Nonlinear optics at the single-photon level inside a hollow core fiber

2011 ◽  
Author(s):  
Sebastian Hofferberth ◽  
Thibault Peyronel ◽  
Qiyu Liang ◽  
Alexander Zibrov ◽  
Vladan Vuletic ◽  
...  
2010 ◽  
Author(s):  
Holger Schmidt ◽  
Aaron R. Hawkins ◽  
Bin Wu ◽  
John F. Hulbert

CLEO: 2015 ◽  
2015 ◽  
Author(s):  
Maria Langbecker ◽  
Mohammad Noaman ◽  
Patrick Windpassinger

1899 ◽  
Author(s):  
D. Aghamalyan ◽  
D. Aghamalyan ◽  
Yu. Malakyan ◽  
Yu. Malakyan

Nanophotonics ◽  
2016 ◽  
Vol 5 (3) ◽  
pp. 392-408 ◽  
Author(s):  
C.M. Haapamaki ◽  
J. Flannery ◽  
G. Bappi ◽  
R. Al Maruf ◽  
S.V. Bhaskara ◽  
...  

AbstractSingle-mode hollow-core waveguides loaded with atomic ensembles offer an excellent platform for light–matter interactions and nonlinear optics at low photon levels. We review and discuss possible approaches for incorporating mirrors, cavities, and Bragg gratings into these waveguides without obstructing their hollow cores. With these additional features controlling the light propagation in the hollow-core waveguides, one could potentially achieve optical nonlinearities controllable by single photons in systems with small footprints that can be integrated on a chip. We propose possible applications such as single-photon transistors and superradiant lasers that could be implemented in these enhanced hollow-core waveguides.


2015 ◽  
Vol 5 (4) ◽  
pp. 1310-1322 ◽  
Author(s):  
Andreas Hoffmann ◽  
Michael Zürch ◽  
Christian Spielmann

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Pablo Roldán-Varona ◽  
Rosa Ana Pérez-Herrera ◽  
Luis Rodríguez-Cobo ◽  
Luis Reyes-González ◽  
Manuel López-Amo ◽  
...  

AbstractIn this work, a novel optical fiber sensor capable of measuring both the liquid level and its refractive index is designed, manufactured and demonstrated through simulations and experimentally. For this, a silica capillary hollow-core fiber is used. The fiber, with a sensing length of 1.55 mm, has been processed with a femtosecond laser, so that it incorporates four holes in its structure. In this way, the liquid enters the air core, and it is possible to perform the sensing through the Fabry–Perot cavities that the liquid generates. The detection mode is in reflection. With a resolution of 4 μm (liquid level), it is in the state of the art of this type of sensor. The system is designed so that in the future it will be capable of measuring the level of immiscible liquids, that is, liquids that form stratified layers. It can be useful to determine the presence of impurities in tanks.


Sensors ◽  
2021 ◽  
Vol 21 (2) ◽  
pp. 478
Author(s):  
Yudai Kudo ◽  
Saiko Kino ◽  
Yuji Matsuura

Human breath is a biomarker of body fat metabolism and can be used to diagnose various diseases, such as diabetes. As such, in this paper, a vacuum ultraviolet (VUV) spectroscopy system is proposed to measure the acetone in exhaled human breath. A strong absorption acetone peak at 195 nm is detected using a simple system consisting of a deuterium lamp source, a hollow-core fiber gas cell, and a fiber-coupled compact spectrometer corresponding to the VUV region. The hollow-core fiber functions both as a long-path and an extremely small-volume gas cell; it enables us to sensitively measure the trace components of exhaled breath. For breath analysis, we apply multiple regression analysis using the absorption spectra of oxygen, water, and acetone standard gas as explanatory variables to quantitate the concentration of acetone in breath. Based on human breath, we apply the standard addition method to obtain the measurement accuracy. The results suggest that the standard deviation is 0.074 ppm for healthy human breath with an acetone concentration of around 0.8 ppm and a precision of 0.026 ppm. We also monitor body fat burn based on breath acetone and confirm that breath acetone increases after exercise because it is a volatile byproduct of lipolysis.


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