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ISM 08
ISM 08

Quantum numbers for relative ground states of antiferromagnetic
Quantum numbers for relative ground states of antiferromagnetic

... numbers N of spin sites and spin quantum numbers s where the interaction is given by antiferromagnetic nearest neighbor exchange7–12 . One quantity of interest is the shift quantum number k = 0, . . . N − 1 associated with the cyclic shift symmetry of the rings. The corresponing crystal momentum is ...
Quantum Mechanical Modelling and Optical Spectroscopy of
Quantum Mechanical Modelling and Optical Spectroscopy of

... We rely on fossil fuels for more than 80% of our current energy needs, a situation which is not sustainable in the long-term. On top of this, the energy demand is expected to grow by almost half over the next two decades.[1] The amount of energy the earth’s surface receives from the sun in one hour ...
FrustrationVSFactorization - School of Mathematical Sciences
FrustrationVSFactorization - School of Mathematical Sciences

Many-Body Localization
Many-Body Localization

... diagrammatics but essentially the same as in class) ...
Random Repeated Interaction Quantum Systems
Random Repeated Interaction Quantum Systems

Few-Particle Effects in Semiconductor Quantum Dots: Spectrum Calculations on
Few-Particle Effects in Semiconductor Quantum Dots: Spectrum Calculations on

Quantum Mechanics II SS 2014
Quantum Mechanics II SS 2014

... In the special case of a central potential, V (r), the orbital angular momentum, L, particle is a constant of motion. Therefore, there exist stationary states with well-defined ~ 2 and Lz . And, as we found in angular momentum, i.e., eigenstates common to H, L QM I, the Schrödinger equation of a sp ...
Adiabatic Quantum Computation is Equivalent to Standard Quantum Computation Dorit Aharonov
Adiabatic Quantum Computation is Equivalent to Standard Quantum Computation Dorit Aharonov

... due to several breakthrough discoveries. Shor’s quantum algorithm for factorization [1], followed by several other algorithms to solve algebraic and combinatorial problems (see, e.g., [2–5]) have demonstrated the possible exponential advantage of quantum computing systems over classical ones. These ...
353, 216 (2006) .
353, 216 (2006) .

Surface polariton resonances and reflectance on a bigrating. Melendez, John Gary. 1987
Surface polariton resonances and reflectance on a bigrating. Melendez, John Gary. 1987

Chapter 5 Harmonic Oscillator and Coherent States
Chapter 5 Harmonic Oscillator and Coherent States

... Coherent States ...
Lindblad driving for nonequilibrium steady
Lindblad driving for nonequilibrium steady

... to two explicitly modeled leads of up to 140 modes each of which is stabilized by its respective Lindblad baths. Starting with an iterated Liouville-von Neumann equation for the reduced density matrix of the system we find that a Born-Markov approximation yields a QME in Lindblad form that describes ...
Quantum defect theory description of weakly bound levels and Feshbach...
Quantum defect theory description of weakly bound levels and Feshbach...

Wellposedness of a nonlinear, logarithmic Schrödinger equation of
Wellposedness of a nonlinear, logarithmic Schrödinger equation of

... rise to a modular type nonlinearity κQψ [6, 25], represents a field through which the electrons interact with themselves and can be interpreted as a quantum diffusion term yielding a theory which contains quantum–mechanical confinement ...
Electronic structure methods
Electronic structure methods

Department of Physics, Chemistry and Biology Master’s Thesis Thomas Fransson
Department of Physics, Chemistry and Biology Master’s Thesis Thomas Fransson

Introduction to Computational Quantum Chemistry: Theory
Introduction to Computational Quantum Chemistry: Theory

... Transition energies and intensities for UV and IR spectra NMR chemical shifts Dipole moments, polarisabilities and hyperpolarisabilities Reaction pathways and mechanisms ...
PPT - Fernando GSL Brandao
PPT - Fernando GSL Brandao

Beyond Effective Potential via Variational Perturbation Theory
Beyond Effective Potential via Variational Perturbation Theory

... a system can only be described correctly in the strong-coupling limit, i.e. for large coupling constants, the original weak-coupling series will be completely inadequate to describe the system. In either case, in order for the description of a system to be closed and complete, it must be possible th ...
Department of Physics, Chemistry and Biology Master’s Thesis
Department of Physics, Chemistry and Biology Master’s Thesis

Classical canonical transformation theory as a tool to describe
Classical canonical transformation theory as a tool to describe

Understanding degenerate ground states of a protected
Understanding degenerate ground states of a protected

Lecture Notes
Lecture Notes

On the adequacy of the Redfield equation and related approaches
On the adequacy of the Redfield equation and related approaches

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Perturbation theory (quantum mechanics)

In quantum mechanics, perturbation theory is a set of approximation schemes directly related to mathematical perturbation for describing a complicated quantum system in terms of a simpler one. The idea is to start with a simple system for which a mathematical solution is known, and add an additional ""perturbing"" Hamiltonian representing a weak disturbance to the system. If the disturbance is not too large, the various physical quantities associated with the perturbed system (e.g. its energy levels and eigenstates) can be expressed as ""corrections"" to those of the simple system. These corrections, being small compared to the size of the quantities themselves, can be calculated using approximate methods such as asymptotic series. The complicated system can therefore be studied based on knowledge of the simpler one.
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