Dynamics of the quantum Duffing oscillator in the driving induced q
... duces an effective dynamic bistability which is manifest by the non-monotoneous dependence of the amplitude A of the stationary vibrations for varying x. For the classical system where all potential energies are allowed, this response curve A(x) is smooth showing only two points of bifurcation for th ...
... duces an effective dynamic bistability which is manifest by the non-monotoneous dependence of the amplitude A of the stationary vibrations for varying x. For the classical system where all potential energies are allowed, this response curve A(x) is smooth showing only two points of bifurcation for th ...
The Beh-MechaNiSM, iNTeracTioNS wiTh ShorT
... could be defined. This means that the amplitude for scattering between electrically charged particles can be written as an expansion in powers of the fine structure constant, α, which is a measure of the strength of the electric force. When computing these terms, most of them are found to be infinit ...
... could be defined. This means that the amplitude for scattering between electrically charged particles can be written as an expansion in powers of the fine structure constant, α, which is a measure of the strength of the electric force. When computing these terms, most of them are found to be infinit ...
Computation of hadronic two-point functions in Lattice QCD
... field theories: not directly measurable parameters need to be adjusted as functions of a scale µ at which QCD is evaluated, to keep physical observables (e.g. hadron masses) constant and well defined. In QCD this is possible and no new terms need to be introduced as µ is sent to infinity. QCD is a r ...
... field theories: not directly measurable parameters need to be adjusted as functions of a scale µ at which QCD is evaluated, to keep physical observables (e.g. hadron masses) constant and well defined. In QCD this is possible and no new terms need to be introduced as µ is sent to infinity. QCD is a r ...
Phys. Rev. Lett. 108, 100501 - APS Link Manager
... state away from resonance. Hence, within the blockade radius, the underlying spatial distribution of the sites is largely irrelevant and the arising many-body ground state washes over the effects of disorder and can lead to the formation of crystalline structures [13]. The dynamic crystal formation ...
... state away from resonance. Hence, within the blockade radius, the underlying spatial distribution of the sites is largely irrelevant and the arising many-body ground state washes over the effects of disorder and can lead to the formation of crystalline structures [13]. The dynamic crystal formation ...
A pairing between super Lie-Rinehart and periodic cyclic
... where µ’s are smooth measures on Y as above, P is a cycle (resp. boundary) then the differential form ιX1 . . . ιXp µ is closed (resp. exact). Let us consider now a smooth proper map p : N → M into a differential space M , possibly singular, contracting each orbit contained in P to a point. Let A := ...
... where µ’s are smooth measures on Y as above, P is a cycle (resp. boundary) then the differential form ιX1 . . . ιXp µ is closed (resp. exact). Let us consider now a smooth proper map p : N → M into a differential space M , possibly singular, contracting each orbit contained in P to a point. Let A := ...
61, 062310 (2000)
... postselection of the measurement results. They showed that a set of nonorthogonal but linear-independent pure states can be faithfully cloned with optimal success probability. Recently, Chelfes and Barnett 关17兴 presented the idea of hybrid cloning, which interpolates between deterministic and probab ...
... postselection of the measurement results. They showed that a set of nonorthogonal but linear-independent pure states can be faithfully cloned with optimal success probability. Recently, Chelfes and Barnett 关17兴 presented the idea of hybrid cloning, which interpolates between deterministic and probab ...
Temporal Multimode Storage of Entangled Photon Pairs
... pairs, we see that the presence of two excitations does not change the efficiency of the QM. The multimode capacity of the QM is given by the number of modes (bins on the histogram) and equal to 10. Those results are direct signatures of temporal multimode capacity of our QM, using simultaneous stor ...
... pairs, we see that the presence of two excitations does not change the efficiency of the QM. The multimode capacity of the QM is given by the number of modes (bins on the histogram) and equal to 10. Those results are direct signatures of temporal multimode capacity of our QM, using simultaneous stor ...
Mysteries of Mass Article in Scientific American
... the hillock [see box on preceding page]. The universe, like a ball, comes to rest somewhere on this circular trench, which corresponds to a nonzero value of the field. That is, in its natural, lowest energy state, the universe is permeated throughout by a nonzero Riggs field. The final distinguishin ...
... the hillock [see box on preceding page]. The universe, like a ball, comes to rest somewhere on this circular trench, which corresponds to a nonzero value of the field. That is, in its natural, lowest energy state, the universe is permeated throughout by a nonzero Riggs field. The final distinguishin ...
PDF only - at www.arxiv.org.
... persists undiminished no matter how far apart A and B may drift. Such entangled systems are known, both theoretically and experimentally, to have nonlocal properties, behaving in many ways like a single unified quantum that can change instantaneously throughout its entire ex ...
... persists undiminished no matter how far apart A and B may drift. Such entangled systems are known, both theoretically and experimentally, to have nonlocal properties, behaving in many ways like a single unified quantum that can change instantaneously throughout its entire ex ...
Ch8lsn22Chem105
... quantum number mℓ. C) The smallest value of the magnetic quantum number mℓ is -9. D) The electron must be in one of the p orbitals. E) The angular momentum quantum number ℓ can have any of the values 0, 1, 2, 3, 4, 5, 6, 7, 8. Kull Spring07 Lesson 22 Ch 7/8 ...
... quantum number mℓ. C) The smallest value of the magnetic quantum number mℓ is -9. D) The electron must be in one of the p orbitals. E) The angular momentum quantum number ℓ can have any of the values 0, 1, 2, 3, 4, 5, 6, 7, 8. Kull Spring07 Lesson 22 Ch 7/8 ...
POLYNOMIAL-TIME ALGORITHMS FOR PRIME FACTORIZATION
... tells us they should. It thus seems plausible that the natural computing power of classical mechanics corresponds to that of Turing machines,1 while the natural computing power of quantum mechanics might be greater. The rst person to look at the interaction between computation and quantum mechanics ...
... tells us they should. It thus seems plausible that the natural computing power of classical mechanics corresponds to that of Turing machines,1 while the natural computing power of quantum mechanics might be greater. The rst person to look at the interaction between computation and quantum mechanics ...
Experimental violation of Bell inequalities for multi
... quantum systems of arbitrarily high dimensionality. In addition to the fundamental interest for revealing fascinating aspects of quantum mechanics, Bell inequalities generalized to d-dimensional systems and their verified quantum nonlocality are also crucial for a variety of quantum information task ...
... quantum systems of arbitrarily high dimensionality. In addition to the fundamental interest for revealing fascinating aspects of quantum mechanics, Bell inequalities generalized to d-dimensional systems and their verified quantum nonlocality are also crucial for a variety of quantum information task ...
How “Quantum” is the D-Wave Machine?
... equally well for both schedules. If the entire process were carried out sufficiently slowly and at zero temperature, then it would be an implementation of adiabatic quantum optimization [13]. Such Pa process is guaranteed to end up in the ground state of the target Hamiltonian H = − i
... equally well for both schedules. If the entire process were carried out sufficiently slowly and at zero temperature, then it would be an implementation of adiabatic quantum optimization [13]. Such Pa process is guaranteed to end up in the ground state of the target Hamiltonian H = − i
Conference booklet - XXXV Workshop on Geometric Methods in
... Supergeometry of gauge PDE and AKSZ sigma models AKSZ sigma models were originally proposed to describe topological systems. In fact, an AKSZ model with finite number of fields and space-time dimension higher than 1 is necessarily topological. These models are quite distinguished in the sense that the ...
... Supergeometry of gauge PDE and AKSZ sigma models AKSZ sigma models were originally proposed to describe topological systems. In fact, an AKSZ model with finite number of fields and space-time dimension higher than 1 is necessarily topological. These models are quite distinguished in the sense that the ...