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Ga2O3 is an ultra-wide-bandgap semiconductor that is receiving considerable attention due to its promising applications in high-frequency, high-power and high-temperature settings. It can be prepared by calcinating the α-GaOOH phase at high temperatures. Understanding the significance of hydroxyl groups in α-GaOOH, de­hydroxy­lation and the structural transition at high temperatures has become a key aspect of preparing high-quality α-Ga2O3 crystals, but the underlying mechanism remains unknown. In this research, α-GaOOH nanorods were hydro­thermally synthesized and the structural evolution of α-GaOOH investigated at high temperatures by in situ X-ray diffraction. The hydroxyl group in α-GaOOH squeezes Ga3+ from the center of the [GaO6] octahedron, resulting in deformed [GaO6] octahedra and significant microstrain in α-GaOOH. The hydroxyl groups are peeled off from α-GaOOH when the temperature exceeds 200°C, resulting in contraction along the c-axis direction and expansion along the a-axis direction of α-GaOOH. When the temperature exceeds 300°C, the Ga—O bond inside the double chains preferentially breaks to generate square-wave-like octahedron chains, and the neighboring chains repack to form hexagonal-like octahedron layers. The octahedron layers are packed up and down by electrostatic interaction to generate the α-Ga2O3 structure. This work highlights the role of hydroxyl groups in α-GaOOH, de­hydroxy­lation and the structural transition on the atomic scale, providing valuable guidelines for the fabrication of high-quality α-Ga2O3 crystals.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600576724000050/ui5002sup1.cif
Contains datablocks GaOOH_30, Ga2O3_500

Computing details top

(GaOOH_30) top
Crystal data top
GaHO2Z = 4
Mr = 102.73Dx = 5.194 Mg m3
Orthorhombic, PnmaCu Kα1, 2 radiation, λ = 1.54060, 1.54440 Å
Hall symbol: -P 2ac 2nT = 303 K
a = 9.78216 (15) ÅParticle morphology: nanorods
b = 2.97127 (4) ÅWhite
c = 4.51938 (11) Åflat_sheet, 20 × 20 mm
V = 131.36 (1) Å3Specimen preparation: Prepared at 303 K and 101 kPa
Data collection top
SmartLabXE
diffractometer
Scan method: continuous
Radiation source: rotating-anode X-ray tube, SmartLabXE2θmin = 10.040°, 2θmax = 120.040°, 2θstep = 0.020°
Data collection mode: reflection
Refinement top
Least-squares matrix: full22 parameters
Rp = 0.060H-atom parameters not refined
Rwp = 0.079
Rexp = 0.025(Δ/σ)max = 0.001
R(F2) = 0.04628Background function: Background function: "chebyschev-1" function with 6 terms: -18.3(20), 14(3), 29.0(31), -1.5(30), 1.0(25), 13.7(24),
5501 data pointsPreferred orientation correction: none
Profile function: Finger-Cox-Jephcoat function parameters U, V, W, X, Y, SH/L: peak variance(Gauss) = Utan(Th)2+Vtan(Th)+W: peak HW(Lorentz) = X/cos(Th)+Ytan(Th); SH/L = S/L+H/L U, V, W in (centideg)2, X & Y in centideg 34.645, -15.632, 21.741, 0.583, 0.091, 0.004,
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ga10.35560 (8)0.250000.55083 (15)0.0046*
O10.1927 (3)0.250000.3001 (7)0.0043*
O20.4437 (3)0.750000.3056 (7)0.0067*
H10.428000.750000.140000.0500*
Geometric parameters (Å, º) top
Ga1—O11.955 (3)O1—Ga1v1.923 (2)
Ga1—O1i1.923 (2)O1—Ga1vi1.923 (2)
Ga1—O1ii1.923 (2)O2—Ga12.044 (2)
Ga1—O2iii2.044 (2)O2—Ga1vii2.044 (2)
Ga1—O22.044 (2)O2—Ga1iv2.068 (3)
Ga1—O2iv2.068 (3)O2—H10.764
O1—Ga11.955 (3)H1—O20.764
O1i—Ga1—O1ii101.14 (15)Ga1v—O1—Ga1vi101.14 (15)
Symmetry codes: (i) x+1/2, y1/2, z+1/2; (ii) x+1/2, y+1/2, z+1/2; (iii) x, y1, z; (iv) x+1, y+1, z+1; (v) x+1/2, y1/2, z1/2; (vi) x+1/2, y+1/2, z1/2; (vii) x, y+1, z.
(Ga2O3_500) top
Crystal data top
Ga2O3Dx = 6.390 Mg m3
Mr = 187.44Cu Kα1, 2 radiation, λ = 1.54060, 1.54440 Å
Trigonal, R3cT = 773 K
Hall symbol: -R 3 2"cParticle morphology: nanorods
a = 4.9995 (2) Åwhite
c = 13.5010 (3) Åflat_sheet, 20 × 20 mm
V = 292.24 (2) Å3Specimen preparation: Prepared at 773 K and 101 kPa
Z = 6
Data collection top
SmartLabXE
diffractometer
Scan method: continuous
Radiation source: rotating-anode X-ray tube, SmartLabXE2θmin = 10.040°, 2θmax = 120.040°, 2θstep = 0.020°
Data collection mode: reflection
Refinement top
Least-squares matrix: fullProfile function: Finger-Cox-Jephcoat function parameters U, V, W, X, Y, SH/L: peak variance(Gauss) = Utan(Th)2+Vtan(Th)+W: peak HW(Lorentz) = X/cos(Th)+Ytan(Th); SH/L = S/L+H/L U, V, W in (centideg)2, X & Y in centideg 34.645, -15.632, 21.741, 0.583, 0.091, 0.004,
Rp = 0.05317 parameters
Rwp = 0.068
Rexp = 0.026(Δ/σ)max = 0.005
R(F2) = 0.06553Background function: Background function: "chebyschev-1" function with 6 terms: -8.1(15), -7.6(26), 14.6(23), 8.1(23), -3.8(20), 4.1(19), Background peak parameters: pos, int, sig, gam: 34.440, 2.13(6)e5, 28000.000, 0.100,
5501 data pointsPreferred orientation correction: none
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ga10.000000.000000.35596 (4)0.0060*
O10.3026 (6)0.000000.250000.0092*
Geometric parameters (Å, º) top
Ga1—O12.0821 (19)Ga1—O1v1.9309 (14)
Ga1—O1i2.0821 (19)O1—Ga12.0821 (19)
Ga1—O1ii2.0821 (19)O1—Ga1vi2.0821 (19)
Ga1—O1iii1.9309 (14)O1—Ga1vii1.9309 (14)
Ga1—O1iv1.9309 (14)O1—Ga1viii1.9309 (14)
O1iii—Ga1—O1iv103.28 (3)O1iv—Ga1—O1v103.28 (3)
O1iii—Ga1—O1v103.28 (3)Ga1vii—O1—Ga1viii118.53 (14)
Symmetry codes: (i) y, xy, z; (ii) yx, x, z; (iii) yx+1/3, y1/3, z+1/6; (iv) y+1/3, x+2/3, z+1/6; (v) x2/3, xy1/3, z+1/6; (vi) xy, y, z+1/2; (vii) yx+2/3, y+1/3, z1/6; (viii) x+1/3, y1/3, z+2/3.
 

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