CHEN Jian-gang, GUO Chang-xin, ZHANG Lin-li, HU Jun-tao, GUO Peng. Crystal Growth and Luminescent Properties of ZnO Sub-microrods and Microrods[J]. Chinese Journal of Luminescence, 2005,26(1): 83-88
CHEN Jian-gang, GUO Chang-xin, ZHANG Lin-li, HU Jun-tao, GUO Peng. Crystal Growth and Luminescent Properties of ZnO Sub-microrods and Microrods[J]. Chinese Journal of Luminescence, 2005,26(1): 83-88DOI:
Crystal Growth and Luminescent Properties of ZnO Sub-microrods and Microrods
Various size ZnO hexagonal microrods have been synthesized onto glass substrates through aqueous growth method with the thermal decomposition of an aqueous solution of equimolar zinc nitrate Zn(NO
3
)
2
·(4H
2
O) and methenamine ((CH
2
)
6
N
4
) by controlling the experimental conditions. The ZnO microrods grow from one center to form radial clusters
which consist of more than 2 pair rods symmetrically grown from the center to both sides
and the rods have a flat top end perpendicularly. When the growth time reached two days
we found that the microrods turned into hollow microtubes with the tube-thickness of tenth of diameter. XRD patterns
SEM images
Raman spectrum have been measured
which revealed all samples were hexa-gonal microrods of ZnO with length of 5~6μm and diameter of 0.8~5μm. The Raman spectrum showed four peaks at 332.2
377.6
435.4 and 577.8 cm
-1
assigned to the 2E
2
A
1
E
2
and E
1
(LO)modes
respectively. The growth mechanism is discussed
Zn(NO
3
)
2
dissolves and forms growth units of tetrahedron Zn-(OH)
4
under the reaction of the surface activator (CH
2
)
6
N
4
then the incorporation of growth units leads to the formation of the ZnO crystal lattice at the interface through a dehydration reaction (OH
-
+OH
-
H
2
O+)O
2-
. The fastest of the growth velocity along [0001] direction leads to the formation of the ZnO microrods. The excitation spectra showed that except the intrinsic inter-band excitation of shorter than 370nm
there was a strong exciton excitation peak located at 387nm with FWHM 30nm at room temperature. The photoluminescent spectra showed that there was a wide orange-red emission with peak at 630 nm and FWHM 250nm when the excitaion wavelength at 387nm. The cathodoluminescent spectra showed a strong orange emission peak at 580nm with FWHM 140nm and a weak UV emission peak at 395nm with FWHM 20nm. Compared with the calculated data of these intrinsic defects by the literature with the theory of FP-LMTO
we attribute the orangered and red emission to the luminescent transition from oxygen vacancies to the valence band.