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Nanostructured CdSe Films in Low Size-Quantization Regime: Temperature Dependence of the Band Gap Energy and Sub-Band Gap Absorption Tails

机译:纳米结构化的CdSe薄膜在低尺寸定量体系中的研究:带隙能量和亚带隙吸收尾巴的温度依赖性

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Temperature dependence of the band gap energy and sub-band gap absorption tails in 3D assemblies of close packed weakly quantized CdSe quantum dots deposited as thin films was studied. The range from cryogenic temperatures (~10 K) up to 340 K was covered. Excitonic absorption peaks were not observed even at temperatures as low as 11 K, which was attributed to the finite particle size distribution and interdot electronic couphng effects. The temperature coefficient of the band gap energy of the nanostructured fihnsof9.4 x 10~(-4) eV K~(-1) ishigherbyafactorof 1.35 than the correspondingvalueforthe bulk CdSespecimen.Ascompared to the case offilms constituted of strongly quantized ZnSe QDs, where the factor α_(nanocrystal)/α_(bulk) was found to be 1.82 (Pejova, B.; Abay, B.; Bineva, I. /. Phys. Chem. C 2011, 115, 37), the present findings imply that this ratio increases upon enhancement of size quantization effects in semiconductor nanocrystals. Analysis of the temperature-dependent optical absorption data within the Bose-Einstein model implies that no phonon confinement effects influence the phonon spectrum in the presently studied material due to the very small size-quantization effects. This situation is opposite to what we have recently found in the case of 3D arrays of strongly quantized ZnSe films. The characteristic Einstein temperature of the presently studied material corresponds to phonon frequency of about 220 cm" , in excellent agreement with the LO mode frequency of bulk CdSe (210-214cm~(-1)). It is demonstrated that the Urbach rule is vahd in the presently studied nanostructured material in low size-quantization regime. Urbach energies are several times higher than the values characteristic for macrocrystalline materials, due to the relatively high degree of inherent structural disorder in the studied QD sohds. At the same time, however, these values are approximately three times smaller than those reported for strongly quantized ZnSe films in our previous study. The dynamical (temperature-dependent) term accounts for only about 22% of the overall Urbach energy values, though this value is higher than the corresponding ratio in the case of strongly quantized ZnSe films.
机译:研究了紧密堆积的弱量化CdSe量子点的3D组件中薄膜沉积时带隙能量和子带隙吸收尾的温度依赖性。涵盖了从低温(〜10 K)到340 K的范围。即使在低至11 K的温度下也未观察到激子吸收峰,这归因于有限的粒度分布和点间电子耦合效应。 9.4 x 10〜(-4)eV K〜(-1)纳米结构薄膜的带隙能的温度系数比Cd样品的相应值高1.35倍。发现因子α_(纳米晶体)/α_(本体)为1.82(Pejova,B .; Abay,B .; Bineva,I./.Phys.Chem.C 2011,115,37),目前的发现暗示当增强半导体纳米晶体中的尺寸量化效果时,该比率增加。对Bose-Einstein模型中与温度相关的光吸收数据的分析表明,由于很小的尺寸量化效应,没有声子限制效应影响当前研究材料中的声子光谱。这种情况与我们最近在强量化ZnSe膜的3D阵列中发现的情况相反。目前研究材料的特征爱因斯坦温度对应于约220 cm“的声子频率,与整体CdSe的LO模频率(210-214cm〜(-1))高度吻合。证明了Urbach律是vahd在目前研究的纳米结构材料的低尺寸量化方案中,由于所研究的量子点中固有的结构无序程度较高,因此Urbach能量比大晶材料的特征值高几倍。这些值大约比我们先前研究中报道的强量化ZnSe薄膜小三倍,动力学(取决于温度)项仅占Urbach能量总值的22%,尽管该值高于相应的比率对于高度定量的ZnSe薄膜。

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