Electron Impact Data on Substituted Acetylenes: Propyne and 2-Butyne1

1955 ◽  
Vol 77 (4) ◽  
pp. 895-896 ◽  
Author(s):  
Fred H. Coats ◽  
Robbin C. Anderson
1968 ◽  
Vol 21 (3) ◽  
pp. 761 ◽  
Author(s):  
WD Crow ◽  
JL Occolowitz ◽  
RK Solly

Electron impact data are presented for the phenylhydrazones of a series of aromatic ketones C6H5-CO-R (R = H, CH3, CD3, C2H5, C6H6), and are discussed in comparison with the results of thermal excitation. Whereas pyrolysis resulted in extensive four-centre migration of R to nitrogen, followed by (or synchronous with) cleavage of the N-X bond, the electron-impact breakdown is largely dominated by N-N bond cleavage. A semi-quantitative assessment is made of the rearrangements which do occur, and the stereochemistry of these and related reactions is discussed.


1966 ◽  
Vol 21 (10) ◽  
pp. 1580-1584 ◽  
Author(s):  
J. H. D. Eland ◽  
P. J. Shepherd ◽  
C. J. Danby

The analytical technique proposed by MORRISON 1 has been tested on ionization efficiency curves obtained using an unmodified mass spectrometer. Ionization potentials of a series of aromatic amines have been found by this method and have been used to determine the best parameters for use in calculations by the STREITWIESER ω-technique.


Author(s):  
Raynald Gauvin ◽  
Gilles L'Espérance

Values of cross sections for ionization of inner-shell electrons by electron impact are required for electron probe microanalysis, Auger-electron spectroscopy and electron energy-loss spectroscopy. In this work, the results of the measurement of inner-shell ionization cross-sections by electron impact, Q, in a TEM are presented for the K shell.The measurement of QNi has been performed at 120 KeV in a TEM by measuring the net X-ray intensity of the Kα line of Ni, INi, which is related to QNi by the relation :(1)where i is the total electron dose, (Ω/4π)is the fractional solid angle, ω is the fluorescence yield, α is the relative intensity factor, ε is the Si (Li) detector efficiency, A is the atomic weight, ρ is the sample density, No is Avogadro's number, t' is the distance traveled by the electrons in the specimen which is equal to τ sec θ neglecting beam broadening where τ is the specimen thickness and θ is the angle between the electron beam and the normal of the thin foil and CNi is the weight fraction of Ni.


1980 ◽  
Vol 77 ◽  
pp. 773-777 ◽  
Author(s):  
F.J. de Heer ◽  
H.A. Van Sprang ◽  
G.R. Mohlmann

1993 ◽  
Vol 03 (C6) ◽  
pp. C6-117-C6-123 ◽  
Author(s):  
M. J. FORD ◽  
J. P. DOERING ◽  
J. W. COOPER ◽  
M. A. COPLAN ◽  
J. H. MOORE

2001 ◽  
Vol 11 (PR2) ◽  
pp. Pr2-309-Pr2-312
Author(s):  
K. M. Aggarwal ◽  
F. P. Keenan ◽  
S. J. Rose

Sign in / Sign up

Export Citation Format

Share Document