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... just nonclassical effects in the field, as it only involves field excitation. For weak fields D2 is exactly A2,g . The entanglement shows up in the value of A1,e ; if this value does not satisfy A1,e = D1Ce = A0,e A1,g , then it is not possible to write the state as a product state. In the presence ...
... just nonclassical effects in the field, as it only involves field excitation. For weak fields D2 is exactly A2,g . The entanglement shows up in the value of A1,e ; if this value does not satisfy A1,e = D1Ce = A0,e A1,g , then it is not possible to write the state as a product state. In the presence ...
Quantum Mechanics
... It is impossible to explain this result on the basis of the classical theory of light as an electromagnetic wave. This is because the energy contained in such a wave would arrive at the metal at a uniform rate and there is no apparent reason why this energy should be divided up in such a way that th ...
... It is impossible to explain this result on the basis of the classical theory of light as an electromagnetic wave. This is because the energy contained in such a wave would arrive at the metal at a uniform rate and there is no apparent reason why this energy should be divided up in such a way that th ...
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... by black hole of mass M . If M is small enough S can be greater than Sb:h:, but in this case absorbtion is impossible. The bound (1) is independent on mass of black hole, which is supposed to be large in comparison with E , but even this independence does not allow us to conclude that the bound cou ...
... by black hole of mass M . If M is small enough S can be greater than Sb:h:, but in this case absorbtion is impossible. The bound (1) is independent on mass of black hole, which is supposed to be large in comparison with E , but even this independence does not allow us to conclude that the bound cou ...
Scattering theory - Theory of Condensed Matter
... incident upon a target. The potential of the target, V (r), might represent that experienced by a fast electron striking an atom, or an α particle colliding with a nucleus. As in the classical problem, the basic scenario involves directing a stream or flux of particles, all at the same energy, at a ...
... incident upon a target. The potential of the target, V (r), might represent that experienced by a fast electron striking an atom, or an α particle colliding with a nucleus. As in the classical problem, the basic scenario involves directing a stream or flux of particles, all at the same energy, at a ...
University of Toronto Strongly Repulsive Ultracold
... where U (ri ) is the trapping potential and V (ri , rj ) is the interaction potential. If the fermions are non-interacting (i.e. V = 0), then a simple exact solution for the properties of the gas exists for any temperature of the gas. Quantum statistical mechanics, in the Thomas-Fermi approximation ...
... where U (ri ) is the trapping potential and V (ri , rj ) is the interaction potential. If the fermions are non-interacting (i.e. V = 0), then a simple exact solution for the properties of the gas exists for any temperature of the gas. Quantum statistical mechanics, in the Thomas-Fermi approximation ...
The semantics of the canonical commutation relation
... ultrafilter? Is its elementary theory (positive theory) uniquely determined? 2. Is the limit object (the space of basic states) unique? 1.6 Note that another very interesting example of a limit representing the algebra pseudo-generated by U α and V β is when αβ is a nonstandard approximation √ to a ...
... ultrafilter? Is its elementary theory (positive theory) uniquely determined? 2. Is the limit object (the space of basic states) unique? 1.6 Note that another very interesting example of a limit representing the algebra pseudo-generated by U α and V β is when αβ is a nonstandard approximation √ to a ...
Charge Rearrangement and Screening in a Quantum Point Contact S. Lu¨scher,
... traces overlapping by 50 mV. To reduce noise we averaged each trace over 40 measurements. No striking features are visible in these raw data. To analyze the data more carefully, we perform two transformations. First, we assign to each VQPC an effective voltage Veff that would produce the same change ...
... traces overlapping by 50 mV. To reduce noise we averaged each trace over 40 measurements. No striking features are visible in these raw data. To analyze the data more carefully, we perform two transformations. First, we assign to each VQPC an effective voltage Veff that would produce the same change ...
Atomic Quantum Metrology with Narrowband Entangled and Squeezed States of Light DISSERTATION
... in the same mode and can form a NOON state with N =2, a so-called 2-NOON state [13]. In the past, high efforts were made to increase the size of NOON states and ‘NOON-like’ states by superposing a 2-NOON state with a coherent beam [14, 15] or by using double-pair emission of an SPDC crystal [16]. Th ...
... in the same mode and can form a NOON state with N =2, a so-called 2-NOON state [13]. In the past, high efforts were made to increase the size of NOON states and ‘NOON-like’ states by superposing a 2-NOON state with a coherent beam [14, 15] or by using double-pair emission of an SPDC crystal [16]. Th ...
On molecular origin of mass-independent fractionation of oxygen
... vibrational motion of O*3 is treated quantum-mechanically using the time-dependent Schrödinger equation and the wave-packet technique. This allows incorporation of all quantum effects associated with molecular vibration (such as ZPE, quantization of states, tunneling, resonances, and symmetry) and c ...
... vibrational motion of O*3 is treated quantum-mechanically using the time-dependent Schrödinger equation and the wave-packet technique. This allows incorporation of all quantum effects associated with molecular vibration (such as ZPE, quantization of states, tunneling, resonances, and symmetry) and c ...
Carbon nanotube quantum dots on hexagonal boron nitride
... resolution, the contrast in scanning electron microscopy the scalability, geometry and in the choice of the conThe next step, however, namely the use hBN as substrate for independent, more complex (SEM) images can beof poor (see below) and AFM imaging tact and gate materials. For example, it is diff ...
... resolution, the contrast in scanning electron microscopy the scalability, geometry and in the choice of the conThe next step, however, namely the use hBN as substrate for independent, more complex (SEM) images can beof poor (see below) and AFM imaging tact and gate materials. For example, it is diff ...
PDF - at www.arxiv.org.
... This document was generated with the 2014 LATEX distribution. The LATEX template is adapted from a template by Iagoba Apellaniz. ...
... This document was generated with the 2014 LATEX distribution. The LATEX template is adapted from a template by Iagoba Apellaniz. ...
Long Term Confidentiality: a Survey
... being processed and stored by online resources beyond physical and logical control of the owner. It is a simple task for an adversary to intercept, copy, and store any data sent across a public network and from this point on, confidentiality is determined solely by the original encryption scheme. He ...
... being processed and stored by online resources beyond physical and logical control of the owner. It is a simple task for an adversary to intercept, copy, and store any data sent across a public network and from this point on, confidentiality is determined solely by the original encryption scheme. He ...
Elec-‐ph. and ph.-‐ph. coupling in semiconductors and bismuth
... ( ph.x, routine ep_matrix_element_wannier.f90 included in Phonon/PH) 5. Obtain first dmns(R,RL) and then dmns(k+q,k) at any k and q by using U from step 1 and dmns(k+q,k) from step 4 (independent code epiq.f90/epik.f90 , not yet included in qe-forge) Advanced Quantum ESPRESSO developer’s meeting : l ...
... ( ph.x, routine ep_matrix_element_wannier.f90 included in Phonon/PH) 5. Obtain first dmns(R,RL) and then dmns(k+q,k) at any k and q by using U from step 1 and dmns(k+q,k) from step 4 (independent code epiq.f90/epik.f90 , not yet included in qe-forge) Advanced Quantum ESPRESSO developer’s meeting : l ...
Nonlinear response of a driven vibrating nanobeam in the quantum...
... fundamental mode vanishes and quartic terms in the Lagrangian have to be taken into account. An effective Hamiltonian has been derived for the amplitude of the fundamental mode being the dynamical variable which moves in an anharmonic potential. Depending on the strain being below ( < c ) or abo ...
... fundamental mode vanishes and quartic terms in the Lagrangian have to be taken into account. An effective Hamiltonian has been derived for the amplitude of the fundamental mode being the dynamical variable which moves in an anharmonic potential. Depending on the strain being below ( < c ) or abo ...
ABSTRACT RANDOM ROUTING AND CONCENTRATION IN QUANTUM SWITCHING NETWORKS
... crossbar concentrators. Sparse crossbar concentrators are rectangular grids of simple 2 × 2 switches or crosspoints, with the switches arranged such that any k inputs can be connected to some k outputs. We give the design of the quantum crosspoints for such concentrators and devise a self-routing me ...
... crossbar concentrators. Sparse crossbar concentrators are rectangular grids of simple 2 × 2 switches or crosspoints, with the switches arranged such that any k inputs can be connected to some k outputs. We give the design of the quantum crosspoints for such concentrators and devise a self-routing me ...