Titlebook: Ultracold Quantum Fields; Henk T.C. Stoof,Koos B. Gubbels,Dennis B.M. Dicker Book 2009 Springer Science+Business Media B.V. 2009 Bose-Eins

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Chaumont hilfreich, der im Zusammenhang mit Edward Youngs jüngst erschienener heftiger Kritk an Weiss’ Auschwitzdrama . von einem Paradigmenwechsel im Erinnerungsdiskurs der Shoah spricht.. Der antifaschistische Erinnerungsdiskurs läßt sich nach Chaumont wie folgt charakterisieren:

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d. Each token capacity is calculated in a reduced net which eliminates the shared resource. The results are used to determine the number of initial tokens in each .-place. This number can be interpreted as the number of jobs which can be dispatched to the system in the same interval without blocking the system.

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Gaussian Integralshe above-mentioned topics, meaning that proofs will often be omitted or replaced by illustrative examples. The more experienced reader who is already familiar with Gaussian integrals, complex analysis, and Grassmann algebras, can use this chapter for reference.

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Quantum Mechanics completely different from the rules that we know in our everyday life. This set of rules is called quantum mechanics and its success in explaining the microscopic world has been enormous. An important example is Bohr‘s explanation for the discrete spectra of light that is absorbed and emitted by at

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Statistical physicsnamely the micro-canonical, the canonical and the grand-canonical ensemble. In the thermodynamic limit these ensembles become essentially equivalent, such that we can choose the ensemble that is most convenient to work with. In our case, this is nearly always the grand-canonical ensemble, which we t

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Path Integralsh integral, we discuss various ways of solving it and apply these methods to the free particle and to a particle in a potential. We also derive the path-integral expressions for matrix elements of operators and expectation values, where we see that the path-integral formalism gives rise to time-orde

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Second Quantizationantum theory still treated classically, it is commonly referred to as second quantization. Another way to understand this name is by introducing a Lagrangian density that generates the Schrödinger equation upon applying the Euler-Lagrange equations. This means that the fields of the Lagrangian densi

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