Elastic Scattering of Polarized Neutrons from 4He

Author(s):  
P. W. Lisowski ◽  
T. C. Rhea ◽  
R. L. Walter ◽  
T. B. Clegg
1965 ◽  
Vol 137 (2B) ◽  
pp. B401-B404 ◽  
Author(s):  
D. W. Kent

1975 ◽  
Vol 237 (1) ◽  
pp. 111-124 ◽  
Author(s):  
R.J. Holt ◽  
F.W.K. Firk ◽  
G.T. Hickey ◽  
R. Nath

1957 ◽  
Vol 108 (1) ◽  
pp. 116-119 ◽  
Author(s):  
B. M. McCormac ◽  
M. F. Steuer ◽  
C. D. Bond ◽  
F. L. Hereford

1982 ◽  
Vol 494 (6) ◽  
pp. 408-416 ◽  
Author(s):  
L. Drigo ◽  
G. Tornielli ◽  
G. Zannoni

1985 ◽  
Vol 32 (1) ◽  
pp. 76-82 ◽  
Author(s):  
S. T. Lam ◽  
W. K. Dawson ◽  
S. A. Elbakr ◽  
H. W. Fielding ◽  
P. W. Green ◽  
...  

Author(s):  
J. Langmore ◽  
M. Isaacson ◽  
J. Wall ◽  
A. V. Crewe

High resolution dark field microscopy is becoming an important tool for the investigation of unstained and specifically stained biological molecules. Of primary consideration to the microscopist is the interpretation of image Intensities and the effects of radiation damage to the specimen. Ignoring inelastic scattering, the image intensity is directly related to the collected elastic scattering cross section, σɳ, which is the product of the total elastic cross section, σ and the eficiency of the microscope system at imaging these electrons, η. The number of potentially bond damaging events resulting from the beam exposure required to reduce the effect of quantum noise in the image to a given level is proportional to 1/η. We wish to compare η in three dark field systems.


Author(s):  
D. L. Misell

In the electron microscopy of biological sections the adverse effect of chromatic aberration on image resolution is well known. In this paper calculations are presented for the inelastic and elastic image intensities using a wave-optical formulation. Quantitative estimates of the deterioration in image resolution as a result of chromatic aberration are presented as an alternative to geometric calculations. The predominance of inelastic scattering in the unstained biological and polymeric materials is shown by the inelastic to elastic ratio, I/E, within an objective aperture of 0.005 rad for amorphous carbon of a thickness, t=50nm, typical of biological sections; E=200keV, I/E=16.


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