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Quantum Computational Renormalization in the - IAP TU
Quantum Computational Renormalization in the - IAP TU

... from measurement outcome |θi on spin j followed by |xi on spin j+1. The dominant AKLT term yields the logical action σx (σx Rz (θ)) = Rz (θ). But the ordering is reversed in the swapped term, and the action on the logical state is instead (σx Rz (θ))σx = Rz (−θ). Interference of the two terms reduce ...
Paper
Paper

... became very broad, we characterized them by an error function fit, with the center of the fitted error function taken as the center of the transition (Fig. 4). In the 1D system, at a very shallow lattice depth of 0.25 ER (corresponding to u=uc  0:08) a sharp transition was observed, and the measure ...
5, 4023 (2014)
5, 4023 (2014)

... optical cavity24. As shown in the following, the interactioninduced spontaneous symmetry breaking of the ground state allows the mapping of the SO-coupled BEC to the well-known Dicke model, leading to the prediction of an intriguing quantum phase transition when the Raman coupling strength is varied ...
Measuring the Rydberg Constant Using Circular Rydberg Atoms in
Measuring the Rydberg Constant Using Circular Rydberg Atoms in

Chapter 12 Thermodynamics and Magnetism
Chapter 12 Thermodynamics and Magnetism

... of local (atomic) or itinerant (conduction) electronic states is lifted (Zeeman effect). At low temperature this results in an induced macroscopic magnetic moment whose vector direction lies parallel to the external field. This is referred to as paramagnetism.3 For most materials removing the extern ...
Newton`s cradle analogue with Bose
Newton`s cradle analogue with Bose

... Classical machines represent a smart way to transmit insight of physical mechanisms concealed into nature. Quantum Mechanics has been one of the most prolific sources of unexpected phenomena, but is often hard to understand. Thus, finding a classical machine which is a paradigm for the quantum natur ...
Ab-initio Modeling of Cold Gases November 11, 2009
Ab-initio Modeling of Cold Gases November 11, 2009

Dynamics of a charged particle in a magnetic
Dynamics of a charged particle in a magnetic

... to zero very slowly we did not determine whether the Lyapunov exponent vanishes exactly or it is very small. For large values of B 1 the calculation does converge to a constant value which is the largest Lyapunov exponent. The transition to extended chaotic motion is seen as an approximate linear ri ...
Spin-polarized transport through two quantum dots Interference and Coulomb correlation effects  P.
Spin-polarized transport through two quantum dots Interference and Coulomb correlation effects P.

... system resistance when magnetic configuration of the system varies from antiparallel to parallel, and is described quantitatively by the ratio (RAP – RP)/RP, where RAP and RP are the resistances in the antiparallel and parallel magnetic configurations, respectively. In the following discussion, we a ...
Phase transitions for N-electron atoms at the large
Phase transitions for N-electron atoms at the large

... values of Z. Figure 5 shows that for Z.Z 1 .2.405 the symmetric solution for N53 is the global minimum, while for 2,Z,Z5Z 1 .2.405 the nonsymmetric solution is the global minimum. At Z52, ionization occurs where one electron moves to an infinite distance and the symmetric N52 solution is the global ...
An edge index for the Quantum Spin-Hall effect
An edge index for the Quantum Spin-Hall effect

Quantum Theory of Molecular Magnetism - cond
Quantum Theory of Molecular Magnetism - cond

... In this chapter I would like to present a short introduction into the field of molecular magnetism and some of the theoretical techniques as well as results. Some parts of the presentation overlap with earlier presentations in Refs. [1, 2]. The synthesis of magnetic molecules shows continuous progre ...
S - ESRF
S - ESRF

... Describe the minimal energy configuration of ground state of electrons in the unfilled shells: 1st rule: Maximization of total spin S consistent with Pauli’s exclusion principle because prevent the electron with the same spin to be in the same place reduces the Coulomb repulsion between electrons 2n ...
114, 125301 (2015)
114, 125301 (2015)

... a stable effective modulation; for very small ω, the SOC strength barely changes and the system is also stable. In the intermediate regime, we use Floquet theory to describe the strong instability of the modulated BEC [17]. Figure 4(c) shows the Floquet band structure of a minimal model spanned by t ...
slides
slides

Multiphoton adiabatic rapid passage: classical transition induced by separatrix crossing
Multiphoton adiabatic rapid passage: classical transition induced by separatrix crossing

Spin States in Graphene Quantum Dots
Spin States in Graphene Quantum Dots

... systems are limited by hyperfine coupling and spin-orbit interactions. In graphene-based nanostructures, both limitations are expected to be significantly reduced in strength [4–7]. The electrostatic tunability of graphene quantum dots as well as the observation of excited states have been demonstra ...
Orbital order in classical models of transition
Orbital order in classical models of transition

... In the t2g compounds (e.g., LaTiO3 ) the general form of Eqs. (1-2) is preserved but the appropriate choice of the π̂rα ’s is now π̂rα = 12 σrα for α = x, y, z, see [13]. This is called the orbital compass model. It is worth noting that an accounting of the strain field in the eg compounds leads dir ...
The Kitaev model
The Kitaev model

... this is true in all the phases. The fermionic spectra can be gapped or gapless In the gapped phases, the different particles (fermions and vortex) have Abelian statistics. Taking any particle around any other, or exchanging two identical particles, only multiplies the wave function by ± 1 Difficult ...
Analysis of a Population Genetics Model with Mutation, Selection
Analysis of a Population Genetics Model with Mutation, Selection

73 013601 (2006)
73 013601 (2006)

Inverse magnetic catalysis in QCD and holography
Inverse magnetic catalysis in QCD and holography

... other than the QCD Lagrangian. The other method, the one we will be using, is to use the holographic principle to try to come up with a dual gravitational theory in which the results can be computed more readily. The above leads to the following problem statement: Can we, using holographic methods, ...
Deviations from exponential law and Van Hove`s “2t” limit
Deviations from exponential law and Van Hove`s “2t” limit

Pdf
Pdf

Midgap states of a two-dimensional antiferromagnetic Mott
Midgap states of a two-dimensional antiferromagnetic Mott

... of charge carriers and that they play a central role in the occurrence of high-temperature superconductivity. While some phenomenological pictures [4], [5] of this anomalous metal have been introduced, a microscopic theory has yet to be formulated. In this paper, we compute the electronic spectrum 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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