X-ray intensifying
designed to your
system requirements


Levy and West, the founders of the renowned laboratories which later became Applied Scintillation Technologies and then Scintacor, were among the pioneers who explored the use of zinc sulphide phosphors for fluoroscopic X-ray imaging [1] [2]. Since then, many additional phosphor systems have been developed and today we find gadolinium oxysulphide (Gd2O2S or simply Gadox / GOS) phosphor is one of the most widely adopted for several reasons. The material morphology is well known and well controlled; the luminescent efficiency is relatively high (approximately 15%) and the emitted light matches well with the spectral response of silicon light detection devices such as charge-coupled detectors (CCD) and complementary metal oxide semiconductors (CMOS) [1].

Gadox intensifying screens were originally developed and commercialized by companies which supplied photographic film and were often described as ‘fine’, ‘regular’ or ‘fast’ depending upon the film speed and spatial resolution of the film with which they were paired [1]. These screens are still widely available up to a maximum size of 14’’x 17’’ but they do not always provide the optimal solution for digital x-ray imaging [1]. Conversely, Scintacor phosphor screens have been specifically designed around digital x-ray imaging systems to provide differentiated performance over standard intensifying screens, in both lens-coupled systems, and direct-coupling to solid-state light detectors, such as CMOS and CCD.

Their insensitivity to moisture, their radiation hardness, and their relatively low cost, make Scintacor Gadox screens the scintillator of choice for x-ray imaging in many different industrial, security and research applications.

Products & Properties  

Designations & Formulations

Scintacor offers three types of Gadox intensifying screens (sometimes referred to as luminescent screens): Luminex and Rapidex for hard x-ray applications (50-300 KeV) and MeVex for use at high-energy energy levels (>450 KeV – 25 MeV). The properties of these screens are listed in Table 1.

Table 1 X-ray Intensifying Screens: Basic Performance

Luminex Light Output (1) MTF % @ 2lp/mm (2) MTF % @ 5lp/mm (2) Attenuation % (2) Decay to 10% μs Afterglow @ 20ms %
Ultrabright 205% 18 4 92 1,500 <0.1%
Bright 175% 21 7 92 1,500 <0.1%
Medium 170% 23 5 91 1,500 <0.1%
Fine 129% 42 15 86 1,500 <0.1%
UltraFine 70% 65 29 83 1,500 <0.1%
UltraFine+ 50% 76 45 76 1,500 <0.1%
Rapidex Light Output (1) MTF % @ 2lp/mm (2) MTF % @ 5lp/mm (2) Attenuation % (2) Decay to 10% μs Afterglow @ 20ms %
Bright 92% 16 4 97 7 <0.1%
Medium 91% 19 5 94 7 <0.1%
Fine 81% 32 9 89 7 <0.1%
MeVex Light Output (1) MTF % @ 1lp/mm (2) MTF % @ 2lp/mm (2) Attenuation % (2) Decay to 10% μs Afterglow @ 20ms %
Medium  242%  16  <10  98  1,500   <0.1%
(1)Relative to Lanex Regular benchmark screen. X-ray source: 150kV unfiltered
(2)X-ray source 70kV

Luminex screens are made of terbium-doped gadolinium oxysulphide (Gadox:Tb). This phosphor, also known as P43 [3], is one of the most efficient scintillators available in terms of light output per incident x-ray energy, due to its high atomic number and density, which make it an effective absorber of x-rays. For a given thickness, Gadox is a more efficient scintillator than Caesium Iodide (CsI), except in a window between 35 and 50 KeV, which corresponds to the interspace between the k-edges of caesium and gadolinium respectively. In addition, the emitted light (545 nm) matches the spectral response of the most common silicon photosensitive devices and allows these to operate at high quantum efficiency (QE).

The Luminex screens are available in six designations, which offer different trade-offs between resolution and light output. Fine, Ultrafine and Ultrafine+ are thin screens designed for high-resolution applications such as digital radiography and are suitable for direct-coupling with large area CMOS and CCD detectors. Ultrabright, Bright and Medium are thicker screens ideal for lens coupled systems, which are generally light-starved but have lower resolution requirements than direct-coupling systems [1]. Typical applications for these thicker screens are cabinet x-ray systems for postal screening or industrial radiography of large-scale objects, such as rocket nozzles or engine blocks.

Rapidex screens are available in three designations and are made of praseodymium-doped gadolinium oxysulphide (Gadox:Pr), a phosphor optimised for high frame rate applications, where minimal afterglow and resistance to latent image burn-in are required. These applications include flying spot backscatter detectors; linear scanners for food and end-of-line inspection and area photosensitive devices for ultra-high speed imaging. As shown in Table 1, the decay time to 10% for the Rapidex screens is some 200 times faster than that of the corresponding Luminex item. However, Gadox:Pr is  less efficient so that the light output of the Rapidex Medium is approximately half of that of a Luminex Medium, despite the two screens having comparable thicknesses and resolution properties. In addition, the emission of Gadox:Pr is slightly shifted to green, with a peak at 513 nm and this is likely to lead to  marginally lower detector quantum efficiency than that achievable with a Luminex screen.

MeVex Medium is a very high coating weight screen made of terbium-doped gadolinium oxysulphide (Gadox:Tb), whose formulation and phosphor particle size distribution have been optimized for high-energy applications (>450 KeV – 25 MeV,) such as patient alignment systems in radiotherapy and gamma radiography in homeland security or scientific research.

Size and geometry

Unlike other commercially available products, Scintacor phosphor screens can be ordered in single units and custom-cut to any shape and size with linear dimensions up to 1,000×1,750mm, to match the specific requirements of each application.  On request, the screens are also supplied in precision-cut strips as thin as 3-4 mm for coupling to linear diode arrays and mounted on a variety of substrates for easier handling and deployment.

Digital X-ray Imaging


Digital radiography (DR) is a one-step process where the x-ray signal is converted into an electrical signal, either directly, as in amorphous selenium (a-Se) based systems, or indirectly, as in the systems using a scintillator layer in combination with a photodetector. Thallium doped micro-columnar Caesium Iodide (CsI:Tl) and Gadox screens are the most common scintillators used in digital radiography. Caesium Iodide is generally the preferred choice in medical and dental applications, where the benefits offered by this structured scintillator (higher resolution and higher sensitivity, which translate into better image quality and lower x-ray doses to patient) offset its considerably higher cost. Gadox screens still retain the lion’s share in industrial applications, such as non-destructive testing (NDT) and end of line inspection (EOL), where pressure on costs is higher, but resolution and dose-efficiency requirements are generally lower than those in the medical industry. Scintacor can provide to their customers both, CsI:Tl plates and Gadox screens whilst advising on the best scintillator characteristics for each specific application. Caesium Iodide (CsI:Tl) is treated more in detail in a separate product page of the website.

Computed radiography (CR) is a two-step process where phosphor plates made in photo-stimulable phosphors (PSP), such as europium-doped barium flurochloride (BaFCl:Eu), are used to store energy upon X-ray exposure. CR is often used as a means of retrofitting analog x-ray systems by replacing the traditional film cassette with a CR-specific cassette, which contains the PSP plate and is exposed to x-rays in the usual way.  During the subsequent reading of the plate in a scanner, a focused laser beam triggers the release of the stored image data in the form of visible light. The emitted light is then detected and converted into a digital image with spatial information provided by the spot being excited by the laser. While Scintacor does not have standard CR offerings, the company has the expertise and equipment necessary to produce tailored photo-stimulable phosphor screens up to 1,000×1,750mm on demand.

Despite the significantly higher cost, DR systems have notably improved workflow vs. CR, as more images can be taken and processed in the same amount of time. Even more significant is that DR has at least twice the dose efficiency of CR or traditional film. This, in turn, results in lower doses to the patient and less exposure risk to the technicians.

General Considerations

For a given substrate, chemical composition and excitation conditions, three main parameters affect the performance of a phosphor screen, as well as the trade-off between light output and resolution. These are the coating thickness, the size of the phosphor particles and the packing density of the coating [4].

Increased thickness of the phosphor coating provides, in general, a higher conversion efficiency for the impinging x-rays into visible photons and this translates into a higher sensitivity and light output. There are nonetheless two caveats. Firstly, the resolution of the scintillator measured in line pairs per mm (lp/mm) will decrease with increased phosphor thickness, as the light is widely scattered within the phosphor layer. Secondly, the incremental gains of light output obtained for higher coating thicknesses will reduce until they will disappear altogether, due to the self-absorption of the visible photons within the phosphor layers. The interested reader can refer to the work of Busselt and Raue, who propose a linear correlation between geometric thickness of the phosphor layer and the width of the light spread function [5].

A smaller size of the phosphor particles results, in general, in a higher resolution but in a lower light output, as the light generated inside the phosphor particles can escape the volume of the particle in any directions and at an arbitrary point of its surface. On this basis, even for a single layer of phosphor particles, the smallest light emission spot approximately coincides with the phosphor particle size [6].

Finally, as a general trend, screens with a high packing density of particles have a better resolution but decreased brightness [7].

All this taken into account it should be remembered that the maximum brightness of the phosphor screen is ultimately limited by the quantum efficiency of the phosphor used. This is the reason why Scintacor intensifying screens are manufactured from highly controlled, premium-grade phosphors.

X-ray Screen Applications

Backscatter detectors

Due to their high sensitivity and fast decay time, Rapidex screens have been successfully used in back-scatter imaging systems, where the photons which are Compton scattered from the target object, rather than those attenuated by it, are used to generate the image [8].

In recent years backscatter detectors have found growing use in security applications, as this technique allows detection of organic materials, such as explosives or human tissue. It also enables the positioning of the detector side by side compactly with the x-ray source with clear operational advantages for the scanning of vehicles and other moving targets.

In this application high sensitivity is essential, as backscatter detectors operate at relatively low energies, when the Compton effect is the predominant method of interaction between photons and free electrons and the probability of scattering back an incident photon towards the origin is higher [9]. In addition, the energy of a scattered photon is always lower than the energy of the incident photon, hence the need of phosphor screens with high sensitivity such as the Rapidex range.

Fast decay time is also important, as backscatter system often operate according to a flying spot technique. Flying spot imaging was developed by American Science & Engineering (AS&E) in the 1970s to image moving objects [10]. In this technique, a thin pencil beam of radiation is created by a rotating collimation disc or “chopper wheel”. This pencil beam repeatedly scans a path creating a fan which is perpendicular to the direction of movement of the target object. The motion of the object is used to create the second dimension of the image [10]. Because the flying spot provides resolution in one dimension, and motion provides resolution in the other direction, the detector does not need to have any spatial resolution capability [10]. However, scintillator and detector must have high rate capability, to enable fast rastering speeds and quick image reconstruction. Rapidex screens with their fast decay time match this application well.

Dual energy detectors

In 1985 Gary Barnes, a professor at the University of Alabama, presented a dual energy detector that allowed the differentiation of soft and hard tissue with a single x-ray exposure [10]. Although this technique was developed to improve the interpretation of chest X-rays, it is now widely adopted in linear scanners for security imaging and end-of-line inspection.

In dual energy imaging systems, two radiation sensitive detectors are superimposed one behind the other. The front detector records and absorbs the low-energy photons, while transmitting the higher energy photons for detection in the thicker back detector. The two data sets are acquired simultaneously and provide information to image the density as in a normal radiograph and the atomic number of the target object [11] which is a considerable advantage.

Luminex and Rapidex screens, which can be precision-cut in strips according to the customers requirements, are the ideal scintillator choice for low energy detectors, due to their low costs, high uniformity between batches and possibility to match the screen resolution to the pixel pitch of the detector. Luminex are generally preferred for low frame rate applications, when light output and resolution are the main priorities. Rapidex are adopted, instead, for high frame rate application for end-of-line inspection up to speeds of a few meters per second.

Radiographic inspection of large-scale objects

X-ray and gamma radiography of large parts such as sculptures, historical objects, large engine blocks or rocket nozzles is straight forward with Luminex screens, which can be provided with linear dimensions up to 1,000×1,750mm and mounted on aluminium or other rigid substrates for ease of handling and deployment.

X-ray cabinets for postal screening

Cabinet x-ray scanners offer a compact and cost effective first line of defence against mail-delivered threats, without the operating costs and space requirements of a conveyor based X-ray system. The Luminex screens Ultrabright, Bright and Medium are relatively thick screens optimized for the lens coupled systems, such as cabinet x-ray scanners, which are generally light-starved but have lower resolution requirements than direct-coupled systems.

Ultra-high speed imaging

Due to their fast decay time, Rapidex screens can be coupled to ultra-fast cameras to image events which cannot be captured using normal x-ray imaging techniques. Applications include flash-radiography for industrial, scientific and defence research applications.


[1] G.C. Tyrrell, Phosphors and scintillators in radiation imaging detectors, Nuclear Instruments and Methods in Physics Research, A 546 (2005) 180–187
[2] L. Levy, D.W. West, Brit. J. Radiol, 87(8) (1935) 184
[3] K.A. Wickersheim, R.V. Alves, R.A. Buchanan, IEEE Trans. Nucl. Sci. NS-17 (1970) 57.
[4] R. Colbeth, Radiology in Small Doses: The Benefits of DR versus CR, http://www.diagnosticimaging.com, 2014
[5] W. Busselt, R. Raue, Optimizing the optical properties of TV phosphor screens, Journal Electrochemistry n. 135, pp 764-771 (1988)
[6] R. Kubrin, Nanophosor coatings: Technology and Applications, Opportunities and Challenges, Kona Powder and Particle Journal No. 31, pp 22-52 (2014)
[7] K.Y. Sasaki and J.B. Talbot, Deposition of Powder Phosphors for Information Displays, Adv, Mater, 11, pp 91-105 (1999)
[8] M. Cooper, X-Ray Compton Scattering, OUP Oxford, 2004
[9] J. B. Birks, The Theory and Practice of Scintillation Counting, MacMillan, New York, 1964
[10] American Science & Engineering Inc v Rapiscan Systems Ltd, All England Reporter [2016] EWHC 756 (Pat)
[11] V. Rebuffel, J. Dinten, Dual-Energy X-Ray Imaging: Benefits and Limits, Th.1.3.1, ECNDT 2006

Further readings

  • J.P. Creasey, G.C. Tyrrell, Proc. SPIE 3942 (2000) 114
  • M. Annis, P. J. Bjorkholm, X-ray imaging particularly adapted for low Z materials, US5313511, 1994
  • G. T. Barnes, Split energy level radiation detection, USRE37536 E1, 2002

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