
Exploring a Classical Model of the Helium Atom
... region decreases. We have plotted the region where tori exist in Fig. 2 for CF-l (circular configuration). Here the initial velocity VI is varied by fixing the radius (Xl)' The lower limit of Xl is about 1.45. Though the tori have a finite measure in the phase space, the region of existence is not c ...
... region decreases. We have plotted the region where tori exist in Fig. 2 for CF-l (circular configuration). Here the initial velocity VI is varied by fixing the radius (Xl)' The lower limit of Xl is about 1.45. Though the tori have a finite measure in the phase space, the region of existence is not c ...
Spin transport through nanostructures B. K ,
... without collective excitations. At zero magnetic field, the total-spin up and totalspin down components are energetically degenerate, and separated from the ground state n = 2q, s = 0,0,0 by δEp = 2p2Eσ. States with an odd number of electrons, n = 2q + 1, can be considered similarly. Here, the excit ...
... without collective excitations. At zero magnetic field, the total-spin up and totalspin down components are energetically degenerate, and separated from the ground state n = 2q, s = 0,0,0 by δEp = 2p2Eσ. States with an odd number of electrons, n = 2q + 1, can be considered similarly. Here, the excit ...
le journal de physique - Département de Physique de l`Ecole
... The next step is to compute the average of the two rates (1.9) in the resemoir state. Such a calculation is not trivial. First, Rf(t) does not cornmute with Si(t) and G(t). Secondly, the system observables Si(t) and G(t) also operate on resemoir states since they have been « contaminated » by resemo ...
... The next step is to compute the average of the two rates (1.9) in the resemoir state. Such a calculation is not trivial. First, Rf(t) does not cornmute with Si(t) and G(t). Secondly, the system observables Si(t) and G(t) also operate on resemoir states since they have been « contaminated » by resemo ...
Including Nuclear Degrees of Freedom in a Lattice Hamiltonian, P. L. Hagelstein, I. U. Chaudhary, This paper has been accepted for publication in J. Cond. Mat. Nucl. Sci. and will be published soon. An earlier version was posted on the LANL ArXiV (/0401667 [cond-mat.other] 20 Jan 2012).
... there were no physical transitions which could serve as the strongly coupled two-level transition within the model. We were optimistic in our writing about the possibility that systems described by three-level systems (or N-level systems) would be able to do the job. After putting in a great deal of ...
... there were no physical transitions which could serve as the strongly coupled two-level transition within the model. We were optimistic in our writing about the possibility that systems described by three-level systems (or N-level systems) would be able to do the job. After putting in a great deal of ...
URL - StealthSkater
... Principle (NMP) states that in a given quantum state the most quantum entangled subsystemcomplement pair can perform the quantum jump. More precisely, the reduction of the entanglement entropy in the quantum jump is as large as possible. This selects the pair in question and in the case of ordinary ...
... Principle (NMP) states that in a given quantum state the most quantum entangled subsystemcomplement pair can perform the quantum jump. More precisely, the reduction of the entanglement entropy in the quantum jump is as large as possible. This selects the pair in question and in the case of ordinary ...
Here - UiO
... like a quantum gas, a gas where quantum mechanical effects are important. The quantum mechanical effect which we see on play here is the Pauli exclusion principle: Two fermions cannot occupy the same energy state. To understand this principle we need to dig even deeper into the quantum theory. Accor ...
... like a quantum gas, a gas where quantum mechanical effects are important. The quantum mechanical effect which we see on play here is the Pauli exclusion principle: Two fermions cannot occupy the same energy state. To understand this principle we need to dig even deeper into the quantum theory. Accor ...
MEASUREMENT OF LIFETIMES OF EXCITED STATES OF THE
... IN measurement of excitation cross sections of energetic ions or atoms in collisions with gas molecules, we must consider the following fact. In the apparatus usually used for this type of experiment, a monoenergetic beam of the ions or atoms being studied enters a collision chamber filled with gas ...
... IN measurement of excitation cross sections of energetic ions or atoms in collisions with gas molecules, we must consider the following fact. In the apparatus usually used for this type of experiment, a monoenergetic beam of the ions or atoms being studied enters a collision chamber filled with gas ...
Ex. = 1s 1 , 0 to (1-1)
... Answers given by 2nd grade school children to the following questions: If you could change one thing about your mom, what would it be? 1. She has this weird thing about me ...
... Answers given by 2nd grade school children to the following questions: If you could change one thing about your mom, what would it be? 1. She has this weird thing about me ...
PH0008 Quantum Mechanics and Special
... • In order to extract the kinetic energy (p2/2m) and total energy (E) in the ...
... • In order to extract the kinetic energy (p2/2m) and total energy (E) in the ...
Adiabatic Quantum State Generation and Statistical Zero Knowledge
... the adiabatic theorem. The second proof is self contained, and does not require knowledge of the adiabatic theorem. Instead it uses the simple Zeno effect[38], thus providing an alternative point of view of adiabatic algorithms using measurements (Such a path was taken also in [11].) This implies th ...
... the adiabatic theorem. The second proof is self contained, and does not require knowledge of the adiabatic theorem. Instead it uses the simple Zeno effect[38], thus providing an alternative point of view of adiabatic algorithms using measurements (Such a path was taken also in [11].) This implies th ...
Quantum Chromodynamical Explanation of the Strong Nuclear Force
... The Strong Nuclear Force was proposed to explain the unintuitive attraction between protons and neutrons within an atomic nucleus, despite the relatively immense repulsion of the electromagnetic force overshadowing the attraction between the particles due to gravitation. It is responsible for bindin ...
... The Strong Nuclear Force was proposed to explain the unintuitive attraction between protons and neutrons within an atomic nucleus, despite the relatively immense repulsion of the electromagnetic force overshadowing the attraction between the particles due to gravitation. It is responsible for bindin ...
The Membrane Vacuum State
... back to the very depths of the sixties, thus predating the emergence of its more illustrious and celebrated sibling, string theory. The birthplace of membrane theory, like many other grand ideas, was in the brilliant mind of Dirac [1]. In 1962, Dirac was pursuing an alternative model for the electro ...
... back to the very depths of the sixties, thus predating the emergence of its more illustrious and celebrated sibling, string theory. The birthplace of membrane theory, like many other grand ideas, was in the brilliant mind of Dirac [1]. In 1962, Dirac was pursuing an alternative model for the electro ...