Effects of e ± Polarization on the Final States at HERA

Size: px
Start display at page:

Download "Effects of e ± Polarization on the Final States at HERA"

Transcription

1 Effcts of ± Polarization on th Final Stats at HERA Ringbrg Workshop Nw Trnds in HERA Physics Sptmbr - 3 Octobr 003 Uta Stösslin (DESY Hamburg) Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 1

2 Outlin HERA II Polarization Dpndnt Inclusiv Cross Sction CC, NC Dply Virtual Compton Scattring cross sction, asymmtris Asymmtris in Particl Production Bam Spin Transfr to Λ-Baryons ZEUS Conclusion Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA

3 First in 003 p 319 GV LPOL 5 min. Avrag Mar003 TPOL 5 min. Avrag Polarization % Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 3 Day

4 Th HERA II Bam Options -bam + and - bam charg dpndncis longitudinally paralll/anti-paralll polarizations with xpctd valus up to 50-60% with a prcision of δp/p~1% bam spin dpndncis nhancd physics potntial! high luminosity up to 1fb -1 until 006, i.. about 00pb -1 pr sampl + (λ=±1), - (λ=±1) xpctd and wantd but p-bam unpolarizd still! no accss to polarizd proton and photon PDFs (rquirs doubl spin asymmtris) Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 4

5 Th Classic s Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 5

6 Classic Goal (I): Sarch for Right-Handd Currnts in CC DIS - L W L ν L? - R W R? ν R? tim u L λ=-1 d L u R λ=+1 d R forbiddn in Standard Modl: σ CC 0 for ± R txtbook masurmnt! Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 6

7 Simulation of σ ± CC (λ) λ ( ) ( ) ± ± Q Y W Y xw ± πα 1± CC 4 W 3 σ = κ xq with Y = - y + y /(1 + R) + Y = 1 -(1 - y) σ CC TOT (Q > 00 GV ) (pb) A.Mhta DIS0 - p Data (Prlim. 16 pb -1 ) - p SM s=30 GV - p SM (MC) s=30 GV (50 pb -1 ) κ = W Q 1 Q + M 4sin θ W W 1 for Q M W 60 + p Data (48 pb -1 ) + p SM s=300 GV 50pb -1 pr λ=±0.6 modst luminosity but high polarization ndd p SM (MC) s=300 GV (50 pb -1 ) nw physics byond SM if any dviation from straight lin Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA HERA I data P

8 Classic Goal (II): Parity Violation in NC γ + Z p X p X intrfrnc of lctromagntic and wak nutral currnts vctor (v) and axial-vctor (a) contributions d σ ( λ) πα dq dν xq { } int = 4 κ Z = ( Q ) Y ( R 0) G (-v ± λa ) Y xg ( a λv ) + - dpnding both on bam polarization λ and bam charg (±) nw structur functions G and xg 3 containing quark couplings to th Z boson q q q ( ( ) ( )) ( ) ( ) G(x) = xσ v q x+q x 3 q q q ( ) xg (x) = -xσ a q x -q x v = T - a = T f 3f f Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 8 f 3f si n θw

9 Asymmtris in NC DIS varying bam polarization [d: SLAC 1978] on parity-violation asymmtry pr bam charg ( ) A λ, λ = 1 ( ) ( ) d 1 ( ) ( ) d dσ λ - σ λ dσ λ + σ λ 1 varying of both λ and bam charg [µc: BCDMS 1981] bam conjugation asymmtry ( ) B λ, λ = 1 ( ) ( ) d 1 ( ) ( ) d - dσ + λ - σ - λ dσ + λ + σ λ 1 = -κ Z λ -λ 1 ( ) 1 1 y a G v xg F F 1+ 1-y ( ) ( ) { ~0 for y 1 ~1 for y 0 ( λ - λ ) xg ( 1-y) F -κ Z a + v 1 ( 1 ) + -y { unpol. γz -intrfrnc contribution masurmnts rquir high polarization valus and high Q valus 1 Q -4 κ Z = 1.7i10 Q /GV 4cos θwsin θ W MZ + Q Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 9 { ~0

10 Simulation of G (x,q ) at high Q for λ =-λ 1 and v =0: using approximation: x 1 G A ( λ ) = κλa ~ ± κλ F Z Z ( ( + ) + ( + )) 1 F x 4 u u d d 9 G (( ) x u+ u + ( d+ d) ) 9 1+ d v/u 4+ d /u xtraction of G (x,q ) using knowldg of F (x,q ) v v v Singltt+ Non-Singltt Singltt 00pb -1 pr λ =± 0.5 M.Klin DIS01 Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 10

11 Tst of Elctrowak Paramtr J.Blümlin t al. HERA WS87 mploy bam polarization and charg to tst M W or sin θ W via parity-violation asymmtry A ± (λ) cross sction ratio R ± (λ) R ± σ λ = σ ( ) ( λ) ( λ ) stat. rror of M W from R - bst and only 5% wors if λ=0 instad of -1 (δλ=1%) although σ CC (λ=-1)/ σ CC (λ=0)~ ± NC ± CC [%] A - R - 00pb -1 Λ=0.8 Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 11

12 Th Nw Classic s Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 1

13 Dply Virtual Compton Scattring DVCS Bth-Hitlr factorization γ * γ γ * γ γ * γ p p p p p t=- nw info on structur a) of nuclon! b) c) p diffractiv production of a ral photon d 4 σ/dxdq d t dф τ DVCS + τ BH + τ* DVCS τ BH + τ DVCS τ BH * DVCS : QCD procss snsitiv to undrlying dynamics Bth-Hitlr : QED procss background and intrfrnc Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 13

14 DVCS : Modls GPD basd modls Color Dipol basd modls dipol siz R x 1 P x P handbag b impact paramtr dominant at low x GPD incorporat both a partonic and distributional amplitud bhavior accss to dynamical rlation btwn diffrnt partons (particl corrlations, orbital angular momntum) thr-dimnsional distribution of nuclon substructur QCD pictur (hard scattring factorization: LO, byond LO, byond twist-) simpl unifid pictur of diffractiv procsss match soft and hard rgims implmntation of.g. saturation ffcts broad phnomnology Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 14

15 Nuclon Holography [V.Blitsky, D.Müllr,hp-ph/006306] [M.Burkhardt,PRD6(000)071503] GPD provid transvrs location of partons in th nuclon form factor parton dnsity GPD at η=0 s also talks by A.Frund and C.Wiss at HERA 3 WS0 1/ b~1/(t) - Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 15

16 DVCS : Exprimntal Signaturs BH γ DVCS intrfrnc rgion γ [hp-x/030508] Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 16

17 DVCS : Cross Sction vs W H1 [EPS03] δ 6pb -1 W dpndnc matchs W 0.7 bhavior of hard VM production Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 17

18 DVCS : Cross Sction vs Q H1 6pb -1 95pb -1 fit Q -n Q dpndnc wll dscribd by GPD or color dipol basd modls (intgratd ovr xp. t rang) HERAII : factor 10 mor statistics xpctd Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 18

19 [V.Blitsky t al.,hp-ph/011108] Angular Dpndncis of p pγ Cross Sction angl btwn th lpton and hadron scattring plans ф = ф N - ф l γ* ф γ rcoild p BH DVCS Intrfrnc Complx and rich angular structur of th cross sction! But, which angular dpndncis ar th rlvant ons? Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 19

20 Contributions for an Unpolarizd p mploy angular structur to accss mor obsrvabls, in particular in dpndnc on bam spin (λ) and charg (±) cosф, cosф cosф, λsinф twist-3! T pol. p only charg dp cosф, λsinф sinф L,T pol. p only known cosф-dpndnc du to lpton BH propagators cosф, λsinф twist-3! DVCS amplitud with gluon transvrsity (twist-, but α S powr supp.) : - squard DVCS trm : cosф and sinф dpndncis - intrfrnc trm : cos3ф and sin3ф dpndncis BH trm: bam polarization dpndnc only in cas of longitudinally or transvrsly (L,T) polarizd targt! Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 0

21 Bam Charg and Azimuthal Asymmtry varying bam charg [HERMES 00] bam charg asymmtry (CA) or counting vnts scattrd up and blow lpton scattring plan to gt cosф wight bins in ф CA ~ R (τ BH τ DVCS ) varying azimuthal angl (bam spin and charg fixd) azimuthal angl asymmtry (AAA) rquirs vry good ф rsolution and control of twist-3 contamination AAA ~ R (τ BH τ DVCS ) Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 1

22 Bam Spin Asymmtry varying bam polarization [HERMES, CLAS 001] on bam spin asymmtry (SSA) pr bam charg or counting vnts scattrd up and blow rotatd-by-90 o lpton scattring plan (lft and right) to gt sinф wight bins in ф SSA ~ Im (τ BH τ DVCS ) combination of SSA and CA or AAA givs accss to full twist- τ BH τ DVCS amplitud BH contributions absnt in CA and SSA masurmnts Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA

23 Unviling GPD H unviling GPDs from dtrmination of Fourir cofficints obtaind from asymmtry masurmnts CA AAA SSA K ~- /Q ~1/10 λ } high y ndd high γ* pol. H (unpol. non-spin-flip) lik q, q, g H (pol. non-spin-flip) lik q, q, g E (unpol. spin-flip) no inlcusiv quivalnt! E (pol. spin-flip) no inlcusiv quivalnt! H Compton Form Factors ar convolutions of cofficint functions and GPDs : H,H,E,E appar in linar combinations in intrfrnc trm but in quadratic combinations in unpol. cross sction accss both parts of CFF H complt spration of GPD would rquir in addition data takn with polarizd (T,L) targt Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 3

24 CA Simulation for HERA intgratd ovr t, -t<0.5gv, and ovr ф [A.Frund, hp-ph/030601] x x Q [GV ] Q [GV ] Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 4

25 SSA Simulation for HERA (( + p) intgratd ovr t, -t<0.5gv, and ovr ф [A.Frund, hp-ph/030601] x x Q [GV ] Q [GV ] Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 5

26 Som Masurmnt Rmarks ф and t ar difficult to masur sinc scattrd proton is not obsrvd [R.Stamn, HERA3 WS0] ф = ф - ф p ф - ф γ t = (p - p ) - p + p T T γ dtrmination of ф and t via scattrd and γ : DVCS : backward and cntral γ and vto on p-diss background ( forward instrumntation) t dominatd by E and θ rsolution of γ ф dominatd by E rsolution of H1 prlim [EPS03] Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 6

27 H1 VFPS and DVCS [L.Favart, Trnto03] bttr supprssion of p-diss background som bins in t sys (b-slop) ±GV - [H1-PRC01/00] mor bins in ф? DVCS vnts for 1fb -1 Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 7

28 Simulations for HERA : Som Rmarks CA and SSA asymmtris prdictd to b sizabl, calculations in LO, NLO, and twist-3 availabl, s also [V.Blitsky t al.,hp-ph/011108] changing of t cut-off to 1GV altrs rsults on 10% lvl AAA prdictd to hav similar siz as CA twist-3 ffcts stimatd to b ngligibl for CA and for SSA NLO corrctions ar larg, up to 100% for CA and up to 50% for SSA (larg NLO gluon contribution in ral part of DVCS amplitud) NLO corrctions important for prcision xtraction of GPDs in gnral: cross sction and asymmtry data can b wll modld, but too many paramtrs not constraind yt! asymmtry masurmnts fasibl! Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 8

29 [V.Blitsky, D.Müllr,hp-ph/ ] Tim-lik Virtual Compton Scattring lctroproduction of muon pairs allows clar study of GPDs via singl bam spin, singl hadron spin, bam charg, azimuthal and doubl spin asymmtris mploying angular dpndncis of rcoild p and of lpton pair mapping in both scaling variabls η and ξ constrain angular momntum sum rul: Ebam E = 11GV = 5GV E = 40GV bam bam q η = p q but cross sction vry small high luminosity! Q ξ ;xb p q 1+ ξ = = ξ Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 9

30 Anothr viw on th angular momntum sum rul [V.Blitsky t al.,hp-ph/011108] with proton and nutron magntic momnts and κ sa is th orbital angular momntum carrid by th quarks momntum fraction P i carrid by th quarks can b dducd from DIS data alon Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 30

31 Elastic Particl Production slct diffrnt GPDs (and quark flavors) via dtction of diffrnt final stats vctor msons :,.g. ρ 0 J u +J d [X.Ji,hp-lat/011016] H,E H,E psudoscalar msons : su transitions within th baryon octt : transition GPDs,.g. Hp-> Λ but additional complication du to prsnc of distribution amplitud of th particl,.g. th pion wav function for unpol. bam and transv. pol.. targt larg asymmtris hav bn prdictd, s.g. [K.Gok t al, hp-ph/010601] HERMES, CLAS, COMPASS γ p -> K L * + spcial : xclusiv strangnss production whr an azimuthal spin asymmtry can b masurd on an unpolarizd targt by masuring th polarization of th rcoiling hypron through its angular distribution not studid yt for HERA Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 31 Λ

32 Singl Spin Asymmtry in π lctroproduction CLAS: first obsrvation of a positiv SSA in SiDIS π + production [CLAS,hp-x/ ] but xpctd to b zro in LO rlatd to ithr NLO or highr twist ffct NLO : [A.Afanasv,C.E.Carlson,hp-ph/ ] final stat gluon xchang dlivr contribution to + anti-symmtric part of hadronic tnsor lpton bam spin asymmtry is gnratd du to intrfrnc btwn absorption of longitudinal and transvrs virtual photons A LU ~r / Q T with transvrs componnt of th final quark momntum r T twist-3 3 : [A.V.Efrmov t al.,hp-ph/00814] SSA ariss from chirally odd twist-3 proton distribution function a (x) in combination with chirally-odd and T-odd twist- Collins FF vry intrsting to tst it also at HERA Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 3

33 Bam Spin Transfr to Λ-Baryon [M.Anslmino,hp-ph/030008] four indpndnt obsrvabls: in currnt fragmntation rgion pol. FF D ( ) Λ /q z snsitiv to distribution of polarizd quarks in unpolarizd nuclon Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 33

34 Longitudinal Λ Polarization parity violating wak dacy of Λ pπ distribution of dcay angl θ* dpnds on Λ pol. P : I(θ*) ~ 1 - α P cos θ* (α=0.64) xp.: P Λ = P bam D(y) S Λ rquirs high bam pol. and high y Λ could contain polarizd quark! using rlation pol FF pol PDF Gribov-Lipatov rciprocity rlation [1971] [C.Rislr,H1,PhDthsis] K S study Λ spin structur and tst SU(3) f : [.g. B.Ma t al., hp-ph/0081] Λ 0 Λ spin proton spin mor data ndd! masurmnts sms to b fasibl π momntum paralll antiparalll to Λ flight dirction Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 34

35 Conclusion HERA II with high luminosity and with longitudinally polarizd lctrons and positrons opns nw horizons to study lctrowak thory and parton dynamics and may dlivr vn surpriss w could not imagin today For fruitful discussions I lik to thank Markus Dihl, Andras Frund, Marco Stratmann, Christian Rislr. Ringbrg Workshop 003 Uta Stösslin Effcts of ± Polarization on th Final Stats at HERA 35

Electroweak studies and search for new phenomena at HERA

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 information

Searches for Contact Interactions at HERA

Searches 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 information

Standard Model - Electroweak Interactions. Standard Model. Outline. Weak Neutral Interactions. Electroweak Theory. Experimental Tests.

Standard 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 information

DVCS and extraction of cross sections in Hall A

DVCS and extraction of cross sections in Hall A DVCS and xtraction of cross sctions in Hall A Eric FUCHEY Ph.D Studnt Laboratoir d Physiqu Corpusculair UMR 6533 CNRS/INP3 Unirsité Blais Pascal Clrmont Frrand Outlin Gnralizd Parton Distributions / DVCS

More information

DIS-Parity. Search for New Physics Through Parity Violation In Deep Inelastic Electron Scattering. The Physics Case

DIS-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 information

Diffractive Dijet Production with Leading Proton in ep Collisions at HERA

Diffractive 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 information

arxiv:hep-ph/ v1 21 May 1998

arxiv: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 information

HERA - Structure of Matter and QCD

HERA - Structure of Matter and QCD 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) DESY/HERA HERA 99-7 H ZEUS HERA: (7.5GV lctron 9GVproton)

More information

IV. e + e annihilation experiments 1. Experimental methods Discovery of the Tau-Lepton 5. hadrons 6. Hadronic resonances

IV. 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 information

Classical Magnetic Dipole

Classical Magnetic Dipole Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg

More information

Measurements with Polarized Hadrons

Measurements with Polarized Hadrons Aug 15, 003 Lepton-Photon 003 Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Contents: Introduction: Spin of Proton Polarized Deep Inelastic Lepton-Nucleon Scattering 1.

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)

fiziks 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 information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Precision Standard Model Tests (at JLab)

Precision 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 information

arxiv: v1 [hep-ex] 21 May 2013

arxiv: 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 information

Neutrino Physics. Caren Hagner, Universität Hamburg

Neutrino 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 information

Relativistic electron microscopy of hadron dynamics

Relativistic 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 information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

LEP Higgs Search Results. Chris Tully Weak Interactions and Neutrinos Workshop January 21-26, 2002

LEP 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 information

Search for the Dark Photon at Belle for 0.27 < m A < 3 GeV/c 2

Search 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 information

Low-energy QED tests (and what we can learn from them)

Low-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 information

Hadronic Structure Functions 1

Hadronic 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 information

Electroweak Correction for the Study of Higgs Potential in LC

Electroweak Correction for the Study of Higgs Potential in LC Elctrowak Corrction for th Study of Higgs Potntial in LC LAPTH-Minamitatya Collaboration LCS05 005.3.19, Stanford U. prsntd by K.Kato(Kogakuin U.) Introduction LC: high-prcision xprimnts Rquirs th sam

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

HERA. 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.

HERA. 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 information

Eigenvalue Distributions of Quark Matrix at Finite Isospin Chemical Potential

Eigenvalue 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 information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

Nuclear reactions The chain reaction

Nuclear reactions The chain reaction Nuclar ractions Th chain raction Nuclar ractions Th chain raction For powr applications want a slf-sustaind chain raction. Natural U: 0.7% of 235 U and 99.3% of 238 U Natural U: 0.7% of 235 U and 99.3%

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Graduate Students Seminar Paul-Scherrer-Institut. Search for Excited Quarks

Graduate 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 information

Mor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration

More information

Magnetic Neutron Scattering and Spin-Polarized Neutrons

Magnetic Neutron Scattering and Spin-Polarized Neutrons agntic Nutron Scattring and Spin-Polarizd Nutrons Physical origin: potntial of magntic dipol momnt of th nutron in magntic fild gnratd by lctron spins and orbital momnts in th solid. µ n µ H Spcializ to

More information

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting 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 information

Gang RONG. Institute of High Energy Physics, CAS. November 27, BES BELLE CELO BABAR 2007 Joint Workshop on Charm Physics

Gang RONG. Institute of High Energy Physics, CAS. November 27, BES BELLE CELO BABAR 2007 Joint Workshop on Charm Physics Charm cays and Ψ(377 non- cays at BESII & BESIII Gang RONG Institut of High Enrgy Physics, CAS Novmbr 7, 7 BES BELLE CELO BABAR 7 Joint Workshop on Charm Physics Nov. 6 7, 7, IHEP, Bijing, China 1 OUTLINE

More information

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves?

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves? Today Wav-Mattr Duality HW 7 and Exam 2 du Thurs. 8pm 0 min rcap from last lctur on QM Finish QM odds and nds from ch.4 Th Standard Modl 4 forcs of Natur Fundamntal particls of Natur Fynman diagrams EM

More information

PHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS

PHYSICS 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 information

Experimental Program of the Future COMPASS-II Experiment at CERN

Experimental Program of the Future COMPASS-II Experiment at CERN Experimental Program of the Future COMPASS-II Experiment at CERN Luís Silva LIP Lisbon lsilva@lip.pt 24 Aug 2012 On behalf of the COMPASS Collaboration co-financed by THE COMPASS EXPERIMENT Common Muon

More information

The DELPHI experiment at the LEP accelerator at the CERN laboratory

The 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 information

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-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 information

THE 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 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 information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

Properties of Quarks ( ) Isospin. π = 1, 1

Properties of Quarks ( ) Isospin. π = 1, 1 Proprtis of Quarks Isospin So far, w hav discussd thr familis of lptons but principally concntratd on on doublt of quarks, th u and d. W will now introduc othr typs of quarks, along with th nw quantum

More information

Γ W. (GeV) 3. τ e universality in W decays

Γ 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 information

PHYSICS 2150 EXPERIMENTAL MODERN PHYSICS. Lecture 3 Statistical vs. Systematic Errors,Rejection of Data; Weighted Averages

PHYSICS 2150 EXPERIMENTAL MODERN PHYSICS. Lecture 3 Statistical vs. Systematic Errors,Rejection of Data; Weighted Averages PHYSICS 150 EXPERIMENTAL MODERN PHYSICS Lctur 3 Statistical vs. Systmatic Errors,Rjction of Data; Wightd Avrags SO FAR WE DISCUSS STATISTICAL UNCERTAINTY. NOW WHAT ABOUT UNCERTAINTY INVOLVED WITH MEASUREMENT

More information

Neutrino Probes of Dark Energy and Dark Matter

Neutrino 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 information

Pair (and Triplet) Production Effect:

Pair (and Triplet) Production Effect: Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

VII. Quantum Entanglement

VII. Quantum Entanglement VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic

More information

Notes 4: Experimental evidence for electroweak

Notes 4: Experimental evidence for electroweak Nots 4: Exprimntal vidnc for lctrowak hav sn how th EM and wak forcs can b arrangd in a unifid way, i.. all dscribd undr a singl combind st of mathmatics. To summaris, th main stps wr (1) Rbundl th 1 2

More information

Y 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall

Y 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)

More information

Helicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois

Helicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois Helicity: Experimental Status Matthias Grosse Perdekamp, University of Illinois Content o The Experimental Effort o Quark and Sea Quark Helicity è DIS, SIDIS, pp è new FFs for global analysis è results

More information

TESTING A SPIN-2 MEDIATOR IN DECAYS

TESTING A SPIN-2 MEDIATOR IN DECAYS TESTING A SPIN- MEDIATOR IN b s DECAYS BAZENA MEIC Thortical Physics Division Rudjr Boskovic Institut, Zagrb arxiv 1801.07115 in collaboration with Svjtlana Fajfr & Monalisa Patra (IJS, jubljana Windows

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

Moon Moon Devi. INO.

Moon Moon Devi. INO. Moon Moon Dvi. INO. Plan of Th Talk: Motivation. Nutrino intractions and cross sctions. Diffrnt Exprimnts to masur nutrino cross sctions Dscriptions. Rsults. Conclusion. Motivation: To study nuclon structur.

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

Nuclear GPDs and DVCS in Collider kinematics. Vadim Guzey. Theory Center, Jefferson Lab. Outline

Nuclear GPDs and DVCS in Collider kinematics. Vadim Guzey. Theory Center, Jefferson Lab. Outline Nuclear GPDs and DVCS in Collider kinematics Vadim Guzey Theory Center, Jefferson Lab Introduction Outline Nuclear PDFs Nuclear GPDs Predictions for DVCS Conclusions Introduction e(k ) Deeply Virtual Compton

More information

BETA DECAY VISUAL PHYSICS ONLINE

BETA DECAY VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE BETA DECAY Suppos now that a nuclus xists which has ithr too many or too fw nutrons rlativ to th numbr of protons prsnt for stability. Stability can b achivd by th convrsion insid

More information

On the Hamiltonian of a Multi-Electron Atom

On 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 information

Generalized Parton Distributions and Nucleon Structure

Generalized Parton Distributions and Nucleon Structure Generalized Parton Distributions and Nucleon Structure Volker D. Burkert Jefferson Lab With pqcd established we have the tool to understand matter at a deeper level. Nobel prize 2004 - D. Gross, D. Politzer,

More information

Status report of Hermes

Status report of Hermes Status report of Hermes Delia Hasch Physics Research Committee, DESY Oct 27/28 2004 Spin physics: finalised and new results on: inclusive, semi-inclusive and exclusive measurements nuclear effects data

More information

Antonio Pich. IFIC, CSIC Univ. Valencia.

Antonio 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 information

Outline. Thanks to Ian Blockland and Randy Sobie for these slides Lifetimes of Decaying Particles Scattering Cross Sections Fermi s Golden Rule

Outline. Thanks to Ian Blockland and Randy Sobie for these slides Lifetimes of Decaying Particles Scattering Cross Sections Fermi s Golden Rule Outlin Thanks to Ian Blockland and andy obi for ths slids Liftims of Dcaying Particls cattring Cross ctions Frmi s Goldn ul Physics 424 Lctur 12 Pag 1 Obsrvabls want to rlat xprimntal masurmnts to thortical

More information

de/dx Effectively all charged particles except electrons

de/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 information

Intro to Nuclear and Particle Physics (5110)

Intro to Nuclear and Particle Physics (5110) Intro to Nuclar and Particl Physics (5110) March 09, 009 Frmi s Thory of Bta Dcay (continud) Parity Violation, Nutrino Mass 3/9/009 1 Final Stat Phas Spac (Rviw) Th Final Stat lctron and nutrino wav functions

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Electroweak Physics and Searches for New Physics at HERA

Electroweak 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 information

Chapter 3 Lecture 14 Longitudinal stick free static stability and control 3 Topics

Chapter 3 Lecture 14 Longitudinal stick free static stability and control 3 Topics Chaptr 3 Lctur 14 Longitudinal stick fr static stability and control 3 Topics 3.4.4 Rquirmnt for propr stick forc variation 3.4.5 Fl of th stability lvl by th pilot Exampl 3.3 3.5 Dtrmination of stick-fr

More information

HERMES status and future running

HERMES status and future running HERMES status and future running Benedikt Zihlmann University of Gent on behalf of the collaboration DESY PRC Mai 24 p.1/18 Access to Transversity Single spin azimuthal asymmetries on a transverse polarized

More information

Results on the proton structure from HERA

Results 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 information

Event shapes and subjet distributions at HERA

Event 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 information

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt

More information

Present and Future Exploration of the Nucleon Spin and Structure at COMPASS

Present and Future Exploration of the Nucleon Spin and Structure at COMPASS Present and Future Exploration of the Nucleon Spin and Structure at COMPASS 1 2 3 4 5 6 Longitudinal spin structure Transverse spin structure Gluon polarization Primakov: pion polarizabilities DY: Transverse

More information

Schrodinger Equation in 3-d

Schrodinger Equation in 3-d Schrodingr Equation in 3-d ψ( xyz,, ) ψ( xyz,, ) ψ( xyz,, ) + + + Vxyz (,, ) ψ( xyz,, ) = Eψ( xyz,, ) m x y z p p p x y + + z m m m + V = E p m + V = E E + k V = E Infinit Wll in 3-d V = x > L, y > L,

More information

Transverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV

Transverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV Transverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV Dipangkar Dutta Mississippi State University (with Dave Gaskell & Garth Huber) Polarized Target Workshop: June 17-18, 2010 Outline

More information

Shape and Structure of the Nucleon

Shape and Structure of the Nucleon Shape and Structure of the Nucleon Volker D. Burkert Jefferson Lab Science & Technology Peer Review June 25-27, 2003 8/7/2003June 25, 2003 Science & Technology Review 1 Outline: From form factors & quark

More information

Target single- and double-spin asymmetries in DVCS off a longitudinal polarised hydrogen target at HERMES

Target single- and double-spin asymmetries in DVCS off a longitudinal polarised hydrogen target at HERMES Target single- and double-spin asymmetries in DVCS off a longitudinal polarised hydrogen target at HERMES David Mahon On behalf of the HERMES Collaboration DIS 2010 - Florence, Italy Overview Mahon DIS

More information

E hf. hf c. 2 2 h 2 2 m v f ' f 2f ' f cos c

E hf. hf c. 2 2 h 2 2 m v f ' f 2f ' f cos c EXPERIMENT 9: COMPTON EFFECT Rlatd Topics Intractions of photons with lctrons, consrvation of momntum and nrgy, inlastic and lastic scattring, intraction cross sction, Compton wavlngth. Principl Whn photons

More information

Deeply Virtual Compton Scattering off 4. He: New results and future perspectives

Deeply Virtual Compton Scattering off 4. He: New results and future perspectives Deeply Virtual Compton Scattering off 4 He: New results and future perspectives M. Hattawy (On behalf of the CLAS collaboration) 2016 JLab Users Group Workshop and Annual Meeting June 20-22, Jefferson

More information

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004

Physics 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

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding PH Modrn Physics SP11 Final Essay Thr will b an ssay portion on th xam, but you don t nd to answr thos qustions if you submit a final ssay by th day of th final: Sat. 5/7 It dosnʼt mattr how smart you

More information

Structure Functions at Very High Q 2 From HERA

Structure 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 information

Gamma-ray burst spectral evolution in the internal shock model

Gamma-ray burst spectral evolution in the internal shock model Gamma-ray burst spctral volution in th intrnal shock modl in collaboration with: Žljka Marija Bošnjak Univrsity of Rijka, Croatia Frédéric Daign (Institut d Astrophysiqu d Paris) IAU$Symposium$324$0$Ljubljana,$Sptmbr$2016$

More information

Introduction to the quantum theory of matter and Schrödinger s equation

Introduction to the quantum theory of matter and Schrödinger s equation Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ 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 information

Structure Functions and Parton Distribution Functions at the HERA ep Collider

Structure 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 information

Non-universal Gauge Bosons Z and the Process e + e f f

Non-universal Gauge Bosons Z and the Process e + e f f Commun. Thor. Phys. (Bijing, China) 41 (2004) pp. 419 424 c Intrnational Acadmic Publishrs ol. 41, No. 3, March 15, 2004 Non-univrsal Gaug Bosons Z and th Procss + f f YUE Chong-Xing 1 and ANG Shun-Zhi

More information

Electroweak measurements at HERA

Electroweak 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 information

Physics 2D Lecture Slides Lecture 14: Feb 1 st 2005

Physics 2D Lecture Slides Lecture 14: Feb 1 st 2005 Physics D Lctur Slids Lctur 14: Fb 1 st 005 Vivk Sharma UCSD Physics Compton Effct: what should Happn Classically? Plan wav [f,λ] incidnt on a surfac with loosly bound lctrons intraction of E fild of EM

More information

Estimation of the two-photon QED background in Belle II

Estimation 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 information

APP-IV Introduction to Astro-Particle Physics. Maarten de Jong

APP-IV Introduction to Astro-Particle Physics. Maarten de Jong APP-IV Introduction to Astro-Particl Physics Maartn d Jong 1 cosmology in a nut shll Hubbl s law cosmic microwav background radiation abundancs of light lmnts (H, H, ) Hubbl s law (199) 1000 vlocity [km/s]

More information

Results on the proton structure from HERA

Results 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 information

New Muon Lifetime and the Fermi Coupling Constant G F. Kevin Giovanetti James Madison University

New 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 information

Probing Generalized Parton Distributions in Exclusive Processes with CLAS

Probing Generalized Parton Distributions in Exclusive Processes with CLAS Probing Generalized Parton Distributions in Exclusive Processes with CLAS Volker D. Burkert Jefferson Lab The nucleon: from structure to dynamics First GPD related results in DVCS and DVMP Experimental

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

GENERALIZED PARTON DISTRIBUTIONS

GENERALIZED PARTON DISTRIBUTIONS Exploring fundamental questions of NUCLEON STRUCTURE with GENERALIZED PARTON DISTRIBUTIONS Florian Herrmann 16.9.2012 Corfu Summer School LHC COMPASS SPS Versatile facility for hadron structure studies

More information