scholarly journals Corrigendum: The Nature of Chalcogen‐Bonding‐Type Tellurium–Nitrogen Interactions: A First Experimental Structure from the Gas Phase

2021 ◽  
Vol 60 (17) ◽  
pp. 9171-9171
Author(s):  
Timo Glodde ◽  
Yury V. Vishnevskiy ◽  
Lars Zimmermann ◽  
Hans‐Georg Stammler ◽  
Beate Neumann ◽  
...  
Keyword(s):  
Gas Phase ◽  
Bonding Type ◽  
Experimental Structure

scholarly journals The Nature of Chalcogen‐Bonding‐Type Tellurium–Nitrogen Interactions: A First Experimental Structure from the Gas Phase

2020 ◽  
Author(s):  
Timo Glodde ◽  
Yury V. Vishnevskiy ◽  
Lars Zimmermann ◽  
Hans‐Georg Stammler ◽  
Beate Neumann ◽  
...  
Keyword(s):  
Gas Phase ◽  
Bonding Type ◽  
Experimental Structure

Octamethylporphyrin copper, C28H28N4Cu – A first experimental structure determination of porphyrins in gas phase

2010 ◽  
Vol 978 (1-3) ◽  
pp. 163-169 ◽  
Author(s):  
Georgiy V. Girichev ◽  
Nina I. Giricheva ◽  
Oleg A. Golubchikov ◽  
Yuriy V. Mimenkov ◽  
Alexander S. Semeikin ◽  
...  
Keyword(s):  
Gas Phase ◽  
Structure Determination ◽  
Experimental Structure

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.

Radiation less transitions in gas phase molecular ions

1980 ◽  
Vol 77 ◽  
pp. 705-718 ◽  
Author(s):  
Sydney Leach ◽  
Gérald Dujardin ◽  
Guy Taieb
Keyword(s):  
Gas Phase ◽  
Molecular Ions
Sign in / Sign up

Export Citation Format

Share Document