Neutrinos are one of the fundamental particles and have only week interaction. Neutrino has a zero mass, a zero charge and a spin 1/2.

Size: px
Start display at page:

Download "Neutrinos are one of the fundamental particles and have only week interaction. Neutrino has a zero mass, a zero charge and a spin 1/2."

Transcription

1 Vladimir Kravtsov

2 Particls of th Standard Modl Within th SM thr ar 3 diffrnt familis of particls. Each lpton has a nutrino associatd with it. Nutrinos ar on of th fundamntal particls and hav only wk intraction. Nutrino has a zro mass, a zro charg and a spin 1/. Dirct masurmnt of th nutrino mass by kinmatical analysis of wak dcays m <. 3V m < 170kV m <18. MV 3/4/011 CSU

3 Th sourcs of nutrinos Natural sourcs = cm E MV = 330/cm 3 E = V S-Kamiokand Sun Nutrinos Rlic Nutrinos Solar Atmosphric Earth (Go ) Suprnova BigBang Artificial sourcs Acclrators Ractors 3/4/011 3 CSU

4 A Brif History of th Nutrino 1914 Th -dcay nrgy consrvation crisis Pauli proposs a nw nutral particl is mittd in -dcay. 193 Frmi nams th nw particl nutrino and introducs four-frmion intraction Th first obsrvation of lctron anti-nutrinos by Rins and Cowan Bruno Pontcorvo proposs nutrino-antinutrino oscillations. 196 Ziro Maki, Masami Nakagawa and Sakata introduc nutrino flavor mixing and flavor oscillations (MNSP matrix). 196 Th muon nutrino is obsrvd at BNL Discovry of nutral currnts at CERN Supr-Kamiokand announcd th vidnc of atmosphric nutrino oscillations 000 First dirct vidnc for th tau nutrino 3/4/011 4 CSU

5 Masurd spctra wr continuous instad of discrt for -body dcay 1914 Nutron dcay Nils Bohr Nils Bohr vn suggstd that prhaps nrgy consrvation did not hold insid th nuclus. At th prsnt stag of atomic thory, howvr, w may say that w hav no argumnt, ithr mpirical or thortical, for upholding th nrgy principl in th cas of -ray disintgrations. n M c E E Pauli proposd that a nutral particl shard th nrgy of bta dcay with th mittd lctron. n p Wolfgang Pauli 1934 n - - M c E E n = p Frmi builds a nw thory of to xplain -dcay basd on th currnt-currnt intraction and namd a nw particl nutrino. E Enrico Frmi 3/4/011 5 CSU

6 Th fist xprimntal dtction cam from th high flux of nutrinos cratd in Savannah Rivr ractor. Discovry of Elctron Nutrino (1956) s Scintillator p n PMTs Cd n 108 n Cd p Scintillator 109 Cd 108 Cd Dlayd signal from n captur on cadmium producing 9 MV in s ' s Prompt signal producing two MV s A fw s latr Positron scop 43 = ( ) 10 cm Scinc 14 (1956) 103; Phys. Rv. 113 (1959) 73 Liquid scintillator tanks Watr CdCl Nutron scop 3/4/011 CSU 6 Th Nobl Priz in Physics 1995 was awardd to Frdrick Rins "for th dtction of th nutrino"

7 Discovry of Muon Nutrino (196) In 196, Schwartz, Stinbrgr and Ldrman built th vry first nutrino bam and prsntd vidnc for th muon nutrino K K Nutrino bam Main sourcs K Scondary sourcs tonn spark chambr dtctor with Al plats n 3/4/011 7 CSU p - 9 intractions wr rgistrd Th Nobl Priz 1998 was awardd to Lon Ldrman, Mlvin Schwartz and Jack Stinbrgr "for th nutrino bam mthod and th dmonstration of th doublt structur of th lptons through th discovry of th muon nutrino "

8 Discovry of Tau Nutrino (000) 800 GV protons from TVatron (FNAL) on Tungstn targt produc Ds msons Dcay of D s mson lpton dcay giv D s l l, l =, =.9x10-13 N X DONUT 9 clan CC vnts wr obsrvd 3/4/011 8 CSU Phys. Rv. D 78 (008) 0500

9 Nutral currnts: triumph of th lctro-wak unification (1973) Winbrg and Salam dvlop a thory of lctrowak intractions, but it rquirs a nutral wak currnt. Th modl introducs two typs of wak intraction: Chargd currnt (CC) and Nutral currnt (NC) CC NC First xampl of NC N X CERN BEBC Gargamll - Gargamll bubbl chambr filld with fron (CF 3 Br) Big Europan Bubbl Chambr 3/4/011 9 CSU

10 Larg nutrino calorimtr typ dtctors A larg sampling calorimtrs can masur larg statistics CC and NC data Nutrino cross sction is vry low FNAL (700 GV) CITF, HPWF, CCFR/NuTV BNL (8 GV) E-776, E-816 CERN (400 GV) Aachn-Padova, CDHS, CHARM IHEP (70 GV) IHEP-ITEP, IHEP-JINR 3/4/ CSU

11 Larg nutrino calorimtr typ dtctors goals 1. Cross sction masurmnts N X - CC DIS N X - NC DIS n p - CC QE p p - NC Elastic. Nuclon structur functions masurmnts - -scattring - Invrs -dcay Bjorkn scaling variabls in th laboratory systm - Enrgy transfrrd to nuclon - 4-momntum transfr In trms of th quark distribution functions 3. Masurmnt of sin W SM paramtrs NuTV Paschos Wolfnstin rlation rmovs - th ffcts of sa quark scattring and is much lss snsitiv to havy quark production 4. Bam-dump xprimnts Sarch prompt nutrinos from charm particls production, Higgs, axion, havy nutrino, 3/4/ CSU 5. Nutrino oscillations

12 CERN: CHARM and CHARM-II ( ) xprimnts CHARM has a fin graind calorimtr with low Z targt plans for good idntification of lctron from lastic -scattring / E 0.0 / E ( GV ) = - lctrons / E = 0.53/ E ( GV ) - hadrons Marbl plans / E = / E ( GV ) - lctrons / E = / E ( GV ) - hadrons Glass plans M=69 t 3/4/011 1 CSU

13 CERN: CDHS ( ) xprimnt CDHS xprimnt was dsignd to study CC DIS and NC DIS nutrino intractions. Dtctor combind th functions of a muon spctromtr and hadron calorimtr. CERN DORTMUND HEIDELBERG SACLAY WARSAW N X N X / E 0.3/ E ( GV ) = - lctrons / E = 0.56 / E ( GV ) - hadrons Di-muon vnt 19 magntizd iron moduls M=150 ton FV=700 ton 13 CSU

14 FNAL: HPWF and NuTV xprimnts Calorimtr / E = 10 1%, GV Nutrino targt: liquid scintillator Activ dtctor: spark chambr and scintillator plans Nutrino targt: iron plans Activ dtctor: drift chambr and scintillator plans M=700 ton 3/4/ CSU

15 3 4 5 At t=0 w hav a flavor ignstats and which ar both mixturs of mass ignstats 1 and : ( 0) = cos sin (0) = sin 1 1 cos According to Schrödingr quation th mass ignstats 1 and with nrgy E 1 and E volv in tim as plan wavs: For rlativistic r m E = p m = p nutrinos (E >> m) E Assuming th sam nrgy for both nutrino componnts w can writ: Th transition probability is, thn, givn by P ( 1 ) = P( ) = sin ( t) If w masur in V, L in km, and E in GV w can writ th abov as: sin = sin Nutrino Oscillations cos 1.7 m ( E (t) L ) (1 = it ( t) ( t) i(p m m / = = 1 1 ie t 1 ie t 1 cos sin 1 /E )t -it m /E E ) 1 sin with m ie ie t t = m sin cos 1 1 sin m Fraction of rmaining nutrinos 1.7 m E L 3/4/011 P ( ) = 1 sin sin ( ) 15 CSU

16 Atmosphric Nutrinos Nutrino Oscillations Discovry (1998) Nutrinos ar producd by cosmic ray intractions in Earth s atmosphr,, Expctation ( ( ) ) SK was masurd th numbr of and intractions as a function of znith angl 41.4m x 39.3m (Diamtr) 50 ktons of pur watr tank with 0 PMTs MC simulation Supr-Kamiokand Particl idntification is basd on th pattrn rcognition of Chrnkov rings arising in watr Muon - clan ring Elctron fuzzy ring 3/4/ CSU

17 ( / ) Data Nutrino Oscillations Discovry (1998) R = ( / ) MC Th rgistration fficincy for muons and lctrons is vry diffrnt R=1 if no oscillation Takuchi, Nutrino 010 At th Nutrino 98 confrnc, SK xprimnt prsntd nw data on th dficit in muon nutrinos producd in th Earth's atmosphr. This dficit dpnds on th distanc th nutrinos travl - an indication that nutrinos oscillat and hav mass. m =.1x10-3 sin 13 =0.0, sin 13 =0.5 R = 0.63 ± 0.03 ± 0.05 (sub-gv) R = 0.65 ± 0.05 ± 0.08 (multi-gv) Jun 5, 1998 oscillation (bst fit) no oscillation Th Nobl Priz in Physics 00 was awardd to Masato Koshiba for pionring contribution to astrophysics, in particular for th dtction of cosmic nutrinos" 3/4/ CSU

18 Mmbr of th IHEP-JINR Nutrino Dtctor Collaboration from 1979 to 000 Nutrino Dtctor Bam dump Exprimnt Sarch of th light Higgs bosons and Axion Limit on th charm production cross sction Oscillation Exprimnt Total cross sction masurmnt 3/4/ CSU

19 IHEP-JINR Nutrino Dtctor Magntic fram X DC Y DC LSC Al Plat - spctromtr M=104 t LSC / - dtctor Targt calorimtr 1.04 X abs Th 70 mkm Mylar containr with liquid scintillator is insrtd into 3mm Al box. Amplitud vs Coordinat MIP position rsolution X = 16 cm 3/4/ CSU

20 Nutrino Dtctor Calibration Tst bam with low momntum sprad Enrgy rsolution vs momntum Th xampls of vnts from pion, lctron, muon and nutrino intractions. Hadrons 7.3%34%/E 1/ (GV) Elctrons 0.1%9.9%/E 1/ (GV) Momntum, GV/c 3/4/011 0 CSU

21 Bam dump Exprimnt 70 GV proton bam Th 70 GV proton bam with 1.1x10 13 avrag proton intnsity pr acclrator puls. Iron bam dump targt was locatd in front of th 54 m long iron muon shild. Th nutrino dtctor followd at a distanc of 64 m downstram of th bam dump. In two runs 1.1x10 18 and 0.6x10 18 protons on targt wr collctd with rlativ targt dnsitis of = 1 and = 3/4/011 1 CSU

22 Bam dump: Sarch of Light Higgs and Axion MSSM Two Higgs doublts with 3 nutral Higgs. Two from ths particls (on scalar H and on psudoscalar A) can b light. Th couplings of (psudo)scalar to frmions s f, p f modl dpndnt coupling constants MSSM SM s f = 1, p f = 0 Th sarch was prformd for dcays into -, - - and - - pairs g g Hf Af = i( = i( G G F F 1/ ) 1/ ) s f = p f for f = u, c, t s f = - f for ratio of vacuum xpctations of Higgs doublts PQ axion p f is th sam as in MSSM m m f f s p f f Four possibl procsss of production 1. Cohrnt proton nuclus intraction Cuts for - and 1. pairs E lm > 3 GV. No track at primary vrtx 3. E had < 1.5 GV rsolution limit of rconstruction program 4. lm < 0.05 rad. Parton parton intraction Cuts for - -pairs 1. Two long tracks (muons). P > 3 GV. /P < 30% 3. E dp E mip < 0.5 GV 4. cos max > Initial stat brmsstrahlung 3/4/011 CSU 4. Bth-Hitlr procss

23 Bam dump: Sarch of Light Higgs and Axion, nd x Scalar x Psudoscalar 95% CL m H, MV m A, MV Higgs boson of SM was xcludd for m H < 80 MV Standard axion was xcludd in th rang < X < 3 and for mass rang MV for most x > MV for most x < 1 95% CL a) Excludd by - and dcays b) Excludd by th - Bth-Hitlr procss c) Excludd by th - Bth-Hitlr procss d) Excludd by a combind fit using a) and b) Particl Data Group, J. Phys. G 33, 1 (006) 3/4/011 3 CSU

24 Bam dump: Charm Production Cross Sction Thr typs of intraction wr studid for stimation of charm production cross sction: 1. Prompt chargd currnt intraction. Prompt chargd currnt intraction 3. Equilibrium or rock muons producd in nutrino intraction at th nd of muon iron shild. Calculation of prompt vnts numbr a) Extrapolation mthod Th charm production dos not dpnd from targt dnsity. Th production of convntional nutrinos is proportionally to th invrs targt dnsity. N prompt = N - N - N ) corrction for th lakag of hadrons showr b) Subtraction mthod Subtraction of calculatd contribution of convntional nutrino intractions from th total numbr of masurd vnts. Cuts for vnts 1. E lm > 3 GV 3. Y = E had /(E lm E had) < 0.4 Cuts for vnts 1. Track lngth in ND 3 abs. Track lngth in magntizd stl 50 cm 3. P 4. Start of track in th fist plan of ND (for muons from muon shild only) Third ordr QCD at m c = 1. GV and m c = 1.5 GV IHEP-ITEP charm <.4 b/nuclon (90% CL) at s = 11.5 GV SCAT IHEP-JINR 3/4/011 4 CSU

25 Oscillation Exprimnt Osc. xprimnt was initiatd by papr of Prof. Conforto from Italy. H studid th rsults of 3 CERN xprimnts and was sing som indication for oscillations. Ths dtctors whr xposd at th sam tim but locatd at th diffrnt distanc from targt. P ( ) x = sin sin 1.7 m L E Masurmnt of Nutrino Total Cross Sction G. Conforto, Nuo. Cim. 103 (1990) 751 Spcial nutrino bam with 1 m short dcay lngth was dvlopd. Th fraction of for such bam was 3.5% which is much highr than for standard nutrino bams. Th lngth of th dcay cavity (L = 1 m) is short whn compard to th distanc from dcay point to th dtctor (7 m avrag) and to th lngth of th nutrino dtctor (L = 5 m). Giv possibility to study ( ) bgd ( L / E) ( ) N xp L / E N 3/4/011 L/E 5 dpndncy R = CSU N L / E MC = ( 1 R) Minimization of with diffrnt L/E paramtrs

26 TK xprimnt ND80 dtctor P0D calibration with rock muons CC QE vnts in P0D First prliminary rsults of TK xprimnt 3/4/011 6 CSU

27 TK (Tokai to Kamioka) xprimnt First off-axis long baslin oscillation nutrino xprimnt with high powr 30 GV proton bam of J-PARC Main Ring 50-kT watr Chrnkov dtctor Japan Proton Acclrator Rsarch Complx Kamioka Tokai 95 km Tokyo J-PARC 3/4/011 7 CSU

28 Main Physics Goals Th Maki Nakagawa Sakata Pontcorvo (MNSP) lpton mixing matrix rlats th mass ignstats ( 1,, 3 ) to th flavor ignstats (,, ) = cos sin 3 3 sin 0 cos U3 3 atmosphric, bam SK atm,kk,minos, TK o o 3 = m ~.5 V 3 10 = cos sin cos i CP sin sin CHOOZ, TK sin cos i CP sin cos 13 < 0.14(90% CL) Masurmnts cos sin sin cos solar, ractor SNO, KamLAND o o 1 = m ~ 8 V 1 10 Masur th mixing paramtr 13 by sarch apparanc ( 1.7 m L E ) P( ) sin sin sin / 13 Prcis masurmnt 3, m 3 by obsrving disapparanc 3 13 ( m L E ) P ( ) 1 sin sin 1.7 / 3/4/ CSU 1 3

29 Off-axis bam Nutrino nrgy dpnds on th angl rlativ to th bam axis Incrasing of th angl givs narrowr nutrino spctrum lik monochromatic narrow bam Off-axis angl was st to.5 whr pak of has an oscillation maximum Narrow nutrino spctrum rducs th backgrounds in th lctron nutrino masurmnt from DIS high nrgy intraction and th high nrgy bam contamination CC QE is dominant procss in rgion of nutrino spctrum at.5 NuFact09 Nutrino flux, au OA /4/011 Enrgy, GV 9 CSU

30 Rconstructd E in CC QE Snsitivity to 13 Dtction of apparanc: intraction 8.3x10 1 POT 5 yars at 750 kw at CP = V Main backgrounds bam contamination NC 0 vnts 3/4/ CSU

31 Dtction of disapparanc Snsitivity to 3 and m 3 SK with oscillation SK w/o oscillation Oscillation changs a form of nutrino spctrum Prsnt limits KK SK 8 x 10 1 POT MINOS 90% CL TK snsitivity sin 3 ) <0.01 m 3 ) < 1 x 10-4 V stat. rror only 3/4/ CSU

32 J-PARC acclrator facility Nar dtctors 30 GV proton acclrator 3/4/011 3 CSU

33 Nar dtctors INGRID ND80 On-axis Nutrino Bam Monitor Off-axis Nutrino Dtctor 3/4/ CSU

34 ND80 off-axis dtctor ND80 dtctor consists of 5 subdtctors: 0 dtctor (PØD) - Optimizd for CC 0 and NC 0 masurmnts - Masurs contamination Trackr: fin-graind dtctor (FGD) and tim projction chambrs (TPC) masurs CC QE, CC 1 and NC 1 intractions Elctromagntic calorimtr (ECAL) dtcts EM activitis coming from PØD/Trackr Sid muon rang dtctor (SMRD) idntification of sid-going muons All dtctors housd in UA1/NOMAD magnt with fild 0. T SMRD Dtctor was commissiond in March 010 and now taking th data during 1 yar 3/4/ CSU

35 Top viw of ND80 dtctor FGDs DSECAL P0D TPCs 3/4/ CSU

36 0 dtctor (P0D) Upstram and Cntral Ecal -catchrs Lad/Scint sandwich 4 suprmoduls (p0duls) Upstram and Cntral Watr Targt Ecals Watr/Scint sandwich P0D 17x35.5mm triangular bars Scintillator dtctors rad out via WLS fibr coupld to Si MPPC: 667 pixl avalanch photodiod, ara of 1.3x 1.3mm First larg-scal us in HEP xprimnts: ~50,000 MPPCs for ND80 3/4/011 CSU 36 Watr Targt SuprP0Dul

37 First nutrino vnt at ND80 Magnt off First nutrino vnt (INGRID) CCQE vnt at Trackr - p 3/4/ CSU

38 First nutrino vnt at SK 3 rd ring 1 st ring 010//4 6:00:06 3 rd ring nd ring 1 st ring nd ring 3/4/ CSU

39 Bottom P0D calibration with rock muons Rock muons ar going outsid to P0D muons producd at nutrino intraction on th outr mattr that is mainly magnt stl, pit construction concrt and rock ground. Top X, mm Y, mm cos X cos Y Enrgy dposition of muon was corrctd by path lngth in scintillator y µ - z 3/4/011 Corrctd CSU cos path lngth 39

40 Chargd currnt quasilastic nutrino intraction (CCQE) in P0D CC QE CC QE is dominant procss in th rgion of TK off-axis nutrino spctra at.5 and has simpl -body kinmatics In th simplst cas of invisibl proton E can b calculatd from masurd momntum and angl of - 3/4/ CSU

41 CCQE: POT s, rquirmnts, cuts, NEUT MC for study of backgrounds, rconstruction fficincy and purity of 1-track and -track CCQE vnts Th total data PoT s numbr is.84x10 19 Th total PoT s numbr of NEUT MC is 1.3x10 0 MC distributions wr normalizd to th total numbr of data PoT s Fiducial Volums 1. Full P0D -34 < Z < mm First 3 and last 1 P0Duls wr xcludd. Watr Targt -136 < Z < mm 4 intrnal P0Duls 3. Cntral Ecal -34 < Z < mm 5 intrnal P0Duls Rquirmnts and cuts 1. 1 or track sgmnts in TPC. Vrtx should b at P0D Fiducial Volum 3. Long track should b ngativ 4. TPC PID corrsponds to muon 3/4/ Good PID via TPC de/dx CSU

42 CCQE: Full P0D Tru Vrtx position Y, mm X, mm 3/4/011 4 Z, mm CSU

43 CCQE: 1-track CCQE and backgrounds for slctd vnts Full P0D Watr CEcal ~ MV shift b/w Data and MC du to th Global rconstructd momntum is not corrctd for track nrgy loss in P0D Small ~ MV shift b/w Data and MC for Ccal du to th short track lngth in P0D 3/4/ Th shift will b corrctd in upcoming vrsion of nd80 softwar CSU

44 CCQE: 1-track CCQE and backgrounds angls for slctd vnts Full P0D Watr CEcal Nic agrmnt btwn Data and MC 3/4/ CSU

45 First TK prliminary rsults 010a data wr collctd during Jan Jun a data Total SK data: 3.3x10 19 PoT (15.5 kw x 10 7 s) Stabl running at 3.8x10 13 PoT/spill ( shots up to 100 kw SK vnt pr-slction was basd on FV cuts, ring counting and PID. and candidats wr slctd for nxt analysis 3/4/ CSU

46 disapparanc analysis Numbr of vnts consistnt with oscillation paramtrs masurd by MINOS/SK/KK 3/4/ CSU

47 Final vnt slction Additional background rjction no dcay lctron m < 105 MV assuming scond ring xist rconstructd E < 150 MV Whn # of dcay lctron cut was applid only 1 candidat of vnt rmains 3/4/ CSU

48 Uppr bound of 13 ar valuatd by indpndnt mthods: A: Fldman-Cousins B: Classical on-sidd limit Systmatic uncrtaintis ar took into account for both analysis. apparanc analysis A B 90% CL uppr limit at m 3= V, CP = 0 Normal hirarchy Invrtd hirarchy 3/4/ CSU

49 Backup slids 3/4/ CSU

50 Futur prospcts Run 010b (from Nov 010 March 011) 9.3x10 13 p/spill (8 bunchs/spill/3.04s) Max bam powr: ~145 kw Total data collctd up to Mar 11: 1.45x10 0 PoT (including run 010a) 3/4/ CSU

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

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

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

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

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

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force By Wndi Wamlr Nutrinos ar charglss, narly masslss articls Most abundant articl in th Univrs Intract with mattr via wak nuclar forc Narly transarnt to mattr Only known ty of articl that can sca from th

More information

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

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

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

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

Refer to Chapter 8 Kaon system Oscillations and CKM mixing matrix Neutrinos

Refer to Chapter 8 Kaon system Oscillations and CKM mixing matrix Neutrinos Chaptr 1 Rfr to Chaptr 8 Kaon systm Oscillations and CKM mixing matrix Nutrinos " # K 1 = 1 $ K K " # K = 1 $ K K C K = K ; C K = K P K = K ; P K = K % ' & % ' & K andk ar not ignstats of CP : CP K = K

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

Department of Radiation Sciences, Uppsala University, Sweden The Svedberg Laboratory, Uppsala, Sweden. 1 Introduction

Department of Radiation Sciences, Uppsala University, Sweden The Svedberg Laboratory, Uppsala, Sweden. 1 Introduction submittd to acta physica slovaca 1 6 η dcay into masurd in pd 3 Hη raction. M. Jacwicz 1, A. Kupść 2 for CELSIUS/WASA Collaboration Dpartmnt of Radiation Scincs, Uppsala Univrsity, Swdn Th Svdbrg Laboratory,

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

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

Final Results from the MEG Experiment and the Status of MEG-II and Mu3e

Final Results from the MEG Experiment and the Status of MEG-II and Mu3e Final Rsults from th MEG Exprimnt and th Status of MEG-II and Mu3 Francsco Rnga INFN Roma BLV 2017 - Clvland, May 15-18 2017 1 LFV in muon dcays µ γ µ µ 2 LFV in muon dcays µ γ µ µ A. D Gouva & P. Vogl

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

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

Neutrino Oscillations Hint at a New Fundamental Interaction

Neutrino Oscillations Hint at a New Fundamental Interaction Nutrino Oscillations Hint at a Nw Fundamntal Intraction Mario Evraldo d Souza Dpartamnto d Física, Univrsidad Fdral d Srgip, São Cristóvão, Srgip, Brazil Abstract It is suggstd that nutrino oscillations

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

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

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

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

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

Neutrino Oscillation Experiments at Reactors and Accelerators

Neutrino Oscillation Experiments at Reactors and Accelerators Nutrino Oscillation Exprimnts at Ractors and Acclrators Gaston Wilqut IIHE-Univrsité Libr d Bruxlls IV èms Rncontrs du Vitnam, Hanoi, July 2000 Contnts CHOOZ and PALO VERDE long baslin xprimnts Sarch for

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

Discovery of first elementary particles

Discovery of first elementary particles Lptons Discovry of first lmntary particls Known particls at th nd of th 30 s Elctron Proton Photon Nutron Positron Muon Pion Nutrino: a particl whos xistnc was hypotsizd without a discovry! Faraday, Goldstin,

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

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

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

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 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

ELECTRON-NEUTRINOS, v e. G. R. Kalbfleisch Brookhaven National Laboratory ABSTRACT

ELECTRON-NEUTRINOS, v e. G. R. Kalbfleisch Brookhaven National Laboratory ABSTRACT -1- SS -121 2251 ELECTRON-NEUTRINOS, v G. R. Kalbflisch Brookhavn National Laboratory ABSTRACT Elctron (rathr than muon) nutrino intractions ar proprly th ons to us in comparing rsults with -p intractions.

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

Lecture 2. Interaction of Radiation with Matter

Lecture 2. Interaction of Radiation with Matter Lctur Intraction of Radiation with Mattr Dats 14.10. Vorlsung 1 T.Stockmanns 1.10. Vorlsung J.Ritman 8.10. Vorlsung 3 J.Ritman 04.11. Vorlsung 4 J.Ritman 11.11. Vorlsung 5 J.Ritman 18.11. Vorlsung 6 J.

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

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

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

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

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

The Search for Supersymmetry

The Search for Supersymmetry Th Sarch for Suprsymmtry Introduction th Standard Modl of Particl Physics Introduction to Collidr Physics Succsss of th Standard Modl What th Standard Modl Dos Not Do Physics Byond th Standard Modl Introduction

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

Physics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma

Physics 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 information

Neutrino Mass and Forbidden Beta Decays

Neutrino 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 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

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

Contemporary, atomic, nuclear, and particle physics

Contemporary, atomic, nuclear, and particle physics Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is

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

Structure of the Atom. Thomson s Atomic Model. Knowledge of atoms in Experiments of Geiger and Marsden 2. Experiments of Geiger and Marsden

Structure of the Atom. Thomson s Atomic Model. Knowledge of atoms in Experiments of Geiger and Marsden 2. Experiments of Geiger and Marsden CHAPTER 4 Structur of th Atom 4.1 Th Atomic Modls of Thomson and Ruthrford 4. Ruthrford Scattring 4.3 Th Classic Atomic Modl 4.4 Th Bohr Modl of th Hydrogn Atom 4.5 Succsss & Failurs of th Bohr Modl 4.6

More information

Search for µ eee at the High Intensity and Technology Frontier: The Mu3e Experiment

Search for µ eee at the High Intensity and Technology Frontier: The Mu3e Experiment Sarch for µ at th High Intnsity and Tchnology Frontir: Th Mu3 Exprimnt Johns-Hopkins Workshop Hidlbrg, July 21-23, 2014 André Schöning Physikalischs Institut, Univrsität Hidlbrg 1 History of LFV Dcay xprimnts

More information

Atomic energy levels. Announcements:

Atomic energy levels. Announcements: Atomic nrgy lvls Announcmnts: Exam solutions ar postd. Problm solving sssions ar M3-5 and Tusday 1-3 in G-140. Will nd arly and hand back your Midtrm Exam at nd of class. http://www.colorado.du/physics/phys2170/

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

TESTING LEPTON UNIVERSALITY WITH RARE PION AND KAON DECAYS Prepared for the 2011 DOE Intensity Frontier Workshop 1

TESTING LEPTON UNIVERSALITY WITH RARE PION AND KAON DECAYS Prepared for the 2011 DOE Intensity Frontier Workshop 1 TESTING LEPTON UNIVESALITY WITH AE PION AND KAON DECAYS Prpard for th 2011 DOE Intnsity Frontir Workshop 1 Douglas Bryman Univrsity of British Columbia Octobr 20, 2011 ABSTACT ar pion and kaon dcays provid

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

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

arxiv: v1 [hep-ex] 7 Jan 2019

arxiv: 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 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

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

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

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

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

Exact formula of 3 flavor ν oscillation probability and its application to high energy astrophysical ν

Exact formula of 3 flavor ν oscillation probability and its application to high energy astrophysical ν Exact formula of 3 flavor ν oscillation probability and its application to high nrgy astrophysical ν Osamu Yasuda Tokyo Mtropolitan nivrsity 1-16 16-5 at Miami5 Contnts 1. Introduction 1.1 Status of ν

More information

A new idea to search for charged lepton flavor violation using a muonic atom

A new idea to search for charged lepton flavor violation using a muonic atom Journal of Physics: Confrnc Sris OPEN ACCESS A nw ida to sarch for chargd lpton flavor violation using a muonic atom To cit this articl: Jo Sato 2014 J. Phys.: Conf. Sr. 485 012036 Rlatd contnt - Sarch

More information

Future neutrino oscillation facilities: physics priorities and open issues

Future neutrino oscillation facilities: physics priorities and open issues Futur nutrino oscillation facilitis: physics prioritis and opn issus Alain Blondl DPNC Sction d Physiqu 24 quai Ansrmt Univrsity of Gnva CH 1211 Gnèv 23 Switzrland basd on an Invitd plnary prsntation at

More information

Learning Spherical Convolution for Fast Features from 360 Imagery

Learning Spherical Convolution for Fast Features from 360 Imagery Larning Sphrical Convolution for Fast Faturs from 36 Imagry Anonymous Author(s) 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 4 5 6 7 8 9 3 3 3 33 34 35 In this fil w provid additional dtails to supplmnt th main papr

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

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with

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

Davisson Germer experiment

Davisson 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 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

4E : The Quantum Universe. Lecture 5, April 5 Vivek Sharma

4E : The Quantum Universe. Lecture 5, April 5 Vivek Sharma 4E : Th Quantum Univrs Lctur 5, April 5 Vivk Sharma modphys@hpmail.ucsd.du An X-ray Tub from 0 th Cntury Xray Th High Enrgy Acclrator of 1900s: producd nrgtic light : X Ray, gav nw optic to subatomic world

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

Detection of Energetic Particles by a Network of HF Propagation Paths in Alaska

Detection of Energetic Particles by a Network of HF Propagation Paths in Alaska Dtction of Enrgtic Particls by a twork of HF Propagation Paths in Alaska A.Y. Wong* HIPAS Obsrvatory, Fairbanks, AK and Dpt of Physics and Astronomy, UCLA *With th assistanc of G. Rosnthal, J. Pau, E.

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

The mechanisms of antihydrogen formation

The mechanisms of antihydrogen formation Th mchanisms of antihydrogn formation E.Lodi Rizzini, L.Vnturlli, N.Zurlo, (ATHENA Collaboration) Prsntd by L.Vnturlli Brscia Univrsity & INFN (Italy) 2.5 cm 10 4 pbars 10 8 + 3T 1 Antihydrogn Exprimnts

More information

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.) Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of

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)

(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 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

N eu trino ()scilla tion

N eu trino ()scilla tion N u trino ()scilla tion Siddhshwar Lal Oscillation as a quantum mchanical phnomnon btwn a nutral particl and its anti particl was first nvisagd in 1955 to undrstand th KO - KO problm. In th study of nuclar

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

Chapter. 3 Wave & Particles I

Chapter. 3 Wave & Particles I Announcmnt Cours wbpag http://highnrgy.phys.ttu.du/~sl/2402/ Txtbook PHYS-2402 Lctur 8 Quiz 1 Class avrag: 14.2 (out of 20) ~ 70% Fb. 10, 2015 HW2 (du 2/19) 13, 17, 23, 25, 28, 31, 37, 38, 41, 44 Chaptr.

More information

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:

1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by: Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any

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

UNIVERSIT.. AT BONN Physikalisches Institut

UNIVERSIT.. AT BONN Physikalisches Institut UNIVERSI.. A BONN Physikalischs Institut Masurmnt of bauty and charm cross sctions in photoproduction using dcays into lctrons with ZEUS at HERA by Markus Jüngst Photoproduction of havy quarks in vnts

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

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

Pion condensation with neutrinos

Pion 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

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

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

Davisson Germer experiment Announcements:

Davisson 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 information

26-Sep-16. Nuclear energy production. Nuclear energy production. Nuclear energy production. Nuclear energy production

26-Sep-16. Nuclear energy production. Nuclear energy production. Nuclear energy production. Nuclear energy production Aim: valuat nrgy-gnration rat pr unit mass. Sun: (chck L /M, human ) nrgy-gnration rat producd from fusion of two nucli a + A: nrgy rlasd pr raction raction rat pr unit volum (includs cross sction and

More information

Paul Scherrer Institut Open Users Meeting BV43 February 22, 2012

Paul Scherrer Institut Open Users Meeting BV43 February 22, 2012 Nw Exprimntal Sarch for μ Paul Schrrr Institut Opn Usrs Mting BV43 Fbruary 22, 2012 André Schöning for th Mu3 Collaboration 1 Lpton Flavor Violating Dcay μ+ ++SUSY Exotic Physics 2 Lpton Flavor Violating

More information

Chapter 8: Electron Configurations and Periodicity

Chapter 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 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

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

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

The Standard Model Lagrangian

The Standard Model Lagrangian Th Standard Modl aranian Elmntary Particl Physics Stron Intraction Fnomnoloy Dio Bttoni Acadmic ar - D. Bttoni Fnomnoloia Intrazioni Forti Dirac Formalism m i j Consrvd Currnt i i i 5 i m Gau Invarianc

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

DRAFT. Future neutrino oscillation facilities: physics priorities and open issues. Alain Blondel

DRAFT. Future neutrino oscillation facilities: physics priorities and open issues. Alain Blondel DRAFT Futur nutrino oscillation facilitis: physics prioritis and opn issus Alain Blondl DPNC Sction d Physiqu 24 quai Ansrmt Univrsity of Gnva CH 1211 Gnèv 23 Switzrland Invitd prsntation at NUFACT05,

More information

ELECTRON-MUON SCATTERING

ELECTRON-MUON SCATTERING ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional

More information