Manohara S R

Dr. Manohara S R


Research Focus & Metrics

Academic Career Length

20Years (2007-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 September 2008 in Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Verified
Journal Article
Closed access
MRManohara S R
Manohara S R
SHS.M. Hanagodimath
S.M. Hanagodimath
KTK.S. Thind
K.S. Thind
LGL. Gerward
L. Gerward

1 September 2009 in Journal of Nuclear Materials
Verified
Journal Article
Closed access
MRManohara S R
Manohara S R
SHS.M. Hanagodimath
S.M. Hanagodimath
LGL. Gerward
L. Gerward

1 May 2007 in Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Verified
Journal Article
Closed access
MRManohara S R
Manohara S R
SHS.M. Hanagodimath
S.M. Hanagodimath

24 September 2008 in Physics in Medicine & Biology
Verified
Journal Article
Closed access
PDF file
MRManohara S R
Manohara S R
SHS M Hanagodimath
S M Hanagodimath
LGL Gerward
L Gerward
The effective atomic number, Z(eff), the effective electron density, N(el), and kerma have been calculated for some fatty acids and carbohydrates for photon interaction in the extended energy range from 1 keV to 100 GeV using an accurate database of photon-interaction cross sections and the WinXCom program. The significant variation of Z(eff) and N(el) is due to the variations in the dominance of different interaction processes in different energy regions. The maximum values of Z(eff) and N(el) are found in the low-energy range, where photoelectric absorption is the main interaction process. The minimum values of Z(eff) and N(el) are found at intermediate energies, typically 0.05 MeV < E < 5 MeV, where Compton scattering is dominant. In this case, Z(eff) is equal to the mean atomic number of the bio-molecule. Wherever possible, the calculations are compared with experimental results. A comparison is also made with the single values of the Z(eff) and N(el) provided by the program XMuDat. It is also observed that carbohydrates have a larger kerma than fatty acids in the low-energy region, where photoelectric absorption dominates. In contrast, fatty acids have a larger kerma than carbohydrates in the MeV range, where Compton scattering is the main interaction process.

1 May 2010 in Radiation Physics and Chemistry
Verified
Journal Article
Closed access
MRManohara S R
Manohara S R
SHS.M. Hanagodimath
S.M. Hanagodimath
LGL. Gerward
L. Gerward

26 December 2007 in Medical Physics
Verified
Journal Article
Closed access
MRManohara S R
Manohara S R
SHS. M. Hanagodimath
S. M. Hanagodimath
LGL. Gerward
L. Gerward