Ultracold Atomic Gases
... a perfect testing ground for a crossover theory due to tunable interactions. Will help understanding high Tc problem. Signature of superfluidity in the crossover / unitary regime is highly nontrivial. We and Duke group have found the strongest evidence for fermionic superfluidity. In the process, we ...
... a perfect testing ground for a crossover theory due to tunable interactions. Will help understanding high Tc problem. Signature of superfluidity in the crossover / unitary regime is highly nontrivial. We and Duke group have found the strongest evidence for fermionic superfluidity. In the process, we ...
PPT - Modeling & Simulation Lab.
... Rigid Body (Single Particle) Newtonian Mechanics (Single Particle) ...
... Rigid Body (Single Particle) Newtonian Mechanics (Single Particle) ...
Homework #1 Chapter 21 The Electric Field I: Discrete Charge
... frictionless taut thread. Find the electric force that acts on the bead as a function of y and determine the sign of q such that this force always points away from the origin. (c) The bead is initially at rest at the origin. If it is given a slight nudge in the +y direction, how fast will the bead b ...
... frictionless taut thread. Find the electric force that acts on the bead as a function of y and determine the sign of q such that this force always points away from the origin. (c) The bead is initially at rest at the origin. If it is given a slight nudge in the +y direction, how fast will the bead b ...
Axioms of Relativistic Quantum Field Theory
... since F (P(−i∂ )G) = P(p)G Klein–Gordon Equation. We study as an explicit example the fundamental solution of the Klein–Gordon equation. The results will be used later in the description of the free boson within the framework of Wightman’s axioms, cf. p. 135, in order to construct a model satisfying ...
... since F (P(−i∂ )G) = P(p)G Klein–Gordon Equation. We study as an explicit example the fundamental solution of the Klein–Gordon equation. The results will be used later in the description of the free boson within the framework of Wightman’s axioms, cf. p. 135, in order to construct a model satisfying ...
The Family Problem: Extension of Standard Model with a
... the gauge fields. In reality, nothing more. Even so far no scalar (Higgs) fields. So it’s a world of “pointlike” Dirac particles (a Dirac world) with interactions. Maybe this is an important guideline to follow. (“Dirac Similarity Principle”.) ...
... the gauge fields. In reality, nothing more. Even so far no scalar (Higgs) fields. So it’s a world of “pointlike” Dirac particles (a Dirac world) with interactions. Maybe this is an important guideline to follow. (“Dirac Similarity Principle”.) ...
