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1 16. The grand canonical ensemble theory for a system in
1 16. The grand canonical ensemble theory for a system in

Phase transition of Light - Universiteit van Amsterdam
Phase transition of Light - Universiteit van Amsterdam

Spin The evidence of intrinsic angular momentum or spin and its
Spin The evidence of intrinsic angular momentum or spin and its

... The evidence of intrinsic angular momentum or spin and its associated magnetic moment came through experiments by Stern and Gerlach and works of Goudsmit and Uhlenbeck. The spin is called intrinsic since, unlike orbital angular momentum which is extrinsic, it is carried by point particle in addition ...
QUANTIZATION OF DISCRETE DETERMINISTIC THEORIES BY
QUANTIZATION OF DISCRETE DETERMINISTIC THEORIES BY

... function of (discrete) time. We can still talk about a “quantization procedure”, although it is really nothing but the formal introduction of a Hilbert space. Each state i of the original system is now associated with a (“primitive”) basis element Ie,) of this Hilbert space. If in some time interval ...
Scaling of geometric phase close to multicritical points in cluster
Scaling of geometric phase close to multicritical points in cluster

... phases of matter. Yet, they can be of very different nature. Some of them exhibit approximate orders on a local scale and they can be characterized by their symmetries. Others possess subtler orders that can only be captured by highly non-local observables. One of the major challenging themes in mod ...
PDF
PDF

... The main idea of tomography is to reconstruct the density matrix  or, equivalently, the expectation value of any observable of the system from repeated measurements on an ensemble of identical states. In this paper a ‘spin tomography’ for reconstructing spin states is developed in the framework of ...
2014-15 Archived Abstracts
2014-15 Archived Abstracts

... layers and a phase coherent bilayer. Earlier studies in Hall bar geometry revealed remarkable signatures of the exciton condensate in tunneling and Coulomb drag experiments. The tunneling is reminiscent of the dc Josephson effect [1] and a quantized Hall drag [2] is also observed. However, whether e ...
Magnetic Order in Kondo-Lattice Systems due to Electron-Electron Interactions
Magnetic Order in Kondo-Lattice Systems due to Electron-Electron Interactions

... achieved intrinsically as well, i.e. through a thermodynamic phase transition to, for instance, a ferromagnetic state. This is our main topic here. In what follows we give a qualitative, physical account to this possibility by introducing step by step the model, the necessary conditions, and the res ...
Statistical Mechanics course 203-24171 Number of points (=pts) indicated in margin. 16.8.09
Statistical Mechanics course 203-24171 Number of points (=pts) indicated in margin. 16.8.09

SU(3) Model Description of Be Isotopes
SU(3) Model Description of Be Isotopes

Phys 446: Solid State Physics / Optical Properties Lattice vibrations
Phys 446: Solid State Physics / Optical Properties Lattice vibrations

... (vibrational frequency does not depend on the direction of q) ...
Model of molecular bonding based on the Bohr
Model of molecular bonding based on the Bohr

... 1913 model for molecules [2], which is derivable from an infinite dimensional reduction of the Schrödinger equation [3]. The resulting electron configurations are reminiscent of the Lewis electron-dot structure introduced in 1916 [4]. The surprising feature of our work is that all molecular binding ...
Document
Document

... A Guide to Monte Carlo Simulations in Statistical Physics (2nd ed. , Cambridge) • A number of preprints will be found in Los Alamos Arxiv on the web. # This slide is added after the talk ...
classification of magnetic mate
classification of magnetic mate

Read PDF - Physics (APS) - American Physical Society
Read PDF - Physics (APS) - American Physical Society

NUCLEAR HYDRODYNAMICS To describe such complex
NUCLEAR HYDRODYNAMICS To describe such complex

Section 5: Lattice Vibrations
Section 5: Lattice Vibrations

... E.Y.Tsymbal ...
Crystalline phase for one-dimensional ultra
Crystalline phase for one-dimensional ultra

Holographic Metals and the Fractionalized Fermi
Holographic Metals and the Fractionalized Fermi

... We now focus on the FFL phase of HA in Eq. (6). In this phase the influence of H1 can be treated perturbatively [12] in Vk , and so we can initially neglect H1 . Then the ck form a small Fermi surface defined by H0 , and the spins of HJ are required [12] to form a spin liquid. As discussed earlier, ...
Prezentacja programu PowerPoint
Prezentacja programu PowerPoint

Chapter 1 - New England Complex Systems Institute
Chapter 1 - New England Complex Systems Institute

... analysis given below. This study is the extension of previous works [Burin, Natelson, Osheroff, Kagan, 1998; Burin, Kagan, Maksimov, Polishchuk, 1998; Burin, 1995] where the relaxation of tunneling defects in amorphous solids caused by their 1/R3 interaction has been investigated. The results are al ...
here
here

... IV. Concluding Remarks and Outlook • Not discussed  Ruddlesdon-Popper series of perovskite iridates  formula for a n-layer quasi-2D system  Srn+1IrnO3n+1 for n = 1, 2, ∞ • The n = 1 case (Sr2IrO4) expected to be a high-Tc superconductor, upon doping, owing to its similarity cuprate parent compou ...
Critical and oÿ-critical singularities in disordered quantum magnets H. Rieger
Critical and oÿ-critical singularities in disordered quantum magnets H. Rieger

... analog of \critical slowing down" in the critical dynamics of classical, thermally driven transitions. Together with a third critical exponent, deþning the anomalous dimension of the order parameter þeld (the magnetization), the thermal exponent ü and the dynamical exponent z give a complete descrip ...
Quantum Phase Transitions - Subir Sachdev
Quantum Phase Transitions - Subir Sachdev

... |ji = 2−N/2 |↑ij − |↓ij ...
Conductance of a quantum wire in the Wigner crystal regime
Conductance of a quantum wire in the Wigner crystal regime

... aB = εh̄2 /me2 is the Bohr radius, ε is the dielectric constant, and m is the electron effective mass.) Electronelectron interaction in a 1D system is expected to lead to the formation of a Luttinger liquid with properties very different from those of the non-interacting Fermi gas. The conductance o ...
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Ising model

The Ising model (/ˈaɪsɪŋ/; German: [ˈiːzɪŋ]), named after the physicist Ernst Ising, is a mathematical model of ferromagnetism in statistical mechanics. The model consists of discrete variables that represent magnetic dipole moments of atomic spins that can be in one of two states (+1 or −1). The spins are arranged in a graph, usually a lattice, allowing each spin to interact with its neighbors. The model allows the identification of phase transitions, as a simplified model of reality. The two-dimensional square-lattice Ising model is one of the simplest statistical models to show a phase transition.The Ising model was invented by the physicist Wilhelm Lenz (1920), who gave it as a problem to his student Ernst Ising. The one-dimensional Ising model has no phase transition and was solved by Ising (1925) himself in his 1924 thesis. The two-dimensional square lattice Ising model is much harder, and was given an analytic description much later, by Lars Onsager (1944). It is usually solved by a transfer-matrix method, although there exist different approaches, more related to quantum field theory.In dimensions greater than four, the phase transition of the Ising model is described by mean field theory.
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