Quantum interference effects of a single photon interacting with an atomic chain inside a one-dimensional waveguide

2008 ◽  
Vol 78 (6) ◽  
Author(s):  
T. S. Tsoi ◽  
C. K. Law
1996 ◽  
Vol 10 (06) ◽  
pp. 701-712 ◽  
Author(s):  
CHANG-MO RYU ◽  
SAM YOUNG CHO ◽  
MINCHEOL SHIN ◽  
KYOUNG WAN PARK ◽  
SEONGJAE LEE ◽  
...  

Quantum interference effects for a mesoscopic loop with three leads are investigated by using a one-dimensional quantum waveguide theory. The transmission and reflection probabilities are analytically obtained in terms of the magnetic flux, arm length, and wave vector. Oscillation of the magnetoconductance is explicitly demonstrated. Magnetoconductance is found to be sharply peaked for certain localized values of flux and kl. In addition, it is noticed that the periodicity of the transmission probability with respect to kl depends more sensitively on the lead position, compared to the case of the two-lead loop.


2013 ◽  
Vol 27 (08) ◽  
pp. 1350026
Author(s):  
B. I. BELEVTSEV ◽  
E. Yu. BELIAYEV ◽  
Yu. A. KOLESNICHENKO

We present transport properties of quench-condensed Au film with nominal thickness ≈3.56 nm and R□ ≈ 5 k Ω for T > 10 K. This film has weak nonmetallic temperature dependence of resistance with logarithmic behavior above 10 K and somewhat stronger dependence at low temperatures. Above 3 K only two-dimensional (2D) quantum interference effects in electron transport have been found; whereas, below 3 K both one-dimensional (1D) and 2D effects of weak localization (WL) and electron–electron interaction (EEI) can be distinguished. This reflects inhomogeneous structure of the film near the thickness-controlled metal-insulator transition (MIT).


2015 ◽  
Vol 92 (2) ◽  
Author(s):  
Zeyang Liao ◽  
Xiaodong Zeng ◽  
Shi-Yao Zhu ◽  
M. Suhail Zubairy

2020 ◽  
Vol 3 (1) ◽  
Author(s):  
Philip Schmidt ◽  
Mohammad T. Amawi ◽  
Stefan Pogorzalek ◽  
Frank Deppe ◽  
Achim Marx ◽  
...  

AbstractLight-matter interaction in optomechanical systems is the foundation for ultra-sensitive detection schemes as well as the generation of phononic and photonic quantum states. Electromechanical systems realize this optomechanical interaction in the microwave regime. In this context, capacitive coupling arrangements demonstrated interaction rates of up to 280 Hz. Complementary, early proposals and experiments suggest that inductive coupling schemes are tunable and have the potential to reach the single-photon strong-coupling regime. Here, we follow the latter approach by integrating a partly suspended superconducting quantum interference device (SQUID) into a microwave resonator. The mechanical displacement translates into a time varying flux in the SQUID loop, thereby providing an inductive electromechanical coupling. We demonstrate a sideband-resolved electromechanical system with a tunable vacuum coupling rate of up to 1.62 kHz, realizing sub-aN Hz−1/2 force sensitivities. The presented inductive coupling scheme shows the high potential of SQUID-based electromechanics for targeting the full wealth of the intrinsically nonlinear optomechanics Hamiltonian.


2017 ◽  
Vol 95 (6) ◽  
Author(s):  
Xun-Wei Xu ◽  
Ai-Xi Chen ◽  
Yong Li ◽  
Yu-xi Liu

1985 ◽  
Vol 54 (5) ◽  
pp. 418-421 ◽  
Author(s):  
Philippe Grangier ◽  
Alain Aspect ◽  
Jacques Vigue

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