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Electron Configuration Worksheet #1
Electron Configuration Worksheet #1

Quantum Error-Correction Codes on Abelian Groups
Quantum Error-Correction Codes on Abelian Groups

... Note that |x + C2  only depends on the coset of C1 /C2 to which x + C2 belongs. Also |x + C2  is orthogonal to |y + C2, if x and y are representatives of different cosets of C2 . The quantum code CSSG (C1 , C2 ) is defined on the vector space spanned by the states |x+C2  , where x ranges in C1 . I ...
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... decreasing the coupling between the superconducting flux qubit and spin ensemble in diamond. Therefore, it is hoped to understand the origin of this unknown state for the realization of a practical long-lived quantum memory. 2. Results of our research NTT, NII, and Osaka University firstly determine ...
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... direction (but overcorrects substantially). The effective Z that gives the correct groundstate energy in the absence of ee interactions is Z eff  1.70 . [We will derive this result next week using the variational methods (Shankar 16.1)]. But this picture ignores the variation of effective Z with r, ...
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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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