A continued fraction resummation form of bath
... perturbation term, this simple summation cannot be applied since K (2k) diverges as the expansion order increases. Instead, a resummation technique is required for a converged result, with one or more high-order corrections of K (2k) (k ≥ 2). For the leading-order QKE correction K (4), various resum ...
... perturbation term, this simple summation cannot be applied since K (2k) diverges as the expansion order increases. Instead, a resummation technique is required for a converged result, with one or more high-order corrections of K (2k) (k ≥ 2). For the leading-order QKE correction K (4), various resum ...
ORAMs in a Quantum World - Cryptology ePrint Archive
... in order to show that the resulting disturbance is tolerable for the protocol itself. This is usually done in many different, ad-hoc, and often complex ways, depending on the scenario [10, 12, 11, 3]. In our work we formalize this problem by introducing the notion of a safe extractor. This can be se ...
... in order to show that the resulting disturbance is tolerable for the protocol itself. This is usually done in many different, ad-hoc, and often complex ways, depending on the scenario [10, 12, 11, 3]. In our work we formalize this problem by introducing the notion of a safe extractor. This can be se ...
Toward the Unification of Physics and Number Theory
... have no degrees of freedom. We define symbol here as “an object that represents itself or something else”. And, finally, we define an object as “anything which can be thought of”. Fundamental particles have distinct geometries and are, in some sense, geometric symbols. For example, at each energy st ...
... have no degrees of freedom. We define symbol here as “an object that represents itself or something else”. And, finally, we define an object as “anything which can be thought of”. Fundamental particles have distinct geometries and are, in some sense, geometric symbols. For example, at each energy st ...
On the quantization of the superparticle action in proper time and the
... More recently, [15–17], several works appear where the problem of the quantization procedure and the square root operators was carefully analyzed. In these articles was demonstrated for different simple problems (harmonic oscillator, massive particle on hyperboloid, etc) that the spectrum changes dr ...
... More recently, [15–17], several works appear where the problem of the quantization procedure and the square root operators was carefully analyzed. In these articles was demonstrated for different simple problems (harmonic oscillator, massive particle on hyperboloid, etc) that the spectrum changes dr ...
Classical Field Theory - Imperial College London
... it transforms like a vector under Lorentz transformations. For this reason it is often called a vector field. Such fields always correspond to particles with spin one though this connection requires a study of the group theory behind the Lorentz transformations. These fields also appear in what is call ...
... it transforms like a vector under Lorentz transformations. For this reason it is often called a vector field. Such fields always correspond to particles with spin one though this connection requires a study of the group theory behind the Lorentz transformations. These fields also appear in what is call ...
Comment on “Non-representative Quantum Mechanical Weak Values”
... Svensson then continues with a few examples where we might have in|S|in = 0. He reiterates that this is “a problem” but does not demonstrate what this problem is, ...
... Svensson then continues with a few examples where we might have in|S|in = 0. He reiterates that this is “a problem” but does not demonstrate what this problem is, ...
![arXiv:1312.4758v2 [quant-ph] 10 Apr 2014](http://s1.studyres.com/store/data/021352507_1-d587dd4045ccae4ae6a47bb17173f358-300x300.png)
Theoretical Chemistry I Quantum Mechanics
... 2.7 Momentum-Space Wave Function . . . . . . . . . . . . . . . . . . . . 2.7.1 Gaussian Wave Packets . . . . . . . . . . . . . . . . . . . . . . 2.7.2 Generalization to three dimensions . . . . . . . . . . . . . . . 2.7.3 Appendix: Position representation of the momentum operator ...
... 2.7 Momentum-Space Wave Function . . . . . . . . . . . . . . . . . . . . 2.7.1 Gaussian Wave Packets . . . . . . . . . . . . . . . . . . . . . . 2.7.2 Generalization to three dimensions . . . . . . . . . . . . . . . 2.7.3 Appendix: Position representation of the momentum operator ...
Quantum Dynamical Systems
... KMS states appear naturally in the modular structure associated with faithful normal states (or more generally semi-finite weight) on von Neumann algebras. They are thus intimately connected with their mathematical structure. This tight relation between dynamics and the structure of the observable a ...
... KMS states appear naturally in the modular structure associated with faithful normal states (or more generally semi-finite weight) on von Neumann algebras. They are thus intimately connected with their mathematical structure. This tight relation between dynamics and the structure of the observable a ...
Quantum walk search on satisfiability problems random
... and David Deutsch in the 1980's, quantum computing remained little more than a curiosity until Peter 8hor's discovery of a polynomial time integer factorization algorithm in 1994 and Lov Grover's subsequent development of a quantum search algorithm in 1996 [13, 12, 29, 14]. The discovery of these pr ...
... and David Deutsch in the 1980's, quantum computing remained little more than a curiosity until Peter 8hor's discovery of a polynomial time integer factorization algorithm in 1994 and Lov Grover's subsequent development of a quantum search algorithm in 1996 [13, 12, 29, 14]. The discovery of these pr ...
