Generation of optical macroscopic quantum superposition states via state reduction with a Mach-Zehnder interferometer containing a Kerr medium

1999 ◽  
Vol 59 (5) ◽  
pp. 4095-4098 ◽  
Author(s):  
Christopher C. Gerry
1999 ◽  
Vol 60 (3) ◽  
pp. 1817-1823 ◽  
Author(s):  
Sergey M. Chumakov ◽  
Alejandro Frank ◽  
Kurt Bernardo Wolf

1993 ◽  
Vol 47 (6) ◽  
pp. 5024-5029 ◽  
Author(s):  
K. Tara ◽  
G. S. Agarwal ◽  
S. Chaturvedi

2008 ◽  
Vol 83 (6) ◽  
pp. 60004 ◽  
Author(s):  
I. E. Mazets ◽  
G. Kurizki ◽  
M. K. Oberthaler ◽  
J. Schmiedmayer

2019 ◽  
Vol 9 (11) ◽  
pp. 2300 ◽  
Author(s):  
Devashish Pandey ◽  
Laura Bellentani ◽  
Matteo Villani ◽  
Guillermo Albareda ◽  
Paolo Bordone ◽  
...  

Measuring properties of quantum systems is governed by a stochastic (collapse or state-reduction) law that unavoidably yields an uncertainty (variance) associated with the corresponding mean values. This non-classical source of uncertainty is known to be manifested as noise in the electrical current of nanoscale electron devices, and hence it can flaw the good performance of more complex quantum gates. We propose a protocol to alleviate this quantum uncertainty that consists of (i) redesigning the device to accommodate a large number of electrons inside the active region, either by enlarging the lateral or longitudinal areas of the device and (ii) re-normalizing the total current to the number of electrons. How the above two steps can be accommodated using the present semiconductor technology has been discussed and numerically studied for a resonant tunneling diode and a Mach-Zehnder interferometer, for classical and quantum computations, respectively. It is shown that the resulting protocol formally resembles the so-called collective measurements, although, its practical implementation is substantially different.


2016 ◽  
Vol 116 (23) ◽  
Author(s):  
M. Abdi ◽  
P. Degenfeld-Schonburg ◽  
M. Sameti ◽  
C. Navarrete-Benlloch ◽  
M. J. Hartmann

2020 ◽  
Vol 9 (1) ◽  
pp. 7
Author(s):  
Dmitri Khokhlov

The schemes of the arrangements based on the Mach-Zehnder interferometer and the interferometer with two polarizing beam splitters are considered. The interferometers in both the schemes are equipped with some devices, creating a Kerr medium, to perform the quantum non-demolition measurement of a single photon. Such a device gives which way information of the photon while preserving the work of the interferometer.


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