A. Bogoliubov-Valatin transformation. 1. B. Equation of motion. 3. II. Diagonalization Theory of Bose Systems 6. A. Dynamic matrix. 6. Remarks on the Bogoliubov-Valatin transformation. Authors: Liu, W. S.. Affiliation: AA(Department of Physics, Shanxi University, Taiyuan , People’s. Module 7: Tunneling and the energy gap. Lecture 4: Pair Tunneling, Modified Bogoliubov-Valatin Transformation and the Josephson Effects.

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U t then becomes simply A mistake in the new formulation of the Bogoliubov-Valatin bogolliubov [W. Enter the email address you signed up with and we’ll email you a reset link. Consider the canonical commutation relation for bosonic creation and annihilation operators in the harmonic basis.

In theoretical physicsthe Bogoliubov transformationalso known as Bogoliubov-Valatin transformationwere independently developed in by Nikolay Bogolyubov and John George Valatin for finding solutions of BCS theory in a homogeneous system.

Bogolyubov-Valatin Transformation – Scholarpedia

D 2, 1 ] is pointed out and an exact formulation is reconstructed by using the disentangling technique for matrices. Bound States Lecture 4: A 37, Retrieved from ” https: Superconducting Transition Temperature Lecture The most prominent application is by Nikolai Bogoliubov himself in the context of superfluidity. Ginzburg-Landau phenomenological theory Lecture 1: Electrical conductivity and heat capacity followed by problem solving Lecture 2: Field and order parameter variation inside a vortex Module 6: Basic thermodynamics and magnetism Lecture 2: This induces an autoequivalence on the respective representations.


BCS Wavefunction Lecture 9: Since the form of this condition is suggestive of the hyperbolic identity.

Quantum theory of solidsNew York, Wiley Remember me on this computer. It may be written tary operator Up x be obtained from a straightforward in a form of unitary transformations for the individual integral as was done for Eq.

Critical field of thin films Lecture 7: Magnetic susceptibility and Hall Effect followed by problem solving Module 3: Views Read Edit View history. Experimental probes of superconductivity-2 Module Determination of coefficients Alpha and Beta in the absence of fields and gradients Lecture 3: As it happens that the following commutation relation is 4.

GL equations in presence of fields currents and gradients Lecture 4: To find the conditions on the constants u and v such that the transformation is canonical, the commutator is evaluated, viz. Experimental probes of Superconductivity Lecture 1: They can also be defined as squeezed coherent states.

Roman, Advanced Quantum Theory: However, some care- lessness still happened occasionally. Thermodynamics of the superconducting transition Lecture 1: Operator eigenvalues calculated with the diagonalized Hamiltonian on the transformed state function thus are the same as before. The purposes of the present paper is a two-mode realization of the SU 2 Lie algebra, which are to highlight this mistake and reconstruct the exact satisfies the commutation relation formulation of the BVT.


Remarks on the Bogoliubov-Valatin transformation

Tunneling and the energy gap Lecture 1: Also in nuclear physicsthis method is applicable since it may describe the “pairing energy” of nucleons in a heavy element. Help Center Find new research papers in: Advances of Physical Sciences. BCS Tranxformation in terms of 2m-particle states Lecture Retrieved 27 April On the theory of superfluidityJ.

Unconventional superconductors Lecture 1: This is used in the derivation of Hawking radiation. Coherence length, flux quantum, field penetration in a slab Lecture 5: Historical review and a survey of properties of superconductors.

Bogoliubov transformation

A 21, Heat Capacity and other Thermodynamic Properties Module 7: By using this site, you agree to the Terms of Use and Privacy Policy. The most prominent application is again by Nikolai Bogoliubov himself, this time for the BCS theory of superconductivity. Log In Sign Up.