WG3 Report. Tau-Charm and Quarkonia Nora Brambilla, MJ. Matthias Jamin ICREA & IFAE Universitat Autònoma de Barcelona. WG3 Report. Matthias Jamin.
|
|
- Bruno Crawford
- 5 years ago
- Views:
Transcription
1 WG3 Report - and Quarkonia Nora Brambilla, MJ ICREA & IFAE Universitat Autònoma de Barcelona 1
2 2
3 3
4 Ultrasoft Renormalization of the potentials in NRQCD Maximilian in collaboration with André Max-Planck-Institut für Physik, München Maximilian EuroFlavour07 p. 1 4
5 ½ ½ ± ¼ ±µ for ¼ ½ ¼ ¾ Æ WG3 Report Status of Calculations / Summary Ultrasoft NLL running of the potentials Î Î, Ö Î, ¾ is essential for a precise prediction of Ø Øµ ØÓØ at threshold. usoft NNLL mixing contributions to ½ Î from Ö Î, ¾ already compensate a bit for the large usoft NNLL nonmixing contribution: What about Î (dominant at NLL)? w.i.p. Current status of the calculation: [«Ë «ÑÚµ, «Í «ÑÚ ¾ µ] Contribution order /«Ë Î Î Ö Î ¾ Î soft + usoft LL «Ë ÐÒ Úµ Ò, «Í ÐÒ Úµ Ò usoft NLL Ò Ò «Í «Í ÐÒ Úµ Ò 0 full usoft NLL «Í «Í ÐÒ Úµ Ò w.i.p. 0 soft NLL «Ë «Ë ÐÒ Úµ Ò Maximilian EuroFlavour07 p. 14 5
6 Finite lifetime effects in nonrelativistic top pair production Christoph Max-Planck-Institut für Physik, Munich in collaboration with André H. and Pedro Ruiz-Femenía EuroFlavour 07 Orsay Nov 2007 C. J. p.1 6
7 Summary Threshold scan allows for precise m t, y t, Γ t, α s determination Effective theory approach crucial to sum up threshold contributions Unstable top leads to Complex matching conditions UV phase space divergencies Matching conditions for the t t phase space that depend on definition of threshold top pair event Cutoff involves mild power counting breaking Phase space corrections are large (NLO) EuroFlavour 07 Orsay Nov 2007 C. J. p.17 7
8 The Yukawa Coupling at 500 GeV Cailin Measurement Motivation ILC at 500 GeV NLL QCD Polarization NLL EW Conclusion The Yukawa Coupling at 500 GeV Ø Cailin in collaboration with André Max-Planck-Institut für Physik, Munich ØÀ [hep-ph/ ], [hep-ph/ ] Orsay,
9 Conclusion The Yukawa Coupling at 500 GeV Cailin Measurement Motivation ILC at 500 GeV NLL QCD Polarization NLL EW Conclusion Yukawa coupling for test of EWSB ILC at 500 GeV: Phase space is non-relativistic vnrqcd Completed: Strong and electroweak matching conditions at O(NLL) Effects of e + e polarization Formula for the total cross section Increase of total cross section of up to 400% δy t /Y t 10 15% might be possible Work in progress: Electroweak NLL decay effects Phase space matching 9
10 Puzzles of excited charm meson masses In collaboration with Sunanda Banerjee, K. Shivaraj, A. Upadhyay, Physics Letters B 651, ,
11 1 α s and the τ hadronic width Work in process (progress?) with: Martin Beneke All results are preliminary! α s and τ hadronic width EuroFlavour 07, Orsay 11
12 Hadronic Decays of the TAU Lepton within RESONANCE CHIRAL THEORY (R ): EuroFlavour ' November 2007 Univ. Paris-Sud 11, Orsay Pablo Garcés Instituto de Física Corpuscular CSIC-UVEG València (Spain) 12
13 SUMMARY: Hadronic decays of the lepton Tools : PT, R T, Large N c (inspired) Previous work: Outlook : (h 1 h 2 h 3 ) (Gómez Dumm, Pich, Portolés 04) (Gómez Dumm, Pich, Portolés, R. 07 to appear) h 1 h 2 h 3 =3K, 2 2 EuroFlavour '07 FlaviAnet in R T Pablo Garcés Instituto de Física Corpuscular 13
Recent Results in NRQCD
Max-Planck-Institute für Physik (Werner-Heisenberg-Institut) Recent Results in NRQCD Pedro D. Ruiz-Femenía Continuous Advances in QCD 2006 Continuous Advances in QCD 2006 May 11-14, University of Minnesota
More informationTop Quarks, Unstable Particles... and NRQCD
Top Quarks, Unstable Particles... and NRQCD André H. Hoang Max-Planck-Institute for Physics Munich (Thanks to A. Manohar, I. Stewart, T. Teubner, C. Farrell, C. Reisser, M. Stahlhofen ) INT Workshop, May
More informationMatthias Jamin ICREA & IFAE Universitat Autònoma de Barcelona
ICREA & IFAE Universitat Autònoma de Barcelona 1 Particles With M τ = 1.777GeV, only τ leptons decay into hadrons. Tau lifetime: τ τ = 290.6 10 15 sec Γ τ = h/τ τ = 2.27 10 3 ev. 2 Discovered 1975 by Martin
More informationarxiv: v1 [hep-ph] 31 Jul 2009
arxiv:0907.5540v1 [hep-ph] 31 Jul 2009 Frascati Physics Series Vol. XLVIII (2009), pp. 19-24 Young Researchers Workshop: Physics Challenges in the LHC Era Frascati, May 11 and 14, 2009 HADRONIC τ DECAYS
More informationNews from Top/QCD. André H. Hoang. Max-Planck-Institute Munich. ECFA Durham 2004 André Hoang p.1
News from Top/QCD André H. Hoang Max-Planck-Institute Munich Top/QCD @ ECFA Durham 2004 André Hoang p.1 Program Top/QCD Session C. Schwinn: Top couling to Higgs and gauge bosons: 6 and 8 fermion final
More informationExclusive Event Generation for the t t Threshold and the Transition to the Continuum
Exclusive Event Generation for the t t Threshold and the Transition to the Continuum Wolfgang Kilian University of Siegen QWG 2017, Peking University November 2017 F. Bach, B. Chokoufé Nejad, A.H. Hoang,
More informationA pnrqcd approach to t t near threshold
LoopFest V, SLAC, 20. June 2006 A pnrqcd approach to t t near threshold Adrian Signer IPPP, Durham University BASED ON WORK DONE IN COLLABORATION WITH A. PINEDA AND M. BENEKE, V. SMIRNOV LoopFest V p.
More informationWG1: KAON PHYSICS. Johan Bijnens Lund University. bijnens
lavi net WG1: KAON PHYSICS Johan Bijnens Lund University bijnens@thep.lu.se http://www.thep.lu.se/ bijnens Various ChPT: http://www.thep.lu.se/ bijnens/chpt.html Euroflavour07 WG1:Kaon physics Johan Bijnens
More informationDAMTP, University of Cambridge HPQCD
Outline of Talk Phenomenological Motivation Overview of lattice methodology Results Future work -Motivation The CKM Matrix After EW symmetry breaking the standard model in the mass basis contains the flavour
More informationCalibration of the Top Quark Mass Parameter in Pythia 8.2 André H. Hoang
Calibration of the Top Quark Mass Parameter in Pythia 8.2 André H. Hoang University of Vienna Why the top quark is not just heavy Top quark: heaviest known particle Most sensitive to the mechanism of mass
More informationCombined analysis of the decays τ K S π ν τ and
Combined analysis of the decays τ K S π ν τ and τ K ην τ Sergi Gonzàlez-Solís Grup de Física Teòrica (Departament de Física) and Institut de Física d Altes Energies (IFAE), Universitat Autònoma de Barcelona,
More informationarxiv: v1 [hep-ph] 8 Nov 2018
Exclusive Top Threshold Matching at Lepton Colliders DESY, Hamburg, Germany E-mail: juergen.reuter@desy.de arxiv:1811.03950v1 [hep-ph] 8 Nov 2018 Bijan Chokoufé Nejad DESY, Hamburg, Germany E-mail: bijan.chokoufe@desy.de
More informationRenormalon Structure. of Correlation Functions in QCD. Matthias Jamin ICREA & IFAE Universitat Autònoma de Barcelona. Renormalon Structure
of Correlation Functions in QCD ICREA & IFAE Universitat Autònoma de Barcelona 1 The vector correlator is central to the τ hadronic width. It s general perturbative expansion reads: Π (1+0) V (s) = N c
More informationHigh order corrections in theory of heavy quarkonium
High order corrections in theory of heavy quarkonium Alexander Penin TTP Karlsruhe & INR Moscow ECT Workshop in Heavy Quarkonium Trento, Italy, August 17-31, 2006 A. Penin, TTP Karlsruhe & INR Moscow ECT
More informationEffects of Reheating on Leptogenesis
Effects of Reheating on Leptogenesis Florian Hahn-Woernle Max-Planck-Institut für Physik München 2. Kosmologietag Florian Hahn-Woernle (MPI-München) Effects of Reheating on Leptogenesis Kosmologietag 2007
More informationTop Quark Precision Physics at Linear Colliders
Top Quark Precision Physics at Linear Colliders Frank Simon 1 on behalf of the ILC Physics and Detector Study and the CLICdp Collaboration 1 Max-Planck-Institut für Physik, Föhringer Ring 6, 80805 München,
More informationarxiv: v1 [hep-lat] 21 Nov 2011
On the Extraction of the Strong Coupling from Hadronic Tau Decay arxiv:1111.54v1 [hep-lat] 21 Nov 211 Diogo Boito Universitat Autonòma de Barcelona, Barcelona, Spain Oscar Catà Universitat de València
More informationWG1: KAON PHYSICS. Johan Bijnens Lund University. bijnens
lavi net WG1: KAON PHYSICS Johan Bijnens Lund University bijnens@thep.lu.se http://www.thep.lu.se/ bijnens Various ChPT: http://www.thep.lu.se/ bijnens/chpt.html Euroflavour07 WG1:Kaon physics Johan Bijnens
More informationRadiative Electroweak Symmetry Breaking with Neutrino Effects in Supersymmetric SO(10) Unifications
KEKPH06 p.1/17 Radiative Electroweak Symmetry Breaking with Neutrino Effects in Supersymmetric SO(10) Unifications Kentaro Kojima Based on the work with Kenzo Inoue and Koichi Yoshioka (Department of Physics,
More informationCorrections of Order β 3 0α 3 s to the Energy Levels and Wave Function
005 International Linear Collider Workshop - Stanford U.S.A. Corrections of Order β 0α s to the Energy Levels and Wave Function M. Steinhauser Institut für Theoretische Teilchenphysik Universität Karlsruhe
More informationFour-fermion production near the W-pair production threshold. Giulia Zanderighi, Theory Division, CERN ILC Physics in Florence September
Four-fermion production near the W-pair production threshold Giulia Zanderighi, Theory Division, CERN ILC Physics in Florence September 12-14 2007 International Linear Collider we all believe that no matter
More informationCoupled-channel effects in radiative. Radiative charmonium transitions
Coupled-channel effects in radiative charmonium transitions Feng-Kun Guo Helmholtz-Institut für Strahlen- und Kernphysik, Universität Bonn IHEP, Beijing, April 16, 2013 Based on: Guo, Meißner, PRL108(2012)112002;
More informationCharmed mesons in nuclear matter
Charmed mesons in nuclear matter L. Tolos, D. Gamermann, C. Garcia-Recio, E. Oset, R. Molina, J. Nieves and A. Ramos Theory Group. KVI. University of Groningen, Zernikelaan 5, 9747 AA Groningen, The Netherlands
More informationExotic spectroscopy and quarkonia at LHCb
Exotic spectroscopy and quarkonia at LHCb Bo Liu 1 on behalf of the LHCb Collaboration Department of Engineering Physics, Tsinghua Unversity, 100084 Beijing, CHINA and Laboratoire de l Accelerateur Lineaire,
More informationarxiv: v1 [hep-ph] 28 Jul 2017
with Calibrated Uncertainty arxiv:1707.09404v1 [hep-ph] 28 Jul 2017 Departamento de Física Teórica Instituto de Física Universidad Nacional Autónoma de México Apartado Postal 20 364, México CDMX 01000,
More informationATLAS studies of spectroscopy and B-decays
ATLAS studies of spectroscopy and B-decays Zdeněk Doležal on behalf of the ATLAS Collaboration Charles University in Prague 53rd International Winter Meeting on Nuclear Physics 26-30 January 2015 Outline
More informationDeconfinement and Polyakov loop in 2+1 flavor QCD
Deconfinement and Polyakov loop in 2+ flavor QCD J. H. Weber in collaboration with A. Bazavov 2, N. Brambilla, H.T. Ding 3, P. Petreczky 4, A. Vairo and H.P. Schadler 5 Physik Department, Technische Universität
More informationPrecision Top Quark Measurements at Linear Colliders. M. E. Peskin LCWS 2015 November 2015
Precision Top Quark Measurements at Linear Colliders M. E. Peskin LCWS 2015 November 2015 In discussion of the physics case for future e+e- colliders, the top quark is often unappreciated. Some people
More informationThe Heavy Quark Spin Symmetry and SU(3)-Flavour Partners of the X(3872)
The Heavy Quark Spin Symmetry and SU(3)-Flavour Partners of the X(3872) Carlos Hidalgo, J. Nieves and M. Pavón-Valderrama Hypernuclear and Strange Particle Physics 2012 IFIC (CSIC - Universitat de València)
More informationPhenomenology of a pseudoscalar glueball and charmed mesons
JUSTUS-LIEBßIG Universität Giessen T Phenomenology of a pseudoscalar glueball and charmed mesons Walaa I. Eshraim Yukawa Institute for Theoretical Physics, Kyoto University, Japan, June 15th, 2018 Introduction
More informationLectures on NRQCD Factorization for Quarkonium Production and Decay
Lectures on NRQCD Factorization for Quarkonium Production and Decay Eric Braaten Ohio State University I. Nonrelativistic QCD II. Annihilation decays III. Inclusive hard production 1 NRQCD Factorization
More informationEffective Field Theories in QCD
Effective Field Theories in QCD N.RipunjayAcharya,2,withFeng-kunGuo 2 &Ulf-G.Meißner HISKP,UniversityofBonn 2 ITP,CASBeijing Les Houches, 04 July, 207 EFTs in QCD: Acharya Chiral Perturbation Theory with
More informationMotivation: Strongly-coupled Dark Sectors near the Weak Scale
Motivation: Strongly-coupled Dark Sectors near the Weak Scale Dark sectors that contain a new, strongly-coupled, confining force near the weak scale are well-motivated from a wide variety of perspectives:
More informationBound-state effects in ttbar production at the LHC
1 Bound-state effects in ttbar production at the LHC Hiroshi YOKOYA (National Taiwan University) based on works in collaboration with K.Hagiwara(KEK) and Y.Sumino(Tohoku U) GGI workshop, Firenze, 2011.09.28
More informationDeviations from the exponential decay law in strong decays
Deviations from the exponential decay law in strong decays Giuseppe Pagliara Institut für Theoretische Physik Heidelberg, Germany in collaboration with Francesco Giacosa (based on arxiv: 1005.4817) Excited
More informationPhysics at LHC. lecture seven. Sven-Olaf Moch. DESY, Zeuthen. in collaboration with Martin zur Nedden
Physics at LHC lecture seven Sven-Olaf Moch Sven-Olaf.Moch@desy.de DESY, Zeuthen in collaboration with Martin zur Nedden Humboldt-Universität, December 03, 2007, Berlin Sven-Olaf Moch Physics at LHC p.1
More informationRecent Progress on. Tau Lepton Physics. ν τ. A. Pich IFIC, Valencia. Euroflavour 08, IPPP, Durham September 2008
Recent Progress on Tau Lepton Physics ν e, μ W, ν, ν μ, e d θ u A. Pich IFIC, Valencia Euroflavour 08, IPPP, Durham -6 September 8 ν 5 GF m Γ( ν lνl ) = f( m / ) 3 l m r 19π EW W e e, μ ν, ν μ 3 4 f (
More informationHiggs mass implications on the stability of the electroweak vacuum
Higgs mass implications on the stability of the electroweak vacuum J. Elias-Miró Universitat Autònoma de Barcelona (UAB) Institut de Física d Altes Energies (IFAE) IV Jornadas CPAN, November 2012 Work
More informationModified Anti-de-Sitter Metric, Light-Front Quantized QCD, and Conformal Quantum Mechanics
GEOMETRY AND PHYSICS II Institut Henri Poincaré, Nov. 8 &9, 013 Modified Anti-de-Sitter Metric, Light-Front Quantized QCD, and Conformal Quantum Mechanics H.G.Dosch Institut für Theoretische Physik der
More informationarxiv: v1 [hep-ph] 18 Oct 2017
Tracks of resonances in electroweak effective Lagrangians arxiv:1710.06622v1 [hep-ph] 18 Oct 2017 Departamento de Matemáticas, Física y Ciencias Tecnológicas, Universidad Cardenal Herrera-CEU, CEU Universities,
More informationIdentification of the Higgs boson produced in association with top quark pairs in proton-proton
Identification of the Higgs boson produced in association with top quark pairs in proton-proton collision: an analysis of the final state containing three leptons with the ATLAS detector Valentina Vecchio,
More informationApplications of Discrete Mathematics to the Analysis of Algorithms
Applications of Discrete Mathematics to the Analysis of Algorithms Conrado Martínez Univ. Politècnica de Catalunya, Spain May 2007 Goal Given some algorithm taking inputs from some set Á, we would like
More informationDiscussion on (Heavy) Flavor Physics
Discussion on (Heavy) Flavor Physics J. Brod, A. Buras, A. El-Khadra, P. Gambino, C. Monahan, A. Petrov Symposium on Effective Field Theories and Lattice Gauge Theory TUM IAS, May 19, 2016 Joachim Brod
More informationOn t th Production at the ILC
On H Producion a he ILC André H. Hoang & Cailin Farrell MPI, Munich Phys.Rev.D72:014007,2005 [hep-ph/0504220] more o come... ILCWS 05, Snowmass, Augus 14-27 2005 A. H. Hoang p.1 Ouline Inroducion & Saus
More informationStrongly Coupled Dark Matter at the LHC
Strongly Coupled Dark Matter at the LHC Graham Kribs University of Oregon Appelquist et al (LSD Collaboration): 1402.6656; 1503.04203; 1503.04205 GK, Adam Martin, Ethan Neil, Bryan Ostdiek, Tom Tong [in
More informationTop Quark Measurements at the ILC. Akimasa Ishikawa (Tohoku University)
Top Quark Measurements at the ILC Akimasa Ishikawa (Tohoku University) Introduction Top quark is the heaviest elementary particle. m t = 173.1 ± 0.9GeV The mass is close to EW scale v/ 2 = 174GeV (y t
More information2. HEAVY QUARK PRODUCTION
2. HEAVY QUARK PRODUCTION In this chapter a brief overview of the theoretical and experimental knowledge of heavy quark production is given. In particular the production of open beauty and J/ψ in hadronic
More informationReview of Standard Tau Decays from B Factories
Review of Standard Tau Decays from B Factories Fabrizio Salvatore, RHUL Tau mass measurement Tau decays to strange particles: - Measurement of V us using τ s decays - τ KKπν τ, KKKν τ branching fractions
More informationSingle-Top at the Tevatron
Single-Top at the Tevatron Bernd Stelzer University of Toronto on behalf of the CDF and DØD Collaborations 15 th International Conference on Hadron Collider Physics, Michigan State University, 14-18 June
More informationSearches for Leptonic Decays of the B-meson at BaBar
Searches for Leptonic Decays of the B-meson at BaBar Stephen Jacob Sekula (MIT) on behalf of the BaBar collaboration Presented at Frontiers in Contemporary Physics III Vanderbilt University May 22-28,
More informationLooking through the Higgs portal with exotic Higgs decays
Looking through the Higgs portal with exotic Higgs decays Jessie Shelton University of Illinois, Urbana-Champaign Unlocking the Higgs Portal (U. Mass. Amherst) May 1, 2014 A light SM-like Higgs is narrow
More informationHeavy quarkonia at finite temperature: The EFT approach
Heavy quarkonia at finite temperature: he EF approach Jacopo Ghiglieri - echnische Universität München 5th Vienna Central European Seminar on QF 28 November 2008 Outline Motivation Introduction to Effective
More informationLong distance weak annihilation contribution to
Long distance weak annihilation contribution to B ± (π/k) ± l + l Sergio Tostado In collaboration with: A. Guevara, G. López-Castro and P. Roig. Published in Phys. Rev. D 92, 054035 (2015). Physics Department,
More informationPoS(DIS2014)183. Charmonium Production at ATLAS. S. Cheatham on behalf of the ATLAS Collaboration. McGill University
on behalf of the ATLAS Collaboration. McGill University E-mail: susan.cheatham@cern.ch Understanding of the production of P-wave charmonium states is a significant bottleneck in the understanding of charmonium
More informationDark matter and IceCube neutrinos
IL NUOVO CIMENTO 38 C (2015) 31 DOI 10.1393/ncc/i2015-15031-4 Colloquia: IFAE 2014 Dark matter and IceCube neutrinos R. Biondi Dipartimento di Scienze Fisiche e Chimiche, Università degli Studi di L Aquila,
More informationHadron Spectroscopy at COMPASS
Hadron Spectroscopy at Overview and Analysis Methods Boris Grube for the Collaboration Physik-Department E18 Technische Universität München, Garching, Germany Future Directions in Spectroscopy Analysis
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More information(3885)/Z c (3900) XYZ: the case of Z c. Journal of Physics: Conference Series. Related content PAPER OPEN ACCESS
Journal of Physics: Conference Series PAPER OPEN ACCESS XYZ: the case of Z c (3885)/Z c (39) To cite this article: M. Albaladejo et al 16 J. Phys.: Conf. Ser. 742 12 Related content - Modeling new XYZ
More informationLECTURE 2: Super theories
LECTURE 2: Super theories Carlos Muñoz Universidad Autónoma de Madrid & Instituto de Física Teórica UAM/CSIC ISAPP09-Como, July 8-16 Carlos Muñoz Super theories 2 ~0.00000001 Carlos Muñoz Super theories
More informationTHE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY
THE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY Young-Ho Song(RISP, Institute for Basic Science) Collaboration with R. Lazauskas( IPHC, IN2P3-CNRS) U. van Kolck (Orsay, IPN & Arizona
More informationarxiv: v1 [hep-ph] 13 Nov 2013
euniversityofmanchester November 14, 2013 arxiv:1311.3203v1 [hep-ph] 13 Nov 2013 Odd- and even-parity charmed mesons revisited in heavy hadron chiral perturbation theory Mohammad Alhakami 1 School of Physics
More informationInclusive B decay Spectra by Dressed Gluon Exponentiation. Einan Gardi (Cambridge)
Inclusive B decay Spectra by Dressed Gluon Exponentiation Plan of the talk Einan Gardi (Cambridge) Inclusive Decay Spectra Why do we need to compute decay spectra? Kinematics, the endpoint region and the
More informationarxiv:hep-ph/ v1 25 Sep 2002
hep-ph/0209302 Direct Higgs production at hadron colliders arxiv:hep-ph/0209302v1 25 Sep 2002 Massimiliano Grazzini (a,b) (a) Dipartimento di Fisica, Università di Firenze, I-50019 Sesto Fiorentino, Florence,
More informationGlobal fits to radiative b s transitions
Global fits to radiative b s transitions Sébastien Descotes-Genon Laboratoire de Physique Théorique CNRS & Université Paris-Sud 11, 9145 Orsay, France Rencontres de Moriond - Electroweak session 16 March
More informationRare Hadronic B Decays
XLI st Rencontres de Moriond QCD and High-Energy Hadronic Interactions La Thuile, Italy, March 18-5, 6 Rare Hadronic B Decays Jürgen Kroseberg Santa Cruz Institute for Particle Physics University of California,
More informationViability of strongly coupled scenarios with a light Higgs like boson
Beijing IHEP, January 8 th 2013 Viability of strongly coupled scenarios with a light Higgs like boson J.J. Sanz Cillero (PKU visitor) A. Pich, I. Rosell and JJ SC [arxiv:1212.6769 [hep ph]] OUTLINE 1)
More informationSigns of supersymmetry
Signs of supersymmetry Bernard Riley 1 Particles resulting from the breaking of symmetries are arranged symmetrically about mass levels that descend in geometric progression from the Planck Mass within
More informationgeneration Outline Outline Motivation Electroweak constraints Selected flavor constraints in B and D sector Conclusion Nejc Košnik
th Discovery Discovery of of the the 4 4th generation generation Outline Outline Motivation Electroweak constraints Selected flavor constraints in B and D sector Conclusion 1 Introduction Introduction
More informationTop quark physics at lepton colliders. Input from theorists + further studies of e + e - 6 fermion composition. IFIC-LAL, feb 2013
Top quark physics at lepton colliders Input from theorists + further studies of e + e - 6 fermion composition M. Vos (IFIC Valencia) Fundamental issues: The good, the bad and the ugly This is the vertex
More informationLepton Flavour Violation
Michael Roney University of Victoria (Babar Collaboration) Electroweak Session, La Thuile, March 10-17, 2007 A bit of history the importance of earnestly seeing nothing μ γ μ γ μ γ μ μ μ History of e-muon
More informationarxiv:hep-ex/ v1 17 Jan 2001
NEW RESULTS ON α S AND OPTIMIZED SCALES S. BRAVO Institut de Física d Altes Energies, Universitat Autònoma de Barcelona, E-08193 Bellaterra, Spain, E-mail: bravo@ifae.es arxiv:hep-ex/0101022v1 17 Jan 2001
More informationTop quark physics and Electroweak measurements at the ILC. Roman Pöschl
Top quark physics and Electroweak measurements at the ILC Roman Pöschl Journees Collisionneur Lineaire - Lyon Mai 2013 The solid pillars of the LC phyics program Top quark W Boson Higgs Boson Discovered
More informationEW theoretical uncertainties on the W mass measurement
EW theoretical uncertainties on the W mass measurement Luca Barze 1, Carlo Carloni Calame 2, Homero Martinez 3, Guido Montagna 2, Oreste Nicrosini 3, Fulvio Piccinini 3, Alessandro Vicini 4 1 CERN 2 Universita
More informationTop quark pole mass measurements in ATLAS
Top quark pole mass measurements in ATLAS Davide Melini University of Granada & IFIC Valencia TAE, 23rd September 2015 Outline Top quark relevance Measure m pole top using t t+jet. The measurement at 7Tev.
More informationarxiv: v1 [hep-ph] 21 Sep 2007
The QCD potential Antonio Vairo arxiv:0709.3341v1 [hep-ph] 1 Sep 007 Dipartimento di Fisica dell Università di Milano and INFN, via Celoria 16, 0133 Milano, Italy IFIC, Universitat de València-CSIC, Apt.
More informationK form factors and determination of V us from decays
form factors and determination of V us from decays Emilie Passemar Los Alamos National Laboratory The 11th International Workshop on Chiral Dynamics Jefferson Laboratory, Virginia, USA August 7, 01 Outline
More informationToward Precision Top Quark Measurements in e + e Collisions at Linear Colliders
CLICdp-Conf-2017-016 06 October 2017 Toward Precision Top Quark Measurements in e + e Collisions at Linear Colliders N. van der Kolk 1) On behalf of the CLICdp collaboration and the ILC Physics Study Max-Planck
More informationhep2001 Theoretical progress in describing the B-meson lifetimes International Europhysics Conference on High Energy Physics DAMIR BECIREVIC
PROCEEDINGS Theoretical progress in describing the B-meson lifetimes Dipartimento di Fisica, Università di Roma La Sapienza, Piazzale Aldo Moro 2, I-00185 Roma, Italy E-mail: Damir.Becirevic@roma1.infn.it
More informationAnalysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments
Analysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments In Collaboration with Manuel Drees August 23rd, 2010 SUSY10 1 Introduction 2 Ghost Events 3 Simulation 4 Outlook and Summary Introduction
More informationRelativistic correction to the static potential at O(1/m)
Relativistic correction to the static potential at O(1/m) Miho Koma (Inst. f. Kernphysik, Mainz Univ.) Yoshiaki Koma, Hartmut Wittig Lattice 2007, Regensburg, 30 July 2007 We investigate the relativistic
More informationKaluza-Klein Masses and Couplings: Radiative Corrections to Tree-Level Relations
Kaluza-Klein Masses and Couplings: Radiative Corrections to Tree-Level Relations Sky Bauman Work in collaboration with Keith Dienes Phys. Rev. D 77, 125005 (2008) [arxiv:0712.3532 [hep-th]] Phys. Rev.
More informationQuarkonium Free Energy on the lattice and in effective field theories
Quarkonium Free Energy on the lattice and in effective field theories J. H. Weber 1,2 in collaboration with A. Bazavov 2, N. Brambilla 1, P. Petreczky 3 and A. Vairo 1 (TUMQCD collaboration) 1 Technische
More informationGluons at high x in Nuclei at EIC
Gluons at high x in Nuclei at EIC in collaboration with: E. Chudakov, D. Higinbotham, C. Hyde, C. Weiss Jefferson Lab DNP 2015 Fall meeting, Santa Fe, NM Outline Motivation HERA and ZEUS experience EIC
More informationSearches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector
Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector Christopher Bock on behalf of the ATLAS Collaboration SUSY5 - August 7, 5 Introduction Outline Introduction
More informationTop pair production near threshold at LHC (NLO/NLL analysis in NRQCD)
Top@LHC LHC TTbar-Threshold Threshold@ILC/LHC Green Functions Top pair production near threshold at LHC (NLO/NLL analysis in NRQCD) Yuichiro Kiyo TTP, Universität Karlsruhe Collaboration with: J. H. Kühn(KA),
More informationMFT: Motivations and Expectations
Physics Week NFN NF Frascati 18 pril 2012 ntonio Uras for the MFT Working Group yon group @ PN Outline Physics Motivations ow mass and low pt dimuon reach: a unique feature at the H ow pt reach for open
More informationarxiv: v1 [hep-ph] 7 Jan 2013
arxiv:1301.1308v1 [hep-ph] 7 Jan 2013 Electric dipole transitions in pnrqcd Faculty of Physics, University of Vienna, Boltzmanngasse 5, A-1090 Wien E-mail: piotr.pietrulewicz@univie.ac.at We present a
More informationPoS(Confinement8)107. Strangeness and charm at FAIR
FIAS. Goethe-Universität Frankfurt am Main, Ruth-Moufang-Str. 1, 6438 Frankfurt am Main, Germany and Theory Group, KVI, University of Groningen, Zernikelaan, 9747 AA Groningen, The Netherlands E-mail:
More informationTesting the low scale seesaw and leptogenesis
based on 1606.6690 and 1609.09069 with Marco Drewes, Björn Garbrecht and Juraj Klarić Bielefeld, 18. May 2017 Remaining puzzles of the universe BAU baryon asymmetry of the universe WMAP, Planck and Big
More informationParticle Physics. All science is either physics or stamp collecting and this from a 1908 Nobel laureate in Chemistry
Particle Physics JJ Thompson discovered electrons in 1897 Rutherford discovered the atomic nucleus in 1911 and the proton in 1919 (idea of gold foil expt) All science is either physics or stamp collecting
More informationMatter, antimatter, colour and flavour in particle physics
Matter, antimatter, colour and flavour in particle physics Sébastien Descotes-Genon Laboratoire de Physique Théorique CNRS & Univ. Paris-Sud, Université Paris-Saclay, 91405 Orsay, France RBI, Zagreb, 5
More informationTop results from CMS
Top results from CMS Alicia Calderon Instituto de Fisica de Cantabria (CSIC - University of Cantabria) Avda. Los Castros, s.n. Santander, SPAIN On behalf of the CMS collaboration. 1 Introduction The top
More informationSoft-Collinear Effective Theory and B-Meson Decays
Soft-Collinear Effective Theory and B-Meson Decays Thorsten Feldmann (TU München) presented at 6th VIENNA CENTRAL EUROPEAN SEMINAR on Particle Physics and Quantum Field Theory, November 27-29, 2009 Th.
More informationA Domino Theory of Flavor
A Domino Theory of Flavor Peter Graham Stanford with Surjeet Rajendran arxiv:0906.4657 Outline 1. General Domino Framework 2. Yukawa Predictions 3. Experimental Signatures General Domino Framework Inspiration
More informationarxiv: v1 [hep-ph] 9 Dec 2017
Heavy Quark Spin Symmetry Violating Hadronic Transitions of Higher Charmonia arxiv:1712.03425v1 [hep-ph] 9 Dec 2017 CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics, Chinese
More informationParticle Physics Outline the concepts of particle production and annihilation and apply the conservation laws to these processes.
Particle Physics 12.3.1 Outline the concept of antiparticles and give examples 12.3.2 Outline the concepts of particle production and annihilation and apply the conservation laws to these processes. Every
More informationNuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007
Nuclear and Particle Physics 3: Particle Physics Lecture 1: Introduction to Particle Physics February 5th 2007 Particle Physics (PP) a.k.a. High-Energy Physics (HEP) 1 Dr Victoria Martin JCMB room 4405
More informationSupersymmetry at the ILC
Supersymmetry at the ILC Abdelhak DJOUADI (LPT Paris Sud). Introduction 2. High precision measurements 3. Determination of the SUSY lagrangian 4. Connection to cosmology 5. Conclusion For more details,
More informationWho is afraid of quadratic divergences? (Hierarchy problem) & Why is the Higgs mass 125 GeV? (Stability of Higgs potential)
Who is afraid of quadratic divergences? (Hierarchy problem) & Why is the Higgs mass 125 GeV? (Stability of Higgs potential) Satoshi Iso (KEK, Sokendai) Based on collaborations with H.Aoki (Saga) arxiv:1201.0857
More informationMeasuring the top quark Yukawa coupling at the ILC at s = 500 GeV
Measuring the top quark Yukawa coupling at the ILC at s = GeV Phys. Rev. D 84, 1433 (11) Katsumasa Ikematsu (Uni Siegen) for Ryo Yonamine (Sokendai/KEK), Tomohiko Tanae (Univ. of Tokyo), Keisuke Fujii
More information