Nonspreading wave packets of Rydberg electrons in molecules with
... Obviously, the Trojan states cannot exist in homonuclear molecules, since by symmetry such molecules do not have dipole moments. However, when one hydrogen atom is replaced by its isotope, by deuterium, or even better by tritium, the center of mass is shifted with respect to the center of charge and ...
... Obviously, the Trojan states cannot exist in homonuclear molecules, since by symmetry such molecules do not have dipole moments. However, when one hydrogen atom is replaced by its isotope, by deuterium, or even better by tritium, the center of mass is shifted with respect to the center of charge and ...
A Suggested Answer To Wallstrom`s Criticism: Zitterbewegung
... has been to derive quantum theory from a classical-like statistical mechanics of particles undergoing Brownian motion. Towards this end, non-relativistic and relativistic models of stochastic mechanics have been constructed for both spin-0 particles [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15 ...
... has been to derive quantum theory from a classical-like statistical mechanics of particles undergoing Brownian motion. Towards this end, non-relativistic and relativistic models of stochastic mechanics have been constructed for both spin-0 particles [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15 ...
Commentary_Basti
... phase transition in terms of the dynamic constitution of different phase coherence domains, like as many SSB conditions of the quantum vacuum ground state, gives a new light to the Schrödinger notion of information as neghentropy in fundamental physics. “Neghentropy” is indeed “free energy”, that is ...
... phase transition in terms of the dynamic constitution of different phase coherence domains, like as many SSB conditions of the quantum vacuum ground state, gives a new light to the Schrödinger notion of information as neghentropy in fundamental physics. “Neghentropy” is indeed “free energy”, that is ...
The evolution of free wave packets
... spread at that instant. This result also shows that a free wave packet which is real at some time cannot be real at any other time. In fact, the probability is symmetric in time about the instant when the wave function was real, because if 共x , t兲 satisfies Schrödinger’s equation, then so does ⴱ共x ...
... spread at that instant. This result also shows that a free wave packet which is real at some time cannot be real at any other time. In fact, the probability is symmetric in time about the instant when the wave function was real, because if 共x , t兲 satisfies Schrödinger’s equation, then so does ⴱ共x ...
Quantum Random Walk via Classical Random Walk With Internal
... to some probabilistic rule is studied. In the simplest model, a particle will move, at every discrete time step, one unit to the left or to the right with probabilities p and 1 − p, respectively, independent of its past positions. Many useful questions can be asked about the dynamics of the particle ...
... to some probabilistic rule is studied. In the simplest model, a particle will move, at every discrete time step, one unit to the left or to the right with probabilities p and 1 − p, respectively, independent of its past positions. Many useful questions can be asked about the dynamics of the particle ...
The pressure increase at 4He l–point explained by means of the
... Even if is not exactly the thermodynamic temperature T, the result (47) is very satisfying since it correctly gives the order of magnitude of the transition temperature of the lambda point. The fact that is close to T can be intuitively understood with the fact that going toward the absolute nul ...
... Even if is not exactly the thermodynamic temperature T, the result (47) is very satisfying since it correctly gives the order of magnitude of the transition temperature of the lambda point. The fact that is close to T can be intuitively understood with the fact that going toward the absolute nul ...
CHAPTER 5 The Bohr Model of the Atom
... pass a given point per unit of time. If we choose an exact position along the path of the wave and count how many crests pass the position per unit time, we would get a value for frequency. Based on this description, the unit for frequency would be cycles per second or waves per second. In science, ...
... pass a given point per unit of time. If we choose an exact position along the path of the wave and count how many crests pass the position per unit time, we would get a value for frequency. Based on this description, the unit for frequency would be cycles per second or waves per second. In science, ...
Can Wavefunction Collapse Conserve Energy? - Philsci
... is, the collapse time of a momentum eigenstate will be zero as its position uncertainty is infinite. This means that the momentum eigenstates of any quantum system will collapse instantaneously to one of its position eigenstates and thus cannot exist. Moreover, the superposition states with very sm ...
... is, the collapse time of a momentum eigenstate will be zero as its position uncertainty is infinite. This means that the momentum eigenstates of any quantum system will collapse instantaneously to one of its position eigenstates and thus cannot exist. Moreover, the superposition states with very sm ...
Non-reciprocal Light-harvesting Antennae
... The wave-like energy transfer or the coherence at room-temperature observed by previous authors might simply signify a collective motion (mechanical movement) instead of quantum coherence[31], as light at this wavelength, in comparison with the size of the antenna, should be considered as a wave ins ...
... The wave-like energy transfer or the coherence at room-temperature observed by previous authors might simply signify a collective motion (mechanical movement) instead of quantum coherence[31], as light at this wavelength, in comparison with the size of the antenna, should be considered as a wave ins ...
Quantum annealing with manufactured spins
... process using a quantum mechanical model as discussed in the Supplementary Information. In addition to the experimental results, in Fig. 3b we show the results of three different numerical simulations. In all three cases, the model parameters were independently measured for the individual devices, l ...
... process using a quantum mechanical model as discussed in the Supplementary Information. In addition to the experimental results, in Fig. 3b we show the results of three different numerical simulations. In all three cases, the model parameters were independently measured for the individual devices, l ...
Downloadable Full Text - DSpace@MIT
... is worse for the excited states, where we have to abandon the crutch of supersymmetry altogether. It is our interest in this paper to construct the supersymmetric and excited states of this model. We will not be able to do so analytically, but there exist numerical methods to compute the eigenspectr ...
... is worse for the excited states, where we have to abandon the crutch of supersymmetry altogether. It is our interest in this paper to construct the supersymmetric and excited states of this model. We will not be able to do so analytically, but there exist numerical methods to compute the eigenspectr ...
Classical limit and quantum logic - Philsci
... (Clarke and Braginski 2004). As an example, let us suppose that we go to an electronics store to buy a transistor. The salesman will first find its location in the shelves, and then will take it with his hand in order to put it in a bag and, finally, to give it to us. From this point of view and for ...
... (Clarke and Braginski 2004). As an example, let us suppose that we go to an electronics store to buy a transistor. The salesman will first find its location in the shelves, and then will take it with his hand in order to put it in a bag and, finally, to give it to us. From this point of view and for ...
Equation of state for solid neon from quantum theory
... are presented in Table I in comparison with recent calculations from other research groups.27,40–42 Taking all terms into account as shown in Eq. !1" leads to results very close to experimental measurements. Only the more elaborate IC coupled-cluster calculations by Rosćiszewski et al.27 are close t ...
... are presented in Table I in comparison with recent calculations from other research groups.27,40–42 Taking all terms into account as shown in Eq. !1" leads to results very close to experimental measurements. Only the more elaborate IC coupled-cluster calculations by Rosćiszewski et al.27 are close t ...
Gravity as a fluid dynamic phenomenon in a superfluid
... to Navier Stokes equations to describe vortex objects (vortex balls) which, unlike Hill's spherical vortices, show intersected streamlines and seem to satisfactorily reproduce fermions' spin by varying their orientation at each revolution. Also Volovik [7] accurately discusses the possible topology ...
... to Navier Stokes equations to describe vortex objects (vortex balls) which, unlike Hill's spherical vortices, show intersected streamlines and seem to satisfactorily reproduce fermions' spin by varying their orientation at each revolution. Also Volovik [7] accurately discusses the possible topology ...
Propensities in Quantum Mechanics - Philsci
... obtain what is known as macroscopic superposition infection: the composite (system + device) goes into a superposition. Formally, the state of the composite at the end of the interaction looks like this: Ψ = Σn,m cnm νn μm, where μm are the eigenstates of the pointer position observable with corre ...
... obtain what is known as macroscopic superposition infection: the composite (system + device) goes into a superposition. Formally, the state of the composite at the end of the interaction looks like this: Ψ = Σn,m cnm νn μm, where μm are the eigenstates of the pointer position observable with corre ...
ppt - CS Technion
... Query transformation U i consists of two transformations (U i0 , U i1 ) U i0 I is applied to all H i | v for which av 0 and U i1 I is applied to all H i | v for which av 1 Z-local transformation * U i (| | v ) H i H ( v ) ...
... Query transformation U i consists of two transformations (U i0 , U i1 ) U i0 I is applied to all H i | v for which av 0 and U i1 I is applied to all H i | v for which av 1 Z-local transformation * U i (| | v ) H i H ( v ) ...
Bohr–Einstein debates
The Bohr–Einstein debates were a series of public disputes about quantum mechanics between Albert Einstein and Niels Bohr. Their debates are remembered because of their importance to the philosophy of science. An account of the debates was written by Bohr in an article titled ""Discussions with Einsteinon Epistemological Problems in Atomic Physics"". Despite their differences of opinion regarding quantum mechanics, Bohr and Einstein had a mutual admiration that was to last the rest of their lives.The debates represent one of the highest points of scientific research in the first half of the twentieth century because it called attention to an element of quantum theory, quantum non-locality, which is absolutely central to our modern understanding of the physical world. The consensus view of professional physicists has been that Bohr proved victorious, and definitively established the fundamental probabilistic character of quantum measurement.