Broadband Guiding Silica Hollow-Core Fibers for Gas-Phase Nonlinear and Quantum Optics

2008 ◽  
Author(s):  
P. J. Roberts ◽  
F. Benabid ◽  
F. Couny ◽  
P. S. Light ◽  
N. V. Wilding
Keyword(s):  
Quantum Optics ◽  
Gas Phase ◽  
Hollow Core

scholarly journals Development of a gas‐phase Raman instrument using a hollow core anti‐resonant tubular fibre

2021 ◽  
Author(s):  
William S.M. Brooks ◽  
Matthew Partridge ◽  
Ian A.K. Davidson ◽  
Charles Warren ◽  
George Rushton ◽  
...  
Keyword(s):  
Gas Phase ◽  
Hollow Core

Atomic spectroscopy and quantum optics in hollow-core waveguides

2010 ◽  
Vol 4 (6) ◽  
pp. 720-737 ◽  
Author(s):  
H. Schmidt ◽  
A.R. Hawkins
Keyword(s):  
Quantum Optics ◽  
Atomic Spectroscopy ◽  
Hollow Core

Synthesis and Characterization of Hollow Core-Shell ZrO2@void@BiVO4 Visible-Light Photocatalyst

2010 ◽  
Vol 148-149 ◽  
pp. 1331-1338
Author(s):  
Bing Hua Yao ◽  
Liu Min ◽  
Zhan Ying Ma ◽  
Cheng Wang
Keyword(s):  
Photocatalytic Activity ◽  
Gas Phase ◽  
Carbon Layer ◽  
Synthesis And Characterization ◽  
Core Shell ◽  
Hollow Core ◽  
Void Space ◽  
Visible Light Photocatalyst ◽  
Pure Phase

Monoclinic scheelite BiVO4 was synthesized from a mixture of aqueous Bi(NO3)3 and NH4VO3 solutions by hydrothermal method. Then using successive coating of BiVO4 with a carbon layer and a ZrO2 layer followed by heat treatment to remove the carbon layer prepared a core-shell(ZrO2@void@BiVO4) nanoparticles with a void layer between the BiVO4 core and the ZrO2 shell. TG-DTA and IR suggest that BiVO4 was coated with ZrO2. TEM shows that there was a void space between the BiVO4 core and the ZrO2 shell. The samples were characterized by XRD and the peaks of ZrO2@void@BiVO4 suits well with the pure phase monoclinic scheelite BiVO4. And its visble-light photocatalytic activity was evaluated by the photodegradation of methylene blue(MB). The results indicated that the photocatalytic activity of ZrO2@void@BiVO4 is similar to that of pure phase BiVO4, which makes it can be used for preparing liquid-gas phase boundary visble-light photocatalyst.

scholarly journals Mesoscale cavities in hollow-core waveguides for quantum optics with atomic ensembles

Nanophotonics ◽  
2016 ◽  
Vol 5 (3) ◽  
pp. 392-408 ◽  
Author(s):  
C.M. Haapamaki ◽  
J. Flannery ◽  
G. Bappi ◽  
R. Al Maruf ◽  
S.V. Bhaskara ◽  
...  
Keyword(s):  
Nonlinear Optics ◽  
Quantum Optics ◽  
Light Propagation ◽  
Single Photon ◽  
Single Mode ◽  
Bragg Gratings ◽  
Single Photons ◽  
Optical Nonlinearities ◽  
Hollow Core ◽  
Atomic Ensembles

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.

Residual Gas Reactions in the Electron Microscope: I. Qualitative Observations on the Water Gas Reaction

1968 ◽  
Vol 26 ◽  
pp. 292-293
Author(s):  
Richard E. Hartman ◽  
Roberta S. Hartman ◽  
Peter L. Ramos
Keyword(s):  
Electron Beam ◽  
Electron Microscope ◽  
Gas Phase ◽  
Absolute Temperature ◽  
Residual Gas ◽  
Gas Reactions ◽  
Image Position ◽  
The Right ◽  
Water Gas ◽  
Thinning Rate

The action of water and the electron beam on organic specimens in the electron microscope results in the removal of oxidizable material (primarily hydrogen and carbon) by reactions similar to the water gas reaction .which has the form:The energy required to force the reaction to the right is supplied by the interaction of the electron beam with the specimen.The mass of water striking the specimen is given by:where u = gH2O/cm2 sec, PH2O = partial pressure of water in Torr, & T = absolute temperature of the gas phase. If it is assumed that mass is removed from the specimen by a reaction approximated by (1) and that the specimen is uniformly thinned by the reaction, then the thinning rate in A/ min iswhere x = thickness of the specimen in A, t = time in minutes, & E = efficiency (the fraction of the water striking the specimen which reacts with it).

Integration of Core-Edge Spectroscopy Methods for the Study of Polymers

1996 ◽  
Vol 54 ◽  
pp. 154-155
Author(s):  
E. G. Rightor
Keyword(s):  
Excited State ◽  
Polymer Blends ◽  
Gas Phase ◽  
Spatial Resolution ◽  
High Spatial Resolution ◽  
Electronic States ◽  
Core Electron ◽  
Bulk Solids ◽  
Development Application

Core edge spectroscopy methods are versatile tools for investigating a wide variety of materials. They can be used to probe the electronic states of materials in bulk solids, on surfaces, or in the gas phase. This family of methods involves promoting an inner shell (core) electron to an excited state and recording either the primary excitation or secondary decay of the excited state. The techniques are complimentary and have different strengths and limitations for studying challenging aspects of materials. The need to identify components in polymers or polymer blends at high spatial resolution has driven development, application, and integration of results from several of these methods.

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