Zobrazeno 1 - 10
of 236
pro vyhledávání: '"Haridas, G."'
Autor:
Czerski, K., Dubey, R., Kaczmarski, M., Kowalska, A., Targosz-Sleczka, N., Haridas, G. Das, Valat, M.
Publikováno v:
Phys. Rev. C 109, L021601 , 2024
Electron emission in the deuteron-deuteron reaction supporting existence of the single-particle threshold resonance in 4 He has been observed for the first time. The measured electron energy spectrum and the electron-proton branching ratio agree very
Externí odkaz:
http://arxiv.org/abs/2305.17101
Akademický článek
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Publikováno v:
In Applied Radiation and Isotopes July 2019 149:48-51
Publikováno v:
In Radiation Physics and Chemistry March 2019 156:252-258
Autor:
Nayak, M.K., Sahu, T.K., Nair, Haridas G., Nandedkar, R.V., Bandyopadhyay, Tapas, Tripathi, R.M., Hannurkar, P.R.
Publikováno v:
In Radiation Physics and Chemistry May 2016 122:77-81
Publikováno v:
In Radiation Physics and Chemistry February 2016 119:51-54
Autor:
R.V. Nandedkar, Tapas Bandyopadhyay, T K Sahu, P.R. Hannurkar, M. K. Nayak, Haridas G. Nair, Rupal Tripathi
Publikováno v:
Radiation Physics and Chemistry. 122:77-81
Optimum target for bremsstrahlung emission is defined as the thickness of the target material, which produces maximum bremsstrahlung yield, on interaction of electron with the target. The bremsstrahlung dose rate per unit electron beam power at a dis
Autor:
T K Sahu, Rupal Tripathi, R.V. Nandedkar, Haridas G. Nair, M. K. Nayak, P.R. Hannurkar, D.N. Sharma, Tapas Bandyopadhyay
Publikováno v:
Radiation Physics and Chemistry. 113:1-5
Thick target bremsstrahlung source term for 450 MeV and 550 MeV electrons are experimentally determined using booster synchrotron of Indus facility at Raja Ramanna Centre for Advanced Technology, Indore, India. The source term is also simulated using
Publikováno v:
In Nuclear Inst. and Methods in Physics Research, A 2000 449(3):624-628
Autor:
Haridas, G.
Publikováno v:
The British Medical Journal, 1932 Feb 01. 1(3709), 236-236.
Externí odkaz:
https://www.jstor.org/stable/25347098