Electroweak Correction for the Study of Higgs Potential in LC
|
|
- Derick Francis
- 5 years ago
- Views:
Transcription
1 Elctrowak Corrction for th Study of Higgs Potntial in LC LAPTH-Minamitatya Collaboration LCS , Stanford U. prsntd by K.Kato(Kogakuin U.)
2 Introduction LC: high-prcision xprimnts Rquirs th sam lvl thortical prdiction = Nds highr ordr calculation Higgs study : Cntral targt Intrsting channls = multi-body final stats 1-loop corrction to - 3, 4-bodis : Grat Progrss sinc Spt. 00
3 cross sctions Main channls H vs ZZH Yukawa coupl. Higgs Potntial 3,4 procsss important
4 numbr of diagrams (GRACE:NLG modl) A.Dnnr, J.Kublbck, R.Mrtig, M.Bohm, Z.Phys.C56(199) 61; B.A.Knihl, Z.Phys.C55(199) yars rquird to dvlop 3 tools Automatd Systms ZH tr 1-loop 4(1) 341(119) RADCOR / Loops & Lgs Spt. 00 ννh H tth ZHH 1() 1350(49) 1(6) 37(758) 7(6) 5417(1597) 4() 4470(510) with(without) -scalar couplings
5 tth ZHH Full 1-loop RC availabl GRACE, PLB559(003)5 ννh Dnnr t al., NPB660(003)89 H GRACE, PLB571(003)163 You t al., PLB571(003)85 Dnnr t al., PLB575(003)90 GRACE, PLB576(003)15 Zhang t al., PLB578(004)349 GRACE, PLB600(004)65 ννγ ννhh ν = ν μ, ν ν τ μ ν τ μ, GRACE, NIM A534(004)334 GRACE, Talk by Y.Yasui at Durham(Sp.004) udsc Dnnr tal., hpph/050063
6 Kinmatics library Usr input REDUCE, Form tc. Diagram gnrator diagram dscription amplitud gnrator LOOP symbolic cod TREE.fin.mdl.rin modl fil Mak fil tc. Thory Drawr Diagrams (figur) PS fil FORTRAN cod kinmatics cod gnratd cod Library CHANEL, loop convrgnc information BASES(MC intgral) paramtr fil Cross sctions distributions SPRING (EG managr) Evnts
7 Higgs Potntial Somthing rquird to provid mass Ky for th structur of standard modl H H H H indow to Nw Physics H H H Doubl (tripl) Higgs production Procss
8 - ννhh [ab/gv] 1 >hhνν (without Z) m h =10 GV RS = 1000 GV (ΛδΛ)/Λ HHH coupling dpndnc SM: δλ= Invariant mass of hh [GV] tr old paramtr st
9 ννhhvszhh M H =10 GV ZHH/nunuHH Tr σ(ab) ZHH ννhh
10 ZHH Low FULL calculation ννhh High dominant mchanism (approximation) H H
11 - ννhh
12 - HH Annihilation Boson Exchang Contact Intraction H H H, χ
13 - HH tr 6 diagrams Annihilation, Boson xch., Contact int. B A, C opposit sign 1-loop 87 diagrams 13 groups A : vrtx corr.hhh, H, A, Z B : vrtx corr. H, χh C : Box
14 Chck : Cuv indpndnc Cuv=0 Cuv=100 Cuv=10000
15 Linar Gaug vs Non-Linar Gaug NLG Cuv=0 Cuv=100 LG Cuv=0
16 lading m t formulas A: C H C B: C C: C 4 M = M Z = M H =10 m t =180 α=1/ C C C H 4 = = α m 4 t N C 3πs w M MH = α m s t N C 8πs w M 1sw α m 8s t N C 8πs w M 6sw
17 m t = ( n1) GV ( n = 1,,3,4,5) ral world : NOT m t >>, M H, M Z, proof of th formulas and th prformanc of GRACE systm OK
18 HH(tr) 6 5 σ(pb) 4 3 trlading mt corrction full E corrction (w/o QED) δ(e) & δ(mt) δ(%) 0% 15% 10% 5% 0% -5%
19 - HH δ δ(%) 40% 0% 0% -0% -40% -60% -80% HH 1-loop corrctions δ (Gm) -100% δ V λ=10-1 Gv δ V QED
20 - ννhh numbr of diagrams ν... tr= 81 loop=19638 (prod. st = 1 x 3416) 50M lins of Fortran cod ν mu... tr= 7 loop=89 (prod. st = 6 x 1754)
21 - ννhh
22 s-channl ZHH hp-ph/ Phys.Ltt.B 576(003)15.
23 nunuhh(tr) ννhh 400 σ(ab) nunuhh δ (E) Full calculation M H =10GV δ(%) δ ( G μ )
24 - ννhh 1 Tr Invariant mass of HH M H =10 GV =.5TV =.0TV =1.5TV =1.0TV M(HH) (TV) =0.5TV
25 Summary Higgs Potntial channl ννhh cross sction and its E corrction is calculatd. σ=o(100 ab)and gratr than ZHH in high-e LC rgion ( s 1TV). δ(gmu) is ~10% for s>700gv. Larg diviation from ZHH dominatd by s-channl. HH is studid to chck th t-channl structur of ννhh and has shown validity and limitation of th lading m t formulas.
26 - ννhh
27 ννh hp-ph/0161 Phys.Ltt.B 559(003) 5. s,t channls show diffrnt bhavior gnuin wak corrction in G-schm is -~-4% δ ( s ) δ ( t ) δ H 5αM t = 16πs M = 1.5% δ O(α)total δ G
28 hp-ph/ tth Phys.Ltt.B 571(003) 163.
29 systm componnts Diagram gnration for input procss Amplitud/Matrix lmnt gnration Kinmatics and Intgration (fficincy) Evnt gnration (fficincy & wight) Priphral tools: rul gnrator, diagram slction, QED radiation, PDF, loop intgral library, multi-procss, color flow and intrfac for hadronization, tc.
30 5-point functions = D D D D D d G I σ ν μ σ μν Ll l l l L j j j X r D X D = = l l l 0 0 F D E N = = 4 ) ( α α α l rank M BOX rank M = D X l = = 4 0 )] ( [ 1 α α α α D r b a j j l scalar 5-pnt BOX ν μ μν j ij i j i ij r A r g r r A 1 = = ] [ ) ( j j ij i j ij i X X D D A r r A r = = μ ν μ μ l l N
31 δ(qed), δ(e) σ = σ (1 δ QED δ 0 ) δ non-qed virtural corrctions QED V QED soft QED δ = δ δ δ phas spac subtraction δ QED = hard QED f LL =radiator ~ ~ σ ( v dσ ) ( ) 0δQED dσ 0 fll dσ1 γ d 0 fll hard
32 Non-linar gaug fixing trms ( ) ( ) A Z Z GF F F F F L ξ ξ ξ = ± = ± ± ± ± ± χ κχ χ δ χ ξ β α μ μ μ μ 3 ~ ~ ~ ~ s i H s M Z s c i A i F m m = 3 3 ~ χ ε χ ξ μ μ H c s M Z F Z Z μ F A μ A =
33 Sampls of NLG Fynman ruls )] )( ~ / (1 ) )( ~ / (1 ) ( [ μρ ν νρ μ νρ μ μρ ν ρ μν ξ α ξ α g p g p g p g p p p g A μν α χ g im A ) ~ 1 ( m μν αg A c c A ~ ± m A s i H c c δξ χ ~ 1 m m ± ghost-ghost- vctor-vctor / ghost-ghost-scalar-scalar modifid
34 Non-linar gaug Numrator structur is th sam as Fynman gaug Loop intgral library Vrtics modifid gnral valus #diagrams μν g ( for ξ = 1) old usag rduc #diagram ~ α = 1 no Aχ ~, ~, ~ α, β δ ~ ε, ~ κ Chck gaug invarianc Indpndnc on gaug paramtrs
Electroweak corrections to tri-boson production at the ILC
Elctrowak corrctions to tri-boson production at th ILC Duc Ninh LE ldninh@mppmu.mpg.d ork in collaboration with Fawzi BOUDJEMA, Hao SUN and Marcus EBER Corfu, 2009 Sp 4th Duc Ninh LE, Gaug boson production
More informationStandard Model - Electroweak Interactions. Standard Model. Outline. Weak Neutral Interactions. Electroweak Theory. Experimental Tests.
Standard Modl - Elctrowak Intractions Outlin ak Nutral Intractions Nutral Currnts (NC) Elctrowak Thory ± and Z and γ Discovry of ± Exprimntal Tsts LEP Z Boson Mass and idth Numbr of Nutrinos ± Boson ±
More information1-loop effects of MSSM particles in Higgs productions at the ILC
1-loop ffcts of MSSM particls in Higgs productions at th ILC Yusaku Kouda, Tadashi Kon, Masato Jimbo A, Yoshimasa Kurihara B, Tadashi Ishikawa B, Kiyoshi Kato C, and Masaaki Kuroda D, Siki Univ., Chiba
More informationPHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS
PHYSICS 489/489 LECTURE 7: QUANTUM ELECTRODYNAMICS REMINDER Problm st du today 700 in Box F TODAY: W invstigatd th Dirac quation it dscribs a rlativistic spin /2 particl implis th xistnc of antiparticl
More informationElectroweak Corrections for the Study of the Higgs Potential at the LC
2005 Intrnational Linar ollidr orkshop Stanford, U.S.A. Elctrowak orrctions for th Study of th Higgs Potntial at th L F. Boudja LAPTH, BP.110, Anncy-l-Viux F-74941, Franc J.Fujioto, T.Ishikawa, T.Kanko,
More informationNLO-QCD calculation in GRACE. - GRACE status - Y. Kurihara (KEK) GRACE Group LoopFest IV
NLO-QCD calculation in GRACE - GRACE status - Y. Kurihara (KEK) GRACE Group 19/Aug./2005 @ LoopFest IV GRACE Author list J. Fujimoto, T. Ishikawa, M. Jimbo, T. Kaneko, K. Kato, S. Kawabata, T. Kon, Y.
More informationSearch for the Dark Photon at Belle for 0.27 < m A < 3 GeV/c 2
Sarch for th Dark Photon at Bll for.7 < m A < 3 GV/c Igal Jagl Univrsity of Hawai i at Mānoa for th Bll Collaboration QCD, Montpllir, 6 Juillt BELLE Igal Jagl (UH) Sarch for th Dark photon at Bll QCD /
More informationLEP Higgs Search Results. Chris Tully Weak Interactions and Neutrinos Workshop January 21-26, 2002
LEP Higgs Sarch Rsults Chris Tully Wak Intractions and Nutrinos Workshop January 1-6, 00 Viw of LEP Exprimnts Spontanous Symmtry Braking Higgs Fild 1-complx doublt Hyprcharg(Y) U(1) Y Symmtry Lft-Handd
More informationDIS-Parity. Search for New Physics Through Parity Violation In Deep Inelastic Electron Scattering. The Physics Case
DIS-Parity Sarch for Nw Physics Through Parity Violation In Dp Inlastic Elctron Scattring Th Physics Cas R. Arnold for th DIS-Parity Collaboration Exprimnt Plan by Stv Rock will follow 12 Jun 2003 DIS-Parity
More informationForces. 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 informationIV. e + e annihilation experiments 1. Experimental methods Discovery of the Tau-Lepton 5. hadrons 6. Hadronic resonances
IV. annihilation xprimnts 1. Exprimntal mthods. 3. 4. Discovry of th Tau-Lpton 5. (γ ) µ µ (γ ) hadrons 6. Hadronic rsonancs Lit.: H.U Martyn, Tst of QED in Quantum Elctrodynamics, T.Kinoshita (d.) 1.
More informationElectroweak 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 informationAndre Schneider P621
ndr Schnidr P61 Probl St #03 Novbr 6, 009 1 Srdnicki 10.3 Vrtx for L 1 = gχϕ ϕ. Th vrtx factor is ig. ϕ ig χ ϕ igur 1: ynan diagra for L 1 = gχϕ ϕ. Srdnicki 11.1 a) Dcay rat for th raction ig igur : ynan
More informationDiffractive Dijet Production with Leading Proton in ep Collisions at HERA
Diffractiv Dijt Production with Lading Proton in p Collisions at HERA JHEP [arxiv:150.01683] Radk Žlbčík Charls Univrsity Eric 015 Diffraction Th scattrd proton stays intact Exchang with vacuum quantum
More informationGraduate Students Seminar Paul-Scherrer-Institut. Search for Excited Quarks
Graduat Studnts Sminar 01.10.2003 Paul-Schrrr-Institut Sarch for Excitd Quarks Jan Bckr Univrsity of Zurich Sarch for Excitd Quarks Framwork Excitd frmions and comositnss Phnomnological framwork Production
More informationOutline. 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 informationTESTING 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 informationSearches for Contact Interactions at HERA
Sarchs for Contact Intractions at HERA A.F.Żarncki Univrsity of Warsaw for ZEUS XVI Intrnational Workshop on Dp-Inlastic Scattring and Rlatd Subjcts 7- April 2008, Univrsity Collg London A.F.Żarncki Sarchs
More informationElectroweak and non-resonant corrections to top-pair production near threshold at NNLO
Elctrowak and non-rsonant corrctions to top-pair production nar thrshold at NNLO Martin Bnk Physik Dpartmnt T31, Jams-Franck-Straß 1, Tchnisch Univrsität Münchn, 85748 Garching, Grmany Andras Mair IPPP,
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationElectroweak radiative corrections at colliders
Elctrowak radiativ corrctions at collidrs LE Duc Ninh ldninh@mppmu.mpg.d LE Duc Ninh, MPI für Physik, Munich p.1/43 Outlin Introduction (SM at th prsnt, why NLO?) Full NLO corrctions to + W + W Z, ZZZ
More informationVSMN30 FINITA ELEMENTMETODEN - DUGGA
VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional
More informationHERA. Marc DAVID. On behalf of. H1 and ZEUS COLLABORATIONS. luminosity that increases steadily from year to year. The positron beam energy E e is 27.
OBSERVATION OF EVENTS AT HIGH Q 2 IN REACTIONS + p! + X AT HERA Marc DAVID CEA-Saclay,DSM/DAPNIA/SPP,99 Gif-sur-Yvtt,FRANCE On bhalf of and ZEUS COLLABORATIONS Both HERA colliding xprimnts, and ZEUS hav
More informationRandom Process Part 1
Random Procss Part A random procss t (, ζ is a signal or wavform in tim. t : tim ζ : outcom in th sampl spac Each tim w rapat th xprimnt, a nw wavform is gnratd. ( W will adopt t for short. Tim sampls
More informationEDM Implications for BSM Physics
EDM Implications for BSM Physics Kaori Fyto Univrsity of Massachstts, Amhrst K. Fyto, M. Ramsy-Msolf, T. Shn, PLB788(2019)52 J. d Vris, P. Drapr, K.Fyto, J. Kozaczk and D. Sthrland, 1809.10143 K. Fyto,
More information3 Finite Element Parametric Geometry
3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,
More informationMolecular Orbitals in Inorganic Chemistry
Outlin olcular Orbitals in Inorganic Chmistry Dr. P. Hunt p.hunt@imprial.ac.uk Rm 167 (Chmistry) http://www.ch.ic.ac.uk/hunt/ octahdral complxs forming th O diagram for Oh colour, slction ruls Δoct, spctrochmical
More informationLight Stop Bound State Production at the LHC. Yeo Woong Yoon (KIAS) In collaboration with P. Ko, Chul Kim at Yonsei U.
Light Stop Bound State Production at the LHC Yeo Woong Yoon (KIAS) In collaboration with P. Ko, Chul Kim 0. 6. 8 at Yonsei U. Outline About stop Motivation for light stop Phenomenology Formalism Summary
More informationPrecision Standard Model Tests (at JLab)
Prcision Standard Modl Tsts (at JLab) Xiaochao Zhng Jun 21st, 2018 Th Standard Modl of Particl Physics How should w sarch for nw physics? Prcision SM tsts at Jffrson Lab Qwak, PVDIS Mollr, 12 GV PVDIS
More informationSelf-interaction mass formula that relates all leptons and quarks to the electron
Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris
More informationThat 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 informationDVCS 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 informationTHE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION. Jiro Murata Rikkyo University for the MTV collaboration INPC2016, Sydney, Sep 11-16, 2016
THE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION Jiro Murata Rikkyo Univrsity for th MTV collaboration INPC2016 Sydny Sp 11-16 2016 Rikkyo J. Murata Y. Nakaya Y. Totsuka S. Tanaka R. Tanuma T.
More informationProperties 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 informationThe Generalized PV θ View and their applications in the Severe Weather Events
Th Gnralizd PV θ Viw and thir applications in th Svr Wathr Evnts Shouting Gao Institut of Atmosphric Physics, Chins Acadmy of Scincs, Bijing, China OUTLINE Background Gnralizd Potntial Tmpratur Th Scond
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationNLO event generator for LHC
NLO event generator for LHC Y. Kurihara (KEK) GRACE Group Physics Simulation for LHC 05/Apr./2004 @ KEK Motivation LHC Experimental requirement New Particle Search/Precision Measurement LO-QCD Event generator+k-factor
More informationON A MISSED MECHANISM OF DIELECTRON PRODUCTION IN NUCLEUS-NUCLEUS COLLISIONS.
O A MISSED MECHAISM OF DIELECRO PRODUCIO I UCLEUS-UCLEUS COLLISIOS. A.S. Khrykin IR, Dubna, Moscow Rgion, Russia. MEU 00 un, Collg William and Mary, Williamsburg, Virginia, USA. OULIE Introduction h cas
More informationHYSTERESIS AND BLEACHING OF ABSORPTION BY ELECTRONS ON HELIUM
HYSERESIS AND BLEACHING O ABSORPION BY ELECRONS ON HELIUM D. Ryvkin, 1 M.J. La, and M.I. Dykman 1 1 Dpartmnt of Physics and Astronomy, Michigan Stat Univrsity Royal Holloway, Univrsity of London Dynamics
More informationThe DELPHI experiment at the LEP accelerator at the CERN laboratory
Th DELPHI xprimnt at th LEP acclrator at th CERN laboratory Part 1. Th LEP acclrator Part 2. Th DELPHI xprimnt Part 3. Particl physics rsarch at LEP Th LEP acclrator Th study of collisions btwn lctrons
More informationHydrogen 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 informationHiggs phenomenology & new physics. Shinya KANEMURA (Univ. of Toyama)
Higgs phenomenology & new physics Shinya KANEMURA (Univ. of Toyama) KEKTH07, Dec. 13. 2007 Content of talk Introduction Electroweak Symmetry Breaking Physics of Higgs self-coupling Self-coupling measurement
More informationComputing and Communications -- Network Coding
89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc
More informationPrecision Standard Model Physics
Prcision Standard Modl Physics Stfan Dittmair MPI Munich LoopFst V, SLAC, Jun 2006 Stfan Dittmair (MPI Munich), Prcision Standard Modl Physics 1 1 Introduction Exprimnts at LEP/SLC/Tvatron confirmation
More informationInstantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect
Advancd Matrials sarch Onlin: -8-6 ISS: 66-8985, Vols. 34-36, pp 389-39 doi:.48/www.scintific.nt/am.34-36.389 rans ch Publications, Switzrland Instantanous Cutting Forc Modl in High-Spd Milling Procss
More informationSelf-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016
Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac
More informationBackground: 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 informationVII. 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 informationData 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 informationPreprint Archive - Chemistry Preprint Archive : EDEFlash - COMPUTER PROGRAM F...
Prprint Archiv - Chmistry Prprint Archiv : EDEFlash - COMPUTER PROGRAM F... Pag 1 of MariaAngla Mirls is loggd in Logout Brows Sarch My Sttings Alrts Hlp Quick Sarch Titl, abstract, kywords Author araújo.g.
More informationRefer 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 informationForces via exchange of particles
Introduction to Elmntary Particl Physics. Not 08 Pa 1 of 8 Forcs via xchan of particls Classical pictur: Particl A sts fild F prmittin th whol of spac Particl intracts with this fild Quantum Fild Thory
More informationTransitional Probability Model for a Serial Phases in Production
Jurnal Karya Asli Lorkan Ahli Matmatik Vol. 3 No. 2 (2010) pag 49-54. Jurnal Karya Asli Lorkan Ahli Matmatik Transitional Probability Modl for a Srial Phass in Production Adam Baharum School of Mathmatical
More informationStudy of QCD critical point at high temperature and density by lattice simulations
Stuy of QCD critical point at high tmpratur an nsity by lattic simulations Shinji Ejiri (Brookhavn ational Laboratory) Canonical partition function an finit nsity phas transition in lattic QCD arxiv:84.7
More informationTREATMENT OF THE PLASMA NONLINEAR ABSORPTION LAW AT LINEARLY POLARIZED LASER RADIATION OF RELATIVISTIC INTENSITIES. A. G.
Armnian Journal of Physics, 15, vol. 8, issu, pp. 64-7 TREATMENT OF THE PLASMA NONLINEAR ABSORPTION LAW AT LINEARLY POLARIZED LASER RADIATION OF RELATIVISTIC INTENSITIES A. G. Ghazaryan Cntr of Strong
More informationTheory of Elementary Particles homework VIII (June 04)
Theory of Elementary Particles homework VIII June 4) At the head of your report, please write your name, student ID number and a list of problems that you worked on in a report like II-1, II-3, IV- ).
More informationNew Results from GRACE/SUSY at 1-loop
New Results from GRACE/SUSY at 1-loop J.Fujimoto, T.Ishikawa, M.Jimo, T.Kaneko T.Kon, Y.Kurihara, M.Kuroda Y.Shimizu (Susy group @ Minami-Tateya Collaoration) RADCOR5 Shonan Village, Japan Octoer 6, 5
More informationTop quark effects in composite vector pair production at the LHC
Top quark effects in composite vector pair production at the LHC Antonio Enrique Cárcamo Hernández. Universidad Tecnica Federico Santa Maria. SILAFAE 01, 10th-14th of December of 01. Based on: A. E. Cárcamo
More informationAddition 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 informationarxiv:hep-ph/ v1 21 May 1998
hp-ph/980540 VUTH 98-6 NIKHEF 98-0 FNT/T-98/04 SPIN PHYSICS WITH SPIN-0 HADONS arxiv:hp-ph/980540v May 998. JAKOB Univrsità di Pavia and INFN, Szion di Pavia, Via Bassi 6, I-700 Pavia, Italy, -mail:jakob@pv.infn.it
More informationOptics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007
Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting
More informationThermodynamical insight on the role of additives in shifting the equilibrium between white and grey tin
hrmodynamical insight on th rol of additivs in shifting th quilibrium btwn whit and gry tin Nikolay Dmntv Dpartmnt of Chmistry, mpl Univrsity, Philadlphia, PA 19122 Abstract In this study mthods of statistical
More informationLow-energy QED tests (and what we can learn from them)
Low-nrgy QED tsts (and what w can larn from thm) (0γ) 2γ (4γ) (1γ) 3γ (5γ) Indirct Sarchs for Nw Physics at th tim of LHC Flornc, March 2010 Andrzj Czarncki U. of Albrta & CERN Outlin Gyromagntic factors
More informationSER/BER in a Fading Channel
SER/BER in a Fading Channl Major points for a fading channl: * SNR is a R.V. or R.P. * SER(BER) dpnds on th SNR conditional SER(BER). * Two prformanc masurs: outag probability and avrag SER(BER). * Ovrall,
More informationAddition 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 informationMoon 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 informationPhysics at LHC. lecture one. Sven-Olaf Moch. DESY, Zeuthen. in collaboration with Martin zur Nedden
Physics at LHC lecture one Sven-Olaf Moch Sven-Olaf.Moch@desy.de DESY, Zeuthen in collaboration with Martin zur Nedden Humboldt-Universität, October 22, 2007, Berlin Sven-Olaf Moch Physics at LHC p.1 LHC
More informationarxiv: v1 [hep-ex] 21 May 2013
ELECTROWEAK RESULTS FROM HERA arxiv:5.98v [hp-x] May A.F. ŻARNECKI (on bhalf of th H and ZEUS collaborations) Faculty of Physics, Univrsity of Warsaw, Hoża 69, -68 Warszawa, Poland Nutral and chargd currnt
More informationΓ W. (GeV) 3. τ e universality in W decays
UCR/DØ/99-22 FERMILAB-CONF-99/39-E W and Z Proprtis at th Tvatron arxiv:hp-x/99137v1 18 Oct 1999 1 Introduction John Ellison (for th CDF and DØ Collaborations) Dpartmnt of Physics, Univrsity of California,
More informationFinite Element Models for Steady Flows of Viscous Incompressible Fluids
Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod
More informationNon-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 informationA nonequilibrium molecular dynamics simulation of evaporation
Intrnational Confrnc Passiv and Low Enrgy Cooling 543 A nonquilibrium molcular dynamics simulation of vaporation Z.-J. Wang, M. Chn and Z.-Y. Guo Dpartmnt of Enginring Mchanics, Tsinghua Univrsity, Bijing
More informationFull Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient
Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full
More informationA Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes
Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical
More informationOutline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-
Outlin Advancd Multimdia Signal Procssing #5:Spch Signal Procssing -Procssing- Intllignt Elctronic Systms Group Dpt. of Elctronic Enginring, UEC Basis of Spch Procssing Nois Rmoval Spctral Subtraction
More informationKinetic Integrated Modeling of Heating and Current Drive in Tokamak Plasmas
1 HW/P-1 Kintic Intgratd Modling of Hating and Currnt riv in okamak Plasmas A. Fukuyama 1), H. Nuga 1), S. Murakami 1) 1) Graduat School of Enginring, Kyoto Univrsity, Kyoto, Japan -mail contact of main
More informationCP violation and electric-dipole-moment at low energy τ production with polarized electrons
Nuclar Physics B 763 (2007) 283 292 CP violation and lctric-dipol-momnt at low nrgy τ production with polarizd lctrons J. Brnabéu a,b, G.A. Gonzálz-Sprinbrg c,j.vidal a,b, a Dpartamnt d Física Tòrica Univrsitat
More informationElectroweak corrections with
Electroweak corrections with MadGraph5_aMC@NLO Marco Zaro, LPTHE-UPMC in collaboration with S.Frixione, V.Hirschi, D.Pagani, H.-S. Shao Radcor-Loopfest@UCLA 15-6-215 1 Motivation No clear sign of new physics
More informationExploring Extended Scalar Sectors with Di Higgs Signals: A Higgs EFT Perspective
Exploring Extended Scalar Sectors with Di Higgs Signals: A Higgs EFT Perspective Tyler Corbett Melbourne Node arxiv:1705.02551, with Aniket Joglekar (Chicago), Hao-Lin Li (Amherst), Jiang-Hao Yu (Amherst).
More informationLinear Non-Gaussian Structural Equation Models
IMPS 8, Durham, NH Linar Non-Gaussian Structural Equation Modls Shohi Shimizu, Patrik Hoyr and Aapo Hyvarinn Osaka Univrsity, Japan Univrsity of Hlsinki, Finland Abstract Linar Structural Equation Modling
More information2. Laser physics - basics
. Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"
More informationPhysics 444: Quantum Field Theory 2. Homework 2.
Physics 444: Quantum Field Theory Homework. 1. Compute the differential cross section, dσ/d cos θ, for unpolarized Bhabha scattering e + e e + e. Express your results in s, t and u variables. Compute the
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationEvent Generation for Next to Leading Order Chargino Production at the International Linear Collider
DEY-THEI-26-29 arxiv:hp-ph/64v 3 Oct 26 Evnt Gnration for Nxt to Lading Ordr Chargino Production at th Intrnational Linar Collidr Dissrtation zur Erlangung ds Doktorgrads ds Dpartmnts Physik dr Univrsität
More information. α β γ δ ε ζ η θ ι κ λ μ Aμ ν(x) ξ ο π ρ ς σ τ υ φ χ ψ ω. Α Β Γ Δ Ε Ζ Η Θ Ι Κ Λ Μ Ν Ξ Ο Π Ρ Σ Τ Υ Φ Χ Ψ Ω. Wednesday March 30 ± ǁ
. α β γ δ ε ζ η θ ι κ λ μ Aμ ν(x) ξ ο π ρ ς σ τ υ φ χ ψ ω. Α Β Γ Δ Ε Ζ Η Θ Ι Κ Λ Μ Ν Ξ Ο Π Ρ Σ Τ Υ Φ Χ Ψ Ω Wednesday March 30 ± ǁ 1 Chapter 5. Photons: Covariant Theory 5.1. The classical fields 5.2. Covariant
More informationPRINCIPLES OF PLASMA PROCESSING Course Notes: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA
Atomic Collisions and Spctra 125 PRINCIPLES OF PLASMA PROCESSING Cours Nots: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA I. ATOMIC ENERGY LEVELS Atoms and molculs mit lctromagntic radiation
More informationGang 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 informationMachine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005.
Intrnational Linar Collidr Machin Dtctor Intrfac Workshop: ILCSLAC, January 68, 2005. Prsntd by Brtt Parkr, BNLSMD Mssag: Tools ar now availabl to optimiz IR layout with compact suprconducting quadrupols
More informationCE 530 Molecular Simulation
CE 53 Molcular Simulation Lctur 8 Fr-nrgy calculations David A. Kofk Dpartmnt of Chmical Enginring SUNY Buffalo kofk@ng.buffalo.du 2 Fr-Enrgy Calculations Uss of fr nrgy Phas quilibria Raction quilibria
More informationHiggs Boson Couplings as a Probe of New Physics
Higgs Boson Couplings as a Probe of New Physics Kei Yagyu Based on S. Kanemura, K. Tsumura, KY, H. Yokoya, PRD90, 075001 (2014) S. Kanemura, M. Kikuchi, and KY, PLB731, 27 (2014) S. Kanemura, M. Kikuchi,
More informationNext-to-Leading Order Jet Physics with BLACKHAT
IPPP/09/96 MIT-CTP-4095 SLAC PUB 3868 SB/F/37-09 UCLA/TEP/09/0 Nxt-to-Lading Ordr Jt Physics with BLACKHAT C. F. Brgr a, Z. Brn b, L. J. Dixon c, F. Fbrs Cordro d, D. Ford, f, T. Glisbrg c, H. Ita b, D.
More informationWeak boson scattering at the LHC
Weak boson scattering at the LHC RADCOR 2009 Barbara Jäger University of Würzburg outline weak boson fusion at the LHC: Higgs production at high precision V V jj production @ NLO QCD strongly interacting
More informationPH300 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 informationSec 2.3 Modeling with First Order Equations
Sc.3 Modling with First Ordr Equations Mathmatical modls charactriz physical systms, oftn using diffrntial quations. Modl Construction: Translating physical situation into mathmatical trms. Clarly stat
More informationElectromagnetics Research Group A THEORETICAL MODEL OF A LOSSY DIELECTRIC SLAB FOR THE CHARACTERIZATION OF RADAR SYSTEM PERFORMANCE SPECIFICATIONS
Elctromagntics Rsarch Group THEORETICL MODEL OF LOSSY DIELECTRIC SLB FOR THE CHRCTERIZTION OF RDR SYSTEM PERFORMNCE SPECIFICTIONS G.L. Charvat, Prof. Edward J. Rothwll Michigan Stat Univrsit 1 Ovrviw of
More informationNew Muon Lifetime and the Fermi Coupling Constant G F. Kevin Giovanetti James Madison University
Nw Muon Liftim and th Frmi Coupling Constant G F Kvin Giovantti Jams Madison Univrsity HallC mting, JLAB, Aug 10, 007 a µ = g µ / Prcision FUNDAMENTAL Muon Phyiscs SYMMETRIES Prcision Masurmnts of Standard
More informationRole of the N (2080) resonance in the γp K + Λ(1520) reaction
Role of the N (2080) resonance in the γp K + Λ(1520) reaction Ju-Jun Xie ( ) IFIC, University of Valencia, Spain Collaborator: Juan Nieves Phys. Rev. C 82, 045205 (2010). @ Nstar2011, Jlab, USA, 05/19/2011
More informationAn Exploratory study of Higgs-boson pair production
High-6 KIAS-NCTS Joint Workshop on Particle Physics, String theory and Cosmology An Exploratory study of Higgs-boson pair production Based on : JHEP 58 (5), arxiv : 55.957 Collaborate with : Prof. Kingman
More informationIntroduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013
18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:
More information