HERA - Structure of Matter and QCD
|
|
- Isaac Powell
- 5 years ago
- Views:
Transcription
1 HERA - Structur of Mattr and QCD p Contnts 5 yar running of HERA and H/ZEUS Elctrowak rsults Structur of th proton Katsuo Tokushuku (KEK, ZEUS)
2 DESY/HERA HERA 99-7 H ZEUS HERA: (7.5GV lctron 9GVproton) th world largst lctron microscop
3 Rsolution ~( Wavlngth) - ~ h Q ( ) Q - i f Rsolvd dimnsion [fm]. Ruthrford Hofstadtr SLAC p nucli proton partons [m] -6 Progrss in acclrator nabls us to invstigat th smallr structur. HERA: (7.5GV lctron(positron) vs. 9 GV proton). CERN μ,ν N Q ma=s=4e E p ~GV.. No sub-parton structur down to.67-8 m (HERA-I/II rsult, prlim.) HERA 9 95 THERA -9 Yar cf. in th rst fram s=e M p In ordr to obtain th sam CMS nrgy as HERA in a fid targt primnt, it ruirs 54TV lctron bam.
4 A viw of th HERA ring tunnl 4 Proton ring Tunnl Construction startd in 984 Elctron ring
5 Eprimnts startd in 99 5
6 6 HERA History (99-7) 5 yars yar brak HERA-I 99- HERA-II -7 HERA will stop at th nd of Jun in 7
7 Nutral Currnt (NC) Chargd Currnt (CC) 7 Scattrd positron Positron Proton Jt Scattrd positron Jt Anti-nutrino positron 7GV γ Z uark (u,d,s,c..) Proton 9GV positron 7GV W d,s-uark Proton 9GV Scattrd uark (jt) u,c-uark (jt)
8 Introduction: Dp Inlastic Scattring 8 p 9GV p p k 7.5GV k Dscribd by kinmatic variabls Q γ rmnant jt W currnt jt Q =- photon virtuality = Q /p. Bjorkn y = p./p.k Inlasticity s=q y Y±=(±(-y) ) F L : Longitudinal Str. Ft. ( in QPM) F : Small at Q << M z F = (,Q ) f f (,Q ) : f uark distribution function
9 pqcd viw of F PDF dpnds on Q F = (,Q ) f f 9 d DGLAP volution (Dokshitzr, Gribov, Lipatov, Altarlli, Parisi) df α s ( Q ) dy = g, ln Q π y [ ( ) ( ) + ( ) ( )] P y y, Q P y g y Q F Q largr: high- and g ar split into low and g. splitting function (known from pqcd) P ( y) y (y-) P g ( y ) y (y-) ~ (+)
10 Kinmatical rgion for HERA structur function masurmnts Q (GV ) 4 ZEUS ZEUS (Prliminary) ZEUS BPT 997 ZEUS SVX 995 ordr highr rgion in Q, ordr lowr rgion in Wid (O( 6 )) span in Q : Prcis masurmnts for Q volution NMC BCDMS CCFR E665 Kinmatic limit y= - y=
11 Prdictions of F Gluck, Rya and Vogt pqcd : parton volution Early HERA data showd rapid incras of F at low. Prcis F dtrmination ( data sampls) Donnachi & Landshoff Hadronic : Rgg thory bhavior of γp total cross sction Fid targt data
12 Rsults of F Structur Function Strong ris of F as dcrass Soft sa of uarks in th proton Slop of ris gts stpr as Q gos up HERA F Q =.7 GV.5 GV 4.5 GV 6.5 GV 8.5 GV GV GV 5 GV 8 GV GV 7 GV 5 GV Good agrmnt with fidtargt primnts at middl -high m F 45 GV 6 GV 7 GV 9 GV Sa + valnc uarks GV 5 GV - - ZEUS NLO QCD fit tot. rror H 96/97 ZEUS 96/97 BCDMS E665 NMC - -
13 F for fid, as a function of Q At low, strong scaling violation is sn. Larg gluon dnsity + g splitting F incrass P g ( y) y (y-) At ~., approimat scaling. At highr, F dcrass as Q Quark radiats off gluon: g P ( y) m F -log () 5 4 HERA F =6.E-5 =. =.6 =.5 =.4 =.5 =.6 =.8 =. =. =. =.5 ZEUS NLO QCD fit =.8 =. tot. rror =. H 94- prlim. H 96/97 ZEUS 96/97 BCDMS E665 NMC =. =.5 =.8 Lin = rsult of QCD fit (comming slids) All data points wll dscribd. y (y-) =. =.8 =.5 =.4 = Q (GV )
14 Kinmatical rgion for HERA structur function masurmnts 4 s=q y Q (GV ) 4 ZEUS ZEUS (Prliminary) ZEUS BPT 997 ZEUS SVX 995 ordr highr rgion in Q, ordr lowr rgion in Wid (O( 6 )) span in Q : Prcis masurmnts for Q volution NMC BCDMS CCFR E665 Kinmatic limit y= - y=
15 γ Z v,a v,a d σ [ ] [ ] + = = Z Z Z Z Q Q P a v a v P a a Q F Q Q P a v a v P v v Q F ), ( ), ( } 4 { ), ( ), ( ), ( } ) )( ( { ), ( + M Q Q sin = P Z w z θ parity - parity +, sin W I a I v = = θ In SM, 5 { } { } [ ] 4 ) ( ) ( F y F y Q ddq d p + = ± m πα σ W ν { } { } [ ] ) ( ) ( F y F y Q M M G ddq d W W F CC p + + = ± m π σ
16 Masurmnts of NC/CC Cross sctions 6 HERA-I Final Rsults At high Q (Q ~M W,Z ), Chargd Currnt Nutral Currnt dσ dq σ NC ~ σ CC α ( Q + M ) Echang α NC ~α CC Elctrowak unification Good agrmnt with th SM Mw = 8. ±.(stat)±.(syst)±.(pdf) GV (from ZEUS p data) NC( + p) < NC( - p) γz intrfrnc CC( + p)<cc( - p) u,d-uark distribution in th proton
17 Sachs of BSM 7 softr scattring If th uark is not point-lik λ SCALAR LEPTOQUARKS WITH F= ( S, L ) - - EXCLUDED H CI L indir. limit Prliminary ZEUS limit H dirct limit ( - p) D limit Ecss in data ( + p) M LQ (GV) p p LQ g LQ p λ LQ Good agrmnt with th SM Quark Radius<.67-6 cm (prlim.) No signal for Lptouarks so far
18 HERA I II 8 Longitudinal polarization of lpton bam : Dirct EW snsitivity Sokolov-Trnov ffct Lpton bam has transvrs polarization + Spin rotator bfor/aftr th H/ZEUS/HERMES dtctors. Polarization build-up at HERA Luminosity Upgrad : High-Q ruirs larg luminosity Final focusing magnts in th dtctor ~4% on avrag
19 Chargd Currnt Scattring ± σ CC (pb) σ CC 8 6 Chargd Currnt p Scattring - p νx H Data 5 (prl.) H Data ZEUS Data 4-5(prl.) ZEUS Data p νx H Data ZEUS Data Lft handd lctron lctron nutrino (lft handd) Proton 8GV d s-uark W(lft handd) u,c-uark (Jt) 9 4 SM (H PDF ) Right handd lctron nutrino Proton 8GV Q > 4 GV y < P lft handd right handd Right handd lctron d s-uark W(right handd) u,c-uark (Jt) σ R =.±.8±.6 pb (H and ZEUS combind prliminary rsult) -> W R mass limit ~ GV Th first masurmnt of Lft/Right asymmtry in CC in this nrgy rgion.
20 Polarizd Nutral Currnt Cross sction (d σ/ddq ) / (d σ m /ddq ) Vry subtl ffct from g-z intrfrnc -> H+ZEUS combind rsults a) Pol=7% - L - R + R + L A A ± P R - P L σ σ p R ± p R HERA H+ZEUS Combind (prl.) ± - σ + σ ± L L ± p p 4 5 Q (GV ) A + A - H PDF ZEUS-JETS PDF - 4 Q (GV )
21 Masurmnt of -Z coupling u-uark d-uark Polarizd data improvs th vctor couplings. HERA-II data maks a significant impact on th uark couplings
22 d σ ± p ddq γz F F ( = F (, Q ) σ πα 4 Q = [{ + ( y ) } F m { ( y ) } F ] { v v P + ( v + a )( v + a ) PZ }[ (, Q ) + (, Q )] (,Q ) F (,Q )/ a P Z 4v ava PZ }[ (, Q ) (, Q )] = a [ - ] γz Z - - σ + F p p, Q ) = { aapz + = Q P In SM, v sin z sin θ + = I θ W w Q MZ a = I HERA cf. νp: F : valnc uark H+ZEUS Combind (prl.) Q =5 GV Quark-charg wightd valnc uark distribution p :F : charg-suar wightd d γz F = { H PDF ZEUS-JETS PDF v v.65 F γz. d u +, d }d = 5 =. ±.9 ±.8 consistnt with QCD fit :.6 ±. - -
23 PDF dtrmination from HERA A fit (almost) clusivly with HERA data Jts cross sctions gluon γchang sa scaling violation gluon Q (GV ) H ZEUS sa, gluon Fid Targt Eprimnts: CCFR, NMC, BCDMS, E665, SLAC y= (HERA s= GV) valnc QCD + EW physics Z chang sa + valnc valnc only W ± chang u or d uark Fid targt primnts Standard fits (a la CTEQ, MRST ) us data from various (fidtargt and collidr) primnts. Why HERA only fits? Singl Eprimnt: Wll known systmatic uncrtaintis including corrlation. Proton Only: No nuclar ffcts. Still w nd following information High Q : No Highr twist from th othr primnts: Strang uark information Ubar-dbar asymmtry
24 ~ σ.5 Q = GV Q = 5 GV Q = 5 GV Q = 45 GV PDF dtrmination from HERA Q ZEUS NC: high Q = 65 GV Q = 8 GV Q = GV =6.E-5 Q = 5 GV =. HERA F A fit (almost) clusivly with HERA data m -log () =.6 ZEUS NLO QCD fit Jts =.5 sa, gluon valnc 5 tot. rror QCD + EW physics =.4 =.5 5 H =.6 H 94- prlim. cross Z chang =.8 4 ZEUS H 96/97 Q = GV Q = GV Q = 5 GV Q = 8 GV.8 Fid Targt Eprimnts: =. ZEUS 96/97.6 sctions sa + valnc CCFR, NMC, BCDMS,.4 BCDMS ZEUS E665, SLAC =. gluon E665 valnc only. 4 Q = 8 GV γchang =. NMC W ± Q = 5 GV Q = 95 GV Q chang = GV Q - - = GV Q = GV.6 ZEUS NC (prl.) = p (4.7 pb ) sa ~577 data points.5 u or d uark ZEUS-pol (prl.) =.8. P = +..5 scaling - Fid targt violation =..6 Q = 7 GV primnts Q = GV Q = 5 GV =..4 gluon -. CC: high Q = = df [.4 ( =.8 ) ( ). ( ) ( )] α s ( Q ) dy = Standard fits (a la CTEQ, MRST ) + P y y, Q Pg y g y, Q d ln Q us data from various (fidtargt and collidr) primnts. Why HERA only fits? Q = 7 GV π y =.. Q = 95 GV Q = GV F Q (GV ) Jt y= (HERA s= GV) =.5 Singl Eprimnt: Wll known systmatic uncrtaintis including corrlation. NC: low Q p (78.8 pb ).6 ZEUS-pol (prl.) =.4 P Proton Only: No nuclar ffcts. Still w nd following information = f() = p High Q =.65 : No Highr twist p (-) p (+p. from 5 ) th at othr Q primnts: =Q Strang uark information Ubar-dbar asymmtry σ ~.5 =.8 Q (GV ) DGLAP uation ZEUS CC (prl.) 4
25 PDFs obtaind from th fits Gluon uncrtainty 5 ~GV As sn in th F ris at low-, many sa uarks. Gluons ar dominant at low- Gluon dnsity is dtrmind at ~ 5% lvl, in th LHC-Higgs rgion. H/ZEUS comparison: Rasonabl agrmnt btwn th primnt Th main diffrnc coms from Initial Paramtr Handling of sys. rrors Slction of low nrgy primnts
26 Simultanous traction of α s and PDF Scaling violation: F / lnq ~ α s g(,q ) Data at low allow disntangling corrlation of α s and g α s -fr fit givs: H+fid targt: α =.5 ±.7(p) +.9 s.5 (additionally ±.5 from rnormalization scal) ZEUS+fid targt: α s =.66 ±.49(p) ±.8(modl) (additionally ±.4 from rnormalization scal) ZEUS only: α s =.8 ±.8(p) ±.8(modl) (additionally ±.4 from rnormalization scal) (modl) Diffrnc in p. rror mainly from th tratmnt of systmatic rror and normalization of data points in th fitting procdur and rror propagation. th. uncrt. p. uncrt....4 α s (M Z ) Jt shaps in NC DIS ZEUS (DESY hp-/4565) Multi-jts in NC DIS ZEUS prl. (contributd papr to ICHEP4) Inclusiv jt cross sctions in γp ZEUS (Phys Ltt B 56 () 7) Subjt multiplicity in CC DIS ZEUS (Eur Phys Jour C () 49) Subjt multiplicity in NC DIS ZEUS (Phys Ltt B 558 () 4) NLO QCD fit ZEUS prl. (contributd papr to ICHEP4) NLO QCD fit ZEUS (Phys Rv D 67 () 7) Inclusiv jt cross sctions in NC DIS ZEUS (Phys Ltt B 547 () 64) Dijt cross sctions in NC DIS ZEUS (Phys Ltt B 57 () 7) World avrag (S. Bthk, hp-/47) Various α s masurmnts at HERA. : All consistnt -> Univrsality of QCD 6
27 Summary 7 HERA and ZEUS/H primnts Collidr = tndd rgion in Q and. High- Q NC and CC: lctrowak ffcts NC: ffct of Z chang (-Z coupling, valnc uark) CC: flavor-spcific (ss positiv and ngativ uarks diffrntly) Masurmnts with th polarizd lctron bam ar mor snsitiv to th EM paramtrs. F masurmnt and PDF dtrmination Vry stp ris of sa and gluon at low. pqcd (DGLAP) givs a fairly good dscription of th data for Q = ~ GV Proton PDF is dtrmind with HERA data. Gluon distribution is wll constraind.
Electroweak studies and search for new phenomena at HERA
Elctrowak studis and sarch for nw phnomna at HERA A.F.Żarncki Warsaw Univrsity for ZEUS A.F.Żarncki Elctrowak studis and sarch for nw phnomna at HERA p./25 Outlin Introduction HERA and xprimnts A.F.Żarncki
More informationSearches for Contact Interactions at HERA
Sarchs for Contact Intractions at HERA A.F.Żarncki Univrsity of Warsaw for ZEUS XVI Intrnational Workshop on Dp-Inlastic Scattring and Rlatd Subjcts 7- April 2008, Univrsity Collg London A.F.Żarncki Sarchs
More informationPhysics at HERA. Contents HERA and ZEUS Electroweak results Structure of the proton. Katsuo Tokushuku (KEK, ZEUS)
Physics at HERA e p Contents HERA and ZEUS Electroweak results Structure of the proton Katsuo Tokushuku (KEK, ZEUS) 3/March/5 K.Tokushuku(KEK) @ KEKPH5 / HERA: 7.5GeV 9GeV the world largest electron microscope
More informationDIS-Parity. Search for New Physics Through Parity Violation In Deep Inelastic Electron Scattering. The Physics Case
DIS-Parity Sarch for Nw Physics Through Parity Violation In Dp Inlastic Elctron Scattring Th Physics Cas R. Arnold for th DIS-Parity Collaboration Exprimnt Plan by Stv Rock will follow 12 Jun 2003 DIS-Parity
More informationDiffractive Dijet Production with Leading Proton in ep Collisions at HERA
Diffractiv Dijt Production with Lading Proton in p Collisions at HERA JHEP [arxiv:150.01683] Radk Žlbčík Charls Univrsity Eric 015 Diffraction Th scattrd proton stays intact Exchang with vacuum quantum
More informationStandard Model - Electroweak Interactions. Standard Model. Outline. Weak Neutral Interactions. Electroweak Theory. Experimental Tests.
Standard Modl - Elctrowak Intractions Outlin ak Nutral Intractions Nutral Currnts (NC) Elctrowak Thory ± and Z and γ Discovry of ± Exprimntal Tsts LEP Z Boson Mass and idth Numbr of Nutrinos ± Boson ±
More informationResults on the proton structure from HERA
Results on the proton structure from HERA Shima Shimizu (Univ. of Tokyo) Introduction HERA physics Proton structure The world only e-p collider: HERA electron proton A unique collider at DESY, Hamburg
More informationarxiv: v1 [hep-ex] 21 May 2013
ELECTROWEAK RESULTS FROM HERA arxiv:5.98v [hp-x] May A.F. ŻARNECKI (on bhalf of th H and ZEUS collaborations) Faculty of Physics, Univrsity of Warsaw, Hoża 69, -68 Warszawa, Poland Nutral and chargd currnt
More informationIV. e + e annihilation experiments 1. Experimental methods Discovery of the Tau-Lepton 5. hadrons 6. Hadronic resonances
IV. annihilation xprimnts 1. Exprimntal mthods. 3. 4. Discovry of th Tau-Lpton 5. (γ ) µ µ (γ ) hadrons 6. Hadronic rsonancs Lit.: H.U Martyn, Tst of QED in Quantum Elctrodynamics, T.Kinoshita (d.) 1.
More informationLEP Higgs Search Results. Chris Tully Weak Interactions and Neutrinos Workshop January 21-26, 2002
LEP Higgs Sarch Rsults Chris Tully Wak Intractions and Nutrinos Workshop January 1-6, 00 Viw of LEP Exprimnts Spontanous Symmtry Braking Higgs Fild 1-complx doublt Hyprcharg(Y) U(1) Y Symmtry Lft-Handd
More informationNeutrino Physics. Caren Hagner, Universität Hamburg
Nutrino Physics Carn Hagnr, Univrsität Hamburg What ar nutrinos? Nutrino mass and mixing Nutrino oscillations Nutrino bams: OPERA Oscillation of acclrator nutrinos Solar Nutrinos: BOREXINO (KamLAND ractor
More informationEvent shapes and subjet distributions at HERA
Evnt shaps and subjt distributions at HERA arxiv:hp-x/5v Dc 5 C. Glasman (on bhalf of th Collaboration) Univrsidad Autónoma d Madrid, Spain Abstract Rcnt rsults on subjt distributions from ar prsntd. h
More informationResults on the proton structure from HERA
Results on the proton structure from HERA Shima Shimizu (CERN) 7/Jan/ @ KEK The world only e-p collider: HERA electron proton A unique collider at DESY, Hamburg H ZEUS Circumference: 6.3 km Operated since
More informationProton Structure Function Measurements from HERA
Proton Structure Function Measurements from HERA Jörg Gayler DESY, Notkestrasse 85, 2263 Hamburg, Germany E-mail: gayler@mail.desy.de Abstract. Measurements of proton structure functions made in neutral
More informationHadronic Structure Functions 1
Hadronic Structur Functions 1 arxiv:hp-x/0009009v1 5 Sp 2000 Martin Erdmann Institut für Exprimntll Krnphysik, Univrsität Karlsruh, Engssrstr. 7, D-76128 Karlsruh, Martin.Erdmann@dsy.d Abstract Exprimntal
More informationep Collisions with the Zeus Detector at HERA
ep Collisions with the Zeus Detector at HERA Wesley Smith, U. Wisconsin Outline: Proton Structure Photon Structure Conclusions W. Smith, U. Wisconsin October, 999 HERA p H North Hall West Hall HERA-B East
More informationLHC Collider Phenomenology
LHC Collider Phenomenology Theorist! You are a theorist working in the CMS experimental collaboration You work on LHC Collider Phenomenology related to CMS By working in the experimental collaboration
More informationInitial-state splitting
QCD lecture (p. 14) 1st order analysis For initial state splitting, hard process occurs after splitting, and momentum entering hard process is modified: p zp. σ g+h (p) σ h (zp) α sc F π dz dkt 1 z kt
More informationElectroweak Physics and Searches for New Physics at HERA
Electroweak Physics and Searches for New Physics at HERA Uwe Schneekloth DESY On behalf of the H1 and ZEUS Collaborations 14th Lomonosov Conference on Elementary Particle Physics 5.08.009 Outline Introduction
More informationThe DELPHI experiment at the LEP accelerator at the CERN laboratory
Th DELPHI xprimnt at th LEP acclrator at th CERN laboratory Part 1. Th LEP acclrator Part 2. Th DELPHI xprimnt Part 3. Particl physics rsarch at LEP Th LEP acclrator Th study of collisions btwn lctrons
More informationPhysics and Physics prospects at HERA
Physics and Physics prospects at HERA 58 th Extended Scientific Council / 130 th Scientific Council 1/ June 004 Yuji Yamazaki (KEK, ZEUS) On behalf of the H1, ZEUS, HERMES and HERA-B collaborations The
More informationStructure Functions at Very High Q 2 From HERA
Structure Functions at Very High Q 2 From HERA Christopher M. Cormack For the H1 and ZEUS Collaborations Rutherford Appleton Laboratory, Chilton, Didcot, Oxford, OX11 0QX, United Kingdom Abstract. Measurements
More informationParticles and Deep Inelastic Scattering
Particles and Deep Inelastic Scattering University HUGS - JLab - June 2010 June 2010 HUGS 1 Sum rules You can integrate the structure functions and recover quantities like the net number of quarks. Momentum
More informationGraduate Students Seminar Paul-Scherrer-Institut. Search for Excited Quarks
Graduat Studnts Sminar 01.10.2003 Paul-Schrrr-Institut Sarch for Excitd Quarks Jan Bckr Univrsity of Zurich Sarch for Excitd Quarks Framwork Excitd frmions and comositnss Phnomnological framwork Production
More informationEffects of e ± Polarization on the Final States at HERA
Effcts of ± Polarization on th Final Stats at HERA Ringbrg Workshop Nw Trnds in HERA Physics 003 8 Sptmbr - 3 Octobr 003 Uta Stösslin (DESY Hamburg) Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization
More informationHERA. Marc DAVID. On behalf of. H1 and ZEUS COLLABORATIONS. luminosity that increases steadily from year to year. The positron beam energy E e is 27.
OBSERVATION OF EVENTS AT HIGH Q 2 IN REACTIONS + p! + X AT HERA Marc DAVID CEA-Saclay,DSM/DAPNIA/SPP,99 Gif-sur-Yvtt,FRANCE On bhalf of and ZEUS COLLABORATIONS Both HERA colliding xprimnts, and ZEUS hav
More information3.2 DIS in the quark parton model (QPM)
Experimental studies of QCD 1. Elements of QCD 2. Tests of QCD in annihilation 3. Studies of QCD in DIS 4. QCD in collisions 3.2 DIS in the quark parton model (QPM) M W Elastic scattering: W = M only one
More informationAntonio Pich. IFIC, CSIC Univ. Valencia.
Antonio Pich IFIC, CSIC Univ. Valncia Antonio.Pich@crn.ch Th Standard Modl A. Pich - CERN Summr Lcturs 2005 1. Constitunts & Intractions 2. Quarks 3. Gaug Invarianc 4. Quantum Chromodynamics 5. Elctrowak
More informationPrecision Standard Model Tests (at JLab)
Prcision Standard Modl Tsts (at JLab) Xiaochao Zhng Jun 21st, 2018 Th Standard Modl of Particl Physics How should w sarch for nw physics? Prcision SM tsts at Jffrson Lab Qwak, PVDIS Mollr, 12 GV PVDIS
More informationMeasurement of F L at HERA. S. Glazov, DESY, Ringberg 2008
Measurement of F L at HERA S. Glazov, DESY, Ringberg 8 DIS kinematics Kinematics of inclusive scattering is determined by and Bjorken x. In x scale parameter / - equal sharing among quarks. Proton structure
More informationNeutrino Probes of Dark Energy and Dark Matter
SNOWPAC@Snowbird March 25, 2010 Nutrino Probs of Dark Enrgy and Dark Mattr Shin ichiro Ando California Institut of Tchnology Dark Enrgy and Dark Mattr 2.0 1.5 1.0 No Big Bang SN Most of th nrgy in th Univrs
More information4th Particle Physcis Workshop. National Center for Physics, Islamabad. Proton Structure and QCD tests at HERA. Jan Olsson, DESY.
th 4 Particle Physics Workshop National Center for Physics, Islamabad Proton Structure and QCD tests at HERA Part 2 The proton structure function F2 NLO QCD describes data over >4 orders of magnitude in
More informationLecture 3 Cross Section Measurements. Ingredients to a Cross Section
Lecture 3 Cross Section Measurements Ingredients to a Cross Section Prerequisites and Reminders... Natural Units Four-Vector Kinematics Lorentz Transformation Lorentz Boost Lorentz Invariance Rapidity
More informationΓ W. (GeV) 3. τ e universality in W decays
UCR/DØ/99-22 FERMILAB-CONF-99/39-E W and Z Proprtis at th Tvatron arxiv:hp-x/99137v1 18 Oct 1999 1 Introduction John Ellison (for th CDF and DØ Collaborations) Dpartmnt of Physics, Univrsity of California,
More informationQCD at HERA. Hans-Christian Schultz-Coulon Universität Heidelberg CORFU 2005
QCD at HERA Hans-Christian Schultz-Coulon Universität Heidelberg CORFU 25 Corfu Summer Institute on EPP Corfu, September 9 th, 25 ... that means... proton structure F 2 quark- & gluon-pdfs ( LHC), Δα s
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More information1-loop effects of MSSM particles in Higgs productions at the ILC
1-loop ffcts of MSSM particls in Higgs productions at th ILC Yusaku Kouda, Tadashi Kon, Masato Jimbo A, Yoshimasa Kurihara B, Tadashi Ishikawa B, Kiyoshi Kato C, and Masaaki Kuroda D, Siki Univ., Chiba
More informationLow-energy QED tests (and what we can learn from them)
Low-nrgy QED tsts (and what w can larn from thm) (0γ) 2γ (4γ) (1γ) 3γ (5γ) Indirct Sarchs for Nw Physics at th tim of LHC Flornc, March 2010 Andrzj Czarncki U. of Albrta & CERN Outlin Gyromagntic factors
More informationarxiv:hep-ph/ v1 21 May 1998
hp-ph/980540 VUTH 98-6 NIKHEF 98-0 FNT/T-98/04 SPIN PHYSICS WITH SPIN-0 HADONS arxiv:hp-ph/980540v May 998. JAKOB Univrsità di Pavia and INFN, Szion di Pavia, Via Bassi 6, I-700 Pavia, Italy, -mail:jakob@pv.infn.it
More informationDavisson Germer experiment Announcements:
Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th
More informationHigh Energy Physics. Lecture 9. Deep Inelastic Scattering Scaling Violation. HEP Lecture 9 1
High Energy Physics Lecture 9 Deep Inelastic Scattering Scaling Violation HEP Lecture 9 1 Deep Inelastic Scattering: The reaction equation of DIS is written e+ p e+ X where X is a system of outgoing hadrons
More informationStructure Functions and Parton Distribution Functions at the HERA ep Collider
Structure Functions and Parton Distribution Functions at the HERA ep Collider by Chris Targett Adams (University College London) on behalf of the ZEUS and H1 collaborations. Moriond QCD, 16/03/2005 Contents
More informationProton Structure Functions: Experiments, Models and Uncertainties.
Proton Structure Functions: Experiments, Models and Uncertainties. S. Glazov, DESY IKTP seminar, July 8. Disclaimer Nothing in this talk should be interpreted as the final knowledge on proton structure.
More informationSearch for the Dark Photon at Belle for 0.27 < m A < 3 GeV/c 2
Sarch for th Dark Photon at Bll for.7 < m A < 3 GV/c Igal Jagl Univrsity of Hawai i at Mānoa for th Bll Collaboration QCD, Montpllir, 6 Juillt BELLE Igal Jagl (UH) Sarch for th Dark photon at Bll QCD /
More informationElectroweak constraints from HERA. 1 Introduction. Elisabetta Gallo INFN Firenze Via G. Sansone 1 I Sesto Fiorentino, ITALY
Elisabetta Gallo INFN Firenze Via G. Sansone I59 Sesto Fiorentino, ITALY Introduction The ep accelerator HERA at the laboratory DESY in Hamburg terminated activity on 3th June 7. The two experiments H
More informationDeep Inelastic Scattering in Lepton-Hadron Collisions Probing the Parton Structure of the Nucleon with Leptons Basic Formalism (indep.
Deep Inelastic Scattering in Lepton-Hadron Collisions Probing the Parton Structure of the Nucleon with Leptons Basic Formalism (indep. of strong dynamics and parton picture) Experimental Development Fixed
More informationPhysics at Hadron Colliders Partons and PDFs
Physics at Hadron Colliders Partons and PDFs Marina Cobal Thanks to D. Bettoni Università di Udine 1 2 How to probe the nucleon / quarks? Scatter high-energy lepton off a proton: Deep-Inelastic Scattering
More informationZEUS 1995 F ZEUS BPC95 ZEUS SVX95 ZEUS94 E665 H1 SVX95 ZEUSREGGE ZEUSQCD
MEASUREMENT AND PHENOMENOLOGY OF THE PROTON STRUCTURE FUNCTION F FROM ZEUS AT HERA A. Quadt Department of Physics, Particle Physics, Keble Road, Oford OX 3RH, England E-mail: quadt@mail.desy.de Measurements
More informationLimits on the effective quark radius and the contact-interaction mass scales from inclusive ep scattering at HERA. Aleksander Filip Żarnecki
38th International Conference on High Energy Physics August 5, 2016 A.F.Żarnecki (University of Warsaw) Quark radius and CI at HERA August 5, 2016 1 / 24 Limits on the effective uark radius and the contact-interaction
More informationorbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the
Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly
More informationarxiv:hep-ph/ v1 3 Nov 1998
MEASUREMENT AND PHENOMENOLOGY OF THE PROTON STRUCTURE FUNCTION F FROM ZEUS AT HERA A. Quadt Department of Physics, Particle Physics, Keble Road, Oford OX 3RH, England E-mail: quadt@mail.desy.de arxiv:hep-ph/9836v
More informationQCD Measurements at HERA
QCD Measurements at HERA Armen Bunyatyan, Max-Planck-Institut für Kernphysik, Heidelberg, Germany Yerevan Physics Institute, Armenia November, 7 Abstract A review is presented of recent results in QCD
More informationNovel Measurements of Proton Structure at HERA
Introduction Combined Cross Sections & QCD Fits NC & CC Cross Section Measurements F L Summary Novel Measurements of Proton Structure at HERA Katie Oliver University of Oxford On behalf of the H1 and ZEUS
More informationOutline: Introduction Quantum ChromoDynamics (QCD) Jet algorithms Tests of QCD QCD analyses at HERA extraction of the proton PDFs
Outline: Introduction Quantum ChromoDynamics (QCD) Jet algorithms Tests of QCD QCD analyses at HERA etraction of the proton PDFs Etraction of the proton PDFs Etraction Etractionof of the proton protonpdfs
More informationQCD at hadron colliders Lecture 3: Parton Distribution Functions
QCD at hadron colliders Lecture : Parton Distribution Functions Gavin Salam CERN, Princeton & LPTHE/CNRS (Paris) Maria Laach Herbtschule für Hochenenergiephysik September, Germany QCD lecture (p. ) PDF
More informationDavisson Germer experiment
Announcmnts: Davisson Grmr xprimnt Homwork st 5 is today. Homwork st 6 will b postd latr today. Mad a good guss about th Nobl Priz for 2013 Clinton Davisson and Lstr Grmr. Davisson won Nobl Priz in 1937.
More informationElectroweak measurements at HERA
Electroweak measurements at HERA Alex Tapper DESY forum 1 th & 13 th September 006 Precision electroweak measurements: What can HERA contribute? Outline Introduction High Q physics at HERA Review of recent
More informationZhong-Bo Kang Los Alamos National Laboratory
Introduction to pqcd and Jets: lecture 1 Zhong-Bo Kang Los Alamos National Laboratory Jet Collaboration Summer School University of California, Davis July 19 1, 014 Selected references on QCD! QCD and
More informationOn the Hamiltonian of a Multi-Electron Atom
On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making
More informationX COLLIDER PHYSICS : BASIC CONCEPTS
COLLIDER PHYSICS : BASIC CONCEPTS 2006 Busstepp Edinburgh 1. INTRODUCTION Physics scenarios and objectives General collider characteristics 2. ELECTRON-PROTON COLLIDER HERA Quark/gluon densities; QCD coupling
More informationChapter 8: Electron Configurations and Periodicity
Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how
More informationNew Muon Lifetime and the Fermi Coupling Constant G F. Kevin Giovanetti James Madison University
Nw Muon Liftim and th Frmi Coupling Constant G F Kvin Giovantti Jams Madison Univrsity HallC mting, JLAB, Aug 10, 007 a µ = g µ / Prcision FUNDAMENTAL Muon Phyiscs SYMMETRIES Prcision Masurmnts of Standard
More informationCharm production at HERA
1 Charm roduction at HERA G.P. Hath a a H.H. Wills Physics Laboratory, Univrsity of Bristol, Bristol BS8 1TL, UK 1. INTRODUCTION Th HERA collidr circulats bams of lctrons (ositrons) and rotons at nrgis
More informationfiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)
NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-) 64 Q. Th radius of a 9Cu nuclus is masurd to b 4.8 - cm. (A). Th radius of a 7 Mg nuclus can b stimatd to b.86 - cm (b) 5. - cm (c).6 - cm (d) 8.6 - cm (c)
More informationPhysics at LHC. lecture one. Sven-Olaf Moch. DESY, Zeuthen. in collaboration with Martin zur Nedden
Physics at LHC lecture one Sven-Olaf Moch Sven-Olaf.Moch@desy.de DESY, Zeuthen in collaboration with Martin zur Nedden Humboldt-Universität, October 22, 2007, Berlin Sven-Olaf Moch Physics at LHC p.1 LHC
More informationProgress in CTEQ-TEA (Tung et al.) PDF Analysis
Progress in CTEQ-TEA (Tung et al.) PDF Analysis Sayipjamal Dulat Xinjiang University University In collaboration with CTEQ-TEA Group April 4, 2016 QCD Study Group CTEQ-TEA group CTEQ Tung et al. (TEA)
More informationOpportunities in low x physics at a future Electron-Ion Collider (EIC) facility
1 Opportunities in low x physics at a future Electron-Ion Collider (EIC) facility Motivation Quantum Chromo Dynamics Proton=uud Visible Universe Galaxies, stars, people, Silent Partners: Protons & Neutrons
More informationPHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS
PHYSICS 489/489 LECTURE 7: QUANTUM ELECTRODYNAMICS REMINDER Problm st du today 700 in Box F TODAY: W invstigatd th Dirac quation it dscribs a rlativistic spin /2 particl implis th xistnc of antiparticl
More informationde/dx Effectively all charged particles except electrons
de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls
More informationEigenvalue Distributions of Quark Matrix at Finite Isospin Chemical Potential
Tim: Tusday, 5: Room: Chsapak A Eignvalu Distributions of Quark Matri at Finit Isospin Chmical Potntial Prsntr: Yuji Sasai Tsuyama National Collg of Tchnology Co-authors: Grnot Akmann, Atsushi Nakamura
More informationSelf-interaction mass formula that relates all leptons and quarks to the electron
Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris
More informationarxiv: v1 [hep-ex] 7 Jan 2019
Masurmnt of Longitudinal Singl-Spin Asymmtry for ± Production in Polarizd Proton+Proton Collisions at STAR arxiv:191.1734v1 [hp-x] 7 Jan 219, for th STAR collaboration Ky Laboratory of Particl Physics
More informationRunning Period. Detector Progress Data Analysis. Background Studies Physics Results Highlights Physics Outlook and Goals
Status Report -3 Running Period Detector Progress Data Analysis Background Studies Physics Results Highlights Physics Outlook and Goals Stathes Paganis Columbia University On behalf of the Collaboration
More informationOpen Issues in DIS The High Energy Perspective
Open Issues in DIS The High Energy Perspective My private point of view using data from DIS in collider mode: Accelerator and Experiments HERA success story: Precision cross sections, structure functions
More informationTHE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION. Jiro Murata Rikkyo University for the MTV collaboration INPC2016, Sydney, Sep 11-16, 2016
THE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION Jiro Murata Rikkyo Univrsity for th MTV collaboration INPC2016 Sydny Sp 11-16 2016 Rikkyo J. Murata Y. Nakaya Y. Totsuka S. Tanaka R. Tanuma T.
More informationNeutrino Mass and Forbidden Beta Decays
NUCLEAR THEORY Vol. 35 016) ds. M. Gaidarov N. Minkov Hron Prss Sofia Nutrino Mass and Forbiddn Bta Dcays R. Dvornický 1 D. Štfánik F. Šimkovic 3 1 Dzhlpov Laboratory of Nuclar Problms JINR 141980 Dubna
More informationSearch for New Physics at HERA
Search for New Physics at HERA Yongdok Ri (KEK) on behalf of the H and ZEUS collaborations Introduction of HERA Model dependent search Model independent search Summary LES RENCONTRES DE PHYSIQUE DE LA
More informationRecent Progress on the Determination of Nuclear Parton Distribution Functions
Recent Progress on the Determination of Nuclear Parton Distribution Functions Shunzo Kumano High Energy Accelerator Research Organization (KEK) Graduate University for Advanced Studies (GUAS) shunzo.kumano@kek.jp
More informationFuture exotic physics at ZEUS and HERA
Future exotic physics at ZEUS and HERA Matthew Wing (UCL) Introduction Inclusive measurements of deep inelastic scattering Deviations from the Standard Model and search for substructure Search for leptoquarks
More informationCalculation of the Gluon Distribution Function Using Alternative Method for the Proton Structure Function
Commun. Theor. Phys. (Beijing, China 40 (2003 pp. 551 557 c International Academic Publishers Vol. 40, No. 5, November 15, 2003 Calculation of the Gluon Distribution Function Using Alternative Method for
More informationPoS(Photon 2013)004. Proton structure and PDFs at HERA. Vladimir Chekelian MPI for Physics, Munich
MPI for Physics, Munich E-mail: shekeln@mail.desy.de The neutral and charged current deep-inelastic ep scattering cross sections are measured in the H and ZEUS eperiments at HERA (99-7), with an electron
More informationGlobal QCD Analysis of Nucleon Structure: Progress and Prospects
Global QCD Analysis of Nucleon Structure: Progress and Prospects Recent Past (say, up to DIS2002): Experiment: More precision DIS measurements (mainly HERA) and Tevatron inclusive jet production (CDF,
More information, 2004 Peter Schleper University of Hamburg Strasbourg, March 12 HC: The decade of Hadron machines L evatron HERA
HERA Tevatron LHC: The decade of Hadron machines University of Hamburg Strasbourg, March 12 th, 2004 1 LHC: Proton-Proton E CMS = 14 TeV HERA LHC: HERA: Elektron-Proton E CMS = 320 GeV 2 Perturbative approach
More informationZEUS New Results. Wesley H. Smith, University of Wisconsin on behalf of the ZEUS Collaboration DIS 2004, Strbské Pleso, Slovakia, April 14, 2004
ZEUS New Results Wesley H. Smith, University of Wisconsin on behalf of the ZEUS Collaboration DIS 2004, Strbské Pleso, Slovakia, April 14, 2004 HERA I: Structure Functions & QCD fits Hadronic Final States
More informationEIC meeting, April 6,7, MIT
F L and the Gluon Density EIC meeting, April 6,7, MIT A. Caldwell Rutherford SLAC-MIT, HERA EIC? Motivation At small x, gluons physics dominates In this region, far from initial conditions: universal properties?
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationPhysics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma
Physics D Lctur Slids Oct 1 Vivk Sharma UCSD Physics Modrn Viw of Photolctric Effct E = hf = KE+ ϕ Is h sam in Photolctric Effct as in BBQ Radiation? Slop h = 6.66 x 10-34 JS Einstin Nobl Priz! No mattr
More informationStandard Model of Particle Physics SS 2012
Lecture: Standard Model of Particle Physics Heidelberg SS 2012 W- and Z-Bosons 1 2 Contents Discovery of real W- and Z-bosons Intermezzo: QCD at Hadron Colliders LEP + Detectors W- and Z- Physics at LEP
More informationPhysics 2D Lecture Slides Lecture 12: Jan 28 th 2004
Brian Wcht, th TA, is away this wk. I will substitut for his offic hours (in my offic 3314 Mayr Hall, discussion and PS sssion. Pl. giv all rgrad rqusts to m this wk (only) Quiz 3 Will Covr Sctions.1-.5
More information(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions)
Spring 01, P67, YK Monday January 30, 01 8 Obsrvabl particl dtction ffcts ar : (most) du to long rang m forcs i.. via atomic collisions or du to short rang nuclar collisions or through dcay ( = wak intractions)
More informationBSM Physics at the LHC, HERA
BSM Physics at the LHC, HERA Few topics that could be interesting for EIC Elisabetta Gallo 19/12/2018 For HERA results Results taken from old slides Leptoquarks l e q LQ e,n q e q LQ q e,n e + e LQ q q
More informationEstimation of the two-photon QED background in Belle II
Estimation of th two-photon QED background in Bll II Elna Ndlkovska, Christian Kisling Max-Planck Institut for physics, Munich Upgrad to th Bll II dtctor Expctd background at Bll II QED xprimnts prformd
More informationMeasurements of the Proton F L and F 2 Structure Functions at Low x at HERA
Measurements of the Proton F L and F 2 Structure Functions at Low x at HERA Andrei Nikiforov DESY on behalf of the H1 and ZEUS collaborations Moriond QCD, La Thuile, 13 March 2008 Andrei Nikiforov DESY
More informationZEUS Highlights for ICHEP02... a personal selection
Highlights for ICHEP... a personal selection Main Questions at HERA: Tancredi.Carli@desy.de What is the structure of the proton? Is DGLAP working at low-x? How are heavy quarks produced? Is the SM valid
More informationParton Uncertainties and the Stability of NLO Global Analysis. Daniel Stump Department of Physics and Astronomy Michigan State University
Parton Uncertainties and the Stability of NLO Global Analysis Daniel Stump Department of Physics and Astronomy Michigan State University J. Huston, J. Pumplin, D. Stump and W.K. Tung, Stability of NLO
More informationF λ A (x, m Q, M Q ) = a
Parton Distributions and their Uncertainties Jon Pumplin DPF22 Williamfburg 5/25/2 CTEQ6 PDF analysis (J. Pumplin, D. Stump, W.K. Tung, J. Huston, H. Lai, P. Nadolsky [hep-ph/21195]) include new data sets
More informationMeasurements of Proton Structure at Low Q 2 at HERA
Measurements of Proton Structure at Low Q 2 at HERA Victor Lendermann Kirchhoff-Institut für Physik, Universität Heidelberg Im Neuenheimer Feld 227, 69120 Heidelberg Germany Abstract. Inclusive ep scattering
More informationInclusive Cross Sections at HERA and Determinations of F L
Inclusive Cross Sections at HERA and Determinations of F L Vladimir Chekelian (MPI for Physics, Munich) on behalf of the H and ZEUS Collaborations HERA The World s Only ep Collider HERA / DIS / NC / CC
More informationRelativistic electron microscopy of hadron dynamics
Impact paramtr analysis in + N + pi+ N 1 Paul Hoyr Univrsity of Hlsinki INT Workshop Novmbr 14-18, 2016 Rlativistic lctron microscopy of hadron dynamics Gold atoms: 3D Th pion: 2D 8 ρπ(b) 6 ρ π (b) [fm
More informationPion condensation with neutrinos
Pion condnsation with nutrinos Or how dos QCD bhav undr high dnsitis of lctron/muon nutrinos Harmn Warringa, Goth Univrsität, Frankfurt Basd on work don with Hiroaki Abuki and Tomas Braunr arxiv:0901.2477
More information