Zobrazeno 1 - 5
of 5
pro vyhledávání: '"Haridas G. Nair"'
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
Autor:
Vijay Kumar, A.K. Bakshi, Rupal Tripathi, Tapas Bandyopadhyay, P K Sahani, Sunil K. Singh, Mukesh Khare, T K Sahu, Saleem Khan, Dimple Verma, D.N. Sharma, Haridas G. Nair, M. K. Nayak, Vipin Dev
Publikováno v:
Radiation protection dosimetry. 164(3)
Five synchrotron radiation beam lines are commissioned and now under regular operation at the Synchrotron Radiation Source, Indus-2 at Raja Ramanna Centre For Advanced Technology (RRCAT), Indore, India. Nine beam lines are under trial operation, and
Publikováno v:
Radiation protection dosimetry. 121(2)
Radiation field during accidental electron beam loss near electron storage rings comprises of high-energy electrons and bremsstrahlung photons. Due to high-energy nature of the radiation, the absorbed dose is expected to build up with depth of the bo
Publikováno v:
Radiation protection dosimetry. 118(3)
Conventional radiation monitors have been found to underestimate the personal dose equivalent in the high-energy bremsstrahlung photon radiation fields encountered near electron storage rings. Depth-dose measurements in a water phantom were carried o