Can a low-energy photon beam be suitable for the treatment of cervical malignancies? A dosimetric analysis

2020 ◽  
Vol 3 (2) ◽  
pp. 55
Author(s):  
Manindra Bhushan ◽  
Deepak Tripathi ◽  
Lalit Kumar ◽  
RahulLal Chowdhary ◽  
Anjali Kakria ◽  
...  
2020 ◽  
Vol 163 ◽  
pp. 109229
Author(s):  
Vu Ngoc Ba ◽  
Le thi Ha Giang ◽  
Bui Ngoc Thien ◽  
Truong Thi Hong Loan ◽  
Ngo Quang Huy

1984 ◽  
Vol 31 (1) ◽  
pp. 138-140
Author(s):  
P. Argan ◽  
A. Bloch ◽  
G. Colin ◽  
G. Tamas ◽  
E. Vincent

2004 ◽  
Vol 31 (7) ◽  
pp. 1960-1963 ◽  
Author(s):  
Inhwan Jason Yeo ◽  
Akbar Beiki-Ardakani ◽  
Young-bin Cho ◽  
Mostafa Heydarian ◽  
Ting Zhang ◽  
...  

1959 ◽  
Vol 37 (12) ◽  
pp. 1418-1437 ◽  
Author(s):  
A. P. Baerg ◽  
R. M. Bartholomew ◽  
F. Brown ◽  
L. Katz ◽  
S. B. Kowalski

Angular distributions of photofission fragments relative to the photon beam have been measured as a function of maximum bremsstrahlung energy in the range 6–20 Mev. The nuclides U-233, U-235, Np-237, Pu-239, and Am-241 give an isotropic distribution at all energies studied. The nuclides Th-232, U-234, U-236, U-238, and Pu-240 give anisotropic distributions which can be described by an equation of the form W(θ) = 1 + α sin2 θ where θ is the angle between fragment and beam. The degree of anisotropy is large at low energy and falls rapidly as the energy is increased. At a given energy Th-232 has the greatest degree of anisotropy and Pu-240 the least.


2009 ◽  
Vol 67 (2) ◽  
pp. 324-328 ◽  
Author(s):  
Jeong-Eun Rah ◽  
Siyong Kim ◽  
Kwang-Ho Cheong ◽  
Jeong-Woo Lee ◽  
Jin-Beom Chung ◽  
...  

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