Erratum: Ranges of nitrogen ions in Se and energy losses of alpha particles in Al, Ni, Se, Ag, and Au

1970 ◽  
Vol 48 (14) ◽  
pp. 1745-1745 ◽  
Author(s):  
Hiroshi Nakata
1969 ◽  
Vol 47 (22) ◽  
pp. 2545-2552 ◽  
Author(s):  
Hiroshi Nakata

The range–energy relation of N in Se was obtained from an energy-loss curve in the energy region of 1–12 MeV. The results are slightly smaller than expected by theory. In view of medium dependence, selenium tends to differ from other media, and it has also been confirmed by energy-loss measurements of alpha particles.


1975 ◽  
Vol 25 (4) ◽  
pp. 271-273 ◽  
Author(s):  
F. G. Neshev ◽  
A. A. Puzanov ◽  
K. S. Shyshkin ◽  
E. I. Sirotinin ◽  
A. F. Tulinov ◽  
...  
Keyword(s):  

1976 ◽  
Vol 40 (4) ◽  
pp. 418-420
Author(s):  
G. N. Potetyunko ◽  
E. T. Shipatov

1995 ◽  
Vol 35 (12) ◽  
pp. 1679-1685 ◽  
Author(s):  
G Kamelander ◽  
Ya.I Kolesnichenko ◽  
V.V Lutsenko

2018 ◽  
Vol 781 ◽  
pp. 3-7 ◽  
Author(s):  
Anatoliy I. Kupchishin ◽  
Nataliya A. Voronova ◽  
Tatyana A. Shmygaleva ◽  
Alexander A. Kupchishin

Computer simulation of vacancy clusters distribution by depth in molybdenum irradiated by alpha particles within Cascade probability method has been carried out. Cascade probability functions have been calculated taking into account energy losses for alpha particles in molybdenum and depending on number of interactions and depth of particles penetration. Microhardness comparison of calculations and modified experimental data show their satisfactory fit.


Author(s):  
Willem H.J. Andersen

Electron microscope design, and particularly the design of the imaging system, has reached a high degree of perfection. Present objective lenses perform up to their theoretical limit, while the whole imaging system, consisting of three or four lenses, provides very wide ranges of magnification and diffraction camera length with virtually no distortion of the image. Evolution of the electron microscope in to a routine research tool in which objects of steadily increasing thickness are investigated, has made it necessary for the designer to pay special attention to the chromatic aberrations of the magnification system (as distinct from the chromatic aberration of the objective lens). These chromatic aberrations cause edge un-sharpness of the image due to electrons which have suffered energy losses in the object.There exist two kinds of chromatic aberration of the magnification system; the chromatic change of magnification, characterized by the coefficient Cm, and the chromatic change of rotation given by Cp.


Author(s):  
C.L. Woodcock ◽  
R.A. Horowitz ◽  
D. P. Bazett-Jones ◽  
A.L. Olins

In the eukaryotic nucleus, DNA is packaged into nucleosomes, and the nucleosome chain folded into ‘30nm’ chromatin fibers. A number of different model structures, each with a specific location of nucleosomal and linker DNA have been proposed for the arrangment of nucleosomes within the fiber. We are exploring two strategies for testing the models by localizing DNA within chromatin: electron spectroscopic imaging (ESI) of phosphorus atoms, and osmium ammine (OSAM) staining, a method based on the DNA-specific Feulgen reaction.Sperm were obtained from Patiria miniata (starfish), fixed in 2% GA in 150mM NaCl, 15mM HEPES pH 8.0, and embedded In Lowiciyl K11M at -55C. For OSAM staining, sections 100nm to 150nm thick were treated as described, and stereo pairs recorded at 40,000x and 100KV using a Philips CM10 TEM. (The new osmium ammine-B stain is available from Polysciences Inc). Uranyl-lead (U-Pb) staining was as described. ESI was carried out on unstained, very thin (<30 nm) beveled sections at 80KV using a Zeiss EM902. Images were recorded at 20,000x and 30,000x with median energy losses of 110eV, 120eV and 160eV, and a window of 20eV.


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