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Three Dimensional Dirac Semimetal and Quantum Transports in
Three Dimensional Dirac Semimetal and Quantum Transports in

... insulator, a Weyl semi-metal, or a quantum spin Hall (QSH) insulator with gap more than 100meV. It can also support sizable linear quantum magnetoresistance (MR) even up to room temperature. The nice aspect of Cd3 As2 is the high carrier mobility up to 1.5 m2 V−1 s−1 at room temperature and 8.0 m2 V ...
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Chapter 46
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... Deutsch developed a notion of a quantum mechanical Turing machine. Bernstein, Vazirani, and Yao showed that quantum computers can do anything a classical computer can do with at most a small (logarithmic) slow down. The early 1990s saw the first truly quantum algorithms, algorithms with no classica ...
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Quantum interference effects in a strongly fluctuating magnetic field
Quantum interference effects in a strongly fluctuating magnetic field

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Special Relativity and Quantum Wave Nature of Matter in “Bridge

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3. Generation of the Quantum Fault Table

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Lectures on Thermodynamics and Statistical Mechanics

... U + p V increases with temperature. The latter quantity is called the enthalpy. In general the two specific heats are functions of temperature. The specific heat at constant volume, Cv , can be calculated using statistical mechanics or it can be measured in experiments. Cp can then be evaluated usin ...
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Quantum and Classical Evolution of Chemical Reaction Wave Front

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Chemistry response 3 investigating orbitals
Chemistry response 3 investigating orbitals

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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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