The Computational Complexity of Linear Optics
... causing any collapse of complexity classes or other disastrous theoretical consequences. Also, of course, there are subexponential-time factoring algorithms (such as the number field sieve), and few would express confidence that they cannot be further improved. And thus, ever since Bernstein and Vaz ...
... causing any collapse of complexity classes or other disastrous theoretical consequences. Also, of course, there are subexponential-time factoring algorithms (such as the number field sieve), and few would express confidence that they cannot be further improved. And thus, ever since Bernstein and Vaz ...
PPT - Physics
... “The model we shall choose is not a popular one, through each other and fall apart (i.e. so that we will not duplicate too much of the no hard scattering). The outgoing work of others who are similarly analyzing particles continue in roughly the same various models (e.g. constituent interchange Part ...
... “The model we shall choose is not a popular one, through each other and fall apart (i.e. so that we will not duplicate too much of the no hard scattering). The outgoing work of others who are similarly analyzing particles continue in roughly the same various models (e.g. constituent interchange Part ...
Observable and hidden singular features of large fluctuations
... can be found from the condition that the energy of the Hamiltonian motion E = 0. The paths infinitesimally close toMPEP ([C(I) I ---, 0) and lyingon the opposite sides of it approach asymptotically the eigenvectors ±qO) as t ~ ~ and then go away from the saddle point. The corresponding limiting path ...
... can be found from the condition that the energy of the Hamiltonian motion E = 0. The paths infinitesimally close toMPEP ([C(I) I ---, 0) and lyingon the opposite sides of it approach asymptotically the eigenvectors ±qO) as t ~ ~ and then go away from the saddle point. The corresponding limiting path ...
Quantum non-demolition - Quantum Optics and Spectroscopy
... from the inability to create pure states. This prevents scaling of this technology to higher numbers of quantum bits. Solid state implementations offer the promise of easy scalability akin to integrated circuits as soon as one is able to reliably manufacture and control the basic building blocks. In ...
... from the inability to create pure states. This prevents scaling of this technology to higher numbers of quantum bits. Solid state implementations offer the promise of easy scalability akin to integrated circuits as soon as one is able to reliably manufacture and control the basic building blocks. In ...
Chapter 13
... In this case, the result is not x multiplied by a constant, so x is not an eigenfunction of the operator d/dx unless either A or B is zero. Chapter 13: The Schrödinger Equation Physical Chemistry 2nd Edition © 2010 Pearson Education South Asia Pte Ltd ...
... In this case, the result is not x multiplied by a constant, so x is not an eigenfunction of the operator d/dx unless either A or B is zero. Chapter 13: The Schrödinger Equation Physical Chemistry 2nd Edition © 2010 Pearson Education South Asia Pte Ltd ...
The book of abstracts - MECO 42
... is possible to travel from an equilibrium state to another in an arbitrary time, much shorter than the natural relaxation time. Such strategies are reminiscent of those worked out in the recent field of Shortcut to Adiabaticity, that aim at developing protocols, both in quantum and in classical regi ...
... is possible to travel from an equilibrium state to another in an arbitrary time, much shorter than the natural relaxation time. Such strategies are reminiscent of those worked out in the recent field of Shortcut to Adiabaticity, that aim at developing protocols, both in quantum and in classical regi ...
Chapter 14.
... Figure 14.3.1: Block “Count Ones” realized using binary Half-Adders and FullAdders. The block at the bottom is the adder from Figure 14.2.2. Ancilla qubits are not shown. The design approach simplifies the circuit design process and the number and complexity of gates, at the price of increasing the ...
... Figure 14.3.1: Block “Count Ones” realized using binary Half-Adders and FullAdders. The block at the bottom is the adder from Figure 14.2.2. Ancilla qubits are not shown. The design approach simplifies the circuit design process and the number and complexity of gates, at the price of increasing the ...
Quantum gauge theory simulation with ultracold atoms
... a 2D lattice under the action of an exotic and external gauge eld related to the Heisenberg-Weyl gauge group. We describe a novel method to simulate the gauge degree of freedom, which consists of mapping the gauge coordinate to a real and perpendicular direction with respect to the 2D space of posi ...
... a 2D lattice under the action of an exotic and external gauge eld related to the Heisenberg-Weyl gauge group. We describe a novel method to simulate the gauge degree of freedom, which consists of mapping the gauge coordinate to a real and perpendicular direction with respect to the 2D space of posi ...
The Monte Carlo Method in Quantum Mechanics Colin Morningstar Carnegie Mellon University
... Monte Carlo estimates require statistically independent random configurations, but configurations generated by a Markov process do depend on previous elements in chain ¾ this dependence is known as autocorrelation this autocorrelation can actually be measured! ¾ for any observable (integrand) , th ...
... Monte Carlo estimates require statistically independent random configurations, but configurations generated by a Markov process do depend on previous elements in chain ¾ this dependence is known as autocorrelation this autocorrelation can actually be measured! ¾ for any observable (integrand) , th ...
Yang-Baxter sigma models based on the CYBE
... The parameter η measures the associated deformation. Note that the model is reduced to a principal chiral model when η = 0 . Then, this deformed model has the following Lax pair; ...
... The parameter η measures the associated deformation. Note that the model is reduced to a principal chiral model when η = 0 . Then, this deformed model has the following Lax pair; ...
DRIFT ACCELERATION AT INTERPLANETARY SHOCKS
... of particles. The most important parameter of the acceleration, measured in velocity units, is the effective shock velocity w, which should be compared to the particle velocity v. As the results of analytical calculations show, for quasi-perpendicular shocks, all physical quantities, including the e ...
... of particles. The most important parameter of the acceleration, measured in velocity units, is the effective shock velocity w, which should be compared to the particle velocity v. As the results of analytical calculations show, for quasi-perpendicular shocks, all physical quantities, including the e ...
Strong luminescence quantum-efficiency enhancement near prolate
... The modifications of the radiative decay rate ⌫R and the total decay rate ⌫tot of a dipole emitter in close proximity to either a spherical or a prolate metal nanoparticle can be calculated with the improved GN model.15 In this model, the decay rate modifications are calculated based on a two-step a ...
... The modifications of the radiative decay rate ⌫R and the total decay rate ⌫tot of a dipole emitter in close proximity to either a spherical or a prolate metal nanoparticle can be calculated with the improved GN model.15 In this model, the decay rate modifications are calculated based on a two-step a ...
PS - USTC, ICTS
... J z lz ~ or ~ sz 1 • For asymmetric em E-M tensor, there should be difference of the diffraction pattern between orbital and spin polarized beams, because only for orbital polarized beam there is momentum density circular flow in the transverse plane. A detailed analysis had been given in arXiv ...
... J z lz ~ or ~ sz 1 • For asymmetric em E-M tensor, there should be difference of the diffraction pattern between orbital and spin polarized beams, because only for orbital polarized beam there is momentum density circular flow in the transverse plane. A detailed analysis had been given in arXiv ...
Chapter I
... Some times the motion of a particle or a system of particles is not free but it is limited by putting some restrictions on the position co-ordinates of the particle or system of particles. The motion under such restrictions is called constraint motion or restricted motion. The mathematical relations ...
... Some times the motion of a particle or a system of particles is not free but it is limited by putting some restrictions on the position co-ordinates of the particle or system of particles. The motion under such restrictions is called constraint motion or restricted motion. The mathematical relations ...