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Ten Lectures on the ElectroWeak Interactions

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... before Nobel prizes were awarded. Because there is no Nobel prize for golf, you can also eliminate Tiger Woods. That leaves one possibility, Marie Curie. Choice C must be the answer. The type of thinking you used to answer the multiple-choice question is known as indirect reasoning. You can use this ...
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... can be achieved using a Poincare section. In the case of a Sinai billiard (motivated by the discussion of Lorentz gas) the dynamics is fully chaotic, leading to ergodization. More generally we might have mixed phase space that contains ”chaotic sea” as well as ”islands”. Ergodization:– The evolution ...
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... 1. An isometry f is a translation if it is direct and is either the identity or has no fixed points. 2. An isometry f is a rotation if it is a direct isometry and is either the identity or there exists exactly one fixed point P (the center of rotation). 3. An isometry f is a reflection through the l ...
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Noether's theorem



Noether's (first) theorem states that every differentiable symmetry of the action of a physical system has a corresponding conservation law. The theorem was proven by German mathematician Emmy Noether in 1915 and published in 1918. The action of a physical system is the integral over time of a Lagrangian function (which may or may not be an integral over space of a Lagrangian density function), from which the system's behavior can be determined by the principle of least action.Noether's theorem has become a fundamental tool of modern theoretical physics and the calculus of variations. A generalization of the seminal formulations on constants of motion in Lagrangian and Hamiltonian mechanics (developed in 1788 and 1833, respectively), it does not apply to systems that cannot be modeled with a Lagrangian alone (e.g. systems with a Rayleigh dissipation function). In particular, dissipative systems with continuous symmetries need not have a corresponding conservation law.
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