TY - JOUR
T1 - Heterointerfaces of stable and metastable ZnO phases
AU - Ashrafi, Almamun
PY - 2008/12/30
Y1 - 2008/12/30
N2 - Thermodynamically ZnO is a prototype material which stabilizes with stable and metastable wurtzite and zincblende phases. In principle, the phase stability of ZnO depends on many parameters; however, heterointerface plays a significant role in controlling the ZnO crystalline structures. ZnO/SiC and ZnO/ZnS heterointerfaces have been studied where ZnO layers grow along the out-of-plane with an epitaxial relationship of (0 0 0 1) ZnO ∥(0 0 01) SiC , [ 1 1 over(2, ̄) 0 ] ZnO ∥ [ 1 1 over(2, ̄) 0 ] SiC and [1 1 0] ZnO ∥[1 1 0] GaAs , [ 1 over(1, ̄) 0 ] ZnO ∥ [ 1 over(1, ̄) 0 ] GaAs , respectively. Although both the ZnO phases grew uniaxially with the substrates, thin-interlayer and imbalanced charge distribution were observed in the ZnO/SiC heterointerfaces, while the ZnO/GaAs heterointerface was dominant with stacking faults and phase coexistence in lattice matrix, together with the common misfit-dislocations. Photoluminescence showed a significant bandgap energy difference in ZnO phases by ∼60 meV, and higher electron mobility in the zincblende ZnO material.
AB - Thermodynamically ZnO is a prototype material which stabilizes with stable and metastable wurtzite and zincblende phases. In principle, the phase stability of ZnO depends on many parameters; however, heterointerface plays a significant role in controlling the ZnO crystalline structures. ZnO/SiC and ZnO/ZnS heterointerfaces have been studied where ZnO layers grow along the out-of-plane with an epitaxial relationship of (0 0 0 1) ZnO ∥(0 0 01) SiC , [ 1 1 over(2, ̄) 0 ] ZnO ∥ [ 1 1 over(2, ̄) 0 ] SiC and [1 1 0] ZnO ∥[1 1 0] GaAs , [ 1 over(1, ̄) 0 ] ZnO ∥ [ 1 over(1, ̄) 0 ] GaAs , respectively. Although both the ZnO phases grew uniaxially with the substrates, thin-interlayer and imbalanced charge distribution were observed in the ZnO/SiC heterointerfaces, while the ZnO/GaAs heterointerface was dominant with stacking faults and phase coexistence in lattice matrix, together with the common misfit-dislocations. Photoluminescence showed a significant bandgap energy difference in ZnO phases by ∼60 meV, and higher electron mobility in the zincblende ZnO material.
KW - Heterointerfaces
KW - Photoluminescence and Hall measurements
KW - Stable and metastable phases
KW - ZnO
UR - http://www.scopus.com/inward/record.url?scp=56949091211&partnerID=8YFLogxK
U2 - 10.1016/j.apsusc.2008.07.103
DO - 10.1016/j.apsusc.2008.07.103
M3 - Article
SN - 0169-4332
VL - 255
SP - 2342
EP - 2346
JO - Applied Surface Science
JF - Applied Surface Science
IS - 5 PART 1
ER -