SOME DISCUSSIONS INSPIRED BY THE FLUCTUATION OF SINGLE-EVENT pt DISTRIBUTION

2007 ◽  
Vol 16 (10) ◽  
pp. 3323-3330
Author(s):  
XU MINGMEI ◽  
LIU LIANSHOU

Starting from the assumption that it is the single-event pt distribution, not only the event-wise Mpt , fluctuates E-by-E, we discuss the relation between the variance of Mpt and the two-particle pt correlation. An evaluation of statistical fluctuation is given. For an example, we use an exponential single-event pt distribution to extract E-by-E dynamical fluctuation of single-event pt distribution from experimental data.

2006 ◽  
Vol 21 (26) ◽  
pp. 5241-5252 ◽  
Author(s):  
MINGMEI XU ◽  
LIANSHOU LIU

Assuming that the single-event transverse momentum distribution fluctuates event by event according to a distribution functional, we derive analytical expressions for both the variance of event-wise mean transverse momentum and the two-particle transverse momentum correlation. The relation between these two is discussed. An evaluation of statistical fluctuation is given. An exponential form for the single-event transverse momentum distribution is taken as an example to demonstrate our method for extracting event-by-event dynamical fluctuation of single-event transverse momentum distribution from experimental data.


Author(s):  
Н.А. Иванов ◽  
О.В. Лобанов ◽  
В.В. Пашук ◽  
М.О. Прыгунов ◽  
К.Г. Сизова

AbstractThe occurrence of single-event upsets (SEUs) in 90-nm SRAM integrated circuits irradiated by 1000-MeV protons has been investigated. The experimental data were analyzed and processed, and the results showed the possibility of multiple cell upsets in the integrated circuits studied.


Author(s):  
A. Gómez ◽  
P. Schabes-Retchkiman ◽  
M. José-Yacamán ◽  
T. Ocaña

The splitting effect that is observed in microdiffraction pat-terns of small metallic particles in the size range 50-500 Å can be understood using the dynamical theory of electron diffraction for the case of a crystal containing a finite wedge. For the experimental data we refer to part I of this work in these proceedings.


Author(s):  
K.B. Reuter ◽  
D.B. Williams ◽  
J.I. Goldstein

In the Fe-Ni system, although ordered FeNi and ordered Ni3Fe are experimentally well established, direct evidence for ordered Fe3Ni is unconvincing. Little experimental data for Fe3Ni exists because diffusion is sluggish at temperatures below 400°C and because alloys containing less than 29 wt% Ni undergo a martensitic transformation at room temperature. Fe-Ni phases in iron meteorites were examined in this study because iron meteorites have cooled at slow rates of about 10°C/106 years, allowing phase transformations below 400°C to occur. One low temperature transformation product, called clear taenite 2 (CT2), was of particular interest because it contains less than 30 wtZ Ni and is not martensitic. Because CT2 is only a few microns in size, the structure and Ni content were determined through electron diffraction and x-ray microanalysis. A Philips EM400T operated at 120 kV, equipped with a Tracor Northern 2000 multichannel analyzer, was used.


Author(s):  
C. C. Ahn ◽  
D. H. Pearson ◽  
P. Rez ◽  
B. Fultz

Previous experimental measurements of the total white line intensities from L2,3 energy loss spectra of 3d transition metals reported a linear dependence of the white line intensity on 3d occupancy. These results are inconsistent, however, with behavior inferred from relativistic one electron Dirac-Fock calculations, which show an initial increase followed by a decrease of total white line intensity across the 3d series. This inconsistency with experimental data is especially puzzling in light of work by Thole, et al., which successfully calculates x-ray absorption spectra of the lanthanide M4,5 white lines by employing a less rigorous Hartree-Fock calculation with relativistic corrections based on the work of Cowan. When restricted to transitions allowed by dipole selection rules, the calculated spectra of the lanthanide M4,5 white lines show a decreasing intensity as a function of Z that was consistent with the available experimental data.Here we report the results of Dirac-Fock calculations of the L2,3 white lines of the 3d and 4d elements, and compare the results to the experimental work of Pearson et al. In a previous study, similar calculations helped to account for the non-statistical behavior of L3/L2 ratios of the 3d metals. We assumed that all metals had a single 4s electron. Because these calculations provide absolute transition probabilities, to compare the calculated white line intensities to the experimental data, we normalized the calculated intensities to the intensity of the continuum above the L3 edges. The continuum intensity was obtained by Hartree-Slater calculations, and the normalization factor for the white line intensities was the integrated intensity in an energy window of fixed width and position above the L3 edge of each element.


2008 ◽  
Author(s):  
Ayala Daie-Gabai ◽  
Idan Aderka ◽  
Edna Foa ◽  
Naama Shafran ◽  
Eva Gilboa-Schechtman

2004 ◽  
Vol 114 ◽  
pp. 149-151 ◽  
Author(s):  
Kyuya Yakushi ◽  
Mikio Uruichi ◽  
Hiroshi Yamamoto ◽  
Reizo Kato

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