Second-order correlation function of entangled photons from a quantum dot in microcavity

2008 ◽  
Vol 5 (7) ◽  
pp. 2469-2472
Author(s):  
Hiroshi Ajiki ◽  
Hajime Ishihara
2005 ◽  
Vol 22 (11) ◽  
pp. 2960-2962 ◽  
Author(s):  
Li Yao-Yi ◽  
Cheng Mu-Tian ◽  
Zhou Hui-Jun ◽  
Liu Shao-Ding ◽  
Wang Qu-Quan

2017 ◽  
Vol 26 (03) ◽  
pp. 1750029 ◽  
Author(s):  
Lina Jaya Diguna ◽  
Yudi Darma ◽  
Muhammad Danang Birowosuto

We investigate the influence of multiple excitons on the photon emission properties of a quantum dot (QD)-cavity system via the master equation for the density matrix. We show that in the intermediate to strong coupling regimes, the multiple excitons lead to the suppressed QD emissions as well as the absence of anti-crossing near zero detuning, arising from the interaction between the multiple excitons and cavity. Furthermore, we analyze the role of the cavity-biexciton detuning in the photon emission properties of cavity and exciton through the second-order correlation function. The small cavity-biexciton detuning yields the significant Purcell effect and the high probability of single photon emissions. The proposed model offers the fundamental approach in developing efficient single-photon emitting devices.


Author(s):  
Tilo Schwalger

AbstractNoise in spiking neurons is commonly modeled by a noisy input current or by generating output spikes stochastically with a voltage-dependent hazard rate (“escape noise”). While input noise lends itself to modeling biophysical noise processes, the phenomenological escape noise is mathematically more tractable. Using the level-crossing theory for differentiable Gaussian processes, we derive an approximate mapping between colored input noise and escape noise in leaky integrate-and-fire neurons. This mapping requires the first-passage-time (FPT) density of an overdamped Brownian particle driven by colored noise with respect to an arbitrarily moving boundary. Starting from the Wiener–Rice series for the FPT density, we apply the second-order decoupling approximation of Stratonovich to the case of moving boundaries and derive a simplified hazard-rate representation that is local in time and numerically efficient. This simplification requires the calculation of the non-stationary auto-correlation function of the level-crossing process: For exponentially correlated input noise (Ornstein–Uhlenbeck process), we obtain an exact formula for the zero-lag auto-correlation as a function of noise parameters, mean membrane potential and its speed, as well as an exponential approximation of the full auto-correlation function. The theory well predicts the FPT and interspike interval densities as well as the population activities obtained from simulations with colored input noise and time-dependent stimulus or boundary. The agreement with simulations is strongly enhanced across the sub- and suprathreshold firing regime compared to a first-order decoupling approximation that neglects correlations between level crossings. The second-order approximation also improves upon a previously proposed theory in the subthreshold regime. Depending on a simplicity-accuracy trade-off, all considered approximations represent useful mappings from colored input noise to escape noise, enabling progress in the theory of neuronal population dynamics.


2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Zi-Heng Xiang ◽  
Jan Huwer ◽  
R. Mark Stevenson ◽  
Joanna Skiba-Szymanska ◽  
Martin B. Ward ◽  
...  

2020 ◽  
Vol 95 (3) ◽  
pp. 034011
Author(s):  
Mojtaba Moazzezi ◽  
Augustine M Urbas ◽  
Vladimir P Drachev ◽  
Yuri Rostovtsev

2009 ◽  
Vol 07 (01) ◽  
pp. 357-363
Author(s):  
E. WU ◽  
XIAO-AN ZHANG ◽  
XI-MING WANG ◽  
LI-XIA ZENG

We consider a semiconductor quantum well in the excitation system. Applying the pertinent Hamiltonian, we investigate the second-order intensity correlation function and the entanglement properties between the cavity and exciton mode. It is found that nonclassical (antibunching) effect and sudden death effect occur in our system.


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