Abstract:We investigate how to control single-photon transport along the photonic crystal waveguide with the recent experimentally demonstrated artificial atoms [i.e.,-type quantum dots (QDs)] [S. G. Carter et al., Nat. Photon. 7, 329 (2013)] in an all-optical way. Adopting full quantum theory in real space, we analytically calculate the transport coefficients of single photons scattered by a-type QD embedded in single-and two-mode photonic crystal cavities (PCCs), respectively. Our numerical results clearly show that … Show more
“…This means that in a neighbourhood of 0 ν = we have S ( ; 4) 1 inel ν π − < and the emitted light is squeezed. This result shows that such a kind of optomechanical systems can generate non-classical light [3,7]. Note that, if light squeezing is present for certain values of the parameters, then the inequality (121) implies that the complementary quadrature is antisqueezed.…”
Section: Homodyne Spectrummentioning
confidence: 77%
“…Indeed the former describes a mechanical oscillator and the latter an optical mode, corresponding to different interactions as discussed in section 2. The same choice is taken, for instance, in [1,2,7,25,36,37], but not in [5,9,10].…”
Section: The Optomechanical Modelmentioning
confidence: 99%
“…Optomechanical systems in the quantum regime are very important for quantum information processing and for testing fundamental issues of quantum mechanics [1][2][3][4][5][6][7][8][9][10]. Their theoretical analysis therefore calls for a first principle description.…”
Section: Introductionmentioning
confidence: 99%
“…We then translate these results into quantum Langevin equations and we show how to obtain a suitable non-Markovian generalization at this level of description. Relying on these results we can consider the description of the simplest optomechanical system, that is a moving mirror interacting with an electromagnetic mode in a cavity via radiation pressure [1,[5][6][7]25]. Again a suitable analysis of the composite system and of the monitoring of the emitted light calls for a consistent quantum description.…”
We provide a fully quantum description of a mechanical oscillator in the presence of thermal environmental noise by means of a quantum Langevin formulation based on quantum stochastic calculus. The system dynamics is determined by symmetry requirements and equipartition at equilibrium, while the environment is described by quantum Bose fields in a suitable non-Fock representation which allows for the introduction of temperature. A generic spectral density of the environment can be described by introducing its state through a suitable P-representation. Including interaction of the mechanical oscillator with a cavity mode via radiation pressure we obtain a description of a simple optomechanical system in which, besides the Langevin equations for the system, one has the exact input-output relations for the quantum noises. The whole theory is valid at arbitrarily low temperature. This allows the exact calculation of the stationary value of the mean energy of the mechanical oscillator, as well as both homodyne and heterodyne spectra. The present analysis allows in particular to study possible cooling scenarios and to obtain the exact connection between observed spectra and fluctuation spectra of the position of the mechanical oscillator.
“…This means that in a neighbourhood of 0 ν = we have S ( ; 4) 1 inel ν π − < and the emitted light is squeezed. This result shows that such a kind of optomechanical systems can generate non-classical light [3,7]. Note that, if light squeezing is present for certain values of the parameters, then the inequality (121) implies that the complementary quadrature is antisqueezed.…”
Section: Homodyne Spectrummentioning
confidence: 77%
“…Indeed the former describes a mechanical oscillator and the latter an optical mode, corresponding to different interactions as discussed in section 2. The same choice is taken, for instance, in [1,2,7,25,36,37], but not in [5,9,10].…”
Section: The Optomechanical Modelmentioning
confidence: 99%
“…Optomechanical systems in the quantum regime are very important for quantum information processing and for testing fundamental issues of quantum mechanics [1][2][3][4][5][6][7][8][9][10]. Their theoretical analysis therefore calls for a first principle description.…”
Section: Introductionmentioning
confidence: 99%
“…We then translate these results into quantum Langevin equations and we show how to obtain a suitable non-Markovian generalization at this level of description. Relying on these results we can consider the description of the simplest optomechanical system, that is a moving mirror interacting with an electromagnetic mode in a cavity via radiation pressure [1,[5][6][7]25]. Again a suitable analysis of the composite system and of the monitoring of the emitted light calls for a consistent quantum description.…”
We provide a fully quantum description of a mechanical oscillator in the presence of thermal environmental noise by means of a quantum Langevin formulation based on quantum stochastic calculus. The system dynamics is determined by symmetry requirements and equipartition at equilibrium, while the environment is described by quantum Bose fields in a suitable non-Fock representation which allows for the introduction of temperature. A generic spectral density of the environment can be described by introducing its state through a suitable P-representation. Including interaction of the mechanical oscillator with a cavity mode via radiation pressure we obtain a description of a simple optomechanical system in which, besides the Langevin equations for the system, one has the exact input-output relations for the quantum noises. The whole theory is valid at arbitrarily low temperature. This allows the exact calculation of the stationary value of the mean energy of the mechanical oscillator, as well as both homodyne and heterodyne spectra. The present analysis allows in particular to study possible cooling scenarios and to obtain the exact connection between observed spectra and fluctuation spectra of the position of the mechanical oscillator.
We study controllable single-photon transport in a one-dimensional waveguide with a nonlinear dispersion relation coupled to a three-level emitter in a cascade configuration. An extra cavity field is introduced to drive one of the level transitions of the emitter. In the resonance case, when the extra cavity does not contain photons, the input single photon will be reflected; when the cavity contains one photon, the full transmission of the input single photon can be obtained. In the off-resonance case, the single-photon transport can also be controlled by the parameters of the cavity. Therefore, we show that single-photon transport can be controlled by an extra cavity field.
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