Rotational IMRT delivery using a digital linear accelerator in very high dose rate ‘burst mode’

2011 ◽  
Vol 56 (7) ◽  
pp. 1931-1946 ◽  
Author(s):  
Bill J Salter ◽  
Vikren Sarkar ◽  
Brian Wang ◽  
Himanshu Shukla ◽  
Martin Szegedi ◽  
...  
2018 ◽  
Vol 45 (6) ◽  
pp. 2369-2376 ◽  
Author(s):  
Tucker Netherton ◽  
Yuting Li ◽  
Paige Nitsch ◽  
Simona Shaitelman ◽  
Peter Balter ◽  
...  

PLoS ONE ◽  
2018 ◽  
Vol 13 (6) ◽  
pp. e0199312 ◽  
Author(s):  
Francesca Buontempo ◽  
Ester Orsini ◽  
Isabella Zironi ◽  
Lorenzo Isolan ◽  
Alessandra Cappellini ◽  
...  

1969 ◽  
Vol 47 (16) ◽  
pp. 3007-3016 ◽  
Author(s):  
C. Willis ◽  
A. W. Boyd ◽  
O. A. Miller

Ammonia vapor has been irradiated with single pulses of electrons at a very high dose rate (1027 eV g−1 s−1) with a Febetron 705. At this dose rate radical–product reactions are not significant. In pure ammonia, hydrogen, nitrogen, and hydrazine are produced and the yields found at 1027 eV g−1 s−1 are: G(H2) = 3.58 ± 0.08; G(N2) = 1.00 ± 0.05; G(N2H4) = 0.58 ± 0.05. The yields are independent of pressure from 1 to 5 atm and of temperature between 20 and 200 °C. Above 250 °C the yields of all three products increase significantly and this is due to reaction [1] competing with radical–radical reactions.[Formula: see text]A rate constant for this reaction has been determined,[Formula: see text]Product yields have been measured for ammonia–propene mixtures. These yields have allowed determination of the primary radiation yields GNH = 0.74; [Formula: see text]; GH = 4.8; and G(−NH3) = 5.4.


2005 ◽  
Vol 113 (4) ◽  
pp. 428-437
Author(s):  
C. S. Melhus ◽  
M. J. Rivard ◽  
J. KurKomelis ◽  
C. B. Liddle ◽  
F. X. Massé

1974 ◽  
Vol 5 (22) ◽  
Author(s):  
YOSHIHIKO HATANO ◽  
SATOSHI TAKAO ◽  
HIDEKI NAMBA ◽  
TAKUMI UENO ◽  
SHOJI SHIDA

2017 ◽  
Vol 6 (S5) ◽  
pp. S761-S768 ◽  
Author(s):  
Paola Scampoli ◽  
Carmela Carpentieri ◽  
Marco Giannelli ◽  
Vera Magaddino ◽  
Lorenzo Manti ◽  
...  

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