Quantum heating of a parametrically modulated oscillator: Spectral signatures M. Marthaler,
... in vibrational systems. It makes the energy levels nonequidistant and the frequencies of different interlevel transitions different, which in turn enables spectroscopic observation of the quantum energy levels. In addition, nonlinearity leads to an interesting behavior of vibrational systems in exte ...
... in vibrational systems. It makes the energy levels nonequidistant and the frequencies of different interlevel transitions different, which in turn enables spectroscopic observation of the quantum energy levels. In addition, nonlinearity leads to an interesting behavior of vibrational systems in exte ...
Interpreting Quantum Mechanics in Terms of - Philsci
... know what physical state the wave function of a quantum system describes, we need to measure the system in the first place, while the measuring process and the measurement result are necessarily determined by the evolution law for the wave function. Fortunately, it has been realized that the conven ...
... know what physical state the wave function of a quantum system describes, we need to measure the system in the first place, while the measuring process and the measurement result are necessarily determined by the evolution law for the wave function. Fortunately, it has been realized that the conven ...
Toward Practical Solid-State Based Quantum Memories
... The figure shows the off-resonant Raman coupling that allows the absorption of a single-photon through the creation of a spin excitation. One can retrieve the stored photon by applying the same control field after the storage time. . . . . . . . . . (a) Shows the control field (red) and the input si ...
... The figure shows the off-resonant Raman coupling that allows the absorption of a single-photon through the creation of a spin excitation. One can retrieve the stored photon by applying the same control field after the storage time. . . . . . . . . . (a) Shows the control field (red) and the input si ...
Exciton Fine-Structure Splitting in Self- Assembled Lateral InAs/GaAs Quantum-Dot Molecular Structures
... values and their absolute values ...
... values and their absolute values ...
Dual-path source engineering in integrated quantum optics
... As we treat the pump field Ep as classical, only the generated fields are described by operators. We do not use subscripts for the quantum fields, as the photons are fundamentally indistinguishable and therefore described by the same operator. To solve the full system Hamiltonian including the coupl ...
... As we treat the pump field Ep as classical, only the generated fields are described by operators. We do not use subscripts for the quantum fields, as the photons are fundamentally indistinguishable and therefore described by the same operator. To solve the full system Hamiltonian including the coupl ...
Weyl`s Spinor and Dirac`s Equation - weylmann.com
... 90 counterclockwise about the x axis as shown. Having done this, let us now rotate the cube again 90 counterclockwise about the y axis. This returns P to its original position in the coordinate system, although the cube itself has been turned around somewhat. Now ask yourself how we might have achie ...
... 90 counterclockwise about the x axis as shown. Having done this, let us now rotate the cube again 90 counterclockwise about the y axis. This returns P to its original position in the coordinate system, although the cube itself has been turned around somewhat. Now ask yourself how we might have achie ...
In Search of Quantum Reality
... (using cards this time instead of gloves) . . . . . 586 14.3.1.4 The EPR Paradox (1935-52) . . . . . . . . . . . . 588 14.3.1.5 The BCHSH Inequality (1964) . . . . . . . . . . . 589 14.3.1.6 A Proof of Bell’s Inequality . . . . . . . . . . . . 591 14.3.1.7 The BCHSH Inequality(or Bell’s inequality i ...
... (using cards this time instead of gloves) . . . . . 586 14.3.1.4 The EPR Paradox (1935-52) . . . . . . . . . . . . 588 14.3.1.5 The BCHSH Inequality (1964) . . . . . . . . . . . 589 14.3.1.6 A Proof of Bell’s Inequality . . . . . . . . . . . . 591 14.3.1.7 The BCHSH Inequality(or Bell’s inequality i ...
Quantum Information with Fermionic Gaussian States - Max
... A.4 Port-based teleportation . . . . . . . . A.4.1 Example: POVM measurement Bibliography ...
... A.4 Port-based teleportation . . . . . . . . A.4.1 Example: POVM measurement Bibliography ...
Achieving quantum supremacy with sparse and noisy commuting
... Our final result is that this notion of noise can be fought using simple ideas from classical errorcorrection, while still remaining within the framework of IQP. We show that for any IQP circuit C on n qubits, we can produce a new IQP circuit C 0 on O(n) qubits in polynomial time such that, if depo ...
... Our final result is that this notion of noise can be fought using simple ideas from classical errorcorrection, while still remaining within the framework of IQP. We show that for any IQP circuit C on n qubits, we can produce a new IQP circuit C 0 on O(n) qubits in polynomial time such that, if depo ...
