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Beam Parameters of the Designed Linac.

Beam Parameters of the Designed Linac.

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Conference Paper
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Emerging evidence indicates that the therapeutic window of radiotherapy can be significantly increased using ultra-high dose rate dose delivery (FLASH), by which the normal tissue injury is reduced without compromising tumor cell killing. The dose rate required for FLASH is 40 Gy/s or higher, 2-3 orders of magnitude greater than conventional radiot...

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Context 1
... best configurations of the bunchers and corresponding beam parameters are summarized in Fig. 4. The same plot demonstrates the simulated energy spectrum of the accelerated beam, the quality of which is very good (narrow beam head and thin low-energy tail). The parameters of the optimized linac simulated in Parmela are presented in Table 1. These numbers demonstrate that we were able to increase the beam current by ~50% thanks to the deep redesign of the buncher, application of solenoid, and due to the decision to operate with longer sections (almost 2.4 m). ...
Context 2
... best configurations of the bunchers and corresponding beam parameters are summarized in Fig. 4. The same plot demonstrates the simulated energy spectrum of the accelerated beam, the quality of which is very good (narrow beam head and thin low-energy tail). The parameters of the optimized linac simulated in Parmela are presented in Table 1. These numbers demonstrate that we were able to increase the beam current by ~50% thanks to the deep redesign of the buncher, application of solenoid, and due to the decision to operate with longer sections (almost 2.4 m). ...

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Citations

... Another factor that allows for improvement in dose rate is increasing the beam energy. The conversion efficiency from electron beam power to X-ray power scales approximately with E 3 , so a small increase in energy can make a big difference in X-ray intensity (Kutsaev et al., 2022). The increased X-ray energy also allows greater penetration. ...
... The structure parameters used for the estimation were considered as follows. The SW structure is a scaled to L-band version of an S-band linac that we are currently building for the demonstration version of FLASH (Kutsaev et al., 2022). The TW structure has a geometry similar to a 40 MeV L-band linac for neutron production that is being built by RadiaBeam for Rensselaer Polytechnic Institute (Adolphsen et al., 2014), optimized for the highest shunt impedance (R sh ). ...
... Two criteria were used for the optimization quality: beam transmission-should be maximized, and beam spectrum width-should be minimized. The approach for the buncher optimization is described in the works (Kutsaev, 2010;2021a;Kutsaev et al., 2022) The best configurations of the bunchers and corresponding beam parameters are summarized in Table 2 and Figure 9. Next, we designed the second acceleration section to accelerate the beam from 9 MeV to 18 MeV. Again, the bore diameter was made as large as possible, and the total length was designed to be less than 2.0 m so that the electric acceleration field would be uniform. ...
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