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Date D 0 -D 0 Oscillation Niels van de Vegte & Roel Tempelaar Supervisor: Johan Messchendorp Kernfysisch Versneller Instituut
Date Basics of the Standard Model
Date Basics of the Standard Model
Date Hadrons: Baryons Proton Neutron
Date Hadrons: Neutral mesons
Date Fundamental force: Strong interaction
Date Fundamental force: Weak interaction
Date generations quark mixing Strong interaction Eigenstates Weak interaction Eigenstates
Date Cabibbo surpressed/favoured WeakStrong
Date Cabibbo surpressed/favoured Rates Cabibbo favoured Cabibbo surpressed
Date Cabibbo surpressed/favoured
Date Cabibbo angle measurement
Date Cabibbo-Kobayashi-Maskawa matrix WeakStrongUnitary matrix
Date Neutral D meson oscillation
Date Schrödinger equation
Date Single particle case Time evolution Mass Inverse lifetime
Date Single particle case Time evolution Time-dependent Schrödinger equation Hamiltonian
Date Hamiltonian Mixing CP violation
Date Hamiltonian CP violation
Date Hamiltonian Eigenstates
Date Hamiltonian Eigenvalues
Date Dimensionless ratios
Weak interactions I. Radulescu Sub-atomic physics seminar October 2005 _____________________________________________ Nuclear Geophysics Division Kernfysisch.
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1Chris Parkes Part II CP Violation in the SM Chris Parkes.
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Atomic Physics – Part 3 Ongoing Theory Development To accompany Pearson Physics PowerPoint presentation by R. Schultz
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Francisco Antonio Physics 129 November 23, 2010 Li Zhengdao and Yang Zhenning, 1953.
A New Theory of Neutrino Oscillations Netta Engelhardt
The Discoveries of Particle & Nuclear Physics Models and Experimental Facts.
10/29/2007Julia VelkovskaPHY 340a Lecture 4: Last time we talked about deep- inelastic scattering and the evidence of quarks Next time we will talk about.
June 11, 2007 Oral Examination Observation of CP Violation in Kaon Decays Igor Senderovich.
SYNTHESIS The Standard Model 1.Elementary particles 2.Strong nuclear force 3.Weak nuclear force 4.The Standard Model.
1 outline ● Part I: some issues in experimental b physics ● why study b quarks? ● what does it take? ● Part II: LHCb experiment ● Part III: LHCb first.
Standard Model. Subatomic World Protons, neutrons, and electrons make up atoms. Photons are particles that convey electromagnetic energy. Force carrierForce.
Particle Physics: Status and Perspectives Part 4: The Standard Model Manfred Jeitler.
Fundamental principles of particle physics G.Ross, CERN, July08.
Gabriel González Sprinberg, July Standard Model and beyond: particles & interactions Gabriel González Sprinberg Instituto de Física, Facultad de.
P Spring 2002 L16Richard Kass B mesons and CP violation CP violation has recently ( ) been observed in the decay of mesons containing a b-quark.
PARTICLE PHYSICS Particles and Interactions. Classifying Particles Most particles fall broadly into two types which can then be broken down further The.
Quantum Electrodynamics Dirac Equation : spin 1/2.
Properties and Decays of Heavy Flavor S-Wave Hadrons Rohit Dhir Department of Physics, Yonsei University, Seoul Dated:11 th June, 2012.
PARTICLE PHYSICS. INTRODUCTION The recorded tracks of sub atomic particles resulting from the collision of two protons in the ATLAS experiment at the.
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Jeopardy Jeopardy PHY101 Chapter 12 Review Study of Special Relativity Cheryl Dellai.
5.3.2 Fundamental Particles. (a) explain that since protons and neutrons contain charged constituents called quarks they are, therefore, not fundamental.
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B s Mixing Parameters and the Search for CP Violation at CDF/D0 H. Eugene Fisk Fermilab 14th Lomonosov Conference Moscow State University August ,
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