Search for RPV at the LHC with Razor Variables. Sung Bong Chun

Size: px
Start display at page:

Download "Search for RPV at the LHC with Razor Variables. Sung Bong Chun"

Transcription

1 Search for RPV at the LHC with Razor Variables Sung Bong Chun

2 Presentation Outline Introduction Background: SUSY? RPV? LHC? Razor Variables? Target Event Event Selection Criteria Bin Shape Ratio Charge Shape Ratio Conclusion Backup 2

3 Introduction - Background SUSY? Relates one elementary particle to another differing only in ½ unit of spin, its superpartner. RPV? R = 2S + 3B + L R-parity = (-1) R = 1 for SM, -1 for SUSY particles RPV: Decay of a superpartner to SM particles 3

4 Introduction - Background LHC? pp collider at CERN currently operating at CM energy level 8 TeV CMS? Compact Muon Solenoid A detector surrounded by muon chambers at LHC or the group using it as a chief experimental device CMS data and MC samples 4

5 Introduction - Background Razor Variables Formulae: 5

6 Introduction Target Event* RPV decay superpartner Involves 2 light quarks, 4 b-quarks, 2 neutrinos, and 2 leptons upon pair production of gluinos. *C. Csáki, Y. Grossman, and B. Heidenreich, Minimal flavor violation supersymmetry: A natural theory for r-parity violation, Phys. Rev. D., vol. 85, p , May

7 Event Selection Criteria Target Event: Involves 2 light quarks, 4 b-quarks, 2 neutrinos, and 2 leptons upon pair production of gluinos. Goal: To suppress SM background as much as possible, Except for SM decays resembling target decay chain, such as pair production and tt T1 tttt 7

8 Event Selection Criteria Target Event: Involves 2 light quarks, 4 b-quarks, 2 neutrinos, and 2 leptons upon pair production of gluinos. Primitive Selection Criteria: 1 reconstructed vertex 4 PFJets with p T > 30GeV & η < 3 1 b-jet Two leptons (muon or electron) 8

9 Primitive Selection (MuMu Channel, M R ) 9

10 Primitive Selection (MuMu Channel, R 2 ) 10

11 Event Selection Criteria Further Restrictions: Baseline cut in M R >100 GeV and R 2 > 0.05 Angular separation of jets from leptons R ( ) 2 ( ) Tighter b-jet ID in leading 4 jets Z-mass window veto m Z 10GeV M m 10GeV ll Z Veto 11

12 Primitive Selection (MuMu Channel, M R ) 12

13 M R, R 2 cut (MuMu Channel, M R ) 13

14 ΔR Isolation - (MuMu Channel, M R ) 14

15 Tighter b-jet ID - (MuMu Channel, M R ) 15

16 Z-mass window - (MuMu Channel, M R ) 16

17 Event Selection Criteria Event Selection Criteria Developed: 1 reconstructed vertex 4 PFJets separated from leptons by ΔR > 0.5 with p T > 30GeV & η < 3 1 b-jet in leading 4 jets with tighter b-jet ID Two leptons (muon or electron) M R > 100GeV, R 2 > 0.05 Veto on M M GeV ll z 10 17

18 Bin Shape Ratio In the absence of signal event, higher bins in b-jet multiplicity are contributed chiefly through migration of lower bin events due to b-jet misidentification SM MC samples, there s no signal event Shape ratio independent of Razor variables (in principle) 18

19 Bin Shape Ratio (MuMu Channel, M R ) 19

20 Bin Shape Ratio (MuMu Channel, M R ) 20

21 Charge Shape Ratio If background is correctly characterized as pair production, lepton charges will be opposite Same charge (SS) events are chiefly migrated events from opposite charge (OS) events, due to lepton charge mistagging tt 21

22 SS/OS Ratio (MuMu Channel, M R ) SS/OS = 116/6580(~1.8%) SS/OS = 19/4934(~0.38%) SS/OS = 9/2350(~0.38%) SS/OS = 2/386(~0.52%) SS/OS ratio is ~4 times higher in 1b bin in MuMu box 22

23 SS/OS Ratio (MuMu Channel, R 2 ) SS/OS = 116/6580(~1.8%) SS/OS = 19/4934(~0.38%) SS/OS = 9/2350(~0.38%) SS/OS = 2/386(~0.52%) 23

24 Conclusion Event Selection Criteria Developed: 1 reconstructed vertex 4 PFJets separated from leptons by ΔR > 0.5 with p T > 30GeV & η < 3 1 b-jet in leading 4 jets with tighter b-jet ID Two leptons (muon or electron) M R > 100GeV, R 2 > 0.05 Veto on Mll M z 10GeV 24

25 Conclusion Bin Shape Ratio Excess in lower bin in b-jet multiplicity at lower p T Current b-tagging algorithm shows efficiency dependent on p T Charge Shape Ratio Observed overall SS/OS ratio greater than known lepton charge mistagging probabilities Dependence on Razor variables 25

26 End of Presentation questions? comments? or any blame? 26

27 Backup Slides Razor Variables Details on Selection Criteria Event Selection All three dilepton channels (MuEle, MuMu, EleEle) Bin Shape Ratio Charge Shape Ratio 27

28 1. Razor Variables Razor Variables Estimates CM rest mass of a reconstructed vertex when Missing Transverse Energy (MET) is involved. Razor frame is the longitudinally boosted frame in which two visible jets have equal magnitude of momenta. When more than two jets are visible in the final state, megajets are construced by summing all jets in hemispheres. The choice of partition is such that the sum of the rest mass of the two megajets are minimized 28

29 1. Razor Variables Razor Variables Formulae: 29

30 2. Details on Criteria Dilepton channel assignment 1 Muon, 1 Electron MuEle channel 2 Muon, no Electron MuMu channel 2 Electron, no Muon EleEle channel b-jet multiplicity bin determination Exclusive, hierarchical assignment of channels 2 loose, 1 medium, 1 tight b-jets bin# = 4 1 loose, 1 medium, 1 tight b-jets bin# = 3 1 medium, 1 tight b-jets bin# = 2 1 tight b-jets bin# =1 Exclusive, hierarchical assignment of bin#s 30

31 3. Event Selection Plots for All 3 Dilepton Channels 31

32 Primitive Selection (MuEle Channel, M R ) 32

33 Primitive Selection (MuEle Channel, R 2 ) 33

34 M R, R 2 cut (MuEle Channel, M R ) 34

35 M R, R 2 cut (MuEle Channel, R 2 ) 35

36 ΔR Isolation (MuEle Channel, M R ) 36

37 ΔR Isolation (MuEle Channel, R 2 ) 37

38 Tighter b-jet ID (MuEle Channel, M R ) 38

39 Tighter b-jet ID (MuEle Channel, R 2 ) 39

40 Z-mass window (MuEle Channel, M R ) 40

41 Z-mass window (MuEle Channel, R 2 ) 41

42 Primitive Selection (MuMu Channel, M R ) 42

43 Primitive Selection (MuMu Channel, R 2 ) 43

44 M R, R 2 cut (MuMu Channel, M R ) 44

45 M R, R 2 cut (MuMu Channel, R 2 ) 45

46 ΔR Isolation (MuMu Channel, M R ) 46

47 ΔR Isolation (MuMu Channel, R 2 ) 47

48 Tighter b-jet ID (MuMu Channel, M R ) 48

49 Tighter b-jet ID (MuMu Channel, R 2 ) 49

50 Z-mass window (MuMu Channel, M R ) 50

51 Z-mass window (MuMu Channel, R 2 ) 51

52 Primitive Selection (EleEle Channel, M R ) 52

53 Primitive Selection (EleEle Channel, R 2 ) 53

54 M R, R 2 cut (EleEle Channel, M R ) 54

55 M R, R 2 cut (EleEle Channel, R 2 ) 55

56 ΔR Isolation (EleEle Channel, M R ) 56

57 ΔR Isolation (EleEle Channel, R 2 ) 57

58 Tighter b-jet ID (EleEle Channel, M R ) 58

59 Tighter b-jet ID (EleEle Channel, R 2 ) 59

60 Z-mass window (EleEle Channel, M R ) 60

61 Z-mass window (EleEle Channel, R 2 ) 61

62 4. Bin Shape Ratio Plot (MuEle Channel) 62

63 4. Bin Shape Ratio Plot (MuMu Channel) 63

64 4. Bin Shape Ratio Plot (EleEle Channel) 64

65 5. SS/OS Ratio Plot (MuEle Channel, M R ) 65

66 5. SS/OS Ratio Plot (MuEle Channel, R 2 ) 66

67 5. SS/OS Ratio Plot (MuMu Channel, M R ) 67

68 5. SS/OS Ratio Plot (MuMu Channel, R 2 ) 68

69 5. SS/OS Ratio Plot (EleEle Channel, M R ) 69

70 5. SS/OS Ratio Plot (EleEle Channel, R 2 ) 70

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 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 information

Top-Quark Studies at CMS

Top-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 information

Top rediscovery at ATLAS and CMS

Top 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 information

variables to investigate Monte Carlo methods of t t production

variables 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 information

How To Teach Physics At The Lhc

How 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 information

Highlights of Recent CMS Results. Dmytro Kovalskyi (UCSB)

Highlights 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 information

Measurement 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 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 information

Single-Top Production at the Tevatron and the LHC: Results and Prospects

Single-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 information

Real 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 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 information

Implications of CMS searches for the Constrained MSSM A Bayesian approach

Implications 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 information

Progress in understanding quarkonium polarization measurements

Progress in understanding quarkonium polarization measurements 1 Progress in understanding quarkonium polarization measurements 1. Why it is essential that we approach the measurement of polarization as a multidimensional problem: we must not average out information!.

More information

PHYSICS WITH LHC EARLY DATA

PHYSICS 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 information

ATLAS 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. 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 information

CMS Physics Analysis Summary

CMS 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 information

Theoretical Particle Physics FYTN04: Oral Exam Questions, version ht15

Theoretical 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 information

Selected Topics in Elementary Particle Physics ( Haupt-Seminar )

Selected Topics in Elementary Particle Physics ( Haupt-Seminar ) Selected Topics in Elementary Particle Physics ( Haupt-Seminar ) Paola Avella, Veronika Chobanova, Luigi Li Gioi, Christian Kiesling, Hans-Günther Moser, Martin Ritter, Pit Vanhoefer Time: Do, 12 ct -14

More information

High 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 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 information

Risultati 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 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 information

Calorimetry in particle physics experiments

Calorimetry 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 information

Open access to data and analysis tools from the CMS experiment at the LHC

Open access to data and analysis tools from the CMS experiment at the LHC Open access to data and analysis tools from the CMS experiment at the LHC Thomas McCauley (for the CMS Collaboration and QuarkNet) University of Notre Dame, USA thomas.mccauley@cern.ch! 5 Feb 2015 Outline

More information

Single Top Production at the Tevatron

Single Top Production at the Tevatron Single Top Production at the Tevatron Daniel Wicke (Bergische Universität Wuppertal) Introduction Outline DØ Cross Section CDF Results DØ V tb Conclusions Revision : 1.7 DESY-Zeuthen, 21-Feb-2007 1 Introduction

More information

The TOTEM experiment at the LHC: results and perspective

The 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 information

Validation of the MadAnalysis 5 implementation of ATLAS-SUSY-13-05

Validation 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 information

Jet Reconstruction in CMS using Charged Tracks only

Jet 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 information

Status of ALICE activities within FKPPL LIA

Status 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 information

arxiv:hep-ph/0310021v2 4 Oct 2003

arxiv: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 information

How To Find The Higgs Boson

How 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 information

Study of the B D* ℓ ν with the Partial Reconstruction Technique

Study 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 information

Bounding the Higgs width at the LHC

Bounding the Higgs width at the LHC Bounding the Higgs width at the LHC Higgs XSWG workshop, June 2014 John Campbell, Fermilab with K. Ellis, C. Williams 1107.5569, 1311.3589, 1312.1628 Reminder of the method This is the essence of the original

More information

Track Trigger and Modules For the HLT

Track Trigger and Modules For the HLT CMS L1 Track Trigger for SLHC Anders Ryd for the CMS Track Trigger Task Force Vertex 2009 Sept. 13-18, 2009 L=1035 cm-2s-1 Outline: SLHC trigger challenge Tracking triggers Track trigger modules Simulation

More information

Measurements of single-top-quark production at the LHC

Measurements of single-top-quark production at the LHC IL NUOVO CIMENTO Vol. 35 C, N. 3 Maggio-Giugno 2012 DOI 10.1393/ncc/i2012-11226-5 Colloquia: TOP2011 Measurements of single-top-quark production at the LHC W. Wagner Bergische Universität Wuppertal - Germany

More information

Image Processing Techniques applied to Liquid Argon Time Projection Chamber(LArTPC) Data

Image Processing Techniques applied to Liquid Argon Time Projection Chamber(LArTPC) Data Image Processing Techniques applied to Liquid Argon Time Projection Chamber(LArTPC) Data Jessica Esquivel On Behalf of the MicroBooNE Collaboration Syracuse University Advisor: Mitch Soderberg Outline

More information

STRING THEORY: Past, Present, and Future

STRING THEORY: Past, Present, and Future STRING THEORY: Past, Present, and Future John H. Schwarz Simons Center March 25, 2014 1 OUTLINE I) Early History and Basic Concepts II) String Theory for Unification III) Superstring Revolutions IV) Remaining

More information

Search for Dark Matter at the LHC

Search 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 information

Jets energy calibration in ATLAS

Jets 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 information

Searching for Physics Beyond the Standard Model at GlueX

Searching for Physics Beyond the Standard Model at GlueX Searching for Physics Beyond the Standard Model at GlueX Justin Stevens & Mike Williams Department of Physics Massachusetts Institute of Technology GlueX Physics Meeting August 13 th, 2012 Mike Williams

More information

Science+ Large Hadron Cancer & Frank Wurthwein Virus Hunting

Science+ 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 information

Concepts in Theoretical Physics

Concepts in Theoretical Physics Concepts in Theoretical Physics Lecture 6: Particle Physics David Tong e 2 The Structure of Things 4πc 1 137 e d ν u Four fundamental particles Repeated twice! va, 9608085, 9902033 Four fundamental forces

More information

PoS(LHCPP2013)033. Rare B meson decays at LHC. Francesco Dettori Nikhef and Vrij Universiteit, Amsterdam E-mail: fdettori@nikhef.nl.

PoS(LHCPP2013)033. Rare B meson decays at LHC. Francesco Dettori Nikhef and Vrij Universiteit, Amsterdam E-mail: fdettori@nikhef.nl. Nikhef and Vrij Universiteit, Amsterdam E-mail: fdettori@nikhef.nl Paolo Iengo INFN Napoli E-mail: paolo.iengo@cern.ch Luca Martini INFN Pisa E-mail: Luca.Martini@cern.ch Rare decays of B mesons are fundamental

More information

FCC 1309180800 JGU WBS_v0034.xlsm

FCC 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 information

Physik des Higgs Bosons. Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216

Physik 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 information

Data analysis in Par,cle Physics

Data analysis in Par,cle Physics Data analysis in Par,cle Physics From data taking to discovery Tuesday, 13 August 2013 Lukasz Kreczko - Bristol IT MegaMeet 1 $ whoami Lukasz (Luke) Kreczko Par,cle Physicist Graduated in Physics from

More information

The Standard Model and the LHC! in the Higgs Boson Era Juan Rojo!

The Standard Model and the LHC! in the Higgs Boson Era Juan Rojo! The Standard Model and the LHC in the Higgs Boson Era Juan Rojo Saturday Mornings of Theoretical Physics Rudolf Peierls Center for Theoretical Physics Oxford, 07/02/2015 1 The Standard Model of Particle

More information

Betriebssystem-Virtualisierung auf einem Rechencluster am SCC mit heterogenem Anwendungsprofil

Betriebssystem-Virtualisierung auf einem Rechencluster am SCC mit heterogenem Anwendungsprofil Betriebssystem-Virtualisierung auf einem Rechencluster am SCC mit heterogenem Anwendungsprofil Volker Büge 1, Marcel Kunze 2, OIiver Oberst 1,2, Günter Quast 1, Armin Scheurer 1 1) Institut für Experimentelle

More information

A Guide to Detectors Particle Physics Masterclass. M. van Dijk

A Guide to Detectors Particle Physics Masterclass. M. van Dijk A Guide to Particle Physics Masterclass M. van Dijk 16/04/2013 How detectors work Scintillation Ionization Particle identification Tracking Calorimetry Data Analysis W & Z bosons 2 Reconstructing collisions

More information

The Mainz LXe TPC MC simulations for a Compton scattering experiment

The 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 information

Solutions to Problems in Goldstein, Classical Mechanics, Second Edition. Chapter 7

Solutions to Problems in Goldstein, Classical Mechanics, Second Edition. Chapter 7 Solutions to Problems in Goldstein, Classical Mechanics, Second Edition Homer Reid April 21, 2002 Chapter 7 Problem 7.2 Obtain the Lorentz transformation in which the velocity is at an infinitesimal angle

More information

arxiv:1508.07811v1 [hep-ph] 31 Aug 2015

arxiv: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 information

t th signal: theory status

t 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 information

A new inclusive secondary vertex algorithm for b-jet tagging in ATLAS

A 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 information

Electron-Muon Ranger (EMR)

Electron-Muon Ranger (EMR) Electron-Muon Ranger (EMR) Digitization and Reconstruction François Drielsma Ruslan Asfandiyarov University of Geneva On Behalf of the EMR Group 38 th MICE Collaboration Meeting February 23, 2014 Electron-Muon

More information

Gamma-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 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 information

Cross section, Flux, Luminosity, Scattering Rates

Cross 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

Low-energy point source searches with IceCube

Low-energy point source searches with IceCube EPJ Web of Conferences 116, 04004 (2016) DOI: 10.1051/epjconf/201611604004 C Owned by the authors, published by EDP Sciences, 2016 Low-energy point source searches with IceCube Sebastian Euler 1,a, David

More information

arxiv:hep-ph/9812492v1 24 Dec 1998

arxiv: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 information

The Standard Model of Particle Physics - II

The Standard Model of Particle Physics - II The Standard Model of Particle Physics II Lecture 4 Gauge Theory and Symmetries Quantum Chromodynamics Neutrinos Eram Rizvi Royal Institution London 6 th March 2012 Outline A Century of Particle Scattering

More information

Delphes, a framework for fast simulation of a general purpose LHC detector

Delphes, a framework for fast simulation of a general purpose LHC detector Delphes, a framework for fast simulation of a general purpose LHC detector S. Ovyn and X. Rouby Center for Particle Physics and Phenomenology (CP3) Université catholique de Louvain B-1348 Louvain-la-Neuve,

More information

THE TOP QUARK Updated September 2013 by T.M. Liss (Univ. Illinois), F. Maltoni (Univ. Catholique de Louvain), and A. Quadt (Univ. Göttingen).

THE TOP QUARK Updated September 2013 by T.M. Liss (Univ. Illinois), F. Maltoni (Univ. Catholique de Louvain), and A. Quadt (Univ. Göttingen). 1 THE TOP QUARK Updated September 2013 by T.M. Liss (Univ. Illinois), F. Maltoni (Univ. Catholique de Louvain), and A. Quadt (Univ. Göttingen). A. Introduction The top quark is the Q = 2/3, T 3 = +1/2

More information

Dirigido por: Susana Cabrera Urbán. Tesis Doctoral Junio 2014. Facultat de Física Departament de Física Atòmica Molecular i Nuclear

Dirigido por: Susana Cabrera Urbán. Tesis Doctoral Junio 2014. Facultat de Física Departament de Física Atòmica Molecular i Nuclear Measurement of the top quark pair production cross section in proton-proton collisions at center-of-mass energies of 7 TeV in final states with a τ lepton with the ATLAS detector María Teresa Pérez García-Estañ

More information

Event display for the International Linear Collider Summer student report

Event display for the International Linear Collider Summer student report Event display for the International Linear Collider Summer student report Stewart Martin-Haugh, supervisor Steve Aplin Physics Computing/IT September 10, 2009 1 Introduction The International Linear Collider

More information

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives Physics 9e/Cutnell correlated to the College Board AP Physics 1 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring

More information

PoS(Kruger 2010)013. Setting of the ATLAS Jet Energy Scale. Michele Petteni Simon Fraser University E-mail: mpetteni@sfu.ca

PoS(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 information

ATLAS NOTE ATLAS-CONF-2013-108. November 28, 2013. Evidence for Higgs Boson Decays to theτ + τ Final State with the ATLAS Detector

ATLAS NOTE ATLAS-CONF-2013-108. November 28, 2013. Evidence for Higgs Boson Decays to theτ + τ Final State with the ATLAS Detector ATLAS NOTE ATLAS-CONF-1-8 November 8, 1 Evidence for Higgs Boson Decays to theτ + τ Final State with the ATLAS Detector The ATLAS Collaboration Abstract ATLAS-CONF-1-8 8 November 1 A search for the Higgs

More information

CMS Computing Model: Notes for a discussion with Super-B

CMS Computing Model: Notes for a discussion with Super-B CMS Computing Model: Notes for a discussion with Super-B Claudio Grandi [ CMS Tier-1 sites coordinator - INFN-Bologna ] Daniele Bonacorsi [ CMS Facilities Ops coordinator - University of Bologna ] 1 Outline

More information

Vrije Universiteit Brussel. Faculteit Wetenschappen Departement Natuurkunde

Vrije Universiteit Brussel. Faculteit Wetenschappen Departement Natuurkunde Vrije Universiteit Brussel Faculteit Wetenschappen Departement Natuurkunde Measurement of the top quark pair production cross section at the LHC with the CMS experiment Michael Maes Promotor Prof. Dr.

More information

0.33 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

0.33 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 information

Rare decays in quark flavour physics

Rare decays in quark flavour physics Available online at www.sciencedirect.com Nuclear and Particle Physics Proceedings 73 75 (6) 5 59 www.elsevier.com/locate/nppp Rare decays in quark flavour physics Johannes Albrecht On behalf of the collaboration

More information

Study of Jet Substructure in the ATLAS Experiment using Distributed Analysis within Spanish Tier-2 Infrastructures

Study of Jet Substructure in the ATLAS Experiment using Distributed Analysis within Spanish Tier-2 Infrastructures Study of Jet Substructure in the ATLAS Experiment using Distributed Analysis within Spanish Tier-2 Infrastructures Elena Oliver García Dirigido por: José Francisco Salt Cairols and Santiago González de

More information

Directed by: Prof. Yuanning Gao, IHEP, Tsinghua University Prof. Aurelio Bay, LPHE, EPFL

Directed by: Prof. Yuanning Gao, IHEP, Tsinghua University Prof. Aurelio Bay, LPHE, EPFL Masters Thesis in High Energy Physics Directed by: Prof. Yuanning Gao, IHEP, Tsinghua University Prof. Aurelio Bay, LPHE, EPFL 1 Study for CP-violation in the ψ π + π J/ψ transition Vincent Fave July 18,

More information

Status Report of the Gerda Phase II Startup

Status Report of the Gerda Phase II Startup Status Report of the Gerda Phase II Startup Valerio D Andrea on behalf of the Gerda Collaboration Gran Sasso Science Institute (INFN), L Aquila ICNPA 2016 18th International Conference on Neutrino Physics

More information

Martino Margoni Universita` di Padova & INFN (on behalf of the BaBar Collaboration)

Martino 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 information

Middle East Technical University. Studying Selected Tools for HEP: CalcHEP

Middle 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 information

Vertex and track reconstruction with the ALICE Inner Tracking System

Vertex 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 information

ATLAS Test Beam Analysis in Stockholm: An Overview

ATLAS 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 information

Web-based pre-analysis Tools

Web-based pre-analysis Tools Summer Student Project Web-based pre-analysis Tools Student: Tetiana Moskalets V. N. Karazin Kharkiv National University Supervisors: Dr. Arturo Rodolfo Sanchez Pineda University of Naples Federico II

More information

BNL Contribution to ATLAS

BNL 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 information

NeuroBayes An advanced statistical tool for high energy physics and business

NeuroBayes An advanced statistical tool for high energy physics and business NeuroBayes An advanced statistical tool for high energy physics and business Prof. Dr. Michael Feindt CETA - Centrum für Elementarteilchen- und Astroteilchenphysik IEKP, Universität Karlsruhe Phi-T GmbH,

More information

Calibration of the muon momentum resolution in view of the W mass measurement with the CMS experiment

Calibration of the muon momentum resolution in view of the W mass measurement with the CMS experiment Calibration of the muon momentum resolution in view of the W mass measurement with the CMS experiment GIULIA RIPELLINO Master of Science Thesis Supervisor CERN: Luigi Rolandi Supervisor KTH: Jonas Strandberg

More information

Calorimeter Upgrades for the High Luminosity LHC

Calorimeter Upgrades for the High Luminosity LHC Calorimeter Upgrades for the High Luminosity LHC A. Straessner FSP 101 ATLAS DPG Frühjahrstagung Göttingen März, 2012 Outline Introduction: ATLAS and CMS Detectors Today Physics at the High-Luminosity

More information

D. Rainwater and D. Zeppenfeld. Department of Physics, University of Wisconsin, Madison, WI 53706. K. Hagiwara

D. 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 information

π 0 γγ calibration Savrina Daria, ITEP, Moscow SINP MSU, Moscow Victor Egorychev, ITEP, Moscow Ivan Belyaev

π 0 γγ calibration Savrina Daria, ITEP, Moscow SINP MSU, Moscow Victor Egorychev, ITEP, Moscow Ivan Belyaev π 0 γγ calibration Savrina Daria, ITEP, Moscow SINP MSU, Moscow Ivan Belyaev Victor Egorychev, ITEP, Moscow Loose cuts for π 0 selection One of the ways to improve the calibration procedure is to increase

More information

FTK the online Fast Tracker for the ATLAS upgrade

FTK the online Fast Tracker for the ATLAS upgrade FTK the online Fast Tracker for the ATLAS upgrade Kostas Kordas Aristotle University of Thessaloniki Annual EESFYE mtg, University of the Aegean, Chios, 25-29 April 2013 Overview ATLAS Trigger and DAQ

More information

The OPERA Emulsions. Jan Lenkeit. Hamburg Student Seminar, 12 June 2008. Institut für Experimentalphysik Forschungsgruppe Neutrinophysik

The OPERA Emulsions. Jan Lenkeit. Hamburg Student Seminar, 12 June 2008. Institut für Experimentalphysik Forschungsgruppe Neutrinophysik The OPERA Emulsions Jan Lenkeit Institut für Experimentalphysik Forschungsgruppe Neutrinophysik Hamburg Student Seminar, 12 June 2008 1/43 Outline The OPERA experiment Nuclear emulsions The OPERA emulsions

More information

Theory 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 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 information

Masses in Atomic Units

Masses 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 information

The Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. D. J. Mangeol, U.

The 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 information

Precise measurements of the proton structure towards the new physics discoveries at the LHC

Precise 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 information

FINDING SUPERSYMMETRY AT THE LHC

FINDING SUPERSYMMETRY AT THE LHC FINDING SUPERSYMMETRY AT THE LHC Tilman Plehn MPI München & University of Edinburgh TeV scale supersymmetry Signals at Tevatron and LHC Measurements at LHC SUSY parameters at LHC (and ILC) Tilman Plehn:

More information

Kísérleti eszközök fejlesztése a nagyenergiájú fizika számára. Development of experimental methods for the high-energy physics.

Kísérleti eszközök fejlesztése a nagyenergiájú fizika számára. Development of experimental methods for the high-energy physics. Kísérleti eszközök fejlesztése a nagyenergiájú fizika számára Töltött Higgs-bozon keresése a CERN-i L3 detektornál és precíziós helyzetmeghatározó-rendszer építése a CERN-i CMS detektor Müon rendszeréhez

More information

Weak Interactions: towards the Standard Model of Physics

Weak Interactions: towards the Standard Model of Physics Weak Interactions: towards the Standard Model of Physics Weak interactions From β-decay to Neutral currents Weak interactions: are very different world CP-violation: power of logics and audacity Some experimental

More information

Prof. Dr. Michael Feindt KCETA - Centrum für Elementarteilchen- und Astroteilchenphysik IEKP, Universität Karlsruhe, KIT Phi-T GmbH, Karlsruhe

Prof. Dr. Michael Feindt KCETA - Centrum für Elementarteilchen- und Astroteilchenphysik IEKP, Universität Karlsruhe, KIT Phi-T GmbH, Karlsruhe NeuroBayes et al.: professional methods for optimised reconstruction algorithms and statistical analysis Prof. Dr. Michael Feindt KCETA - Centrum für Elementarteilchen- und Astroteilchenphysik IEKP, Universität

More information

A SUSY SO(10) GUT with 2 Intermediate Scales

A SUSY SO(10) GUT with 2 Intermediate Scales A SUSY SO(10) GUT with 2 Intermediate Scales Manuel Drees Bonn University & Bethe Center for Theoretical Physics SUSY SO(10) p. 1/25 Contents 1 Motivation: SO(10), intermediate scales SUSY SO(10) p. 2/25

More information

Physics for the 21 st Century. Unit 1: The Basic Building Blocks of Matter. Bonnie Fleming and Mark Kruse

Physics for the 21 st Century. Unit 1: The Basic Building Blocks of Matter. Bonnie Fleming and Mark Kruse Physics for the 21 st Century Unit 1: The Basic Building Blocks of Matter Bonnie Fleming and Mark Kruse What are the basic building blocks that make up all matter? BONNIE FLEMING: The basic building blocks

More information

Introduction to Elementary Particle Physics. Note 01 Page 1 of 8. Natural Units

Introduction to Elementary Particle Physics. Note 01 Page 1 of 8. Natural Units Introduction to Elementary Particle Physics. Note 01 Page 1 of 8 Natural Units There are 4 primary SI units: three kinematical (meter, second, kilogram) and one electrical (Ampere 1 ) It is common in the

More information

Search for SUSY in Same-Sign Di-Lepton Events with the CMS Detector

Search for SUSY in Same-Sign Di-Lepton Events with the CMS Detector Search for SUSY in Same-Sign Di-Lepton Events with the CMS Detector Dissertation zur Erlangung des Doktorgrades des Department Physik der Universität Hamburg vorgelegt von Matthias Stein aus Göttingen

More information

How To Understand The Physics Of The Pp Collision At The Lhc

How To Understand The Physics Of The Pp Collision At The Lhc Study of supersymmetric signals with R-parity violation in ALAS at LHC Emma orró Pastor Dirigida por Vasiliki Mitsou y Salvador Martí i Garcia utor: José Ros Pallares Doctorado en Física Diciembre 22 Facultat

More information

Large Hadron Collider am CERN

Large Hadron Collider am CERN The CMS Silicon Tracker Lutz Feld 1. Physikalisches Institut, RWTH Aachen GSI Darmstadt, 18. 4. 2007 Large Hadron Collider am CERN proton proton quarks & gluons circumference 27 km 1200 superconducting

More information

Pearson Physics Level 30 Unit VIII Atomic Physics: Chapter 17 Solutions

Pearson 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 information

POSSIBL-E EXPERIMENTS ON THE 200-GeV ACCELERATOR. A. D. Krisch University of Michigan. R. Serber Columbia University.

POSSIBL-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 information

Hadro-Production Experiments: Impact on T2K and LBNE

Hadro-Production Experiments: Impact on T2K and LBNE Hadro-Production Experiments: Impact on T2K and LBNE Alysia Marino University of Colorado Boulder LBNE Scientific Workshop, Santa Fe, NM April 25-26, 24 2 Outline T2K Datasets used Flux prediction Flux

More information