Factors affecting gas-phase continuous wave infrared laser sensitized pyrolysis

1988 ◽  
Vol 92 (8) ◽  
pp. 2184-2188 ◽  
Author(s):  
Jianzhong Zhu ◽  
Edward S. Yeung
Keyword(s):  
Gas Phase ◽  
Continuous Wave ◽  
Infrared Laser ◽  
Factors Affecting

scholarly journals Porcine skin damage thresholds for 0.6 to 9.5 cm beam diameters from 1070-nm continuous-wave infrared laser radiation

2014 ◽  
Vol 19 (03) ◽  
pp. 1 ◽  
Author(s):  
Rebecca L. Vincelette ◽  
Gary D. Noojin ◽  
Corey A. Harbert ◽  
Kurt J. Schuster ◽  
Aurora D. Shingledecker ◽  
...  
Keyword(s):  
Laser Radiation ◽  
Continuous Wave ◽  
Infrared Laser ◽  
Skin Damage ◽  
Porcine Skin

Imino Tautomers of Gas-Phase Guanine from Mid-Infrared Laser Spectroscopy

2007 ◽  
Vol 111 (28) ◽  
pp. 6217-6221 ◽  
Author(s):  
Kai Seefeld ◽  
Robert Brause ◽  
Thomas Häber ◽  
Karl Kleinermanns
Keyword(s):  
Gas Phase ◽  
Laser Spectroscopy ◽  
Infrared Laser ◽  
Mid Infrared ◽  
Infrared Laser Spectroscopy

Spectroscopic investigations of hydrogen bonding interactions in the gas phase. VIII. Microwave rotational spectrum of the heterodimer H—C≡C—C≡N ∙ ∙ ∙ HF

1984 ◽  
Vol 394 (1807) ◽  
pp. 387-403 ◽  
Keyword(s):  
Gas Phase ◽  
Continuous Wave ◽  
Spectroscopic Constants ◽  
State Transitions ◽  
Rotational Spectrum ◽  
Microwave Spectra ◽  
Hydrogen Bonding Interactions ◽  
Microwave Rotational Spectrum ◽  
Microwave Techniques ◽  
Pulsed Nozzle

The hydrogen bonded dimer formed between cyanoacetylene and hydrogen fluoride has been identified through its infrared and microwave spectra. Two microwave techniques, continuous wave and pulsed-nozzle Fourier-transform spectroscopy, have been combined to identify unambiguously the vibrational ground state transitions and to assign vibrational satellites. In making the assignments, much use has been made of computer simu­lation of spectra, which is described in an Appendix. Analysis of the microwave spectra led to the following spectroscopic constants and molecular parameters. HC 3 N ∙ ∙ ∙HF HC 3 N∙ ∙ ∙DF B 0 /MHz 1220.68431 (9) 1204.9051 (2) D J /kHz 0.306 (2) 0.296 (3) α β /MHz ─7.20 (2) — γ β /MHz 0.094 (3) — γ 11 /MHz ─0.030 (2) — α σ /MHz ─13.7 (2) — q β /MHz 3.12 (2) — r 0 (N ∙ ∙ ∙ F)/nm 0.2788 0.2785 X /MHz ─ 3.876 ─ 3.854 v β /cm -1 30 — v σ /cm -1 139 — k σ /(N m -1 ) 16.3 — k s /(N m -1 ) 770 — Finally, the variation of ∆ v̄ as a function of r 0 (N ∙ ∙ ∙ F) has been examined for a series of dimers RCN ∙ ∙ ∙ HF.

Crystallization in Unsaturated Glycine/D2O Solution Achieved by Irradiating a Focused Continuous Wave Near Infrared Laser

2010 ◽  
Vol 10 (11) ◽  
pp. 4686-4688 ◽  
Author(s):  
Thitiporn Rungsimanon ◽  
Ken-ichi Yuyama ◽  
Teruki Sugiyama ◽  
Hiroshi Masuhara
Keyword(s):  
Near Infrared ◽  
Continuous Wave ◽  
Infrared Laser

Probing factors affecting the gas phase stabilities of noncovalent complexes formed by peptides bound to the Grb2 SH2 domain protein

2004 ◽  
Vol 6 (10) ◽  
pp. 2572 ◽  
Author(s):  
M. Isabel Catalina ◽  
Nico J. de Mol ◽  
Marcel J. E. Fischer ◽  
Albert J. R. Heck
Keyword(s):  
Gas Phase ◽  
Sh2 Domain ◽  
Noncovalent Complexes ◽  
Factors Affecting ◽  
Domain Protein

Some factors affecting gas phase ore transport

1965 ◽  
Vol 60 (1) ◽  
pp. 117-123 ◽  
Author(s):  
Alan L. Walker
Keyword(s):  
Gas Phase ◽  
Factors Affecting

Effect of infrared laser radiation on gas-phase pyrolysis of ethane

2018 ◽  
Vol 134 ◽  
pp. 122-129 ◽  
Author(s):  
N. Masyuk ◽  
A. Sherin ◽  
V.N. Snytnikov ◽  
Vl.N. Snytnikov
Keyword(s):  
Laser Radiation ◽  
Gas Phase ◽  
Infrared Laser
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