Electrofission ofPb208in the intermediate energy region

1990 ◽  
Vol 41 (1) ◽  
pp. 354-357 ◽  
Author(s):  
J. D. T. Arruda-Neto ◽  
M. Sugawara ◽  
H. Miyase ◽  
T. Kobayashi ◽  
T. Tamae ◽  
...  
Keyword(s):  
Energy Region ◽  
Intermediate Energy

Calculation of orientation and alignment parameters in e-He excitation

1996 ◽  
Vol 74 (11-12) ◽  
pp. 914-919
Author(s):  
Dmitry V. Fursa
Keyword(s):  
Energy Region ◽  
Intermediate Energy ◽  
Close Coupling ◽  
Electron Photon

Convergent close-coupling (CCC) calculations are used to obtain electron–photon coincidence parameters for 21P,31,3P, and 31,3D states of helium in the intermediate energy region. Results of the CCC calculations are compared with experiment and other calculations. Consistent agreement of the CCC calculations with experiment has been achieved for these states at all scattering angles.

Performance of Multilayer Array Analyzer Detector in the Intermediate Energy Region (1 KeV to 3 KeV)

2007 ◽  
Author(s):  
Ke Zhang ◽  
Gerd Rosenbaum ◽  
Qian Liu ◽  
Daniel Fischer
Keyword(s):  
Energy Region ◽  
Intermediate Energy

The electronic structure and spin-charge separation of one-dimensional SrCuO2

2019 ◽  
Vol 33 (02) ◽  
pp. 1950006
Author(s):  
Huaisong Zhao ◽  
Jiasheng Qian ◽  
Sheng Xu ◽  
Feng Yuan
Keyword(s):  
Electronic Structure ◽  
Charge Separation ◽  
Energy Region ◽  
Doping Concentration ◽  
High Energy ◽  
Intermediate Energy ◽  
Low Energy ◽  
One Dimensional ◽  
High Energy Peak ◽  
Energy Peak

Based on the t-J model and slave-boson theory, we have studied the electronic structure in one-dimensional SrCuO2 by calculating the electron spectrum. Our results show that the electron spectra are mainly composed of three parts in one-dimensional SrCuO2, a sharp low-energy peak, a broad intermediate-energy peak and a high-energy peak. The sharp low-energy peak corresponds to the main band (MB) while the broad intermediate-energy peak and high-energy peak are associated with the shadow band (SB) and high-energy band (HB), respectively. From low-energy to intermediate-energy region, a clear two-peak structure (MB and SB) around the momentum [Formula: see text] appears, and the distance between two peaks decreases along the momentum direction from [Formula: see text] to [Formula: see text], then disappears at the critical momentum point [Formula: see text], leaving a single peak above [Formula: see text]. The electron spectral function in one-dimensional SrCuO2 is also the doping and temperature dependent. In particular, in the very low doping concentration, the HB merges into the MB. However, with the increases of the doping concentration, the HB separates from the MB and moves quickly to the high-binding energy region. The HB and MB are the direct results of the spin-charge separation while SB is the result of strong interaction between charge and spin parts. Therefore, our theoretical result predicts that the HB is more likely to be found at the low doping concentration, and it will be drowned in the background when the doping concentration is larger. Then with the temperature increases, the magnitude of the SB decreases, and it disappears at high temperature.

The importance of polarization for electron scattering in the intermediate energy region

1971 ◽  
Vol 9 (4) ◽  
pp. 299-305 ◽  
Author(s):  
D.G. Truhlar ◽  
J.K. Rice ◽  
S. Trajmar ◽  
D.C. Cartwright
Keyword(s):  
Electron Scattering ◽  
Energy Region ◽  
Intermediate Energy
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