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21 protocols using clinac 2100 cd

1

Preclinical Cancer Immunotherapy Protocol

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C57BL/6AnCrl and BALB/cAnCrl female mice were injected subcutaneously with 2.105 TC1, CT26, MC38, B16F10, or B16OVA cells in 100 µL of phosphate buffered saline (PBS 1×, Gibco, France) into the left flank. Tumor growth was monitored every 3 days with a caliper and groups were formed when tumor reached a mean diameter of 50–60 mm2. All CT procedures were conducted in the Pharmacy Department of the University Hospital of Besançon (France). Mice were administered a single dose of intraperitoneal cisplatin (5 mg/kg) and 5-fluorouracil (25 mg/kg). After 2 days, mice were anesthetized by injection of ketamine (100 mg/kg) and xylazine (10 mg/kg) and received single-fraction beam photon irradiation (8 Gy) using Clinac 2100 CD (Varian Medical System) with a maximal energy of 6 MV and in 2D with one beam. Mice from control group were injected with the solvent used to dilute the drug (the Pharmacy Department of the University Hospital of Besançon, France). Anti-mouse CTLA-4 antibody (9H10, Euromedex) and anti-PD-1 (RMP1-14, Euromedex) injections (200 µg/mouse two times a week for 2 weeks) started 2 days prior to CT and 3 days after RT, respectively. All experimental studies were approved by the local ethics committee in accordance with the European Union’s Directive 2010/63.
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2

MLC Leakage Measurement Protocol

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The 6 MV photon beam of the Clinac 2100C/D dual-energy linear accelerator equipped with a 120-leaf Millennium multi-leaf collimator system and an aS1000 EPID (Varian Medical Systems, Inc., USA) was used in this study. In order to measure the DLG, sweeping gap fields of varying widths were used. To measure the MLC leakage, two completely blocked MLC fields (one with MLC bank A completely closing the field, as shown in Figure 1, and the other with MLC bank B closed in a similar manner) were employed since a single blocked field with both MLC banks closed at the center would result in over-estimating the MLC leakage due to the abutting leaf-end transmission. A plan was created in Eclipse™ TPS (Varian Medical Systems, Inc., USA) consisting of seven sweeping gap fields of widths 2 mm, 4 mm, 6 mm, 10 mm, 14 mm, 16 mm, and 20 mm, respectively, apart from two closed MLC fields and an open field. A reference field size of 10 cm × 10 cm was set by the X and Y jaws for all the above ten fields, which will hereafter be referred to as DLG fields. Each sweeping gap traveled across this reference field, and had a control point for every centimeter. The leaf sequences for the same were calculated using LMC.
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3

X-Ray Irradiation of Cell Cultures

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One day after infection, the relevant experimental cultures were irradiated at Turku University Hospital (Department of Oncology and Radiotherapy) using a linear accelerator (Clinac 2100C/D, Varian Medical Systems, Palo Alto, CA) at a total dose of 2 Gy of 6 MV x-ray irradiation at a dose rate of 3 Gy/min. Mock-irradiated cell cultures were included in the experiment (Figure 1).
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4

IMRT Delivery Using IGRT Technique

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IMRT was performed using a treatment planning system (TPS; Eclipse ver. 8.9, Varian Medical Systems, USA) and a linear accelerator (CLINAC 2100CD, Varian Medical Systems, USA). A total prescription dose of 74 Gy (2 Gy per fraction; Monday to Friday) was delivered using 10 MV photon beams. All treatment fractions were conducted using image-guided radiation therapy (IGRT) to correct positional errors for target and critical organs. The median duration of the IMRT (from the start to the end of treatment) was 55 days (range, 50–61 days).
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5

Zebrafish Irradiation Protocol

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Anaesthetized zebrafish larvae and adults were transferred to an acrylic phantom box to achieve a certain thickness and exposed to LDIR as described previously11 (link). Briefly, a computed tomography (CT) scan (Somatom Sensation, Siemens) was performed and a volumetric acquisition was carried out; acquired images were reconstructed with axial slices width of 1 mm, and cross sectional data was transferred to the image processing system work station for contouring the planning target volume (PTV). The radiotherapy plan was devised on a dedicated 3D planning system (PLATO, Nucletron) using an isocentric dose distribution of two opposite fields (0°, 180°) at 6 MV energy, normalized to a reference point. IR delivery was performed at room temperature using a linear accelerator x-rays photon beam (Varian Clinac 2100 CD) operating at a dose rate of 300 MU/min. A 0.6 cm3 PTW farmer ionizing chamber, connected to UNIDOS electrometers, was used to validate the IR doses calculated by PLATO, according to the IAEA TRS-398 protocol. We obtained, in average, differences lower than 2% between the experimental and the PLATO planning system dose values.
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6

Electron FLASH Beam Delivery Protocol

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The electron FLASH beam used in this study was derived from a Varian Clinac 2100 C/D (Palo Alto, CA) after reversible conversion procedures developed in our previous work (27 ). Briefly, the LINAC was converted to deliver 10 MeV electron FLASH beam by selecting 10 MV photon beam energy in the treatment console, retracting the x-ray target from the beam’s path and positioning the carousel on an empty port. For the in vitro experiments, a 10 MeV electron FLASH beam with a wide field size of 20 × 20 cm2 covered the whole solution sample, and the dose rate was 300 Gy/s at the isocenter. For the in vivo experiments, a 6 × 6 cm2 electron applicator with a circular diaphragm (1.5 cm in diameter) was used to project the electron FLASH beam on tissue at a specific position on each mouse. The average dose rate was 270 Gy/s at the beam isocenter. Table S1 summarizes the dosimetric parameters as used. The central axis percentage depth dose (PDD) and 2D surface dose distributions are shown in Fig. S1, as measured by Gafchromic Film EBT-XD (Ashland Inc., Covington, KY).
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7

Monte Carlo Simulation of Electron Beams

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In this study, the 6 and 9 MeV electron beams were adopted, due to their common clinical use. The initial particle source files for the electron beams with 10 × 10 cm fields from the Varian Clinac 2100CD medical linear accelerator were the PSFs obtained from the IAEA official website [20 ]. The operating system used was 64-bit Windows 10, and the C++ compiler employed was Microsoft Visual Studio Community 2019 (version 16.10.2). To simulate the transport process of the electron beams and calculate the dose deposition in the models, the geant4 Monte Carlo software package (version 10_07_p02) was utilized. The chosen physics model was LowE_Livermore with a cutoff range of 1 mm. For both 6 and 9 MeV electron beams, a total of 56 871 296 [21 ] and 56 197 810 [22 ] particles were sampled, respectively, from the initial PSFs. Subsequently, the particle transport process in air was simulated, and information on the particles reaching a plane with dimensions of 16 × 16  × 0.1 cm, positioned 3 cm above the bolus (i.e. at a distance of 97 cm from the virtual source) was recorded to generate corresponding new PSFs. These new PSFs were used as the particle sources for the subsequent calculations.
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8

Cherenkov Photon Emission from 6MV X-rays

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Previous Monte Carlo simulations documented by Glaser et al. 7 (link) provide the fluence rate over a wide spectral range for Cherenkov photons produced in tissue as the result of an external 6MV X-ray photon beam. This average fluence rate (nW/cm2) is provided as a function of radiation dose rate (Gy/sec) and can be converted to photon flux (photons/cm2) by accounting for the energy at each wavelength. The photon flux is then dependent on the radiation dose rate, which can be simplified to be assumed at a standard 0.1Gy/sec (600MU/min, the standard Monitor Unit rate of the Varian Clinac2100CD at 6MV). The Varian higher energy clinical linear accelerator (Clinac 2100C) referenced in previous CEL publications provides a 3–4μs radiation pulse at a variable repetition rate of 60Hz–360Hz, but commonly at 360 Hz for the higher MU/min.6 (link),8 (link),18 (link)The number of Cherenkov photons can then be estimated for the area detected by a single pixel (0.1mm2) based on the total dose delivered. For simplicity, this is calculated for the following: a single pulse (0.028 cGy), 30 pulses (0.83 cGy), 60 pulses (1.67 cGy), and 7200 pulses (2 Gy), where 2Gy is a typical daily dose given during fractionated radiotherapy.
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9

Characterization of MOSFET Dosimeters

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The characteristics of the MOSFET dosimeters were determined for Co-60 gamma rays (1.25 MeV) of Theratron 780C (MDS Nordian, Canada) and for 6 and 15 MV x-rays beams of Clinac 2100 C/D (Varian Medical Systems, USA). During the experimental measurements, the MOSFET dosimeters were placed on the top of acrylic slab (each of thickness 10 mm) phantom [Figure 1] of density 1.18 g/cm3. The total thickness of this slab phantom was about 10 cm, which was sufficient to provide adequate backscattering [22 (link)25 (link)] for the photon beams in this study.
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10

Radiation Exposure in Rabbit Bone

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Radiation on rabbits was performed by radiotherapists in Department of Clinical Oncology, Queen Mary Hospital, The University of Hong Kong, using the protocol reported in our previous study [8 (link)]. The tibial and femoral metaphysis region of left hind leg was subjected to a single dose of 15 Gy irradiation, whereas the other parts of the animals were protected. Electron beams of 9 MeV from a Varian Clinac 2100CD were delivered with a 15 × 15 cm2 applicator at a source to surface distance of 60 cm.
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