Eliminating light shifts in single
... red side (left) of the peak and heating on the blue side (right) of the peak. Furthermore, the peak number of photon scatters reduces as the light shifts increase due to fluctuating dipole force heating and inhomogeneous detuning, that is, the fact that the atom will see a range of detunings as it s ...
... red side (left) of the peak and heating on the blue side (right) of the peak. Furthermore, the peak number of photon scatters reduces as the light shifts increase due to fluctuating dipole force heating and inhomogeneous detuning, that is, the fact that the atom will see a range of detunings as it s ...
Pascual Jordan`s resolution of the conundrum of the wave
... (1924a), which can be seen as a last-ditch effort to avoid light quanta, was that light consisted of particles guided by waves (Duncan and Janssen, 2007, sec. 4.2). In this picture, the waves and the particles presumably give separate contributions to the mean square energy fluctuation, just as Eins ...
... (1924a), which can be seen as a last-ditch effort to avoid light quanta, was that light consisted of particles guided by waves (Duncan and Janssen, 2007, sec. 4.2). In this picture, the waves and the particles presumably give separate contributions to the mean square energy fluctuation, just as Eins ...
A Quantum Explanation of Sheldrake`s Morphic Resonance
... and temporally. Somehow the micro DNA strand of one single cell has to exert influence on a vast collection of cells spread across a Macro region of spatial volume and over the whole time that the embryo development takes. In materialist theories (apart from the concept of particles), there is also ...
... and temporally. Somehow the micro DNA strand of one single cell has to exert influence on a vast collection of cells spread across a Macro region of spatial volume and over the whole time that the embryo development takes. In materialist theories (apart from the concept of particles), there is also ...
QEFS Hong Wei Yu
... The Dirac theory in Quantum Mechanics shows: the states, 2s1/2 and 2p1/2 of hydrogen atom are degenerate. ...
... The Dirac theory in Quantum Mechanics shows: the states, 2s1/2 and 2p1/2 of hydrogen atom are degenerate. ...
Laser Molecular Spectroscopy CHE466 Fall 2007
... fact that a molecule contains more than one electron that is somehow shared at different extents by a set of nuclei. In addition, the interaction between electrons is difficult to represent. These problems translate in our inability to solve the Schrodinger equation exactly for a molecule. Furthermo ...
... fact that a molecule contains more than one electron that is somehow shared at different extents by a set of nuclei. In addition, the interaction between electrons is difficult to represent. These problems translate in our inability to solve the Schrodinger equation exactly for a molecule. Furthermo ...
An equation for the waves - University College London
... • Energy quantized to particular values (characteristic of bound-state problems in quantum mechanics, where a particle is localized in a finite region of space. • Potential is even under reflection; stationary state wavefunctions may be even or odd (we say they have even or odd parity) • Compare not ...
... • Energy quantized to particular values (characteristic of bound-state problems in quantum mechanics, where a particle is localized in a finite region of space. • Potential is even under reflection; stationary state wavefunctions may be even or odd (we say they have even or odd parity) • Compare not ...
PDF only - at www.arxiv.org.
... Wheeler-Feynman “absorber theory” [8] originally proposed to explain classical electromagnetic interaction, was later generalized by Cramer [9] into a comprehensive model for all quantum interactions. Admittedly, TSVF is not acknowledged as superior to more conservative, one-vector formulations of q ...
... Wheeler-Feynman “absorber theory” [8] originally proposed to explain classical electromagnetic interaction, was later generalized by Cramer [9] into a comprehensive model for all quantum interactions. Admittedly, TSVF is not acknowledged as superior to more conservative, one-vector formulations of q ...
Resonant Tunneling Between Quantum Hall Edge States
... leads are one-dimensional, interactions are believed to de-stablize the Fermi liquid, forming a Luttinger liquid. In this case, the tunneling conductance through a point contact is predicted to vanish as a power law of temperature, due to the absence of long-lived singleparticle excitations in the i ...
... leads are one-dimensional, interactions are believed to de-stablize the Fermi liquid, forming a Luttinger liquid. In this case, the tunneling conductance through a point contact is predicted to vanish as a power law of temperature, due to the absence of long-lived singleparticle excitations in the i ...
![arXiv:1302.5365v1 [quant-ph] 21 Feb 2013](http://s1.studyres.com/store/data/002010390_1-09efe73c4824d019b499134a0467e0f3-300x300.png)
arXiv:1302.5365v1 [quant-ph] 21 Feb 2013
... Selected issues of the concept of spontaneous collapse are discussed, with the emphasis on the gravity-related model. We point out that without spontaneous collapses the Schrödinger cat states would macroscopically violate the standard conservation laws even in the presence of environmental noise. ...
... Selected issues of the concept of spontaneous collapse are discussed, with the emphasis on the gravity-related model. We point out that without spontaneous collapses the Schrödinger cat states would macroscopically violate the standard conservation laws even in the presence of environmental noise. ...
Ground states and excitations of spatially anisotropic quantum antiferromagnets Oleg Starykh
... ✦ Good for weakly ordered states: abundance of multi-particle excitations ✦ Delicate details of 3d ordering are determined by minute, and often anisotropic, sub-leading interactions • T-H phase diagram of Cs2CuCl4 and Cs2CuBr4 remain to be understood – commensurate AF state in Cs2CuCl4 – 2/3 and oth ...
... ✦ Good for weakly ordered states: abundance of multi-particle excitations ✦ Delicate details of 3d ordering are determined by minute, and often anisotropic, sub-leading interactions • T-H phase diagram of Cs2CuCl4 and Cs2CuBr4 remain to be understood – commensurate AF state in Cs2CuCl4 – 2/3 and oth ...
Chapter 2 Rydberg Atoms
... it was also possible to derive scaling laws for the atomic properties in terms of n, which were later verified from the full quantum mechanical treatment of Schrödinger in 1926 [89]. Table 2.1 summarises the scalings of the atomic properties for the low-� Rydberg states. The most important property ...
... it was also possible to derive scaling laws for the atomic properties in terms of n, which were later verified from the full quantum mechanical treatment of Schrödinger in 1926 [89]. Table 2.1 summarises the scalings of the atomic properties for the low-� Rydberg states. The most important property ...
Theoretische und Mathematische Grundlagen der Physik
... finally able to compute the so-called “Wilson loop observables” (WLOs) of this theory explicitly. These WLO are heuristic path integral expressions and the interesting thing about the values Witten obtained for them is that they are given by highly non-trivial link invariants like the Jones, the Hom ...
... finally able to compute the so-called “Wilson loop observables” (WLOs) of this theory explicitly. These WLO are heuristic path integral expressions and the interesting thing about the values Witten obtained for them is that they are given by highly non-trivial link invariants like the Jones, the Hom ...
Cosmology
... thermodynamics, was obliged to separate energy into tiny parts, the quanta, by introducing a new principle, h=6,6/10-27 erg.second which is called Planck principle. That is how the biggest crisis in the history of physics took place, since for the first time after Newton’s era it was supported that ...
... thermodynamics, was obliged to separate energy into tiny parts, the quanta, by introducing a new principle, h=6,6/10-27 erg.second which is called Planck principle. That is how the biggest crisis in the history of physics took place, since for the first time after Newton’s era it was supported that ...
E4. Free Fall
... −k x : harmonic oscillator at a very early point in his/her education, and with the first & last of those systems we are never done: they are—for reasons having little to do with their physical importance—workhorses of theoretical mechanics, traditionally employed to illustrated formal developments a ...
... −k x : harmonic oscillator at a very early point in his/her education, and with the first & last of those systems we are never done: they are—for reasons having little to do with their physical importance—workhorses of theoretical mechanics, traditionally employed to illustrated formal developments a ...
Introduction to Quantum Field Theory
... path integral) which was not the original one, but became popular, even essential, with new advances in the 1970s. However, to set this in its context, it is useful to have some historical perspective on the development of the subject (dates are only rough). • 19th C. Maxwell’s equations – a classic ...
... path integral) which was not the original one, but became popular, even essential, with new advances in the 1970s. However, to set this in its context, it is useful to have some historical perspective on the development of the subject (dates are only rough). • 19th C. Maxwell’s equations – a classic ...
PDF
... ity of a measurement, and they observables such as position x and momentum p, the product of the consequence of the quantized naprovide an interesting challenge to spreads is lower-bounded: DxDp Q I/2, where I is Planck’s constant. The ture of the electromagnetic field devise quantum strategies that ...
... ity of a measurement, and they observables such as position x and momentum p, the product of the consequence of the quantized naprovide an interesting challenge to spreads is lower-bounded: DxDp Q I/2, where I is Planck’s constant. The ture of the electromagnetic field devise quantum strategies that ...
QUANTUM COMPUTING
... quantum mechanics, however, we are permitted to have a zero and a one at the same time present in one physical system. In fact, we are permitted to have an infinite range of states between zero and one – which we called a qubit. The number of states a qubit could occupy is infinite because in princi ...
... quantum mechanics, however, we are permitted to have a zero and a one at the same time present in one physical system. In fact, we are permitted to have an infinite range of states between zero and one – which we called a qubit. The number of states a qubit could occupy is infinite because in princi ...
On the correspondence principle
... ‘at small (absolute) values of the energy the quantum spectrum becomes very dense, while it becomes sparse for larger field strengths and binding energies’ [18]. Hence, the classical limit is said to be reached when the spectrum is dense and, hence, the effective value of Planck’s constant is small. ...
... ‘at small (absolute) values of the energy the quantum spectrum becomes very dense, while it becomes sparse for larger field strengths and binding energies’ [18]. Hence, the classical limit is said to be reached when the spectrum is dense and, hence, the effective value of Planck’s constant is small. ...
Low-energy fusion dynamics of weakly bound nuclei
... observables are useful for planning and interpreting particle-gamma coincidence measurements [8]. In Ref. [8], the spin and excitation energy distributions from PLATYPUS are used in combination with the evaporation code PACE for calculating the production of specific evaporation residues. Some evapor ...
... observables are useful for planning and interpreting particle-gamma coincidence measurements [8]. In Ref. [8], the spin and excitation energy distributions from PLATYPUS are used in combination with the evaporation code PACE for calculating the production of specific evaporation residues. Some evapor ...