TY - JOUR
T1 - CsCdInQ3 (Q = Se, Te)
T2 - New photoconductive compounds as potential materials for hard radiation detection
AU - Li, Hao
AU - Malliakas, Christos D.
AU - Peters, John A.
AU - Liu, Zhifu
AU - Im, Jino
AU - Jin, Hosub
AU - Morris, Collin D.
AU - Zhao, Li Dong
AU - Wessels, Bruce W.
AU - Freeman, Arthur J.
AU - Kanatzidis, Mercouri G.
PY - 2013/5/28
Y1 - 2013/5/28
N2 - Two new compounds CsCdInQ3 (Q = Se, Te) have been synthesized using a polychalcogenide flux. CsCdInQ3 (Q = Se, Te) crystals are promising candidates for X-ray and γ-ray detection. The compounds crystallize in the monoclinic C2/c space group with a layered structure, which is related to the CsInQ2 (Q = Se, Te) ternary compounds. The cell parameters are: a = 11.708(2) Å, b = 11.712(2) Å, c = 23.051(5) Å, β = 97.28(3) for CsCdInSe3 and a = 12.523(3) Å, b = 12.517(3) Å, c = 24.441(5) Å, β = 97.38(3) for CsCdInTe 3. Both the Se and Te analogues are wide-band-gap semiconductors with optical band gaps of 2.4 and 1.78 eV for CsCdInSe3 and CsCdInTe 3, respectively. High-purity polycrystalline raw material for crystal growth was synthesized by the vapor transfer method for CsCdInQ3. Large single crystals up to 1 cm have been grown using the vertical Bridgman method and exhibit photoconductive response. The electrical resistivity of the crystals is highly anisotropic. The electronic structure calculation within the density functional theory (DFT) framework indicates a small effective mass for the carriers. Photoconductivity measurements on the as grown CsCdInQ3 crystals gives high carrier mobility-lifetime (μτ) products comparable to other detector materials such as α-HgI2, PbI2, and CdxZn1-xTe (CZT).
AB - Two new compounds CsCdInQ3 (Q = Se, Te) have been synthesized using a polychalcogenide flux. CsCdInQ3 (Q = Se, Te) crystals are promising candidates for X-ray and γ-ray detection. The compounds crystallize in the monoclinic C2/c space group with a layered structure, which is related to the CsInQ2 (Q = Se, Te) ternary compounds. The cell parameters are: a = 11.708(2) Å, b = 11.712(2) Å, c = 23.051(5) Å, β = 97.28(3) for CsCdInSe3 and a = 12.523(3) Å, b = 12.517(3) Å, c = 24.441(5) Å, β = 97.38(3) for CsCdInTe 3. Both the Se and Te analogues are wide-band-gap semiconductors with optical band gaps of 2.4 and 1.78 eV for CsCdInSe3 and CsCdInTe 3, respectively. High-purity polycrystalline raw material for crystal growth was synthesized by the vapor transfer method for CsCdInQ3. Large single crystals up to 1 cm have been grown using the vertical Bridgman method and exhibit photoconductive response. The electrical resistivity of the crystals is highly anisotropic. The electronic structure calculation within the density functional theory (DFT) framework indicates a small effective mass for the carriers. Photoconductivity measurements on the as grown CsCdInQ3 crystals gives high carrier mobility-lifetime (μτ) products comparable to other detector materials such as α-HgI2, PbI2, and CdxZn1-xTe (CZT).
KW - chalcogenide
KW - crystal growth
KW - hard radiation detection
KW - photoconductivity
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U2 - 10.1021/cm400634v
DO - 10.1021/cm400634v
M3 - Article
AN - SCOPUS:84878286999
SN - 0897-4756
VL - 25
SP - 2089
EP - 2099
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 10
ER -