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Nuclear and Particle Physics - Lecture 11 Parity and charge
Nuclear and Particle Physics - Lecture 11 Parity and charge

Quantum gases in optical lattices
Quantum gases in optical lattices

... the same and does not fluctuate. How- (a) Controlled interactions between atoms on the lab. The ETH team has compared ever, this means that the phase coherence different lattice sites are possible with the help of the oscillation frequencies of an axial lattice potentials. In such a between atoms on ...
Low-energy fusion dynamics of weakly bound nuclei
Low-energy fusion dynamics of weakly bound nuclei

... The PLATYPUS model uses two notions: classical trajectory and MonteCarlo sampling of probability densities. This approach has been developed in close collaboration with experimenters [3, 4]. The model is implemented in the PLATYPUS code [5]. For a given impact parameter and bombarding energy, a weak ...
Fine Structure Constant Variation from a Late Phase Transition
Fine Structure Constant Variation from a Late Phase Transition

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... emerge during concept conjunction, one is making use of world knowledge, or `extensional feedback’. He states: `We can not expect any model of conceptual combination to account directly for such e€ ects, as they clearly relate to information that is obtained from another sourceÐnamely familiarity wi ...
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... more detailed considerations in favour of the epistemic conception of quantum states related to quantum nonlocality, based on Einstein's remarks on entangled states. 7 This is at least what happens if one assumes, as usual, the so-called eigenstate-eigenvalue link which says that for a system in a s ...
Gravitational Quantum States of Neutrons and the New GRANIT
Gravitational Quantum States of Neutrons and the New GRANIT

String Theory as a Theory of Quantum Gravity
String Theory as a Theory of Quantum Gravity

The interpretation of the Einstein-Rupp experiments and their
The interpretation of the Einstein-Rupp experiments and their

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Vincent Gammill
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... down when the system is infinitely large, and symmetries can be “broken”. We return to this point in the next Section. Quantum phase transitions, on the other hand, can only be achieved by scaling some parameter (such as electric field) at T = 0, by definition. They are driven by quantum, rather tha ...
Fano-Feshbach resonances in two
Fano-Feshbach resonances in two

... Starting from the fact that in scattering systems EPs give rise to a second order pole in the Green’s function, in addition to the usual first order pole, we have investigated the impact on the shape of the scattering cross section as one approaches the EP. We have demonstrated that the merging of t ...
PULLEYS - Mathematics with Mr Walters
PULLEYS - Mathematics with Mr Walters

... When two particles A and B collide, they exert equal and opposite forces, and hence impulses, on each other. The impulse that A exerts on B (equal to B’s change in momentum) is therefore equal and opposite to the impulse that B exerts on A (equal to A’s change in momentum). If these changes are equa ...
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Adaptive beam combining and interferometry with photorefractive quantum wells *

... transport nonlinearity.10,16 In Eq. (8) the modulation amplitude is given by the index m multiplied by a parameter ␰, which expresses the contrast ratio of the field within the device relative to the modulation expressed by Eq. (7). Most of the electron-transport physics of the photorefractive effec ...
Interaction- and measurement-free quantum Zeno gates for universal computation
Interaction- and measurement-free quantum Zeno gates for universal computation

... qubit is coherently driven on a time scale slow compared to the measurement time. The coherent evolution of the probe qubit will be allowed or prohibited depending on the state of the object qubit and thus will create entanglement to implement the gate operation. This gate, however, requires the two ...
Chapter 38 - Quantum scattering
Chapter 38 - Quantum scattering

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... ChaosBook.org version15.7, Apr 8 2015 ...
Atom InterferometryPrecision D. E. Pritchard
Atom InterferometryPrecision D. E. Pritchard

... scattered from each atom. Scattering multiple photons causes the same type of time-evolution of decoherence as interaction with a thermal bath, and is theoretically similar to any situation where the quantum system undergoes multiple independent dephasing events. The heart of this experiment is the ...
Niels Bohr - Nobel Lecture
Niels Bohr - Nobel Lecture

... of heat radiation, which, because of its independence of the individual prop erties of substances, lent itself peculiarly well to a test of the applicability of the laws of classical physics to atomic processes. Planck considered the equilibrium of radiation between a number of systems with the same ...
Quantum Computation and Quantum Information
Quantum Computation and Quantum Information

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Non aligned hydrogen molecular ion in strong magnetic fields

Interacting Fock spaces: central limit theorems and quantum
Interacting Fock spaces: central limit theorems and quantum

... field operator (i.e. an operator given by addiction of creation, annihilation and suitable preservation) are uniquely determined by the norm of the test function chosen. This result, which is fundamental in the proof of central limit theorem, it is not true in a generic IFS, as shown by Lu in [46]. ...
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Magnon collapse near the Lifshitz point and Leon Balents, KITP, UCSB
Magnon collapse near the Lifshitz point and Leon Balents, KITP, UCSB

... figure. Integrating Cm/T between 1.8 K and 60 K, we find a value of 4.1 J/mol K which is about 30 % smaller than the total magnetic entropy (Rln2) for S = 1/2. The discrepancy is most likely due to crudeness of the estimation of the lattice contribution particularly at high temperature. To be noted ...
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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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