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Quantum Memory in Atomic Ensembles - Oxford Physics
Quantum Memory in Atomic Ensembles - Oxford Physics

... Thanks to my Oxford massif, Andy Scott and Tom Rowlands-Rees, who know a good lunch when they see one. And in that vein, thanks to Matthijs Branderhorst, who along with Ben, introduced me to the burrito. There is a growing ultrafast diaspora — good people in far-off places — and of these I should li ...
THE RENORMALIZATION GROUP AND CRITICAL PHENOMENA
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... 3 4’ the distinction between water and steam disappears, and the whole boiling phenomenon vanishes. The principal distinction between water and steam is that they have different densities. As the pressure and temperature approach their critical values, the difference in density between water and ste ...
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Annals of Physics Classical impurities and boundary Majorana zero

... modes remain true zero modes, and their existence implies the two-fold degeneracy of the ground state in the ordered phase of the QIC. It is worth mentioning that the usefulness of the Majorana fermions in the QIC hinges on the exact Z2 symmetry of the spin model (2). Local terms (in the x or y ) wh ...
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... of undergraduate and introductory graduate quantum courses. It is necessary to choose a zero of energy, and it is possible to multiply the wave function by an overall global phase factor, and that’s about it. Continuum-state quantum mechanics, by contrast, presents four options—all of which, as we s ...
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Quantum Physics

Stimulated emission from single quantum dipoles
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... field lab (NHMFL) at Tallahassee, FL. I here thank the NHMFL staff Bruce Brandt, Eric Palm, Tim Murphy and Glover Jones for their assistance in my experiments. I also thank Dr. Lloyd Engel, Dr. Zhigang Jiang and Dr. Murthy Ganapathy for the great conversations and suggestions in my every trip to NHM ...
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Anti Heisenberg. The end of Heisenberg`s uncertainty principle.

... ‘When the position is determined .. the electron undergoes a discontinuous change in momentum. This change is the greater the smaller the wavelength of the light employed, i.e., the more exact the determination of the position ... thus, the more precisely the position is determined, the less precise ...
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... cooperations have noticeably increased. As this Report demonstrates, the scientific output has also grown. The idea behind the Junior Research Groups program is beginning to work. It is this kind of academic environment we are having, which is a prerequisite for fruitful scientific work. Most recent ...
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... as well as for the numerical calculation of path integrals. The described discretization procedure is most straightforwardly numerically implemented by the Path-Integral Monte-Carlo approach [55]. Note that the O(1/N ) convergence can be also achieved with other choices of space-time points at which ...
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... Ic ranged from a few tens of nanoamperes to almost 1 microampere, depending on the gate voltage and on the geometrical dimensions of the junctions. The typical device width was  1 µm and contact separations between 200 and 500 nm were studied. Note, in passing, that what we actually measure is the ...
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... the time scale τs , which gives the time to perform a two-qubit operation, there is a time scale associated with the rise/fall-time of the exchange J(t). This is the switching time τsw . When the relevant two-spin Hamiltonian takes the form of an ideal (isotropic) exchange, as given in (1.1), the to ...
Implementation of a combined charge-phase quantum bit - ENS-phys
Implementation of a combined charge-phase quantum bit - ENS-phys

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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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