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Quantum Electro-Dynamical Time-Dependent Density Functional
Quantum Electro-Dynamical Time-Dependent Density Functional

... [1] E. Runge and E. K. U. Gross, PRL. 52, 997 (1984) [2] M. Farzanehpour and I. V. Tokatly, PRB 86,125130 (2012). ...
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... nonzero eigenspace of H gives a vanishing contribution to (1.9). On the other hand, zero modes of H are zero modes of Q, and (1.9) follows. We consider here two examples with qualitatively different vacuum structures. The first model is a quantum mechanics version of the N = 1 Wess-Zumino field theo ...
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... Since the early days of quantum theory, progress in understanding the physics of quantum many-body systems has been hindered by a serious, well-known computational obstacle. The number of parameters required to describe an arbitrary state of n quantum systems grows exponentially with n, a fact that ...
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Identical Quantum Particles and Weak Discernibility - Philsci

... considering. Because of the symmetry, any feature that can be attributed to one element of the domain can also be attributed to any other. We can therefore not uniquely refer and assign names on the basis of the given structure of properties and relations. It is clearly impossible, for example, to s ...
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The Electronic Partition Function for Atoms or Ions

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Chapter 15 External field problems

... for the exact S-matrix. One easily checks that SS † = I as it must be. Note that a particle subject to a harmonic force with time-dependent coupling strength as defined in (15.11) reflected with probability one. This is a particular feature of the chosen coupling. For systems which are not exactly s ...
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Chemistry 354 - Homework Set IV

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... to rotation in one direction positive m values to rotations in the other direction. For m values of the same absolute value but opposite signs the energies are the same. The two ...
adiabatic quantum computing
adiabatic quantum computing

... Problems which are classically difficult to solve may be solved much more quickly by quantum computing. A new strategy for quantum computing, called adiabatic quantum computing, has been developed to solve a particularly hard problem called exact cover. Preliminary simulations suggest that the new q ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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