The renormalization of the energy-momentum tensor for an effective initial... Hael Collins R. Holman *
... The expansion during inflation, which provides this elegant explanation for the original fluctuations in the background, has a rather peculiar consequence if we continue to look yet further back in time. To fit all of the observed universe within a single causally connected region at some point duri ...
... The expansion during inflation, which provides this elegant explanation for the original fluctuations in the background, has a rather peculiar consequence if we continue to look yet further back in time. To fit all of the observed universe within a single causally connected region at some point duri ...
![arXiv:1008.1839v2 [hep-th] 12 Aug 2010](http://s1.studyres.com/store/data/016703481_1-ea69a133ddf2690980f0d44baa68ff8f-300x300.png)
Coherent States
... some elementary material that originated in Dirac’s treatment of the theory of quantum oscillators, but which acquired new interest and was carried to a higher state of development when Roy Glauber2 and others laid the foundations of quantum optics. My interest here is not in quantum optics but in t ...
... some elementary material that originated in Dirac’s treatment of the theory of quantum oscillators, but which acquired new interest and was carried to a higher state of development when Roy Glauber2 and others laid the foundations of quantum optics. My interest here is not in quantum optics but in t ...
as PDF
... The formation of classical quantum states is carried out ergodically, i.e., without considering any possible dynamical constraints that may decompose phase space. The electronic phase space is extended to have a spin up and a spin down half-space which are both included in the summation to find the ...
... The formation of classical quantum states is carried out ergodically, i.e., without considering any possible dynamical constraints that may decompose phase space. The electronic phase space is extended to have a spin up and a spin down half-space which are both included in the summation to find the ...
Entanglement and its Role in Shor`s Algorithm
... In fig. 2 we plot the entanglement in Shor’s algorithm using the entropy of the subsystem where possible (full state is pure) and the negativity where the single register state is mixed. The negativity turns out to be zero for both registers throughout the algorithm (except the measurement leaves th ...
... In fig. 2 we plot the entanglement in Shor’s algorithm using the entropy of the subsystem where possible (full state is pure) and the negativity where the single register state is mixed. The negativity turns out to be zero for both registers throughout the algorithm (except the measurement leaves th ...
International Journal of Mathematics, Game Theory and Algebra
... is dense in the space C(Rn ) in the topology of uniform convergence on all compacta (see, e.g., [2,3,4,7,10]). More general result of this type belongs to Leshno, Lin, Pinkus and Schoken [11]. They proved that the necessary and sufficient condition for any continuous activation function to have the ...
... is dense in the space C(Rn ) in the topology of uniform convergence on all compacta (see, e.g., [2,3,4,7,10]). More general result of this type belongs to Leshno, Lin, Pinkus and Schoken [11]. They proved that the necessary and sufficient condition for any continuous activation function to have the ...
3. Generation of the Quantum Fault Table
... simple case one can make no statements as to the probability that a fault is present at location X in the circuit prior to running a given test. It is only running the test that allows us to make one of the following statements: (1) the fault is definitely not present at location X, or (2) the fault ...
... simple case one can make no statements as to the probability that a fault is present at location X in the circuit prior to running a given test. It is only running the test that allows us to make one of the following statements: (1) the fault is definitely not present at location X, or (2) the fault ...
Stochastic Switching Circuit Synthesis
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
Stochastic Switching Circuit Synthesis Daniel Wilhelm Jehoshua Bruck
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
Stochastic Switching Circuit Synthesis - Paradise
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
... Using this equation, we can prove statements about all stochastic switching circuits (beyond those which are enumerably series-parallel). Note that C > O. Intuitively, by adding a new pswitch we create a new potential path between the terminals. Hence, for the new circuit M, P r(M) > O. Since closin ...
Quantum electrodynamics
In particle physics, quantum electrodynamics (QED) is the relativistic quantum field theory of electrodynamics. In essence, it describes how light and matter interact and is the first theory where full agreement between quantum mechanics and special relativity is achieved. QED mathematically describes all phenomena involving electrically charged particles interacting by means of exchange of photons and represents the quantum counterpart of classical electromagnetism giving a complete account of matter and light interaction.In technical terms, QED can be described as a perturbation theory of the electromagnetic quantum vacuum. Richard Feynman called it ""the jewel of physics"" for its extremely accurate predictions of quantities like the anomalous magnetic moment of the electron and the Lamb shift of the energy levels of hydrogen.