We report on the scintillation properties of Cs2HfCl6 (cesium hafnium chloride or CHC) as an example of a little-known class of non-hygroscopic compounds having the generic cubic crystal structure of K2PtCl6. The crystals are easily growable from the melt using the Bridgman method with minimal precursor treatments or purification. CHC scintillation is centered at 400 nm, with a principal decay time of 4.37 μs and a light yield of up to 54 000 photons/MeV when measured using a silicon CCD photodetector. The light yield is the highest ever reported for an undoped crystal, and CHC also exhibits excellent light yield nonproportionality. These desirable properties allowed us to build and test CHC gamma-ray spectrometers providing energy resolution of 3.3% at 662 keV.

No abstract

No abstract

To answer the title question -the technology and properties of the (Cd,Mn)Te crystals is discussed as compared with those of the more commonly used (Cd,Zn)Te crystals. The composition homogeneity of the large single crystals of the ternary compound seems to be easier to achieve in the case of (Cd,Mn)Te because the segregation coefficient of Mn in CdTe is negligible with respect to that (approx. 1.3) of Zn. Only 15% of MnTe has to be added to CdTe to reach the best for the detector application value of the energy gap (in the range 1.7 -2.2 eV), while the necessary amount of ZnTe is over 30%! This is because the composition dependence of the CdTe energy gap is for Mn twice as strong as for Zn. Using a smaller amount of the second cation diminishes many alloying-related problems. Dopant-free as grown (Cd,Mn)Te crystals are of p-type, which is related to the Cd vacancies acting as acceptors. The number of vacancies can be reduced by the post-growth annealing in the Cd vapours and the high (~ 10 10 Ωcm ) resistivity, required for good detectors, can be obtained by doping with donors. The technology of the (Cd,Mn)Te crystals, undoped and compensated in the very large range of concentrations, and Cdannealing of the samples is discussed. Characterization of the obtained crystals is described. The behaviour of the preliminary detectors is shown.