A new method for measuring the neutron-induced background in BGO Compton-suppressed Ge detectors applied to in-beam γ-ray studies

1987 ◽  
Vol 260 (1) ◽  
pp. 153-156 ◽  
Author(s):  
R. Holzmann ◽  
I. Ahmad ◽  
R.V.F. Janssens ◽  
T.L. Khoo ◽  
D.C. Radford ◽  
...  
Keyword(s):  
New Method ◽  
Γ Ray

scholarly journals A new method to unveil blazars among multiwavelength counterparts of unassociated Fermi γ-ray sources

2017 ◽  
Vol 468 (4) ◽  
pp. 4902-4937 ◽  
Author(s):  
S. Paiano ◽  
A. Franceschini ◽  
A. Stamerra
Keyword(s):  
New Method ◽  
Γ Ray

A new method for measuring γ-ray energy at the internal calibration of a radioactive source

2000 ◽  
Vol 43 (3) ◽  
pp. 300-305
Author(s):  
V. A. Morozov ◽  
V. B. Zlokazov ◽  
A. I. Kalinin ◽  
V. G. Kalinnikov ◽  
N. A. Lebedev ◽  
...  
Keyword(s):  
Radioactive Source ◽  
New Method ◽  
Internal Calibration ◽  
Γ Ray

scholarly journals Overview of two deterministic modelings for prompt emission in fission

2021 ◽  
Vol 256 ◽  
pp. 00017
Author(s):  
Anabella Tudora
Keyword(s):  
Experimental Data ◽  
Kinetic Energy ◽  
Excitation Energy ◽  
The Other ◽  
New Method ◽  
Total Kinetic Energy ◽  
Γ Ray ◽  
Total Excitation Energy ◽  
The University ◽  
Prompt Emission

Two models with a deterministic treatment of prompt emission in fission were developed at the University of Bucharest. Both models work with the same ranges of initial fragments and total kinetic energy and they use the same partition of the total excitation energy at full acceleration based on modelling at scission. The main difference between these modelings regards the prompt emission treatment itself. I.e. the Point-by-Point (PbP) model uses a global treatment of sequential emission while the other modeling is based on an event-by-event treatment of sequential emission. Both models are submitted to a rigorous validation. This paper focuses on model results of different prompt γ-ray quantities, which describe very well the existing experimental data. A new method to calculate prompt γ-ray spectra, including a global treatment based on the distribution of prompt γ-ray energy per quanta, is proposed.

Selective Sampling and Orientation of Non-Homogeneous Tissues

1968 ◽  
Vol 26 ◽  
pp. 98-99
Author(s):  
C. C. Clawson ◽  
L. W. Anderson ◽  
R. A. Good
Keyword(s):  
Electron Microscopy ◽  
Electron Microscope ◽  
Light Microscopy ◽  
Random Sampling ◽  
New Method ◽  
Microscope Examination ◽  
Small Areas ◽  
Selective Sampling ◽  
Large Numbers ◽  
Specific Orientation

Investigations which require electron microscope examination of a few specific areas of non-homogeneous tissues make random sampling of small blocks an inefficient and unrewarding procedure. Therefore, several investigators have devised methods which allow obtaining sample blocks for electron microscopy from region of tissue previously identified by light microscopy of present here techniques which make possible: 1) sampling tissue for electron microscopy from selected areas previously identified by light microscopy of relatively large pieces of tissue; 2) dehydration and embedding large numbers of individually identified blocks while keeping each one separate; 3) a new method of maintaining specific orientation of blocks during embedding; 4) special light microscopic staining or fluorescent procedures and electron microscopy on immediately adjacent small areas of tissue.

A new method for the determination of nitrates

1960 ◽  
Vol 23 ◽  
pp. 227-232 ◽  
Author(s):  
P WEST ◽  
G LYLES
Keyword(s):  
New Method
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