Near field heat transfer between metamaterials
... permanence energy and momentum [1] throughout the thermally and quantum fluctuating electromagnetic field they radiate in their surrounding. At long separation distance compared to the Wien wavelength ( T c /( k B T) ), energy radiative transfer is maximal when both media behave like black ...
... permanence energy and momentum [1] throughout the thermally and quantum fluctuating electromagnetic field they radiate in their surrounding. At long separation distance compared to the Wien wavelength ( T c /( k B T) ), energy radiative transfer is maximal when both media behave like black ...
First-principles study of the electronic structure of CdS/ZnSe coupled
... site is taken as the reference level for the evaluation of the valence band offsets. The calculated valence band offsets using this method are shown in Table I. We find both the method provide nearly identical value for the HOMO offsets. The LUMO offsets calculated using the latter method, i.e. addi ...
... site is taken as the reference level for the evaluation of the valence band offsets. The calculated valence band offsets using this method are shown in Table I. We find both the method provide nearly identical value for the HOMO offsets. The LUMO offsets calculated using the latter method, i.e. addi ...
![Probability in Bohmian Mechanics[1]](http://s1.studyres.com/store/data/001567507_1-29d8fd2fe0d2e1e754834ae0307e0c62-300x300.png)
Probability in Bohmian Mechanics[1]
... 3. Why Justify the Distribution Postulate? The status of the distribution postulate has been controversial since Bohm announced his theory. Pauli 1953 and Keller 1953 soon objected to simply stipulating (3). They wanted Bohmian mechanics to work with any initial probability distribution; that is, th ...
... 3. Why Justify the Distribution Postulate? The status of the distribution postulate has been controversial since Bohm announced his theory. Pauli 1953 and Keller 1953 soon objected to simply stipulating (3). They wanted Bohmian mechanics to work with any initial probability distribution; that is, th ...
atom-ph/9606004 PDF
... this paper the language of continuous measurement theory [7] to describe a single realization of an interference experiment between two independent condensates. We will discuss how the state of the two condensates evolves as atoms are detected. In particular, from our analysis it follows how a state ...
... this paper the language of continuous measurement theory [7] to describe a single realization of an interference experiment between two independent condensates. We will discuss how the state of the two condensates evolves as atoms are detected. In particular, from our analysis it follows how a state ...
Quantum computation and Shor`s factoring algorithm
... in superposition and produce a final output depending on the interference of all of them. This is in contrast to a classical probabilistic Turing machine, which follows only some single (randomly chosen) path. This feature has been called ‘‘computation by quantum parallelism’’ (Deutsch, 1985; Jozsa, ...
... in superposition and produce a final output depending on the interference of all of them. This is in contrast to a classical probabilistic Turing machine, which follows only some single (randomly chosen) path. This feature has been called ‘‘computation by quantum parallelism’’ (Deutsch, 1985; Jozsa, ...
Entanglement and its Role in Shor`s Algorithm
... of qubits and calculating the negativity [9, 10] given by η = Tr|ρT | − 1 i.e., the sum of the negative eigenvalues of the transposed matrix ρTL or ρTS . If the negativity is zero for all possible subsets of qubits in the register, then we can say that at most the register has bound entanglement [11 ...
... of qubits and calculating the negativity [9, 10] given by η = Tr|ρT | − 1 i.e., the sum of the negative eigenvalues of the transposed matrix ρTL or ρTS . If the negativity is zero for all possible subsets of qubits in the register, then we can say that at most the register has bound entanglement [11 ...
py354-final-121502
... transmit a very particular incident energy such that all other near-by energies would be effectively reflected. One way to accomplish this is to build a repeating series of barriers, all the same width and height, such that the resonant condition is always met. Show by sketch what happens to the tra ...
... transmit a very particular incident energy such that all other near-by energies would be effectively reflected. One way to accomplish this is to build a repeating series of barriers, all the same width and height, such that the resonant condition is always met. Show by sketch what happens to the tra ...
Structure, Individuality and Quantum Gravity
... “primitive thisness,” is called their “haecceity.”9 Traditionally, it was always assumed that every entity has such a unique individuality: a haecceity as well as a quiddity. However, modern physics has reached a point, at which we are led to postulate entities that have quiddity but no haecceity th ...
... “primitive thisness,” is called their “haecceity.”9 Traditionally, it was always assumed that every entity has such a unique individuality: a haecceity as well as a quiddity. However, modern physics has reached a point, at which we are led to postulate entities that have quiddity but no haecceity th ...
Decoherence in Excited Atoms by Low-Energy Scattering
... Current experimental techniques have allowed the manipulation of atomic systems to previously unthinkable degrees, paving the way to the development of new technologies and the observation of very small quantum effects. One such technology is the quantum computer; trapped-ion systems have been imple ...
... Current experimental techniques have allowed the manipulation of atomic systems to previously unthinkable degrees, paving the way to the development of new technologies and the observation of very small quantum effects. One such technology is the quantum computer; trapped-ion systems have been imple ...
Phys. Rev. A 92, 032304
... arbitrary, real gain values, ĈZj k (g) ≡ e2igx̂j x̂k , leading to certain weighted (real-valued) graph states, with g = 1 as the special case of unweighted graph states. More generally, any physical graph state can be described by complex weights and a complex adjacency matrix (including self-loops ...
... arbitrary, real gain values, ĈZj k (g) ≡ e2igx̂j x̂k , leading to certain weighted (real-valued) graph states, with g = 1 as the special case of unweighted graph states. More generally, any physical graph state can be described by complex weights and a complex adjacency matrix (including self-loops ...
Quantum and private capacities of low
... while for p = 1/4, we know that Q(D1/4 ) = 0. However, for 0 < p < 1/4 the quantum capacity of D p is unknown despite substantial effort (see e.g. [21, 6, 10]). For p ≈ 0.2, communication rates higher than the 1-shot coherent information are achievable [5, 21, 6], but even the threshold value of p w ...
... while for p = 1/4, we know that Q(D1/4 ) = 0. However, for 0 < p < 1/4 the quantum capacity of D p is unknown despite substantial effort (see e.g. [21, 6, 10]). For p ≈ 0.2, communication rates higher than the 1-shot coherent information are achievable [5, 21, 6], but even the threshold value of p w ...