PDF file - Physics & Astronomy
... Springer Dordrecht Heidelberg New York London Library of Congress Control Number: 2013955251 Springer Science+Business Media Dordrecht 2013 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights o ...
... Springer Dordrecht Heidelberg New York London Library of Congress Control Number: 2013955251 Springer Science+Business Media Dordrecht 2013 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights o ...
quantum transport phenomena of two
... made ultrathin (< 1 nm), in which case the electrons in adjacent wells can readily couple to each other via quantum-mechanical tunneling and the discrete energy levels broaden ...
... made ultrathin (< 1 nm), in which case the electrons in adjacent wells can readily couple to each other via quantum-mechanical tunneling and the discrete energy levels broaden ...
Circuit QED — Lecture Notes - Royal Holloway, University of London
... give a system which is very strongly quantum mechanical—they are fundamental particles which are so small that only quantum physics can describe their behaviour; and 2) it may be possible to achieve very good isolation from the environment. • Key disadvantages: 1) we are stuck with what nature provi ...
... give a system which is very strongly quantum mechanical—they are fundamental particles which are so small that only quantum physics can describe their behaviour; and 2) it may be possible to achieve very good isolation from the environment. • Key disadvantages: 1) we are stuck with what nature provi ...
Scaling theory polymers general polymer good
... the n-vector model in the limit n - 0 (see (3.5)) and does not depend on the details of topology of the network. On the other hand, the exponents yg and jig are universal quantities. They do not depend on the details of the underlying lattice but do depend on the spatial dimensionality d and the top ...
... the n-vector model in the limit n - 0 (see (3.5)) and does not depend on the details of topology of the network. On the other hand, the exponents yg and jig are universal quantities. They do not depend on the details of the underlying lattice but do depend on the spatial dimensionality d and the top ...
Polarization control of single photon quantum
... mentum) imposes significant limitations to the protocols that may be implemented. In recent years the orbital angular momentum (OAM) of light, related to the photon’s spatial mode structure, has been recognized as a promising resource for novel quantum information protocols, allowing the implementa ...
... mentum) imposes significant limitations to the protocols that may be implemented. In recent years the orbital angular momentum (OAM) of light, related to the photon’s spatial mode structure, has been recognized as a promising resource for novel quantum information protocols, allowing the implementa ...
Single-Site Green-Function of the Dirac Equation for Full
... of materials research and condensed matter physics. Desired material properties are highly diverse, ranging from mechanical requirements for a reliably constructed aeroplane, over electrical specifications in solar cells, up to magnetoelectric properties in hard disk drives – to name just a few out ...
... of materials research and condensed matter physics. Desired material properties are highly diverse, ranging from mechanical requirements for a reliably constructed aeroplane, over electrical specifications in solar cells, up to magnetoelectric properties in hard disk drives – to name just a few out ...
![arXiv:1210.1847v1 [hep-ph] 4 Oct 2012](http://s1.studyres.com/store/data/016134331_1-89b462677ee8890a2a821c4d84b8db52-300x300.png)
Squeezed light
... (1) the product ∆X 2 ∆P 2 = 1/4 is the same as that for the vacuum state. Squeezing is best visualized by means of the Wigner function — the quantum analogue of the phase-space probability density. Figure 1(c,d) display the Wigner functions of the position- and momentum-squeezed vacuum states, respe ...
... (1) the product ∆X 2 ∆P 2 = 1/4 is the same as that for the vacuum state. Squeezing is best visualized by means of the Wigner function — the quantum analogue of the phase-space probability density. Figure 1(c,d) display the Wigner functions of the position- and momentum-squeezed vacuum states, respe ...
Level shifts of rubidium Rydberg states due to binary interactions
... 兩C典 are single-particle Rydberg states. Generally, the interaction operator, VInt, can be expanded in multipole terms that scale with increasing negative powers of the interatomic separation, R 关25–27兴. This paper primarily addresses situations in which the typical Rydberg-atom separation, R, is abo ...
... 兩C典 are single-particle Rydberg states. Generally, the interaction operator, VInt, can be expanded in multipole terms that scale with increasing negative powers of the interatomic separation, R 关25–27兴. This paper primarily addresses situations in which the typical Rydberg-atom separation, R, is abo ...
Entangling Dipole-Dipole Interactions and Quantum Logic in Optical
... remains finite, the time scales for coherent and incoherent interactions separate, providing a mechanism for controlled entanglement of the atoms. In order to analyze our system we must choose an appropriate basis of states. There are two natural choices: the atomic and molecular bases. In the atom ...
... remains finite, the time scales for coherent and incoherent interactions separate, providing a mechanism for controlled entanglement of the atoms. In order to analyze our system we must choose an appropriate basis of states. There are two natural choices: the atomic and molecular bases. In the atom ...
Spin-dependent Transport of Interacting Electrons in Mesoscopic
... The basis for many nanosystems are semiconductor heterostructures which are produced by epitaxial growth of layers of different semiconductor materials such as GaAs and AlGaAs [4]. With present techniques atomically sharp interfaces between the different materials can be achieved. Because of the dif ...
... The basis for many nanosystems are semiconductor heterostructures which are produced by epitaxial growth of layers of different semiconductor materials such as GaAs and AlGaAs [4]. With present techniques atomically sharp interfaces between the different materials can be achieved. Because of the dif ...