The chamber in which X-ray scintillator layers are grown · effusion cells for caesium iodide and thallium iodide, a heated rotating substrate holder, and the pressure and temperature that decide whether the layer grows as light-guiding columns
A caesium iodide scintillator converts X-rays into visible light that a silicon sensor can read, and when it is grown as fine columns those columns guide the light straight down instead of letting it spread. The columns are made in a vacuum chamber: CsI and a thallium dopant are evaporated from heated cells, and the vapour condenses on a heated, rotating substrate above. The chamber's pressure, the substrate temperature, the source arrangement and the deposition rate together decide the layer's structure, its thallium content and so its brightness and sharpness.
Vacuum chambers and their in-chamber equipment used to grow thallium-doped caesium iodide (CsI:Tl) scintillator layers by thermal evaporation for X-ray imaging detectors: effusion cells or boats for CsI and thallium iodide, heated and rotating substrate holders, pressure control with inert gas, and post-deposition heat treatment. General-purpose process and test chambers, their materials, outgassing and leak testing are covered on the Vacuum chamber page; the welded chamber shell and flanges on the Vacuum chamber body page; door hinges on the Vacuum chamber door hinge system page; steel degassing tanks on the Degassing chamber for liquid steel page; and optical coating chambers on the Optical lens vacuum coating chamber page.
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Three groups report the chamber conditions they used; the first shows the pressure itself switching the structure between columns and a dense layer.
Editorial calculation: 10⁻² Torr is about 1.3 Pa and 10⁻⁵ Torr about 1.3 × 10⁻³ Pa, so the NanoFocusRay and KAIST comparison spans three decades of pressure; BINP's 5·10⁻³ Pa (about 4 × 10⁻⁵ Torr) lies between the two. [1] [3] At BINP's 17 Å/s, a layer grows about 6.1 µm per hour, so its 14 µm film needed roughly 2.3 hours; the same rate would need about 38 hours for the 230 µm screens the IHEP group tested, which shows why the deposition rate is a design figure for a production chamber. [3] [4]
The chamber therefore needs a way to hold the chosen pressure during evaporation, not only to reach base pressure: the KAIST group controlled process pressure by injecting argon. [2]
| Chamber and source | Pressure | Substrate | Geometry and rate | Result reported |
|---|---|---|---|---|
| NanoFocusRay / KAIST, two effusion cells | 10⁻² Torr and 10⁻⁵ Torr compared [1] | About 150 °C, heated by a coil in the holder; rotating [1] | Holder 200 mm above the cells; CsI charge 100 to 300 g [1] | Columnar (needle) structure at 10⁻² Torr; dense structure with some cracks at 10⁻⁵ Torr; higher light output at 10⁻⁵ Torr [1] |
| KAIST, glass substrate | 4×10⁻⁶ torr, controlled by argon injection [2] | 250 °C [2] | — | Polycrystalline layer; thallium concentrated at the substrate interface after deposition [2] |
| BINP (CERN proceedings), tantalum boat | 5·10⁻³ Pa [3] | 25 °C, following the Thornton zone model [3] | Rotated disk 65 cm from the boat; boat at 680 °C; 17 ± 2 Å/s [3] | 2 to 14 µm films; grain size about 3 ± 2 µm [3] |
State the layer thickness and structure required (columnar or dense), the substrate size and material, the base and process pressure, the substrate temperature range and the target deposition rate.
02
The dopant evaporates more readily than the host, which shapes how the sources inside the chamber are laid out.
Editorial note: when a single boat holds both materials, the thallium content falls as the run goes on (BINP's 80 % figure at 8 µm). Separate, independently heated cells, or a step-wise process, are the two answers the sources describe. [3] [1]
| Finding | Value | Source |
|---|---|---|
| Melting points | CsI 660 °C; TlI 440 °C; for a simple evaporation process the KAIST group writes that “Most of TlI particles are supposed to be evaporated before CsI powder melts” | [2] |
| Two-cell layout | Two effusion cells on opposite sides of the chamber, run at different temperatures to set the Tl:CsI ratio | [1] |
| Thallium loss with thickness | Tl density in an 8 µm film is 80 % of that in a 2 µm film; Tl sufficient only below 10 µm, so thicker layers need serial, step-by-step deposition | [3] |
| Doping levels used | About 0.08 mol% (BINP); 0.3 to 1 mol% (NanoFocusRay/KAIST); 0.1 % and 20 % test samples (KAIST) | [3] [1] [2] |
| Effect of doping | 0.3 mol% gave the highest image contrast and 1 mol% the highest resolution; lower Tl and larger CsI charge gave the highest light output | [1] |
Specify the number of sources, their maximum temperature and control, the target Tl concentration and how it will be held through the layer thickness.
03
What happens in or after the chamber also sets the finished screen's performance.
Editorial calculation: on graphite, tripling the thickness from 70 to 230 µm (3.3 times) raised relative light output 4.3 times, while on fibre optic plate the same change raised it about 1.9 times (8.7 ÷ 4.6). [4] Substrate and thickness are therefore part of the chamber specification, because the holder has to carry the chosen substrate at the chosen temperature for the hours a thick layer takes.
The image above shows a horizontal cylindrical chamber with its door open and a rack of coated panels inside, an arrangement for batch processing of flat substrates.
| Step or choice | Reported value |
|---|---|
| Heat treatment window | 250 to 400 °C for 2 h 30 min [1] |
| Thallium redistribution | 250 °C for 0, 10, 100 and 200 h; the authors call 200 h “promising a measure of uniform concentration of thallium”, and a 0.1 % Tl sample after 200 h gave about 40 % of the light intensity of a single crystal [2] |
| Thickness and light output | On graphite, relative light output 1, 2.8 and 4.3 at 70, 150 and 230 µm; on fibre optic plate 4.6, 7.4 and 8.7 [4] |
| Thickness and resolution | MTF falls as the CsI:Tl layer gets thicker [1] [3] |
| Substrate | Graphite gave the darkest image but higher MTF and NEQ; fibre optic plate the brightest image with the lowest MTF; silver-coated silica raised light output over plain silica [4] |
Give the substrate type (glass, graphite, fibre optic plate, sensor panel), its size and heat limit, and whether the post-deposition anneal is done in the same chamber or a separate oven.
04
Paste it into your enquiry below or into an email to a maker, then replace every bracket.
Layer: [thickness µm; columnar or dense; Tl mol%] Substrate: [material; size; max temperature] Pressure: [base; process; inert gas control] Sources: [number of cells; max temperature; CsI charge g] Holder: [heating range; rotation; distance to source] Rate: [Å/s or µm/h] Post-treatment: [anneal °C and hours; in situ or separate]
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NanoFocusRay and KAIST obtained needle-shaped columns at 10⁻² Torr with a 150 °C substrate, and a dense structure with cracks at 10⁻⁵ Torr. [1]
Sources checked 2026-10-13. Four research reports from three publishers: two Korean Nuclear Society conference papers (NanoFocusRay with KAIST, 2011; KAIST), the Budker Institute's paper in the CERN proceedings (2017), and the Institute of High Energy Physics paper on CsI(Tl) substrates (arXiv).
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