Coherent states and projective representation of the linear canonical
... representation in terms of coherent states, Ref. 4 for applications of this treatment of the homogeneous linear canonical transformations, Ref. 5 for an application of the inhomogeneous linear canonical transformations, and Ref. 6 for a relation with Bogoliubov transformations and quasi-free states ...
... representation in terms of coherent states, Ref. 4 for applications of this treatment of the homogeneous linear canonical transformations, Ref. 5 for an application of the inhomogeneous linear canonical transformations, and Ref. 6 for a relation with Bogoliubov transformations and quasi-free states ...
Guidance Applied to Quantum Operations in Josephson
... where ac is the acceleration required or ‘commanded’, N’ is a constant known as the navigation constant and typically chosen between 4 and 8. ZEM is the Zero Effort Miss. The controls are moderated by 1/tgo2 where tgo is the time to go until the end of the operation. Classically proportional navigat ...
... where ac is the acceleration required or ‘commanded’, N’ is a constant known as the navigation constant and typically chosen between 4 and 8. ZEM is the Zero Effort Miss. The controls are moderated by 1/tgo2 where tgo is the time to go until the end of the operation. Classically proportional navigat ...
view Pdf - Informatik - FB3
... following the default mapping scheme, each Toffoli gate is mapped to a quantum realization of depth 5 as shown in Fig. 6(b). However, as the second and the third gate share the same control line, an additional helper line allows for a concurrent execution of both gates as shown in Fig. 6(c). Since a ...
... following the default mapping scheme, each Toffoli gate is mapped to a quantum realization of depth 5 as shown in Fig. 6(b). However, as the second and the third gate share the same control line, an additional helper line allows for a concurrent execution of both gates as shown in Fig. 6(c). Since a ...
Toward Quantum Computational Agents.
... The Hadamard gate creates a superposed qubit state for standard basis states, demonstrates destructive quantum interference if applied to superposed quantum states (MH ( √12 (|0 > +|1 >)) = |0 >), and can be physically realized, for example, by a 50/50-beamsplitter in a Mach-Zehnder interferometer [ ...
... The Hadamard gate creates a superposed qubit state for standard basis states, demonstrates destructive quantum interference if applied to superposed quantum states (MH ( √12 (|0 > +|1 >)) = |0 >), and can be physically realized, for example, by a 50/50-beamsplitter in a Mach-Zehnder interferometer [ ...
QUANTUM COMPUTING: AN OVERVIEW
... the state |λi is given by |ci |2 (i = 1, 2). The complex coefficient ci is called the probability amplitude in this sense. It should be noted that a measurement produces one outcome λi and the probability of obtaining it is experimentally evaluated only after repeating measurements with many copies ...
... the state |λi is given by |ci |2 (i = 1, 2). The complex coefficient ci is called the probability amplitude in this sense. It should be noted that a measurement produces one outcome λi and the probability of obtaining it is experimentally evaluated only after repeating measurements with many copies ...
The Need for Structure in Quantum Speedups
... and Q(f ) are both tiny but D(f ) is huge. As an example, consider the Deutsch-Jozsa problem [17]: given a Boolean input (x1 , . . . , xN ), decide whether the xi ’s are all equal or whether half of them are 1 and the other half are 0, under the promise that one of these is the case. Second, if M = ...
... and Q(f ) are both tiny but D(f ) is huge. As an example, consider the Deutsch-Jozsa problem [17]: given a Boolean input (x1 , . . . , xN ), decide whether the xi ’s are all equal or whether half of them are 1 and the other half are 0, under the promise that one of these is the case. Second, if M = ...
Black Hole Entropy: From Shannon to Bekenstein
... forms of quantum mechanical modes of the states inside and outside the BH horizon (see also [9]). This directly yields the probabilities of individual ingoing modes being trapped inside the BH horizon, (which is indeed unity), or tunneling out of the BH horizon and escaping to infinity to be perceiv ...
... forms of quantum mechanical modes of the states inside and outside the BH horizon (see also [9]). This directly yields the probabilities of individual ingoing modes being trapped inside the BH horizon, (which is indeed unity), or tunneling out of the BH horizon and escaping to infinity to be perceiv ...
Atomic Quantum Metrology with Narrowband Entangled and Squeezed States of Light DISSERTATION
... per second N is measured, the intrinsic error or quantum noise will be N . Photons in a laser beam and rain drops follow the same behavior as they are both governed by the statistics of random √ independent events: the Poisson distribution. The N -limit is generally called shot-noise limit and in qu ...
... per second N is measured, the intrinsic error or quantum noise will be N . Photons in a laser beam and rain drops follow the same behavior as they are both governed by the statistics of random √ independent events: the Poisson distribution. The N -limit is generally called shot-noise limit and in qu ...
Full-text PDF - American Mathematical Society
... assuming that our states are always Hecke eigenstates. This is the means by which we circumvent the issue of the unlikely, but potentially possible, high multiplicities m(λ). It is known that the multiplicities of the spaces of such joint Hecke eigenfunctions is small and, in particular for Y , it i ...
... assuming that our states are always Hecke eigenstates. This is the means by which we circumvent the issue of the unlikely, but potentially possible, high multiplicities m(λ). It is known that the multiplicities of the spaces of such joint Hecke eigenfunctions is small and, in particular for Y , it i ...
Continuous Variable Quantum Information: Gaussian States and
... of a particle. This second approach has witnessed considerable success due to its versatility, with implementations often encompassing different physical systems, e.g. light quadratures and collective magnetic moments of atomic ensembles, which obey the same canonical algebra. The aim of this paper i ...
... of a particle. This second approach has witnessed considerable success due to its versatility, with implementations often encompassing different physical systems, e.g. light quadratures and collective magnetic moments of atomic ensembles, which obey the same canonical algebra. The aim of this paper i ...
Introduction to the Bethe Ansatz II
... the model system which inspired Bethe to formulate the now celebrated method for calculating eigenvalues, eigenvectors, and a host of physical properties. Interest in quasi-1D magnetic materials has stimulated theoretical work on quantum spin chains from the early sixties until the present. Some of ...
... the model system which inspired Bethe to formulate the now celebrated method for calculating eigenvalues, eigenvectors, and a host of physical properties. Interest in quasi-1D magnetic materials has stimulated theoretical work on quantum spin chains from the early sixties until the present. Some of ...