Measurement of Beauty & Charm Photoproduction at H1 using Inclusive Lifetime Tagging
|
|
- Tyler Franklin
- 7 years ago
- Views:
Transcription
1 Measurement of Beauty & Charm Photoroduction at H using Inclusive Lifetime Tagging Lars Finke Aril, 9th 005 Heavy Flavors Working Grou
2 Photoroduction of Beauty & Charm at HERA e g c, b g Relevant scales: m c,b :.5 (4.75) GeV Theory models: LO O (α s ) + Parton shower c,b T : Event selection:, t >, 8 GeV DGLAP evolution, incl. flavor excitation PYTHIA CCFM evolution CASCADE NLO O (α s ) calculations Heavy quarks: Multiscale roblem in QCD. FMNR (fixed order massive) Lars Finke, Hamburg University DIS 005 9/04/005 µ
3 Motivation Heavy quark roduction in e collisions at HERA: Sensitivity to roton and hoton structure. Parton dynamics of the hard scattering. Hard scale rovided by the heavy quark masses (m c, m b ). Factorisation and erturbative QCD (massive/massless). Aims of this analysis: First inclusive measurement of beauty & charm Dis at high t in hotoroduction. Inclusive lifetime tag Large statistics Large t ( t > m b ). Lars Finke, Hamburg University DIS 005 9/04/005 µ
4 Heavy Flavor Signal Extraction Use of recise tracking information available from H vertex detector Signed Imact Parameter: α < π/ DCA = + DCA α > π/ DCA α Jet DCA DCA = DCA. Vertex Jet α Tracks 5 4 B C UDS Sum. Vertex Track Track MC used for simulation of b, c and uds DCA [cm] Marked asymmetry for heavy quarks. Anti strangeness cut: DCA < mm (remove e.g. K 0 S ) Tracks B C UDS Sum Significance= DCA i σ(dca i ) Significance Lars Finke, Hamburg University DIS 005 9/04/005 µ
5 Lifetime Observables I Using significances of the two highest significance tracks, S and S y cm samle event Events 5 4 B C UDS Sum S S rim. vertex S Highest significance track for track events. x cm Events S B C UDS Sum S Significance of the nd highest significance track for > track events S Lars Finke, Hamburg University DIS 005 9/04/005 µ 4
6 Negative Subtraction Subtract negative bins in S & S from the ositive Entries Entries 400 B B C UDS Fit C UDS Fit S S Reduces sensitivity to resolution descrition of light quarks. Subtracted sectrum dominated by charm. Increasing beauty fraction at higher significances. Contribution from light quarks negligible. Fit scale factors for beauty, charm and uds from negative subtracted sectra (+ total number of events). S Lars Finke, Hamburg University DIS 005 9/04/005 µ 5
7 Integrated Cross Section Kinematic range: Q < GeV, 0.5 < y < 0.8, t > (8) GeV, 0.88 < η <. Beauty: σ(e eb bx ejjx) = 49 ± 8 ± b Charm: σ(e ec cx ejjx) = 694 ± 69 ± 97 b Dominating systematic error. Main contributions come from the track resolutions and model uncertainties. Fractions: Beauty (Charm) fraction tyically 7% ( 5%). Lars Finke, Hamburg University DIS 005 9/04/005 µ 6
8 Lifetime Observables II Alternative lifetime tag Jet Probability*: Use all selected tracks within the two leading s. Entries 5 4 B C Construct a robability P MIP (from the significances) that the s are comatible with the rimary vertex. UDS Fit Low (i.e. large negative logarithm) robabilities indicate secondary vertex. Fit fractions of beauty, charm and light quarks. (*follows ALEPH aer Phys. Lett. B (99) 55) log (P MIP ) Resulting cross sections are found to agree with the results obtained with S and S. Lars Finke, Hamburg University DIS 005 9/04/005 µ 7
9 Beauty & Charm in Photoroduction dσ/d t (e > ecc(bb)x > ejjx) H 99/00 e + data: Q 0, 0.5 < y < 0.8 t > (8) GeV, 0.88 < η <. [b/gev] dσ/d t BEAUTY dσ/d t (e >ebbx >ejjx) Pythia Pythia res. Cascade NLO QCD had Q < GeV, 0.5 < y < 0.8 t > (8) GeV 0.88 < η Jet <. [b/gev] dσ/d t CHARM dσ/d t (e >eccx >ejjx) Pythia Pythia res. Cascade NLO QCD had Q < GeV, 0.5 < y < 0.8 t > (8) GeV Jet 0.88 < η < t [GeV] LO + PS QCD Models: Good descrition of shae. NLO QCD (FMNR): Slightly higher (at low t ) t LO + PS QCD Models: Good descrition of shae and norm. NLO QCD (FMNR): Fits within uncertainties. [GeV] Lars Finke, Hamburg University DIS 005 9/04/005 µ 8
10 Beauty & Charm in Photoroduction dσ/dη (e > ecc(bb)x > ejjx) H 99/00 e + data: Q 0, 0.5 < y < 0.8 t > (8) GeV, 0.88 < η <. [b] dσ/dη BEAUTY Pythia Pythia res. Cascade NLO QCD had dσ/dη (e >ebbx >ejjx) [b] dσ/dη CHARM Pythia Pythia res. Cascade NLO QCD had dσ/dη (e >eccx >ejjx) Q < GeV, 0.5 < y < 0.8 t > (8) GeV Jet 0.88 < η <. Q < GeV, 0.5 < y < t > (8) GeV Jet 0.88 < η < η η LO + PS QCD Models & NLO QCD (FMNR): Main differences in forward region. LO + PS QCD Models: Good descrition of shae and norm. NLO QCD (FMNR): Fits within uncertainties. Lars Finke, Hamburg University DIS 005 9/04/005 µ 9
11 Beauty Contributions from Resolved Photons dσ/dx obs (e > ebbx > ejjx) H 99/00 e + data: Q 0, 0.5 < y < 0.8 t > (8) GeV, 0.88 < η <. [b] obs dσ/dx 4 BEAUTY Pythia Pythia res. Cascade NLO QCD NLO QCD had obs dσ/dx (e >ebbx >ejjx) resolved like excitation g x obs = P, (E P z ) P hadrons (E P z) obs x LO + PS QCD Models: PYTHIA shae okay but too low in normalisation. CASCADE too hard. NLO QCD (FMNR): Lower than data at low x obs. Significant resolved like comonent (x obs < 0.85). Lars Finke, Hamburg University DIS 005 9/04/005 µ
12 Charm Contributions from Resolved Photons dσ/dx obs (e > eccx > ejjx) H 99/00 e + data: Q 0, 0.5 < y < 0.8 t > (8) GeV, 0.88 < η <. [b] obs dσ/dx 4 CHARM Pythia Pythia res. Cascade NLO QCD NLO QCD had Q < GeV, 0.5 < y < 0.8 t > (8) GeV Jet 0.88 < η <. obs dσ/dx (e >eccx >ejjx) resolved like x obs = excitation P, (E P z ) P hadrons (E P z) g obs x Significant resolved like comonent (x obs < 0.85). LO + PS QCD Models: PYTHIA with large excitation comonent okay, but too low for high x obs. CASCADE too hard. NLO QCD (FMNR): Good agreement between Data and NLO QCD within (large) uncertainties! Lars Finke, Hamburg University DIS 005 9/04/005 µ
13 Conclusion Measurement of beauty & charm di cross sections in hotoroduction has been resented. H Silicon Vertex Detector 99/00 data. High t : Beauty (Charm) fraction 7% ( 5%) of total samle with x obs > In agreement with quark charge counting. Charm: Data in general agreement with NLO QCD rediction (within uncertainties). Resolved contributions somewhat underestimated by the NLO calculation. Beauty: Data somewhat higher than NLO QCD, PYTHIA and CASCADE. Shae well described. Main differences seen at low x obs and at lower t. Lars Finke, Hamburg University DIS 005 9/04/005 µ
14 Backu NLO Calculations FMNR: fixed order massive calculation: BGF and HO Calculations done in MS scheme using CT EQ5M, GRV -HO and m C =.5 GeV (m B = 4.75 GeV). µ r = m t = m q + t,q q µ beauty f = m t ; µ charm f = m t t weighted k t clustering algorithm used. Perturbative uncertainties estimated by variation of the scales µ r and µ f (/ ). Parameter uncertainties estimated by variation of the quark masses and the df (added quadratically). Parton to hadron level corrections done using PYTHIA. Total uncertainties: 0% for both, beauty and charm. Lars Finke, Hamburg University DIS 005 9/04/005 µ
Measurement of Neutralino Mass Differences with CMS in Dilepton Final States at the Benchmark Point LM9
Measurement of Neutralino Mass Differences with CMS in Dilepton Final States at the Benchmark Point LM9, Katja Klein, Lutz Feld, Niklas Mohr 1. Physikalisches Institut B RWTH Aachen Introduction Fast discovery
More informationH & II in Inclusive Jet Production
on behalf of the Collaboration Universität Hamburg, Institut für Experimentalphysik, Luruper Chaussee 49, 76 Hamburg, Germany E-mail: monica.turcato@desy.de A summary of the most recent results by the
More informationMeasurement of the Mass of the Top Quark in the l+ Jets Channel Using the Matrix Element Method
Measurement of the Mass of the Top Quark in the l+ Jets Channel Using the Matrix Element Method Carlos Garcia University of Rochester For the DØ Collaboration APS Meeting 2007 Outline Introduction Top
More informationJet Reconstruction in CMS using Charged Tracks only
Jet Reconstruction in CMS using Charged Tracks only Andreas Hinzmann for the CMS Collaboration JET2010 12 Aug 2010 Jet Reconstruction in CMS Calorimeter Jets clustered from calorimeter towers independent
More informationvariables to investigate Monte Carlo methods of t t production
Using the M 2 and variables to investigate Monte Carlo methods of t t production Caitlin Jones September 8, 25 Abstract In this project the behaviour of Monte Carlo simulations for the event t t! ` `+b
More informationCalorimetry in particle physics experiments
Calorimetry in particle physics experiments Unit n. 8 Calibration techniques Roberta Arcidiacono Lecture overview Introduction Hardware Calibration Test Beam Calibration In-situ Calibration (EM calorimeters)
More informationTop rediscovery at ATLAS and CMS
Top rediscovery at ATLAS and CMS on behalf of ATLAS and CMS collaborations CNRS/IN2P3 & UJF/ENSPG, LPSC, Grenoble, France E-mail: julien.donini@lpsc.in2p3.fr We describe the plans and strategies of the
More informationHow To Find The Higgs Boson
Dezső Horváth: Search for Higgs bosons Balaton Summer School, Balatongyörök, 07.07.2009 p. 1/25 Search for Higgs bosons Balaton Summer School, Balatongyörök, 07.07.2009 Dezső Horváth MTA KFKI Research
More informationSingle-Top Production at the Tevatron and the LHC: Results and Prospects
Single-Top Production at the Tevatron and the LHC: Results and Prospects Wolfgang Wagner Bergische Universität Wuppertal DESY Zeuthen, June 16, 2011 Content: 1) Introduction / History 2) Experimental Status
More informationSelected Results on Diffraction at HERA
Selected Results on Diffraction at HERA Grzegorz Gach Various Faces of QCD May 014 Grzegorz Gach Selected Results on Diffraction at HERA 1 HERA DESY, Hamburg 199-007 e/e + - p 7.5 GeV 80 GeV 90 GeV Ldt
More informationPoS(Kruger 2010)013. Setting of the ATLAS Jet Energy Scale. Michele Petteni Simon Fraser University E-mail: mpetteni@sfu.ca
Setting of the ALAS Energy Scale Simon Fraser University E-mail: mpetteni@sfu.ca he setting of the energy scale and its uncertainty in the ALAS detector is presented. After a brief introduction of the
More informationMeasurement of the Beauty Cross Section using the Semileptonic Decay into Electrons at HERA
Measurement of the Beauty Cross Section using the Semileptonic Decay into Electrons at HERA Dissertation zur Erlangung des Doktorgrades des Fachbereichs Physik der Universität Hamburg vorgelegt von Bengt
More informationPhenomeological Determination of the Orbital Angular Momentum
Phenomeological Determination of the Orbital Angular Momentum Gordon P. Ramsey Loyola University Chicago and Argonne National Lab Collaboration with Y. Binder & D. Sivers SPIN 2008, University of Virginia-Oct.
More informationFrom Jet Scaling to Jet Vetos
From Jet Scaling to Jet Vetos Heidelberg DESY, 2/202 LHC Higgs analyses Two problems for LHC Higgs analyses [talks Rauch, Englert] observe H b b decays [fat Higgs jets, Marcel s talk] 2 understand jet
More informationarxiv:hep-lat/9704002v1 6 Apr 1997
Quenched Hadron Spectrum and Decay Constants on the Lattice L. Giusti 1 Scuola Normale Superiore, P.zza dei Cavalieri 7 and INFN, Sezione di Pisa, 56100 Pisa, Italy. Abstract arxiv:hep-lat/9704002v1 6
More informationCMS Tracking Performance Results from early LHC Running
CMS Tracking Performance Results from early LHC Running CMS PAPER TRK-10-001 L. Spiegel, K. Stenson, M. Swartz 1 First Collisions Tracking Paper Provide description of tracker, tracking algorithm, and
More informationExtraction of Polarised Quark Distributions of the Nucleon from Deep Inelastic Scattering at the HERMES Experiment
Extraction of Polarised Quark Distributions of the Nucleon from Deep Inelastic Scattering at the HERMES Experiment Marc Beckmann FAKULTÄT FÜR PHYSIK ALBERT-LUDWIGS-UNIVERSITÄT FREIBURG Extraction of Polarised
More informationStudy of the B D* ℓ ν with the Partial Reconstruction Technique
Study of the B D* ℓ ν with the Partial Reconstruction Technique + University of Ferrara / INFN Ferrara Dottorato di Ricerca in Fisica Ciclo XVII Mirco Andreotti 4 March 25 Measurement of B(B D*ℓν) from
More informationResearch Management Plan (RMP) for the. STAR Heavy Flavor Tracker (HFT)
Research Management Plan (RMP) for the STAR Heavy Flavor Tracker (HFT) Version 4 March 31, 2009 1. Introduction This document describes the plans of a group of institutions within the STAR collaboration
More informationParticle Physics. Bryan Webber University of Cambridge. IMPRS, Munich. 19-23 November 2007
Monte Carlo Methods in Particle Physics University of Cambridge IMPRS, Munich 19-23 November 2007 See also ESW: QCD and Collider Physics, C.U.P. 1996 http://www.hep.phy.cam.ac.uk/theory/webber/qcdupdates.html
More informationTop-Quark Studies at CMS
Top-Quark Studies at CMS Tim Christiansen (CERN) on behalf of the CMS Collaboration ICHEP 2010, Paris 35th International Conference on High-Energy Physics tt 2 km 22 28 July 2010 Single-top 4 km New Physics
More informationATLAS NOTE ATLAS-CONF-2010-063. July 21, 2010. Search for top pair candidate events in ATLAS at s = 7 TeV. The ATLAS Collaboration.
ATLAS NOTE ATLAS-CONF-2010-063 July 21, 2010 Search for top pair candidate events in ATLAS at s = 7 TeV The ATLAS Collaboration Abstract A search is performed for events consistent with top quark pair
More informationJets energy calibration in ATLAS
Jets energy calibration in ATLAS V.Giangiobbe Università di Pisa INFN sezione di Pisa Supported by the ARTEMIS Research Training Network Workshop sui Monte Carlo, la Fisica e le Simulazioni a LHC V.Giangiobbe
More informationt th signal: theory status
t th signal: theory status M.V. Garzelli MTA - DE Particle Physics Research Group, Univ. Debrecen, Hungary e-mail: garzelli@to.infn.it LHC HXSWG Workshop CERN, June 12-13th, 2014 t th production at LHC
More informationPrecise measurements of the proton structure towards the new physics discoveries at the LHC
June 2015 Precise measurements of the proton structure towards the new physics discoveries at the LHC Voica Radescu Physikalisches Institut Heidelberg Early ideas Ideas for detecting quarks were formulated
More informationCMS Physics Analysis Summary
Available on the CERN CDS information server CMS PAS RK-10-002 CMS Physics Analysis Summary Contact: cms-pog-conveners-tracking@cern.ch 2010/07/20 Measurement of racking Efficiency he CMS Collaboration
More informationMacromodels of Packages Via Scattering Data and Complex Frequency Hopping
F. G. Canavero ½, I. A. Maio ½, P. Thoma ¾ Macromodels of Packages Via Scattering Data and Complex Frequency Hopping ½ Dept. Electronics, Politecnico di Torino, Italy ¾ CST, Darmstadt, Germany Introduction
More informationVertex and track reconstruction with the ALICE Inner Tracking System
Vertex and track reconstruction with the ALICE Inner Tracking System The 5th International Nordic "LHC and Beyond" Workshop St.Petersburg, 8-11 June 2010 Leonardo Milano Univ. & INFN, Torino for the ALICE
More informationarxiv:hep-ph/0310021v2 4 Oct 2003
Physics in Collision - Zeuthen, Germany, June 6-8, 003 arxiv:hep-ph/0300v 4 Oct 003 SEARCHES FOR NEW PARTICLES AT THE ENERGY FRONTIER AT THE TEVATRON Patrice VERDIER LAL, Université Paris-Sud, 9898 Orsay
More informationDiese Dissertation ist auf den Internetseiten der Hochschulbibliothek online verfügbar.
! "#%$'&)( *,+.-/. 24365 -.38795 :*,;=?( @A-B3DCE/ FHGI$.7J#)*K@A-B3DCE/:$ &LM-B3>:*ON,CQPDPD()$?PSR.=?-.7T39( $ &)( *VUW=?(.CX$ CQPSR.=BY[Z\(BP93]7^5 -_2QCQP`RB=_( $'ab(.r.=:$ CQPSR.=?( $dce#fr.=?psr.=:)2g(ihe-?r.=?(
More informationarxiv:hep-ph/9812492v1 24 Dec 1998
MPI-PhT/96-14(extended version) July 1996 A Note on QCD Corrections to A b FB using Thrust to arxiv:hep-ph/9812492v1 24 Dec 1998 determine the b-quark Direction Bodo Lampe Max Planck Institut für Physik
More informationCharged meson production - status and perspectives
Charged meson production - status and perspectives Tanja Horn π, K, etc. Known process GP D H H ~ E E ~ π, K, etc. INT09, Seattle, WA 14 Sept 2009 Tanja Horn, CUA Colloquium status and perspectives, INT
More informationarxiv:hep-ph/0310009v1 1 Oct 2003
arxiv:hep-ph/319v1 1 Oct 23 HADRONISATION AT LEP ELI BEN-HAIM Laboratoire de l Accélérateur Linéaire (L.A.L.), Université Paris-Sud, Bâtiment 2, BP 34, F-91898 Orsay cedex, France An overview of recent
More informationTheory versus Experiment. Prof. Jorgen D Hondt Vrije Universiteit Brussel jodhondt@vub.ac.be
Theory versus Experiment Prof. Jorgen D Hondt Vrije Universiteit Brussel jodhondt@vub.ac.be Theory versus Experiment Pag. 2 Dangerous cocktail!!! Pag. 3 The basics in these lectures Part1 : Theory meets
More informationCombining fixed order QCD calculation with the parton shower Monte Carlo new PV prescription for IR singularities
Combining fixed order QCD calculation with the parton shower Monte Carlo new PV prescription for IR singularities O. Gituliar, S. Jadach, A. Kusina, W. Płaczek, S. Sapeta, A. Siódmok, M. Skrzypek Partly
More informationHigh Energy Physics. Lecture 4 More kinematics and a picture show of particle collisions
High Energy Physics Lecture 4 More kinematics and a picture show of particle collisions 1 Recall from the previous lecture: the momentum of the scattered Particle in an elastic collision is given by p
More informationarxiv:1006.5339v1 [hep-ph] 28 Jun 2010
FR-PHENO-2010-021 arxiv:1006.5339v1 [hep-ph] 28 Jun 2010 NLO QCD corrections to 4 b-quark production University of Illinois at Urbana-Champaign, Urbana IL, 61801 USA E-mail: ngreiner@illinois.edu Alberto
More informationarxiv:1508.07811v1 [hep-ph] 31 Aug 2015
DESY 5-47 RAL-P-05-007 reating jet correlations in high pile-up at hadron colliders arxiv:508.078v [hep-ph] 3 Aug 05 F. Hautmann,, H. Jung, 3, 4 and H. Van Haevermaet 4 Rutherford Appleton Laboratory &
More informationImplications of CMS searches for the Constrained MSSM A Bayesian approach
Implications of CMS searches for the Constrained MSSM A Bayesian approach Małgorzata Kazana, Yue-Lin Sming Tsai On behalf of the BayesFITS group National Centre for Nuclear Research Warsaw, Poland BayesFITS,
More informationHighlights of Recent CMS Results. Dmytro Kovalskyi (UCSB)
Highlights of Recent CMS Results Dmytro Kovalskyi (UCSB) Introduction Number of CMS publication is over 0 already It is very hard to review all the recent results in one talk This talk concentrates on
More informationPart 4 fitting with energy loss and multiple scattering non gaussian uncertainties outliers
Part 4 fitting with energy loss and multiple scattering non gaussian uncertainties outliers material intersections to treat material effects in track fit, locate material 'intersections' along particle
More informationarxiv:nucl-ex/0507023v2 18 Jul 2005
Diffraction Dissociation - 50 Years later Sebastian N. White Brookhaven National Laboratory, Upton, N.Y. 11973, USA arxiv:nucl-ex/0507023v2 18 Jul 2005 Abstract. The field of Diffraction Dissociation,
More informationTracking/Vertexing/BeamSpot/b-tag Results from First Collisions (TRK-10-001)
Tracking/Vertexing/BeamSpot/b-tag Results from First Collisions (TRK-1-1) Yanyan Gao, Fermilab on behalf of Tracking-Btagging POGs 3 March 21 / CERN CMS General Weekly Meeting: GWM8 Contributors and Acknowledgement
More informationElectroweak effects in Higgs boson production
Electroweak effects in Higgs boson production Frank Petriello University of Wisconsin, Madison w/c. Anastasiou, R. Boughezal 0811.3458 w/ W. Y. Keung, WIP Outline Brief review of experiment, theory for
More informationMiddle East Technical University. Studying Selected Tools for HEP: CalcHEP
Middle East Technical University Department of Physics Advanced Selected Problems in Physics Studying Selected Tools for HEP: CalcHEP Author: Jack Yakup Araz Supervisor: Assoc. Prof Ismail Turan December
More informationGamma-rays from Dark Matter Mini-Spikes in Andromeda Galaxy M31. Mattia Fornasa Dipartimento di Fisica G. Galilei I.N.F.N. Padova
Gamma-rays from Dark Matter Mini-Spikes in Andromeda Galaxy M31 Mattia Fornasa Dipartimento di Fisica G. Galilei I.N.F.N. Padova based on astro-ph/0703757 by M. Fornasa, M. Taoso and G.Bertone Journal
More informationValidation of the MadAnalysis 5 implementation of ATLAS-SUSY-13-05
Validation of the MadAnalysis 5 implementation of ATLAS-SUSY-3-5 Guillaume Chalons (LPSC Grenoble) email: chalons@lpsc.in2p3.fr October 27, 24 Abstract In this note we summarise our validation of the ATLAS
More informationEffect Sizes Based on Means
CHAPTER 4 Effect Sizes Based on Means Introduction Raw (unstardized) mean difference D Stardized mean difference, d g Resonse ratios INTRODUCTION When the studies reort means stard deviations, the referred
More informationThe TOTEM experiment at the LHC: results and perspective
The TOTEM experiment at the LHC: results and perspective Edoardo Bossini Università degli studi di Siena and INFN-Pisa (on behalf of the TOTEM collaboration) Trieste, 24 Settembre 2013 OUTLINE: Detector
More informationarxiv:hep-ph/9607427v1 25 Jul 1996
DFTT 44/96 IFT-96-16 MPI-PhT/96-63 hep-ph/967427 arxiv:hep-ph/967427v1 25 Jul 1996 New proton polarized structure functions in charged current processes at HERA M. Anselmino, P. Gambino, J. Kalinowski,1
More informationDetectors in Nuclear and Particle Physics
Detectors in Nuclear and Particle Physics Prof. Dr. Johanna Stachel Deartment of Physics und Astronomy University of Heidelberg June 17, 2015 J. Stachel (Physics University Heidelberg) Detectorhysics June
More informationTheoretical Particle Physics FYTN04: Oral Exam Questions, version ht15
Theoretical Particle Physics FYTN04: Oral Exam Questions, version ht15 Examples of The questions are roughly ordered by chapter but are often connected across the different chapters. Ordering is as in
More informationOn the R and R, Ratios at the Five-Loop Level of Perturbative &CD* ABSTRACT
On the R R, Ratios at the Five-Loop Level of Perturbative &CD* SLAC-PUB-6370 October 1993 T/E MARK A. SAMUEL Department of Physics Oklahoma State University Stillwater, OK 74078 Stanford Linear Accelerator
More informationProbability of detecting compact binary coalescence with enhanced LIGO
Probability of detecting compact binary coalescence with enhanced LIGO Richard O Shaughnessy [V. Kalogera, K. Belczynski] GWDAW-12, December 13, 2007 Will we see a merger soon? Available predictions Isolated
More informationRecent developments in Electromagnetic Hadron Form Factors
Recent developments in Electromagnetic Hadron Form Factors (JOH7RPDVL*XVWDIVVRQ '$31,$63K16DFOD\ :KDW are Form Factors? :K\ to measure? +RZ to measure? :KDWLVQHZ" Consequences, Conclusions 6SRNHSHUVR QV
More information0.33 d down 1 1. 0.33 c charm + 2 3. 0 0 1.5 s strange 1 3. 0 0 0.5 t top + 2 3. 0 0 172 b bottom 1 3
Chapter 16 Constituent Quark Model Quarks are fundamental spin- 1 particles from which all hadrons are made up. Baryons consist of three quarks, whereas mesons consist of a quark and an anti-quark. There
More informationPinhole Optics. OBJECTIVES To study the formation of an image without use of a lens.
Pinhole Otics Science, at bottom, is really anti-intellectual. It always distrusts ure reason and demands the roduction of the objective fact. H. L. Mencken (1880-1956) OBJECTIVES To study the formation
More informationA new inclusive secondary vertex algorithm for b-jet tagging in ATLAS
Home Search Collections Journals About Contact us My IOPscience A new inclusive secondary vertex algorithm for b-jet tagging in This content has been downloaded from IOPscience. Please scroll down to see
More informationPrHEP JHW2002. Experiments on high energy reactions in the diffractive regime at LHC. 1. Introduction. Twenty-sixth Johns Hopkins Workshop
PROCEEDINGS Experiments on high energy reactions in the diffractive regime at LHC Helsinki Institute for Physics, c/o CERN, Route de Meyrin, CH-1211 Geneva 23, Switzerland E-mail: Stefan.Tapprogge@cern.ch
More informationMartino Margoni Universita` di Padova & INFN (on behalf of the BaBar Collaboration)
B Xs/d γ & B + - Xs/d l l Martino Margoni Universita` di Padova & INFN (on behalf of the BaBar Collaboration) Outlook: B Xs/d γ : Motivations Xsγ (Belle), Acp (Xs+d γ) (BaBar), Vtd/Vts (BaBar) Spectral
More informationInformation about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
More informationPhysik des Higgs Bosons. Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216
: Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216 1 Reminder 10.6.2014 Higgs couplings: 2 Reminder 10.6.2014 Higgs BF as a function of mh Higgs total
More informationPOSSIBL-E EXPERIMENTS ON THE 200-GeV ACCELERATOR. A. D. Krisch University of Michigan. R. Serber Columbia University.
FN-68 POSSIBL-E EXPERIMENTS ON THE 200-GeV ACCELERATOR A. D. Krisch University of Michigan R. Serber Columbia University August 23, 1967 We will describe a number of experiments that might be dcne on.,he
More informationFundamental parameters from future lattice calculations
Fundamental parameters from future lattice calculations Lattice QCD Executive Committee R. Brower, (Boston U.) N. Christ (Columbia U.), M. Creutz (BNL), P. Mackenzie (Fermilab), J. Negele (MIT), C. Rebbi
More informationReal Time Tracking with ATLAS Silicon Detectors and its Applications to Beauty Hadron Physics
Real Time Tracking with ATLAS Silicon Detectors and its Applications to Beauty Hadron Physics Carlo Schiavi Dottorato in Fisica - XVII Ciclo Outline The ATLAS Experiment The SiTrack Algorithm Application
More informationParton showering effects in central heavy-boson hadroproduction
Parton showering effects in central heavy-boson hadroproduction DOI: will be assigned M. Deak, A. Grebenyuk 2, F. Hautmann 3, H. Jung 2,4 and K. Kutak 2 IFT, University of Madrid 2 Deutsches Elektronen
More informationThe Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. D. J. Mangeol, U.
Available on CMS information server CMS NOTE 6/96 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH11 GENEVA 3, Switzerland July, 6 Search for χ decays to ττ and SUSY mass spectrum
More informationNara Women s University, Nara, Japan B.A. Honors in physics 2002 March 31 Thesis: Particle Production in Relativistic Heavy Ion Collisions
Maya SHIMOMURA Brookhaven National Laboratory, Upton, NY, 11973, U.S.A. PROFILE I am an experimentalist working for high-energy heavy ion at Iowa State University as a postdoctoral research associate.
More informationHow To Teach Physics At The Lhc
LHC discoveries and Particle Physics Concepts for Education Farid Ould- Saada, University of Oslo On behalf of IPPOG EPS- HEP, Vienna, 25.07.2015 A successful program LHC data are successfully deployed
More informationMasses in Atomic Units
Nuclear Composition - the forces binding protons and neutrons in the nucleus are much stronger (binding energy of MeV) than the forces binding electrons to the atom (binding energy of ev) - the constituents
More informationQuark Model. Quark Model
Quark odel Outline Hadrons Isosin Strangeness Quark odel Flavours u d s esons Pseudoscalar and vector mesons Baryons Deculet octet Hadron asses Sin-sin couling Heavy Quarks Charm bottom Heavy quark esons
More informationPHYSICS WITH LHC EARLY DATA
PHYSICS WITH LHC EARLY DATA ONE OF THE LAST PROPHETIC TALKS ON THIS SUBJECT HOPEFULLY We may have some two month of the Machine operation in 2008 LONG HISTORY... I will extensively use: Fabiola GIANOTTI
More informationThe Mainz LXe TPC MC simulations for a Compton scattering experiment
The Mainz LXe TPC MC simulations for a Compton scattering experiment Pierre Sissol Johannes Gutenberg Universität Mainz 12 November 2012 1 / 24 Outline 1 Dark Matter 2 Principle of a dual-phase LXe TPC
More informationBNL Contribution to ATLAS
BNL Contribution to ATLAS Software & Performance S. Rajagopalan April 17, 2007 DOE Review Outline Contributions to Core Software & Support Data Model Analysis Tools Event Data Management Distributed Software
More informationATLAS Test Beam Analysis in Stockholm: An Overview
ATLAS Test Beam Analysis in Stockholm: An Overview Elin Bergeås, Stockholm University Stand-alone test beam 2003 and before - test beam targeted at TileCal modules only Combined test beam 2004 - test beam
More informationThe Experimental H.E.P. Group of the. Outline
The Experimental H.E.P. Group of the Universidad Autónoma de Madrid a http://hepexp.ft.uam.es Luis Labarga Departamento de Física Teórica Universidad Autónoma de Madrid Dates and People Outline The ZEUS
More informationMeasurement of the t -Channel Single Top-Quark Production Cross-Section with the ATLAS Detector at s = 7 TeV
FACHBEREICH MAHEMAIK UND NAURWISSENSCHAFEN FACHGRUPPE PHYSIK BERGISCHE UNIVERSIÄ WUPPERAL Measurement of the t -Channel Single op-quark Production Cross-Section with the ALAS Detector at s = 7 ev Dissertation
More informationFCC 1309180800 JGU WBS_v0034.xlsm
1 Accelerators 1.1 Hadron injectors 1.1.1 Overall design parameters 1.1.1.1 Performance and gap of existing injector chain 1.1.1.2 Performance and gap of existing injector chain 1.1.1.3 Baseline parameters
More informationDetector-related. related software development in the HEPP project. Are Strandlie Gjøvik University College and University of Oslo
Detector-related related software development in the HEPP project Are Strandlie Gjøvik University College and University of Oslo Outline Introduction The ATLAS New Tracking project HEPP contributions Summary
More informationConsumer Price Index Dynamics in a Small Open Economy: A Structural Time Series Model for Luxembourg
Aka and Pieretii, International Journal of Alied Economics, 5(, March 2008, -3 Consumer Price Index Dynamics in a Small Oen Economy: A Structural Time Series Model for Luxembourg Bédia F. Aka * and P.
More informationManaging specific risk in property portfolios
Managing secific risk in roerty ortfolios Andrew Baum, PhD University of Reading, UK Peter Struemell OPC, London, UK Contact author: Andrew Baum Deartment of Real Estate and Planning University of Reading
More informationD. Rainwater and D. Zeppenfeld. Department of Physics, University of Wisconsin, Madison, WI 53706. K. Hagiwara
University of Wisconsin - Madison MADPH-98-1057 KEK-TH-589 August 1998 Searching for H ττ in weak boson fusion at the LHC D. Rainwater and D. Zeppenfeld Department of Physics, University of Wisconsin,
More informationWIMP dark matter and the isotropic radio signal Roberto A. Lineros R. Instituto de Física Corpuscular - CSIC/U. Valencia @Roberto_Lineros Outline Introduction Cosmic ray propagation Synchrotron emission
More informationStatus of ALICE activities within FKPPL LIA
Status of ALICE activities within FKPPL LIA 1 Development of the online monitoring software for the ALICE Muon Trigger And Suppression Study for Υ S A N G - U N A H N K O N K U K U N I V E R S I T Y S
More informationNeural networks in data analysis
ISAPP Summer Institute 2009 Neural networks in data analysis Michal Kreps ISAPP Summer Institute 2009 M. Kreps, KIT Neural networks in data analysis p. 1/38 Outline What are the neural networks 1 Basic
More informationIMPROVEMENT OF JET ENERGY RESOLUTION FOR SEGMENTED HCAL USING LAYER WEIGHTING TECHNIQUE
IMPROVEMEN OF JE ENERGY RESOLUION FOR SEGMENED HCAL USING LAYER WEIGHING ECHNIQUE V. Andreev 1, I. Golutvin 2, A. Nikitenko 3,V.Palichik 2 1 Lebedev Physical Institute, Moscow, Russia 2 Joint Institute
More informationPresenting limits of simplified dark matter models from collider searches in. 0 m DM planes and self-annihilation cross-sections.
Internal working document not intended for broader distribution Presenting limits of simplified dark matter models from collider searches in SD/SI m DM planes and self-annihilation cross-sections. Oliver
More informationScience+ Large Hadron Cancer & Frank Wurthwein Virus Hunting
Shared Computing Driving Discovery: From the Large Hadron Collider to Virus Hunting Frank Würthwein Professor of Physics University of California San Diego February 14th, 2015 The Science of the LHC The
More informationJUST THE MATHS UNIT NUMBER 1.8. ALGEBRA 8 (Polynomials) A.J.Hobson
JUST THE MATHS UNIT NUMBER 1.8 ALGEBRA 8 (Polynomials) by A.J.Hobson 1.8.1 The factor theorem 1.8.2 Application to quadratic and cubic expressions 1.8.3 Cubic equations 1.8.4 Long division of polynomials
More informationTHE RELATIONSHIP BETWEEN EMPLOYEE PERFORMANCE AND THEIR EFFICIENCY EVALUATION SYSTEM IN THE YOTH AND SPORT OFFICES IN NORTH WEST OF IRAN
THE RELATIONSHIP BETWEEN EMPLOYEE PERFORMANCE AND THEIR EFFICIENCY EVALUATION SYSTEM IN THE YOTH AND SPORT OFFICES IN NORTH WEST OF IRAN *Akbar Abdolhosenzadeh 1, Laya Mokhtari 2, Amineh Sahranavard Gargari
More informationProton tracking for medical imaging and dosimetry
Proton tracking for medical imaging and dosimetry J.Taylor, P.Allport, G.Casse For the PRaVDA Consortium 1 Background and motivation - What is the PRaVDA experiment? - Why are we using Monte Carlo? GEANT4
More informationPearson Physics Level 30 Unit VIII Atomic Physics: Chapter 17 Solutions
Pearson Physics Level 30 Unit VIII Atomic Physics: Chapter 17 Solutions Student Book page 831 Concept Check Since neutrons have no charge, they do not create ions when passing through the liquid in a bubble
More information1 Experiments (Brahms, PHENIX, and STAR)
1 Experiments (Brahms, PHENIX, and STAR) This section describes the three experiments capable of making spin measurements. 1.1 PHENIX RHIC has made great strides towards providing high luminosity beams
More informationLocal and Global Duality and the Determination of α(m Z )
MZ-TH/99-18, CLNS/99-1619, hep-ph/9905373, May 1999 Local and Global Duality and the Determination of α(m Z ) arxiv:hep-ph/9905373v1 17 May 1999 Stefan Groote Institut für Physik, Johannes-Gutenberg-Universität,
More informationCosmological Analysis of South Pole Telescope-detected Galaxy Clusters
Cosmological Analysis of South Pole Telescope-detected Galaxy Clusters March 24th Tijmen de Haan (McGill) - Moriond 2014 Photo credit: Keith Vanderlinde Outline The galaxy cluster sample Calibrating the
More informationRisultati recenti dell'esperimento CMS ad LHC e prospettive per il run a 14 TeV
Risultati recenti dell'esperimento CMS ad LHC e prospettive per il run a 14 TeV Luca Lista INFN Napoli 1 78 reconstructed vertices CMS experiment CMS recorded 5fb-1 at 7 TeV and 20 fb-1 at 8 TeV 2 Electroweak
More information17609: Continuous Data Protection Transforms the Game
17609: Continuous Data Protection Transforms the Game Wednesday, August 12, 2015: 8:30 AM-9:30 AM Southern Hemishere 5 (Walt Disney World Dolhin) Tony Negro - EMC Rebecca Levesque 21 st Century Software
More informationAppendix A. An Overview of Monte Carlo N-Particle Software
Appendix A. An Overview of Monte Carlo N-Particle Software A.1 MCNP Input File The input to MCNP is an ASCII file containing command lines called "cards". The cards provide a description of the situation
More informationSearch for Dark Matter at the LHC
Search for Dark Matter at the LHC Steven Lowette Vrije Universiteit Brussel - IIHE 19 November 2014 3rd CosPa Meeting Université de Liège Content Introduction Generic DM searches at the LHC Explicit DM
More informationCross section, Flux, Luminosity, Scattering Rates
Cross section, Flux, Luminosity, Scattering Rates Table of Contents Paul Avery (Andrey Korytov) Sep. 9, 013 1 Introduction... 1 Cross section, flux and scattering... 1 3 Scattering length λ and λ ρ...
More information