Low-energy levels and gamma transitions inCo58

1975 ◽  
Vol 11 (3) ◽  
pp. 1042-1047 ◽  
Author(s):  
B. J. Brunner ◽  
R. G. Arns ◽  
S. E. Caldwell ◽  
C. M. Rozsa ◽  
J. W. Smith ◽  
...  
Keyword(s):  
Energy Levels ◽  
Low Energy ◽  
Gamma Transitions

scholarly journals Low-energy levels calculation for 193Ir

2006 ◽  
Vol 36 (4b) ◽  
pp. 1354-1356
Author(s):  
Guilherme Soares Zahn ◽  
Cibele Bugno Zamboni ◽  
Frederico Antonio Genezini ◽  
Joel Mesa-Hormaza ◽  
Manoel Tiago Freitas da Cruz
Keyword(s):  
Energy Levels ◽  
Low Energy

scholarly journals Performance Improvement of Ultra Wideband Multiple Access Modulation System using a new Optimal Pulse Shape

2017 ◽  
Vol 6 (1) ◽  
pp. 20
Author(s):  
V. Goyal ◽  
B. S. Dhaliwal
Keyword(s):  
Performance Improvement ◽  
Pulse Shape ◽  
Multiple Access ◽  
Energy Levels ◽  
Rake Receiver ◽  
Correct Choice ◽  
Low Energy ◽  
Ultra Wideband ◽  
High Data ◽  
Very High

Ultra-wideband (UWB) uses very low energy levels to transfer data at very high data rate and bandwidth. An optimal and correct choice of transmission pulse shape is an important criterion in this technology. In this paper, we will present an approach for the generation of an optimal pulse shape with the optimal generation of pulse shape values that can provide effective results when transmitted using multiple access modulation technique over a multipath channel and received by a RAKE type receiver. The bit error analysis of constructed model is also given using Ideal Rake, selective RAKE, and partial RAKE receiver configurations.

Study of High-spin States for 90,91,92Y Isotopes by Using Oxbash Code

2021 ◽  
Vol 14 (1) ◽  
pp. 25-33
Keyword(s):  
Experimental Data ◽  
Transition Probabilities ◽  
Energy Levels ◽  
Model Space ◽  
Low Energy ◽  
Energy Spectra ◽  
Spin States ◽  
Nuclear Shell Model ◽  
High Spin States ◽  
Nuclear Shell

Abstract: In this paper, calculations of 90,91,92Y isotopes have been performed by application of nuclear shell model in the Gloeckner (Gl) model space for two different interactions (Gloeckner (Gl) and Gloeckner pulse bare G-Matrix (Glb) using Oxbash code. The energy levels are compared and discussed with experimental data and based on our results, many predictions about spins and parity were observed between experimental states, in addition to the predictions of low-energy spectra and B (E2; ↓) and B (M1; ↓)) transitional strengths in the isotopes 90,91,92Y. These predictions were not known in the experimental data. Keywords: Energy levels, Transition probabilities, Oxbash code.

Excited fluorescence in low-Z elements by the low-energy gamma transitions and L X-rays from a 241-am XRF source

1987 ◽  
Vol 16 (3) ◽  
pp. 143-146 ◽  
Author(s):  
V. Delgado ◽  
L. González ◽  
A. López ◽  
P. Morán ◽  
E. Vañó
Keyword(s):  
Low Energy ◽  
X Rays ◽  
Energy Gamma ◽  
Gamma Transitions

scholarly journals Multiphoton Ionization Mass Spectrometric (MPIMS) Study of Phenol: Mechanism of Ionic Fragment Formation

1983 ◽  
Vol 3 (1-6) ◽  
pp. 29-47 ◽  
Author(s):  
R. S. Pandolfi ◽  
D. A. Gobeli ◽  
Jonathan Lurie ◽  
M. A. El-Sayed
Keyword(s):  
Laser Pulse ◽  
Energy Levels ◽  
Multiphoton Ionization ◽  
Pulsed Laser ◽  
Ionic Species ◽  
Low Energy ◽  
Ionization Mass ◽  
Fragmentation Pattern ◽  
Dissociation Channel ◽  
532 Nm

Time of flight (TOF) mass spectrometry is used in conjunction with a variable repelling voltage technique to elucidate the mechanism by which phenol ionizes and dissociates under 266 nm pulsed laser irradiation in combination with a 532 nm or 355 nm pulsed laser. The results suggest that, like benzene, the molecular ion is the predominant precursor of all ionic species generated in the process. Predominance of C5Hx+ species at relatively low powers confirms the presence of a low energy dissociation channel involving the elimination of CO. The use of a second laser at 532 nm is found to selectively destroy the C5Hx+ (as compared to the parent ion) species. The parent ion is found to be protected from the radiation of the second laser pulse at 532 nm but not at 355 nm if the second laser pulse is delayed by 50 ns. This is explained in terms of relaxation within the parent ion energy levels, the location of a low energy dissociation channel and the wavelengths of the lasers used. The main aspects of the fragmentation pattern are discussed in terms of the statistical theory of Rebentrost and Ben-Shaul.

101Ru Low-Energy Levels Calculation

2007 ◽  
Author(s):  
F. A. Genezini ◽  
G. S. Zahn ◽  
J. Mesa-Hormaza ◽  
C. B. Zamboni ◽  
M. T. F. da Cruz
Keyword(s):  
Energy Levels ◽  
Low Energy

Low energy levels in cobalt 60

1958 ◽  
Vol 8 ◽  
pp. 79-84 ◽  
Author(s):  
F.A. El Bedewi ◽  
S. Tadros
Keyword(s):  
Energy Levels ◽  
Low Energy

Lifetimes of low-energy levels in 45Ti

1970 ◽  
Vol 32 (1) ◽  
pp. 38-40 ◽  
Author(s):  
F.J. Lynch ◽  
K.-E. Nystén ◽  
R.E. Holland ◽  
R.D. Lawson
Keyword(s):  
Energy Levels ◽  
Low Energy
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