Spin Qubits for Quantum Information Processing
... Figure 14.7: The internal and external magnetic fields created by a single nuclear spin with a magnetic moment µn . where µ̂e = −h̄γe Ŝ and µ̂n = h̄γn Iˆ are used. The Hamiltonian (14.69) is called a contact Hyperfine interaction, which exists only for the case that the electron and nucleus wavefu ...
... Figure 14.7: The internal and external magnetic fields created by a single nuclear spin with a magnetic moment µn . where µ̂e = −h̄γe Ŝ and µ̂n = h̄γn Iˆ are used. The Hamiltonian (14.69) is called a contact Hyperfine interaction, which exists only for the case that the electron and nucleus wavefu ...
Presentation Slides
... Dark Matter and Dark Energy (if it exists) is currently assumed to explain the inflation of our universe (structure and galaxy formation, anisotropies in cosmic microwave background, new state of matter?). The Particle/Antiparticle imbalance in our universe (10,000:1) cannot be explained by the ...
... Dark Matter and Dark Energy (if it exists) is currently assumed to explain the inflation of our universe (structure and galaxy formation, anisotropies in cosmic microwave background, new state of matter?). The Particle/Antiparticle imbalance in our universe (10,000:1) cannot be explained by the ...
Majorana and Condensed Matter Physics
... Having emphasized the value of solutions of Eqns. (1,2) for spin- 21 , we turn to the the task of obtaining them. The general problem can only be solved numerically. There is, however, a powerful yet, approximate result available when the evolution is slow and smooth, namely the adiabatic theorem. I ...
... Having emphasized the value of solutions of Eqns. (1,2) for spin- 21 , we turn to the the task of obtaining them. The general problem can only be solved numerically. There is, however, a powerful yet, approximate result available when the evolution is slow and smooth, namely the adiabatic theorem. I ...
The Impact of Energy Band Diagram and Inhomogeneous
... Digital Object Identifier 10.1109/JQE.2004.837953 ...
... Digital Object Identifier 10.1109/JQE.2004.837953 ...
Syllabys for BSc(Major):
... equipartition of energy, mean free path, transport phenomena (viscosity, conduction and diffusion), Avogadro number-experimental determination by the kinetic theory method, Brownian motion (theory of translational Brownian movement). Compressibility and expansion coefficient of gases, difference bet ...
... equipartition of energy, mean free path, transport phenomena (viscosity, conduction and diffusion), Avogadro number-experimental determination by the kinetic theory method, Brownian motion (theory of translational Brownian movement). Compressibility and expansion coefficient of gases, difference bet ...
Lectures on String Theory - UCI Physics and Astronomy
... as a quantum field theory on the (1+1) dimensional worldsheet of the string, S = d σ Lstring . There exist many such quantum field theories and so there exist many string theories. Further, for some string theories the strings themselves arise from wrapped higher-dimensional objects and hence can ha ...
... as a quantum field theory on the (1+1) dimensional worldsheet of the string, S = d σ Lstring . There exist many such quantum field theories and so there exist many string theories. Further, for some string theories the strings themselves arise from wrapped higher-dimensional objects and hence can ha ...
![arXiv:math/0606118v4 [math.PR] 5 Dec 2006](http://s1.studyres.com/store/data/013514025_1-1bac3cda767b4b11f4a6d27e549df5b9-300x300.png)
arXiv:math/0606118v4 [math.PR] 5 Dec 2006
... interaction between an atom and the electromagnetic field. First, however, we need to demonstrate how probability theory fits in the framework of quantum mechanics. 2.1. Random variables in quantum mechanics. The basic setting of quantum mechanics, as one would find it in most textbooks, is somethin ...
... interaction between an atom and the electromagnetic field. First, however, we need to demonstrate how probability theory fits in the framework of quantum mechanics. 2.1. Random variables in quantum mechanics. The basic setting of quantum mechanics, as one would find it in most textbooks, is somethin ...
Theoretical calculations of dielectronic recombination in crossed electric and magnetic... D. C. Griffin F. Robicheaux and M. S. Pindzola
... angular momenta and, thereby, opening up many more recombination channels. However, in the presence of an electric field alone, M is a good quantum number and the recombination probability falls off rapidly with the magnetic quantum number @8#. In the presence of a magnetic field alone or a magnetic ...
... angular momenta and, thereby, opening up many more recombination channels. However, in the presence of an electric field alone, M is a good quantum number and the recombination probability falls off rapidly with the magnetic quantum number @8#. In the presence of a magnetic field alone or a magnetic ...
Use of Rotating Coordinates in Magnetic Resonance Problems
... until it reaches the second oscillating field. As a result of this precession the nucleus will in general have a diBerent orientation relative to H, „ in the second rota, ting field region than it did in the first. On the other hand, if the average value of Hs — a&/y in the intermediate region is ze ...
... until it reaches the second oscillating field. As a result of this precession the nucleus will in general have a diBerent orientation relative to H, „ in the second rota, ting field region than it did in the first. On the other hand, if the average value of Hs — a&/y in the intermediate region is ze ...
A statistical mechanics approach to the factorization problem
... the archetypical Ising spin glass model. The coupling parameters Jij are quenched random variables, for example Gaussian distributed with mean zero. The combination of disorder and frustration makes spin glass models very challenging to solve, and there is no known general solution. However, in the ...
... the archetypical Ising spin glass model. The coupling parameters Jij are quenched random variables, for example Gaussian distributed with mean zero. The combination of disorder and frustration makes spin glass models very challenging to solve, and there is no known general solution. However, in the ...
Renormalization
... dimensional analysis would tell us that the dimensionless transition amplitude cannot depend on the momentum! However, because the cutoff parameter a has dimension, the renormalized parameter can have a different dimension than the coupling in the Hamiltonian. We say that the renormalized coupling h ...
... dimensional analysis would tell us that the dimensionless transition amplitude cannot depend on the momentum! However, because the cutoff parameter a has dimension, the renormalized parameter can have a different dimension than the coupling in the Hamiltonian. We say that the renormalized coupling h ...
Bell-Inequality Violations with Single Photons Entangled in Momentum and Polarization
... analysis of the CH inequality and show that two-qubit systems can be used to perform tests of the original CH inequality because single probabilities reduce to combinations of joint probabilities with the same detection efficiency. Thus, the detection efficiencies drop out of the inequality altogeth ...
... analysis of the CH inequality and show that two-qubit systems can be used to perform tests of the original CH inequality because single probabilities reduce to combinations of joint probabilities with the same detection efficiency. Thus, the detection efficiencies drop out of the inequality altogeth ...