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Varian linac 2100cd

Manufactured by Agilent Technologies

The Varian Linac 2100CD is a medical linear accelerator designed for radiation therapy. It generates high-energy X-rays or electrons for the treatment of cancer. The device is capable of delivering precise and targeted radiation doses to affected areas while minimizing exposure to healthy tissues.

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2 protocols using varian linac 2100cd

1

Cherenkov-Excited Luminescence Imaging

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As shown in Fig.1A, the light source of CELI is Cherenkov light generated in tissues induced by a linear accelerator (Varian Linac 2100CD, Varian Medical System), at the Norris Cotton Cancer Center, Dartmouth-Hitchcock Medical Center. For radiotherapy, 6MV X-ray radiation delivered from the Linac with a beam size adjusted to cover the entire tumor for treatment purpose. The CELI imaging system was previously reported. In brief, a time-gated intensified CCD camera (ICCD, PI-MAX4 1024i, Princeton Instruments) coupled with a commercial lens (Canon EF 135mmf/2L USM) was used as the detector. To shield the MV X-ray, the camera was put in a homemade lead box about 2 meters away from the imaging field. A band pass filter with center wavelength of 750 nm and spectral bandwidth of 100 nm was used to collect phosphorescence from Oxyphor PtG4. The time-gated ICCD camera was synchronized with the radiation pulse, which was ~3.25 μs long delivered at 360 Hz repetition rate from the Linac. Four CELI images were acquired with the delay times of 5 μs, 10 μs, 20 μs, and 30 μs to fit the lifetime image. To accumulate high enough phosphorescence signals, the intensifier gain was set to the maximum of 100, and 360 repeat cycles were integrated with 200 μs gate width in each cycle. The Linac room was kept dark during the acquisition to minimize stray light.
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2

Cherenkov Imaging of Tumor Radiation

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Cherenkov light was induced in the tissue by irradiation from a linear accelerator (Varian Linac 2100CD; Varian Medical System) at the Norris Cotton Cancer Center, Dartmouth-Hitchcock Medical Center. The beam size was adjusted to cover the entire tumor area. To minimize the background, all lights in the room were switched off. The imaging system consisted of a time-gated intensified CCD camera (ICCD, PI-MAX4 1024i; Princeton Instruments), a lens (Canon EF 135 mm f/2L USM), and a 750 nm/100 nm band pass filter. The camera was contained in a homemade lead box, placed ~2 m away from the imaging field to protect it from Compton scattered X-ray photons. The noise induced by X-ray photons was therefore significantly suppressed, and the signal-to-noise ratio (SNR) was more than seven times higher after shielding (Supplementary Fig. 10). The time-gated ICCD camera was synchronized with the radiation pulses, which were ~3.25 μs long and delivered with 360 Hz repetition rate. The camera gate was turned on at 5, 10, 20, and 30 μs delay times and the phosphorescence was integrated on the CCD for 200 μs. The intensifier gain was ×100.
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