'Lorentz' presentation slideshows

Lorentz and CPT violation

Lorentz and CPT violation. Robertus Potting University of the Algarve and CENTRA Faro, Portugal DISCRETE 2012, CFTP, Lisbon, December 2012. Outline. Introduction CPT and Lorentz invariance violation Models with Lorentz Invariance violation (LIV) Kinematic frameworks

935 views • 64 slides

Relativity: from Special to General

Geraint F. Lewis Sydney Institute for Astronomy School of Physics University of Sydney. Relativity: from Special to General.

785 views • 54 slides

PH300 Modern Physics SP11

678 views • 50 slides

Introduction to Event Generators

733 views • 48 slides

Chiral freedom and the scale of weak interactions

Chiral freedom and the scale of weak interactions. proposal for solution of gauge hierarchy problem. model without fundamental scalar new anti-symmetric tensor fields mass term forbidden by symmetry chiral couplings to quarks and leptons chiral couplings are asymptotically free

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Teoria da Relatividade Especial

1.08k views • 42 slides

How perfect is the RHIC liquid?

How perfect is the RHIC liquid?. Jean-Yves Ollitrault, IPhT Saclay BNL colloquium, Feb. 24, 2009 based on Drescher Dumitru Gombeaud & JYO, arXiv:0704.3553 Gombeaud, Lappi, JYO, arXiv:0901.4908 . A nucleus-nucleus collision at RHIC. Two Lorentz-contracted nuclei. collide.

430 views • 33 slides

Introduction The hypercentral Constituent Quark Model

Electromagnetic form factors in the relativized Hypercentral CQM M. De Sanctis, M.M.Giannini, E. Santopinto, A. Vassallo. Introduction The hypercentral Constituent Quark Model The elastic nucleon form factors (relativistic effects) Conclusion. N 05 Frascati, 13 october 2005.

455 views • 31 slides

Special Relativity

Special Relativity. David Berman Queen Mary College University of London. Symmetries in physics. The key to understanding the laws of nature is to determine what things can depend on.

551 views • 30 slides

THE CASE FOR MODIFIED GRAVITY

THE CASE FOR MODIFIED GRAVITY. James Binney Oxford University. Outline. MOND as a replacement for DM (Sanders & McGaugh 02) Absence of DM interior to the Sun (Bissantz et al 03, 04) TeVeS Lorentz-covariant MOND (Bekenstein 2004). NGC 3198. Begeman (1987).

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???????????? ? ??????? ? 6 ?????? (3) ???????

???????????? ? ??????? ? 6 ?????? (3) ???????. ????????????????? ????. ??????. ????????????????? ???????????????????? ??????????????? Drude ??? ???????????? (intraband transition) ??????????????? Lorentz ??? ???????????? (interband transition)

445 views • 26 slides

Mott phases, phase transitions , and the role of zero-energy states in graphene

Mott phases, phase transitions , and the role of zero-energy states in graphene. Igor Herbut (Simon Fraser University) Collaborators: Bitan Roy (SFU) Vladimir Juricic (SFU) Oskar Vafek (FSU). Graphene: 2D carbon ( 1s2, 2s2, 2p2 ) .

404 views • 21 slides

Spontaneous Breakdown (SB) of Symmetry ( ????????? )

Spontaneous Breakdown (SB) of Symmetry ( ????????? ). SB of Discrete Symmetry ( ?????? ). Lagrangian density. real scalar field j with. model. potential. with. This is invariant under. signature change of j :. discrete group Z 2. "discrete symmetry". ???. m 2 j + lj 3 = 0.

352 views • 20 slides

Renmin University of China School of Finance

Renmin University of China School of Finance Bubble or Burst An Exercise in Forecasting Jim Cook Global Technology Management Council Preliminary Remarks "I hold that that man is in the right who is most in league with the future." Henrik Ibsen (1828-1906)

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Higgs Working Group Hans Peter Beck Bern University

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B mesons and CP violation

CP violation has recently (1999-2001) been observed in the decay of mesons containing a b-quark. Previous CP violation studies had always used mesons with an s-quark. Review of CP violation with kaons from Lecture 7. B mesons and CP violation.

342 views • 15 slides

REL3 and REL4 Slides

REL3 and REL4 Slides. Double Slit Experiment. Einstein. More Einstein images. Einstein at the age of three in 1882. Albert Einstein in 1893 (age 14). Lorentz. Measuring the aether. Diagram of Interferometer.

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Decay Rates: Pions

Decay Rates: Pions. u. dbar. Look at pion branching fractions (BF) The Beta decay is the easiest. ~Same as neutron beta decay Q= 4.1 MeV. Assume FT=1600 s. LogF=3.2 (from plot) F= 1600 gives partial width(-1) T=1600/F=1 sec or partial width = 1 sec-1. Pi Decay to e-nu vs mu-nu.

293 views • 10 slides