Effective gravitational interactions of dark matter axions
... If the PQ phase transition occurs after inflation, it can be different for each QCD horizon. Even if the PQ phase transition occurs before inflation, there are fluctuations originating from quantum fluctuations. The coherently oscillating axions have momenta comparable to or less than the Hubble ...
... If the PQ phase transition occurs after inflation, it can be different for each QCD horizon. Even if the PQ phase transition occurs before inflation, there are fluctuations originating from quantum fluctuations. The coherently oscillating axions have momenta comparable to or less than the Hubble ...
Wallace-etalJAP2014-bias-dependence-and
... the CL intensity to decrease and the induced current to increase, which fits the model of a larger electric field driving carriers out of the active region. It is evident from the CL maps that as the electric field in the junction is increased (i.e., a more negative applied bias) both the size and n ...
... the CL intensity to decrease and the induced current to increase, which fits the model of a larger electric field driving carriers out of the active region. It is evident from the CL maps that as the electric field in the junction is increased (i.e., a more negative applied bias) both the size and n ...
Particle Statistics Affects Quantum Decay and Fano Interference
... (a quantum wire), each with energy ϵ ¼ 0 [see Figs. 1(a) and 1(b)]. Thus, states j1i and j2i can decay by tunnelling to the common continuum given by the tight-binding lattice band of the quantum wire. The energy of the band spans the interval −2κ < E < 2κ, κ being the hopping rate between two adjac ...
... (a quantum wire), each with energy ϵ ¼ 0 [see Figs. 1(a) and 1(b)]. Thus, states j1i and j2i can decay by tunnelling to the common continuum given by the tight-binding lattice band of the quantum wire. The energy of the band spans the interval −2κ < E < 2κ, κ being the hopping rate between two adjac ...
A Functional Architecture for Scalable Quantum Computing
... show the pulse shape of the fluxonium qubit and the phase accumulated by |11i state. For these parameters, the √ CPhase gate fidelity is 99.97% with a gate time t CPhase = π/ 2g = 70.7 ns. IV. Fig. 5. Eigenfrequencies of the transmon-fluxonium coupled system showing avoided crossing between differen ...
... show the pulse shape of the fluxonium qubit and the phase accumulated by |11i state. For these parameters, the √ CPhase gate fidelity is 99.97% with a gate time t CPhase = π/ 2g = 70.7 ns. IV. Fig. 5. Eigenfrequencies of the transmon-fluxonium coupled system showing avoided crossing between differen ...
Science Journals — AAAS
... quantum computers (1–3), which, as they increase in scale, will allow enhanced performance of tasks in secure networking, simulations, distributed computing, and other key tasks where exponential speedups are available. Processing circuits to realize these applications are built up from logic gates ...
... quantum computers (1–3), which, as they increase in scale, will allow enhanced performance of tasks in secure networking, simulations, distributed computing, and other key tasks where exponential speedups are available. Processing circuits to realize these applications are built up from logic gates ...