TY - JOUR
T1 - High temperature phases with wurtzite-derived structure in Zn2LiGaO4–ZnO alloy system
AU - Kita, Masao
AU - Fukada, Tomoaki
AU - Yamaguchi, Shu
AU - Omata, Takahisa
N1 - Funding Information:
This work was partially supported by the First Bank of Toyama Scholarship Foundation.
Publisher Copyright:
© 2016 Elsevier B.V.
PY - 2016
Y1 - 2016
N2 - We investigated the structural phase transformations of Zn2LiGaO4, which is a quaternary oxide semiconductor with a wide band gap of 4.0 eV, and its alloys with ZnO by using in-situ high-temperature X-ray diffraction (XRD), room-temperature XRD and selected-area electron diffraction of samples quenched from high temperatures of >873 K. Three types of phases with the wurtzite-derived structure were found in the y(Zn2LiGaO4)1/4–(1−y)ZnO alloy system. First is the low-temperature phase, phase I, in which constituent cations are ordered similarly to those in a Cd2AgGaS4-type structure. Phase I has an incommensurate modulation vector of 1.04b* and is stable at <1070 K and compositions of 0.96 ≤ y ≤ 1 and is stable at room temperature for y = 0.92. The second phase, phase II, appears at intermediate temperatures of 773–1373 K at 0.96 ≤ y ≤ 1, and its incommensurate modulation vector is 1.08b*. Phase III, which has no long-range cation ordering but still has short-range cation ordering, is stable for 0.92 ≤ y ≤ 1 at high temperatures and for 0.2 ≤ y < 0.92 from room temperature to high temperatures. We discuss the driving force of the transformations among the three phases in terms of their crystal structure and the mismatch in thermal expansion between –Zn–O–Zn–O– and –Li–O–Ga–O– linkages.
AB - We investigated the structural phase transformations of Zn2LiGaO4, which is a quaternary oxide semiconductor with a wide band gap of 4.0 eV, and its alloys with ZnO by using in-situ high-temperature X-ray diffraction (XRD), room-temperature XRD and selected-area electron diffraction of samples quenched from high temperatures of >873 K. Three types of phases with the wurtzite-derived structure were found in the y(Zn2LiGaO4)1/4–(1−y)ZnO alloy system. First is the low-temperature phase, phase I, in which constituent cations are ordered similarly to those in a Cd2AgGaS4-type structure. Phase I has an incommensurate modulation vector of 1.04b* and is stable at <1070 K and compositions of 0.96 ≤ y ≤ 1 and is stable at room temperature for y = 0.92. The second phase, phase II, appears at intermediate temperatures of 773–1373 K at 0.96 ≤ y ≤ 1, and its incommensurate modulation vector is 1.08b*. Phase III, which has no long-range cation ordering but still has short-range cation ordering, is stable for 0.92 ≤ y ≤ 1 at high temperatures and for 0.2 ≤ y < 0.92 from room temperature to high temperatures. We discuss the driving force of the transformations among the three phases in terms of their crystal structure and the mismatch in thermal expansion between –Zn–O–Zn–O– and –Li–O–Ga–O– linkages.
KW - Incommensurate modulation
KW - Phase transformation
KW - Thermal expansion
KW - Wurtzite-derived structure
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U2 - 10.1016/j.jallcom.2016.06.249
DO - 10.1016/j.jallcom.2016.06.249
M3 - Article
AN - SCOPUS:84978898064
SN - 0925-8388
VL - 688
SP - 69
EP - 76
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
ER -