Quantum optical master equations: The use of damping bases

1993 ◽  
Vol 47 (4) ◽  
pp. 3311-3329 ◽  
Author(s):  
Hans-Jürgen Briegel ◽  
Berthold-Georg Englert
1994 ◽  
Vol 50 (3) ◽  
pp. 2667-2679 ◽  
Author(s):  
Berthold-Georg Englert ◽  
Martin Naraschewski ◽  
Axel Schenzle

2012 ◽  
Vol 85 (5) ◽  
Author(s):  
Adam Stokes ◽  
Andreas Kurcz ◽  
Tim P. Spiller ◽  
Almut Beige

1993 ◽  
Vol 48 (1) ◽  
pp. 732-738 ◽  
Author(s):  
Christian Ginzel ◽  
Hans-Jürgen Briegel ◽  
Ullrich Martini ◽  
Berthold-Georg Englert ◽  
Axel Schenzle

Author(s):  
Gianpiero Colonna ◽  
mario Capitelli ◽  
Lucia Daniela Pietanza ◽  
Annarita Casavola

2021 ◽  
Vol 103 (4) ◽  
Author(s):  
Wei Zhong ◽  
Lan Zhou ◽  
Yu-Bo Sheng

2021 ◽  
Vol 103 (21) ◽  
Author(s):  
Vasilii Vadimov ◽  
Jani Tuorila ◽  
Tuure Orell ◽  
Jürgen Stockburger ◽  
Tapio Ala-Nissila ◽  
...  
Keyword(s):  

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Dmitriy S. Shapiro

AbstractUnder nonequilibrium conditions, quantum optical systems reveal unusual properties that might be distinct from those in condensed matter. The fundamental reason is that photonic eigenstates can have arbitrary occupation numbers, whereas in electronic systems these are limited by the Pauli principle. Here, we address the steady-state transport of pseudothermal photons between two waveguides connected through a cavity with Bose–Hubbard interaction between photons. One of the waveguides is subjected to a broadband incoherent pumping. We predict a continuous transition between the regimes of Lorentzian and Gaussian chaotic light emitted by the cavity. The rich variety of nonequilibrium transport regimes is revealed by the zero-frequency noise. There are three limiting cases, in which the noise-current relation is characterized by a power-law, $$S\propto J^\gamma$$ S ∝ J γ . The Lorentzian light corresponds to Breit-Wigner-like transmission and $$\gamma =2$$ γ = 2 . The Gaussian regime corresponds to many-body transport with the shot noise ($$\gamma =1$$ γ = 1 ) at large currents; at low currents, however, we find an unconventional exponent $$\gamma =3/2$$ γ = 3 / 2 indicating a nontrivial interplay between multi-photon transitions and incoherent pumping. The nonperturbative solution for photon dephasing is obtained in the framework of the Keldysh field theory and Caldeira-Leggett effective action. These findings might be relevant for experiments on photon blockade in superconducting qubits, thermal states transfer, and photon statistics probing.


2021 ◽  
Vol 3 (1) ◽  
Author(s):  
Adam Hewgill ◽  
Gabriele De Chiara ◽  
Alberto Imparato
Keyword(s):  

Crystals ◽  
2021 ◽  
Vol 11 (3) ◽  
pp. 288
Author(s):  
Sven Reitzig ◽  
Michael Rüsing ◽  
Jie Zhao ◽  
Benjamin Kirbus ◽  
Shayan Mookherjea ◽  
...  

Nonlinear and quantum optical devices based on periodically-poled thin film lithium niobate (PP-TFLN) have gained considerable interest lately, due to their significantly improved performance as compared to their bulk counterparts. Nevertheless, performance parameters such as conversion efficiency, minimum pump power, and spectral bandwidth strongly depend on the quality of the domain structure in these PP-TFLN samples, e.g., their homogeneity and duty cycle, as well as on the overlap and penetration depth of domains with the waveguide mode. Hence, in order to propose improved fabrication protocols, a profound quality control of domain structures is needed that allows quantifying and thoroughly analyzing these parameters. In this paper, we propose to combine a set of nanometer-to-micrometer-scale imaging techniques, i.e., piezoresponse force microscopy (PFM), second-harmonic generation (SHG), and Raman spectroscopy (RS), to access the relevant and crucial sample properties through cross-correlating these methods. Based on our findings, we designate SHG to be the best-suited standard imaging technique for this purpose, in particular when investigating the domain poling process in x-cut TFLNs. While PFM is excellently recommended for near-surface high-resolution imaging, RS provides thorough insights into stress and/or defect distributions, as associated with these domain structures. In this context, our work here indicates unexpectedly large signs for internal fields occurring in x-cut PP-TFLNs that are substantially larger as compared to previous observations in bulk LN.


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