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Kev-Fusion published presentations and documents on DocSlides.

Status of LGAD RD50 projects
Status of LGAD RD50 projects
by barbara
G. Pellegrini. ,. M. . Baselga. , M. . Carulla. ,...
Measurement situation Ground surface measurement (for environmental monitoring
Measurement situation Ground surface measurement (for environmental monitoring
by desha
) : detect the radiation energy spectrum at 1m abo...
Nuclear Medicine procedures in prostate cancer: from diagnosis to treatment
Nuclear Medicine procedures in prostate cancer: from diagnosis to treatment
by joy
Francesco GIAMMARILE. « . Aut tace aut loquere m...
APS Upgrade Brian Stephenson
APS Upgrade Brian Stephenson
by riley
Argonne National Lab. 7 December 2010. The APS Upg...
RadInspector Radioisotope Identification and Measurement
RadInspector Radioisotope Identification and Measurement
by desha
Aman. . Kataria. (EE), Johnny . Klarenbeek. (EE),...
Investigation of a single plane Compton gamma camera as a radiation Imager
Investigation of a single plane Compton gamma camera as a radiation Imager
by isla
Om Prakash Dash*, Tomislav Bokulić, Damir Bosnar,...
Capillary Collimated XRF-imaging with
Capillary Collimated XRF-imaging with
by dorothy
Timepix. 3. Siwen . An. , David Krapohl, Börje N...
Status of the Astrosat
Status of the Astrosat
by madeline
mission. A R . Rao. Tata Institute of Fundamental ...
BINGO: B i- I sotope 0 ν
BINGO: B i- I sotope 0 ν
by delcy
2. β. . N. ext . G. eneration . O. bservatory. H...
The HUNTER experiment - searching for keV sterile neutrinos
The HUNTER experiment - searching for keV sterile neutrinos
by barbara
by energy-momentum reconstruction of atomic K-capt...
Balraj Singh 50 years in Nuclear Science and Nuclear Data
Balraj Singh 50 years in Nuclear Science and Nuclear Data
by nicole
22nd Technical Meeting of the NSDD . Network, 22-2...
Image Reconstruction and Processing for Alpha Emitters
Image Reconstruction and Processing for Alpha Emitters
by skylar
Yong Du. Ph.D.. Department of Radiology, Johns Hop...
Solar Physics with X-ray
Solar Physics with X-ray
by zoe
Observations. Gordon D. Holman. Solar Physics Labo...
Radiation Protection 03.05.2017
Radiation Protection 03.05.2017
by genevieve
Lab coat → shields already approx. 80% of soft ...
RF Hobbs (Johns Hopkins University)
RF Hobbs (Johns Hopkins University)
by julia
Growth and Potential Isotope Needs in Medicine . ...
Gamma Ray Attenuation Properties of Common
Gamma Ray Attenuation Properties of Common
by wilson
Shielding Materials Daniel R. McAlister , Ph.D. PG...
Introduction to Bubble Chamber:
Introduction to Bubble Chamber:
by SkylineBabe
Ops Training. https://. wiki.jlab.org/ciswiki/inde...
PHYS389 : Semiconductor Applications
PHYS389 : Semiconductor Applications
by SimplySweet
L14. Lecture . 14: . Radiation detectors III. Germ...
eROSITA: Status & Scientific Prospects
eROSITA: Status & Scientific Prospects
by Dollface
t. o . extend the ROSAT all-sky survey up to . 10 ...
Radiation Protection in
Radiation Protection in
by LovableLatina
Laboratory. . work. Mats Isaksson, prof.. Departm...
Lively Accreting Black Holes in X-ray Binaries
Lively Accreting Black Holes in X-ray Binaries
by InLoveWithLife
Jeff McClintock. Harvard-Smithsonian Center for As...
Radio studies of mysterious Type
Radio studies of mysterious Type
by margaret
IIn. supernovae. Poonam Chandra. National Centre ...
Enhancement of Peak to Compton Ratio (P/C) using a New
Enhancement of Peak to Compton Ratio (P/C) using a New
by anastasia
Array. . Design for Safeguards . Applications. R....
Gd and Gd2O3 coatings as neutron converters
Gd and Gd2O3 coatings as neutron converters
by davies
Dorothea . Pfeiffer. 23. .09.2014. Content. 2. Ins...
AMEGO – A Wide Field Astrophysics Discovery Mission for the MeV Band
AMEGO – A Wide Field Astrophysics Discovery Mission for the MeV Band
by hanah
1. Julie . McEnery. (NASA/GSFC) on behalf of the ...
High Energy Solar Flares
High Energy Solar Flares
by morton
-. What Fermi Adds to the Picture. Brian R. Dennis...
First Results of Deuterium Beam Operation on Neutral Beam Injectors in the Large Helical Device
First Results of Deuterium Beam Operation on Neutral Beam Injectors in the Large Helical Device
by gelbero
K. . Ikeda. 1). , . K. . . Tsumori. 1)2. ). , M. ....
When latest data differ from earlier ones: An example of
When latest data differ from earlier ones: An example of
by walsh
187. Hg. Shamsuzzoha. . Basunia. Lawrence Berkele...
57 Fe neutron inelastic scattering
57 Fe neutron inelastic scattering
by ida
The interplay between experiment and theory. . A....
DEPENDENCE OF THE MGA CODE PERFORMANCE ON DETECTOR ENERGY RESOLUTION C
DEPENDENCE OF THE MGA CODE PERFORMANCE ON DETECTOR ENERGY RESOLUTION C
by dandy
results during isotopic analysis Traditionally it ...
L Cosentino
L Cosentino
by helene
meeting EURISOL-NET CERN 28 June 2011L CosentinoIN...
BEGe projectBEGe project
BEGe projectBEGe project
by garcia
Results from detector operationsResults from detec...
ADA230 480 UMENTATION PAGE Form Approved
ADA230 480 UMENTATION PAGE Form Approved
by daniella
LVol[ ... .... OMB No. 0704-0188 Public reporling ...
Available
Available
by osullivan
performance 2013 Extended Performance (1) E ( Me...
Matthew Szydagis M. Szydagis, N
Matthew Szydagis M. Szydagis, N
by bikersnomercy
. Barry. , . K. . Kazkaz. , . J. Mock. , . D. . St...
The XENIA mission Cosmic chemical evolution of baryons
The XENIA mission Cosmic chemical evolution of baryons
by mjnt
. Luigi Piro. C. . Kouveliotou. , . J.W.. den . H...
Cooperation of Czech Republic and
Cooperation of Czech Republic and
by vamput
Laboratoire. . Soutterain. de . Modane. (LSM, F...
Alex Bogacz Optics for UITF
Alex Bogacz Optics for UITF
by fluental
-. ‘. keV. ’ and ‘MeV’ beam-lines. UITF M...
PHY582 ― Particle Physics II (Experiment)
PHY582 ― Particle Physics II (Experiment)
by vamput
Lecture 8: Dark Matter detectors. Ar. á. n Garc. ...
Direct Dark Matter (WIMPs) Searches and the XMASS Experiment
Direct Dark Matter (WIMPs) Searches and the XMASS Experiment
by envrrolex
S. earches and the XMASS Experiment. Y. Suzuki. Ka...