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Renormalization techniques, quantum

In this chapter, we will focus on the entanglement behavior in QPT for the two-dimensional array of quantum dots, which provide a suitable arena for implementation of quantum computation [88, 89, 103]. For this purpose, the real-space renormalization group technique [91] will be utilized and developed for the finite-size analysis of entanglement. The model that we will be using is the Hubbard model [83],... [Pg.519]

In 1948, techniques introduced by Schvttinger and Feynman enabled these difficulties to be avoided, without being removed. Their relativisti-cally covariant development of the theory allowed such infinite terms to be treated unambiguously, and in particular terms which are to be understood as electrodynamic contributions to the charge and mass of a particle were put in a form which is invariant under Lorentz transformations. The program of charge renormalization and renormalization of mass then enabled such terms to be related to the experimentally observed charge and mass of the particle. See also Quantum Mechanics. [Pg.1393]


See other pages where Renormalization techniques, quantum is mentioned: [Pg.246]    [Pg.199]    [Pg.437]    [Pg.78]    [Pg.91]    [Pg.473]    [Pg.657]    [Pg.455]    [Pg.125]    [Pg.21]    [Pg.268]    [Pg.104]    [Pg.366]    [Pg.296]    [Pg.283]    [Pg.208]    [Pg.191]    [Pg.213]   


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Renormalization

Renormalization techniques

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