PPT-The signature of the CE in the weakest relativistic explo

Raffaella Margutti Harvard Institute for Theory and Computation On behalf of the Harvard SN forensic team Kyoto2013 What happens when jets barely break out of a star Type Ic SN core. g executor or administrator Printed Name Useful reviews:. Waxman astro-ph/0103186. Ghisellini astro-ph/0111584. Piran astro-ph/0405503. Meszaros astro-ph/0605208. Useful links. http://www-astro.physics.ox.ac.uk/~garret/teaching/. http://www.cv.nrao.edu/course/astr534/. Electromagnetism . (Maxwell) is Lorentz-. invariant. Nuclear . interactions have Lorentz-. invariant . form. Quantum . relativistic version (. Quantum Field Theory . 1940. /. 1972. .. Gravity. ????. 1. Relativistic Programming. Concurrent reading and writing improves performance and scalability. concurrent readers may disagree on the order of concurrent updates. orders may be non-. linearizable. i. Yuri . Lyubarsky. Ben-Gurion University. Beer-. Sheva. , Israel . Universality of . relativistic jets. M 87. M 87. Crab in X-rays. GRBs. t. ime, s. t. ime, s. PKS 2155-304 . Pulsar magnetosphere. when . constraining the stiffness of the symmetry energy. Qingfeng. Li. 1. Outline. 2. Background: on the theoretical side . . Microscopic Many-Body Approaches. . Non-relativistic . Brueckner. -Bethe-Goldstone (BBG) Theory. Yoram. . Bachrach. , Omer Lev, . Shachar. Lovett,. Jeffrey S. . Rosenschein. & . Morteza. . Zadimoghaddam. CoopMAS. 2013. St. Paul, Minnesota. Weakest link scenarios. Cooperative games. I. is a group consisting of . . In classical mechanics, the momentum of a particle is defined as a product of its mass and its velocity, . . In an isolated system of particles, with no net force acting on the system, the total momentum of the system remains the same. However , we can see from a simple though experiment that the quantity . Lecture 4. Books Recommended:. Lectures on Quantum Field Theory by Ashok Das. Advanced Quantum Mechanics by . Schwabl. Relativistic Quantum Mechanics by Greiner. . Quantum Field Theory by Mark . Srednicki. Michael Kolodrubetz. UC Berkeley/LBL. Collaborators:. Anatoli Polkovnikov, Pankaj. Mehta (Boston University). arXiv:1602.01062. http://mkolodru.weebly.com/talks.html. Emergent Newtonian EOM. Emergent Newtonian EOM. PlasMA. Nonequilibrium. Dynamics. in Astrophysics and Material Science. YITP, Kyoto, Japan, Oct. 31-Nov. 3, 2011. Tetsufumi. Hirano. Sophia Univ./. the Univ. of Tokyo. Outline. Introduction. Physics of the quark gluon plasma. PH101. Lec-5. Geometrical properties of 3D space. I. magine . a suitable set of rulers so that the position of a point . P . can . be specified . by the three coordinates (. x. , . y. , . z. ) with respect to this coordinate system, which we . Nuno Lopes . and. José Monteiro. Deriving preconditions by hand is hard; WPs are often non-trivial. WPs derived by hand are often wrong!. Weaker preconditions expose more optimization opportunities. Ball Lightning with Plasma Simulations. Amanda Elliott. Faculty Advisor: Dr. Vladislav Bukshtynov, . Dept. of Mathematical Sciences, Florida Institute of Technology. . Introduction. Ball lightning (BL) is an unexplained phenomenon reported by thousands of eyewitnesses as a fireball, a few cm to 1 m in diameter, moving unpredictably and independently of the wind, sometimes observed during lightning storms. Here a potential theory for the creation of BL is explored [1]. .