透射峰频率依赖于缺陷层的位置。
The frequency of the defect models depends on the positions of the defects.
在缺陷模频率处存在尖锐的共振透射峰。
The resonant transmission occurs at the frequency of the defect models.
随着偏压的增大，透射峰位置向低能量区域移动。
The transmission peaks of high_energy electron are moved toward low_energy ranges with the increasing of the bias voltage.
随着结构阵列的增加，透射峰与禁带都有加强的趋势。
The transmission peaks and forbidden band gaps increase with increase of the structure arrays.
用数学归纳法得到了简单的迭代关系式用以计算多个完全透射峰的频率。
A simple recursion relation is derived by means of the mathematical induction to calculate the frequencies of the complete transmission peaks.
特窄的子能带，与透射谱中尖锐的透射峰相对应，其布洛赫光学模具有强局域的特点。
The narrow bands shows a very sharp peak in the transmission spectra and the corresponding photon Bloch modes are strongly localized.
谐振波长随温度和轴向应变线性变化，透射峰幅值随轴向应变线性减小但对温度不敏感。
The amplitude of the loss peak decreases linearly with axial strain, whereas, it is hardly affected by temperature change.
研究发现：一维双周期光子晶体的光子带隙结构中在两光子晶体带隙交叠处具有很明显的两共振透射峰。
The investigation results show that two transmittance peaks exist at the crossover of the two photonic crystal PBG in 1-d dual-periodical photonic crystal.
研究结果表明：一维右手材料和左手材料构成的光子晶体具有宽禁带的特点，禁带中出现多个共振透射峰。
The investigation results show that the band gap of the photonic crystal made of LHM is wide and multi-transmittance peaks appear in the forbidden band.
由于缺陷的存在，使得光子晶体的透射谱中产生缺陷峰。
Because of the defect, the defect peak appears in the transmission spectra.
通过对酒精透射光谱和吸收光谱的研究发现，其特征吸收峰随浓度不同发生漂移，从分子结构能级角度对其做了定性解释；
The transmission spectrum and the absorption spectrum of alcohol shows that the characteristic absorption peak shifts with alcoholicity due to the molecular configuration.
通过实验给出了三元组合双折射滤光片的透射曲线，其透射光谱带宽较窄，次峰被抑制在10%以下。
The transmission curve of birefringent filter is given experimentally. Its transmission bandwidth is very narrow and all the sub-peaks are suppressed fewer than 10%.
通过实验给出了三元组合双折射滤光片的透射曲线，其透射光谱带宽较窄，次峰被抑制在10%以下。
The transmission curve of birefringent filter is given experimentally. Its transmission bandwidth is very narrow and all the sub-peaks are suppressed fewer than 10%.
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