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:
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.