Caesium iodide
Chemical compound From Wikipedia, the free encyclopedia
Caesium iodide or cesium iodide (chemical formula CsI) is the ionic compound of caesium and iodine. It is often used as the input phosphor of an X-ray image intensifier tube found in fluoroscopy equipment. Caesium iodide photocathodes are highly efficient at extreme ultraviolet wavelengths.[7]
CsI crystal | |
Scintillating CsI crystal | |
Crystal structure | |
Names | |
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IUPAC name
Caesium iodide | |
Other names
Cesium iodide | |
Identifiers | |
3D model (JSmol) |
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ChemSpider | |
ECHA InfoCard | 100.029.223 |
EC Number |
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PubChem CID |
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RTECS number |
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UNII | |
CompTox Dashboard (EPA) |
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Properties | |
CsI | |
Molar mass | 259.809 g/mol[2] |
Appearance | white crystalline solid |
Density | 4.51 g/cm3[2] |
Melting point | 632 °C (1,170 °F; 905 K)[2] |
Boiling point | 1,280 °C (2,340 °F; 1,550 K)[2] |
848 g/L (25 °C)[2] | |
−82.6·10−6 cm3/mol[3] | |
Refractive index (nD) |
1.9790 (0.3 µm) 1.7873 (0.59 µm) 1.7694 (0.75 µm) 1.7576 (1 µm) 1.7428 (5 µm) 1.7280 (20 µm)[4] |
Structure | |
CsCl, cP2 | |
Pm3m, No. 221[5] | |
a = 0.4503 nm | |
Lattice volume (V) |
0.0913 nm3 |
Formula units (Z) |
1 |
Cubic (Cs+) Cubic (I−) | |
Thermochemistry | |
Heat capacity (C) |
52.8 J/mol·K[6] |
Std molar entropy (S⦵298) |
123.1 J/mol·K[6] |
Std enthalpy of formation (ΔfH⦵298) |
−346.6 kJ/mol[6] |
Gibbs free energy (ΔfG⦵) |
−340.6 kJ/mol[6] |
Hazards | |
GHS labelling: | |
Warning | |
H315, H317, H319, H335 | |
P201, P202, P261, P264, P270, P271, P272, P273, P280, P281, P301+P312, P302+P352, P304+P340, P305+P351+P338, P308+P313, P312, P321, P330, P332+P313, P333+P313, P337+P313, P362, P363, P391, P403+P233, P405, P501 | |
Flash point | Non-flammable |
Lethal dose or concentration (LD, LC): | |
LD50 (median dose) |
2386 mg/kg (oral, rat)[1] |
Related compounds | |
Other anions |
Caesium fluoride Caesium chloride Caesium bromide Caesium astatide |
Other cations |
Lithium iodide Sodium iodide Potassium iodide Rubidium iodide Francium iodide |
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
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Synthesis and structure
Bulk caesium iodide crystals have the cubic CsCl crystal structure, but the structure type of nanometer-thin CsI films depends on the substrate material – it is CsCl for mica and NaCl for LiF, NaBr and NaCl substrates.[9]
Caesium iodide atomic chains can be grown inside double-wall carbon nanotubes. In such chains I atoms appear brighter than Cs atoms in electron micrographs despite having a smaller mass. This difference was explained by the charge difference between Cs atoms (positive), inner nanotube walls (negative) and I atoms (negative). As a result, Cs atoms are attracted to the walls and vibrate more strongly than I atoms, which are pushed toward the nanotube axis.[8]
Properties
Т (°C) | 0 | 10 | 20 | 25 | 30 | 40 | 50 | 60 | 70 | 80 | 90 | 100 |
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S (wt%) | 30.9 | 37.2 | 43.2 | 45.9 | 48.6 | 53.3 | 57.3 | 60.7 | 63.6 | 65.9 | 67.7 | 69.2 |
Applications
An important application of caesium iodide crystals, which are scintillators, is electromagnetic calorimetry in experimental particle physics. Pure CsI is a fast and dense scintillating material with relatively low light yield that increases significantly with cooling,[11] and a fairly small Molière radius is 3.5 cm. It exhibits two main emission components: one in the near ultraviolet region at the wavelength of 310 nm and one at 460 nm. The drawbacks of CsI are a high temperature gradient and a slight hygroscopicity.
Caesium iodide is used as a beamsplitter in Fourier transform infrared (FTIR) spectrometers. It has a wider transmission range than the more common potassium bromide beamsplitters, working range into the far infrared. However, optical-quality CsI crystals are very soft and hard to cleave or polish. They should also be coated (typically with germanium) and stored in a desiccator, to minimize interaction with atmospheric water vapors.[12]
In addition to image intensifier input phosphors, caesium iodide is often also used in medicine as the scintillating material in flat panel x-ray detectors.[13]
References
Cited sources
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