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Market Availability & Pricing

The Gafchromic™ film is a commercialized product offered by Ashland. It is available through authorized distributors and comes in various models like EBT3, EBT-XD, RTQA2, and LD-V1, each designed for specific radiotherapy and radiology applications.

In June 2022, Ashland introduced the Gafchromic™ LD-V1 film, which features improved contrast and imaging detail, making it a suitable QA tool for radiology in processor-less environments.

For the most accurate and up-to-date pricing information, please contact Ashland directly or consult their authorized distributors.

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The spelling variants listed below correspond to different ways the product may be referred to in scientific literature.
These variants have been automatically detected by our extraction engine, which groups similar formulations based on semantic similarity.

Product FAQ

12 protocols using «gafchromic film»

1

Proton UHDR Beam Characterization

2024
We do not expect the beam characteristics (energy, spot size and spot position, as well as beam divergence) to be significantly different between the clinical and UHDR mode. Nevertheless, in UHDR mode, beam optics may exhibit slight variations owing to the space charge effect caused by densely bunched protons. Beam tuning is also likely to be adjusted due to the implementation of new extraction RF patterns. Most critically, certain safety interlocks, including feedback mechanisms for spot size and position from BMIC, are temporarily bypassed with SPSI in UHDR mode. As a precautionary measure, we decided to measure some aspects of the beam characteristics and confirm its consistency between UHDR and clinical mode.
Gafchromic film (Ashland Inc., Bridgewater, NJ, USA) has been widely used for dosimetry purposes in UHDR studies. The dose response of Gafchromic film was found to be consistent with dose rates up to 1500 Gy/s in previous studies [28 (link),29 (link),30 (link)]. Specifically, the MD-V3 film has a large dynamic dose range (>100 Gy), making it suitable for the cross-comparison of proton beam dosimetry at conventional and UHDR dose rates. It was used extensively in this study to quantify the characteristics of proton UHDR beams such as the spot size and spot position, as well as absolute dose profile, in proton UHDR irradiations.
The spot size and spot positions were measured with MD-V3 film in both clinical and UHDR mode using a spot pattern containing nine spots (4 spots with 10 cm grid spacing, 4 spots with 5 cm grid spacing and 1 spot at the central axis). As a standard commissioning requirement to derive beam model parameters associated with the propagation of in-air spot size and beam divergence, the measurement of this spot pattern was repeated at several positions along the beam axis. These positions ranged from 40 cm upstream to 20 cm downstream of the isocenter, with intervals of 10 cm.
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2

Dose Mapping of X-ray Irradiator for Mosquito Pupae

2023
The Radsource RS2400V X-ray irradiator, equipped with X-ray tube model of Quastar DT-1084, was used to irradiate all mosquito pupae in the study (Rad Source Technologies Inc, USA). The system comprises six individual X-ray containers that rotate around the central X-ray tube (Additional file: Fig. S3) to ensure uniform X-ray exposure. An ionization chamber (10X6-0.18, RadCal Corporation, USA) and a digitizer module (ADDM-plus Accu-Dose, RadCal Corporation, USA) were used as a reference dosimetry system to measure the dose rate. During the dose rate measurement, the ionization chamber was fixed at the centre of the X-ray canister by a customized acrylic holder to simulate X-ray irradiation exposure by mosquito pupae at a similar position (Additional file: Fig. S4). The irradiation doses used in this study were set by adjusting the exposure time based on the dose rate according to the manufacturer. To simulate the pupae irradiation setup during the dose mapping, three Petri dishes (94 × 16 mm, Cat: 633,181, Greiner Bio-One) were stacked together, and 20 mL sterile water was added to the middle Petri dish. A piece of Gafchromic™ film (Ashland Advanced Materials, USA) was inserted in between the middle and bottom petri dish and the entire setup (Additional file: Fig. S5) was placed into one of six X-ray canisters for irradiation at a predetermined dose. The dose map and dose uniformity (DUR) of the X-ray irradiator was determined by scanning the Gafchromic™ film using a flatbed scanner (Canon LiDE 400) post-irradiation. The analysis involved assessing the colour channel information from the scanned image within the effective pupae irradiating area (Additional file: Fig. S6). The scanning and analysis method adhered to the procedure recommended by FAO/IAEA (available ta https://www.iaea.org/sites/default/files/dose-mapping-gafchromic-2020-11-02.pdf).
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3

Managing Metal Artifact in Radiotherapy

2023
The CT artifacts caused by the metal-ports are managed using two density override strategies at our institution. The first strategy (hereafter called RS1) consists of identifying the metal by adjusting the image window-level to display only the brightest region, assumed occupied by the metal port. Subsequently, a contour is delineated enclosing the artifact and the density of surrounding voxels is set to unity. The second strategy (hereafter called RS2) consists of registering rigidly a geometry template with the dimensions, materials, and densities from the corresponding metal-ports obtained from the vendor; the density of voxels outside the port geometry is set to unity. Both strategies were compared using Collapsed Cone Convolution (CCC) version 5.5 in RayStation version 11A, and TOPAS Monte Carlo simulations. The resolution of the dose grid for RayStation and TOPAS calculations was 2 x 2 x 2 mm3. Calculated results were compared with Gafchromic film (Ashland Inc.) measurements using two irradiation setups as described below.
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4

Calibrating EBT3 Film Dosimetry

2021
We carried out absorbed dose measurements using GAFCHROMIC™ films (Ashland Specialty Ingredients G.P., Bridgewater, NJ, USA) type EBT3.36 EBT3 film are suitable for dose map measurements in radiation fields with high dose gradients, as in our measurements, because of the high spatial resolution and energy independence. To convert the response of the film into dose, we measured a calibration curve. For this purpose, we exposed n = 8 pieces of cut films (10 cm × 13 cm) to known different doses (0, 0.2, 0.4, 0.6, 0.8, 1, 1.2, 1.9 Gy), obtained by changing the exposure time. To ensure the stabilization of the polymers, 24 hours after irradiation, the films were scanned with an Epson Expression 11000XL scanner of San Raffaele Hospital (Milan, Italy) in transmission mode at a resolution of 72 dpi (0.35 mm pixel size). To obtain the calibration curve, we utilized the FilmQA™ Pro Software (Ashland Inc.), a quantitative analysis tool designed for film scanning, pixel value extraction, and dose conversion. This software works with a method called “triple channel evaluation,” which uses pixel values from all color channels together to construct the dose map, providing “corrected” red, green, and blue dose maps. It is also possible to separate the dose‐dependent part of the signal from the dose‐independent part, where the latter derives from nonhomogeneity related to film manufacturing, scanner artifacts, or film manipulation (dust, fingerprints).37 Practically, the method varies the dose values until the corresponding pixel values are best matched for all three‐color channels.
In the case of 6 MV irradiation, to plan the fields and beam arrangements for cell lines irradiations, the Medical Physics team of San Raffaele Hospital acquired a CT image of the experimental setup, then they imported it into the treatment planning system (TPS) Eclipse (Varian Medical Systems, Inc., USA) and simulated the irradiation session. To deliver a dose of 1 Gy to the cells, with an uncertainty of 5%, the TPS indicated the necessity to deliver 92 Monitor Unit (MU); for 2 Gy the TPS indicated a value of 184 MU, where MU measures the output of the clinical accelerator, measured by ionization chambers.38 The correct delivery of 1 and 2 Gy, respectively, was also checked placing a piece of EBT3 above the cell arrangement.
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5

GafChromic Film Dosimetry Protocol

2021
This protocol is designed for the analysis of GafChromic films (Ashland Inc., Bridgewater, NJ, USA). In radiation therapy, GafChromic EBT3 and EBT-XD films are recommended. The difference between EBT3 and EBT-XD films lies in the length of the needles of the active component. EBT-XD needles are shorter, which leads to less darkening for the same absorbed dose and to higher saturation doses. Therefore, EBT-XD films are recommended for higher doses. EBT3 films can be used for applications with doses in the range of 0.01–20 Gy. However, for doses larger than 10 Gy and up to 40 Gy, EBT-XD films are preferred.10 (link)
EBT3 and EBT-XD films are considered energy independent for MV photon beams. However, they under-respond to photon energies lower than 100 keV8 (link), and exhibit LET dependence for protons.10 (link)
In kV X-rays applications, such as dose measurements in interventional radiology or IORT11 (link), XR-RV3 films should be used instead. In the energy range of these applications, films are strongly energy dependent and should be calibrated for each energy in use.12 (link)
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