowledge city, Sector 81, SAS Nagar, Manauli PO 140306, India 3Present address: Physics Department, Brookhaven National Laboratory, Upton, NY 11973, USA 4Present address: Department of Experimental Particle Physics, Jožef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, Slovenia 5Present address: Ruhr-Universität Bochum, 44780 Bochum, Germany Abstract The Time-Of-Propagation detector is a Cherenkov particle identification detector based on quartz radiator bars for the Belle II experiment at the SuperKEKB e+e– collider. -
Glueball Searches in Babar
' $ Glueball Searches in BaBar. Antimo Palano INFN and University of Bari, Italy Summary: • Introduction. • Experimental techniques. • The BaBar experiment. • Three body Dalitz plot analysis. • First experimental results. • Conclusions. & % 1 ' $ Introduction: Physics Motivations • New generation experiments, fixed target and B-factories, are accumulating high quality, large data samples on Beauty and Charm Physics. • Important information related to glueball searches can come from: • The Dalitz plot analysis of 3-body Charm and B decays. • The study of the process: b → sg • The Dalitz Plot Analysis of three-body decays is a relatively new powerful technique for studying Beauty and Charm Physics. • It is the most complete way of analyzing the data. • It allows to measure decay amplitudes and phases. • The final state is the result of the interference of all the intermediate states. & % 2 ' $ Introduction • One of the most important Motivations for continuing working on Light Meson Spectroscopy is the search for Glueballs and Exotic mesons. • From Lattice QCD, the lightest glueball, with J PC =0++ i s expected around 1.7 GeV. & % 3 ' $ • A variety of exotics is also expected below 2.5 GeV. Hybrids (¯qqg mesons) or 4-quark states. Some of them could be narrow enough to be detected. Some of them have quantum numbers forbidden for qq¯ mesons, such as: J PC =1−+,0−−, 0+−, etc. • The structure of the lowestqq ¯ multiplets is mostly still undefined and this prevents unique “exotic assignments” of gluonic candidates. • Strategy to find these states: they do not fit in the standard qq¯ nonet. They are extra states. • New inputs from heavy mesons decays could solve old and new puzzles in light meson spectroscopy. -
The Belle II Experiment: Status and Prospects
universe Article The Belle II Experiment: Status and Prospects Paolo Branchini † INFN Sezione di RomaTre Via Della Vasca Navale, 84, 00146 Roma, Italy; [email protected] † On behalf of the Belle II Collaboration. Received: 16 September 2018; Accepted: 29 September 2018; Published: 1 October2018 Abstract: The Belle II experiment is a substantial upgrade of the Belle detector and will operate at the SuperKEKBenergy-asymmetric e+e− collider. The accelerator has already successfully completed the first phase of commissioning in 2016. The first electron versus positron collisions in Belle II were delivered in April 2018. The design luminosity of SuperKEKB is 8 × 1035 cm−2 s−1, and the Belle II experiment aims to record 50 ab−1 of data, a factor of 50 more than the Belle experiment. This large dataset will be accumulated with low backgrounds and high trigger efficiencies in a clean e+e− environment. This contribution will review the detector upgrade, the achieved detector performance and the plans for the commissioning of Belle II. Keywords: flavor; dark matter 1. Introduction Even though the Standard Model (SM) is currently the best description of the subatomic world, it does not explain the complete picture. The theory incorporates only three out of the four fundamental forces, omitting gravity. Moreover, there are also important questions that it does not answer, such as the matter versus antimatter asymmetry in the number of quark and lepton generations. Many New Physics (NP) scenarios have been proposed. Experiments in high-energy physics search for NP using two complementary approaches. The first, at the energy frontier, is able to discover new particles directly produced in pp collisions (ATLAS, CMS). -
Extending the Full Event Interpretation to the Upsilon(5S) Resonance
ETP-KA/2020-06 Extending the Full Event Interpretation to the Υ(5S) Resonance Moritz Bauer Master’s thesis 29th February 2020 Institut für Experimentelle Teilchenphysik (ETP) Advisor: Prof. Dr. Günter Quast Coadvisor: Prof. Dr. Florian Bernlochner Editing time: 1st March 2019 – 29th February 2020 KIT – Universität des Landes Baden-Württemberg und nationales Forschungszentrum in der Helmholtz-Gemeinschaft www.kit.edu ETP-KA/2020-06 Erweiterung der Full Event Interpretation auf die Υ(5S)-Resonanz Moritz Bauer Masterarbeit 29. Februar 2020 Institut für Experimentelle Teilchenphysik (ETP) Referent: Prof. Dr. Günter Quast Korreferent: Prof. Dr. Florian Bernlochner Bearbeitungszeit: 1. März 2019 – 29. Februar 2020 KIT – Universität des Landes Baden-Württemberg und nationales Forschungszentrum in der Helmholtz-Gemeinschaft www.kit.edu Ich versichere wahrheitsgemäß, die Arbeit selbstständig angefertigt, alle benutzten Hilfsmittel vollständig und genau angegeben und alles kenntlich gemacht zu haben, was aus Arbeiten anderer unverändert oder mit Abänderungen entnommen wurde. Karlsruhe, 29. Februar 2020 ......................................... (Moritz Bauer) Contents 1. Introduction1 2. B Factories and the Belle Detector3 2.1. B Mesons and Υ Resonances..........................3 2.2. Belle Experiment.................................5 2.2.1. KEKB...................................5 2.2.2. Belle Detector...............................7 3. Methods and Algorithms 11 3.1. Software Setup.................................. 11 3.1.1. Belle II Analysis Software Framework and B2BII Conversion Package 11 3.2. B Meson Tagging at Belle and Belle II..................... 12 3.2.1. Method.................................. 12 3.2.2. Full Reconstruction............................ 14 3.2.3. Full Event Interpretation........................ 15 3.3. Variables Used for Particle Candidates Reconstructed by the FEI...... 19 4. Full Event Interpretation at Υ(5S) 25 0 4.1.