'Mass matrix' diaporamas de présentation

A. Yu. Smirnov

892 views • 74 slides

Flavor Mixing of Quarks and Neutrinos

779 views • 63 slides

720 views • 56 slides

ASTROPARTICLES IN THE LHC ERA

612 views • 54 slides

Nature of neutrino mass

Nature of neutrino mass. Nature of neutrino mass. Smallness may indicate that nature of the neutrino mass (or at least what we observe in oscillations) differs from masses of other fermions. Is it of the same nature as the mass of electron or top quark?.

662 views • 53 slides

Lepton Flavour Violation: an experimental review

563 views • 44 slides

Matakuliah : Dinamika Struktur & Teknik Gempa Tahun : S0774

SINGLE DEGREE OF FREEDOM SYSTEM Equation of Motion, Problem Statement & Solution Methods Pertemuan 19. Matakuliah : Dinamika Struktur & Teknik Gempa Tahun : S0774. Systems with two degree of freedom. Recap. Analysis of various 2DOF systems such as:. Linear systems. Torsional systems.

713 views • 32 slides

Modeling of Plants

Modeling of Plants. Josh Markwordt November 27, 2007. Overview. Modeling Plants L-systems and plants Turtle interpretation of L-systems 2D and 3D examples Simulating plant motion Common plant representations Plant motion based on wind Competition between plants

949 views • 30 slides

Phenomenological Aspects of SUSY B-L Extension of the SM

Phenomenological Aspects of SUSY B-L Extension of the SM. Shaaban Khalil. Centre for Theoretical Physics British University in Egypt. Outline. TeV scale B-L : Minimal bottom-up extension of the SM B-L signatures at LHC Supersymmetric B-L B-L Right-handed (s)neutrino

449 views • 28 slides

Introduction to SimCreator and Multi-Body Dynamics

April 25, 2005. Introduction to SimCreator and Multi-Body Dynamics. What is SimCreator?. GUI Based System Modeling Package Similar to Simulink, SystemBuild, EASY5 Specialized for Realtime System Modeling: Driving Simulation, Flight Simulation, Games, Embedded Control

427 views • 27 slides

Linear System

Linear System. function [A,b,c] = assem_boundary(A,b,p,t,e); np = size(p,2); % total number of nodes bound = unique([e(1,:) e(2,:)]); % boundary nodes inter = setdiff([1:np],bound); % interior nodes

394 views • 27 slides

Dirac equation

Dirac equation. Majorana equation. LRSM ( = Left-Right Symmetric Model ) ??????????????? ?????????? ????????? ??? ??????? ???????? ? ????????? ???????? ?? ????????? ??? ?????? ?????????, ?????? ????????? ??? ???????? ?????? ,

488 views • 27 slides

HOW TO SOLVE THE NAVIER-STOKES EQUATION

1.79k views • 26 slides

MA557/MA578/CS557 Lecture 22

MA557/MA578/CS557 Lecture 22. Spring 2003 Prof. Tim Warburton timwar@math.unm.edu. Interpolation on the Triangle. Recall we are considering a two-dimensional domain. We assume that a triangulation of the domain is given.

338 views • 26 slides

Next Generation Iterative Solvers: Belos & Anasazi November 3 rd , 9:30-10:30am Mike Heroux Ulrich Hetmaniuk Rich L

Next Generation Iterative Solvers: Belos & Anasazi November 3 rd , 9:30-10:30am Mike Heroux Ulrich Hetmaniuk Rich Lehoucq Heidi Thornquist.

443 views • 25 slides

Calculation of absolute neutrino masses in the seesaw extension

Calculation of absolute neutrino masses in the seesaw extension. D . J ur ?iukonis , T. Gajdosik and A. Juodagalvis. Vilnius University , Institute of Theoretical Physics and Astronomy. Content. Seesaw mechanism One-loop corrections Case n R = 1 Case n R = 2 Conclusions.

486 views • 24 slides

Non-standard Higgs Boson interactions and (inverse) implications for LHC

Non-standard Higgs Boson interactions and (inverse) implications for LHC. Daniel Phalen, Brooks Thomas, James Wells Michigan/MCTP, April 2006. Measured Sensitivities to Higgs mass. EWWG, 2005. Observables Compatible with SM. Many observables computed at LEP, SLC, and Tevatron

307 views • 23 slides

AUTOMATIC GENERATION AND INTEGRATION OF EQUATIONS OF MOTION BY OPERATOR OVER-LOADING TECHNIQUES

1. 2. N. AUTOMATIC GENERATION AND INTEGRATION OF EQUATIONS OF MOTION BY OPERATOR OVER-LOADING TECHNIQUES. D. Todd Griffith, Andrew J. Sinclair, James D. Turner, John E. Hurtado, and John L. Junkins Texas A&M University Department of Aerospace Engineering College Station, TX 77840.

339 views • 23 slides

Analysis of Lepton Flavor Violation in SUSY GUT model

Analysis of Lepton Flavor Violation in SUSY GUT model. S.-G. Kim, N. Maekawa, A. Matsuzaki, K. Sakurai, T. Yoshikawa. SI2006 Kazuki Sakurai 8/29. Contents. Review of Lepton Flavor Violation Our Model Estimation and Prediction Numerical Results Summary. Experiment:.

303 views • 19 slides

Lecture 25 Structural Approximation (Fast Reanalysis)

Lecture 25 Structural Approximation (Fast Reanalysis). EGM6365 Structural Optimization 03/12 Given by Shu Shang. Introduction.

253 views • 15 slides