激光脉宽对谐波频移和振幅强度的影响

数值研究了激光脉宽对H_2~+和T_2~+谐波辐射的影响.计算结果表明:(i)对于谐波频移现象:在少周期激光场下,H_2~+和T_2~+谐波辐射呈现红移.随着激光脉宽增大,H_2~+谐波辐射呈现蓝移; T_2~+谐波辐射红移减弱.(ii)对于谐波振幅强度:H_2~+和T_2~+谐波辐射强度会随着激光脉宽增大而增强.但是,在少周期激光场下,H_2~+谐波截至能量附近的强度要大于T_2~+.在多周期激光场下,T_2~+谐波截至能量附近的强度要大于H_2~+.     

基于小波神经网络的振动速度传感器幅频特性补偿研究

为了实现超低频振动速度测量, 提出补偿其幅频特性的小波神经网络方法.该方法以振动速度传感器动态实验数据为基础, 通过小波神经网络训练来确定传感器幅频特性补偿网络.介绍振动速度传感器幅频特性补偿原理, 分析网络的拓扑结构, 给出网络参数训练和初始化方法.采用引入动量项的最速下降法训练网络权值、尺度因子和平移因子, 将小波网络参数的初始化与小波类型、小波时频参数和学习样本等联系起来.结果表明, 采用小波神经网络进行振动速度传感器幅频特性补偿具有良好的鲁棒性,并能实现在线补偿,网络训练的速度和精度优于同等规模的BP网络,在测试领域有重要的实用价值. 关键词： 振动速度传感器 小波神经网络 幅频特性 补偿     

频率调制强吸收光谱中残余幅度调制的理论分析

由电光调制器(EOM)中双折射效应及线偏光不完全沿EOM调制方向诱发的残余幅度调制(RAM)使频率调制(FM)光谱技术在微量气体检测中的应用受到极大的限制。基于光场与晶体相互作用及光学干涉原理推导出存在RAM时FM光谱的线型表达式,确定出输入线偏光角度、EOM中双折射效应、FM系数等是影响线型的主要因素,且当入射EOM光的偏振角度偏离调制方向越大,双折射效应引起的特征偏振方向相位差越大,线型扭曲越严重;同时在FM色散光谱中存在一个受两者影响的直流偏置;最后给出通过伺服控制这两过程可以达到抑制RAM的目的。这些现象及线型的分析将为基于光纤器件的FM光谱提供必要的理论支持。     

Spectral reflectance characteristics of different snow and snow-covered land surface objects and mixed spectrum fitting

The field spectroradiometer was used to measure spectra of different snow and snow-covered land surface objects in Beijing area.The result showed that for a pure snow spectrum,the snow reflectance peaks appeared from visible to 800 nm band locations;there was an obvious absorption valley of snow spectrum near 1 030 nm wavelength.Compared with fresh snow,the reflection peaks of the old snow and melting snow showed different degrees of decline in the ranges of 300～1 300,1 700～1 800 and 2 200～2 300 nm,the lowe...     

荷控忆阻器等效电路分析模型及其电路特性研究

忆阻器是物理上新实现的具有记忆特性的基本二端电路元件. 根据φ-q关系式的泰勒级数形式构建了荷控忆阻器等效电路分析模型, 以三次非线性荷控忆阻器模型为例, 对不同参数条件下的荷控忆阻器进行了伏安关系、有无源性等电路特性的理论分析. 结果表明: 荷控忆阻器的伏安关系具有斜体“8”字形紧磁滞回线特性, 随其参数符号的不同, 荷控忆阻器呈现出无源性和有源性, 导致其电路特性发生相应的变化; 相比无源荷控忆阻器, 有源荷控忆阻器更适用于作为二次谐波信号产生电路使用. 制作了荷控忆阻器特性分析等效电路的实验电路, 实验测量结果很好地验证了理论分析结果. 关键词： 荷控忆阻器 等效电路 伏安关系 电路特性     

A nonlinear constitutive audio frequency magneto-sensitive rubber model including amplitude, frequency and magnetic field dependence

A novel constitutive model of magneto-sensitive rubber in the audible frequency range is presented. Characteristics inherent to magneto-sensitive rubber within this dynamic regime are defined: magnetic sensitivity, amplitude dependence, elasticity and viscoelasticity. Prior to creating the model assumptions based on experimental observations concerning these components are formulated. The first observation is that not only does the rubber display a strong amplitude dependence even for small strains, but also the magnetic sensitivity is strongly amplitude dependent. The second and third are, respectively, that the elastic component is magneto-sensitive, whereas the viscoelastic dependence on magnetic induction appears to be small. Thus, the model is developed from these assumptions and parameters are optimized with respect to experimental values for one case and subsequently validated for others; a very good agreement is obtained.     

皮肤组织容积脉搏波400~1000 nm光谱特性仿真研究

根据皮肤组织解剖结构特性建立了六层层状模型,并给出了皮肤组织各层的特性参数;考虑了氧合血红蛋白和还原血红蛋白的吸收特性,依据皮肤组织各层的水、血、脂肪、血氧饱和度含量以及血管大小给出了皮肤组织各层的光谱吸收系数;对不同波长散射系数做了适当简化,给出了皮肤组织各层的光谱散射系数。利用蒙特卡罗方法仿真血管组织在收缩与舒张两种状态下, 400~1 000 nm波长光在皮肤组织多层模型中的传输过程,并通过统计大量光子的分布特性,获得了皮肤组织光谱反射系数,并利用模拟所得的两种状态下的反射系数计算得到了光谱容积脉搏波幅度。仿真结果表明,当入射光强一定时,绿光的容积脉搏波幅度优于红光和蓝光。通过计算不同波长光沿皮肤组织深度方向光能流率衰减为1/e时对应的皮肤组织深度,获得了皮肤组织光谱穿透深度。结果显示,血管舒张状态下蓝光和绿光的穿透深度较小,蓝光大部分只能达到表皮层,绿光能到达微循环层,红光可直达真皮层。考虑到光在皮肤组织中传播包含了一个从收缩到舒张的动态过程,基于此,根据穿透深度定义了脉搏波信号产生深度,利用血管舒张与收缩两种不同状态下的穿透深度计算得到了光谱产生深度。结果表明,不同波长光产生深度大于其穿透深度,蓝光产生深度较浅,且其受到的血液吸收调制较小,因而其获得的脉搏信号易受噪声干扰;红光的容积脉搏波产生深度较大,但是相比于绿光其受血液吸收调制较小,且绿光产生深度足够达到真皮血管层,因而红光容积脉搏波的幅度小于绿光。上述仿真结果明确了皮肤组织部分光谱特性,为皮肤组织多光谱容积脉搏波的精确获取及其他相关研究提供了一定的理论基础。     

Detection of quasitrapezoidal frequency and amplitude modulation

It has been proposed that the detection of frequency modulation (FM) of sinusoidal carriers can be mediated by two mechanisms; a place mechanism based on FM-induced amplitude modulation (AM) in the excitation pattern, and a temporal mechanism based on phase locking in the auditory nerve. The temporal mechanism appears to be "sluggish" and does not play a role for FM rates above about 10 Hz. It also does not play a role for high carrier frequencies (above about 5 kHz). This experiment provided a further test of the hypothesis that the effectiveness of the temporal mechanism depends upon the time spent close to frequency extremes during the modulation cycle. Psychometric functions for the detection of AM and FM were measured for two carrier frequencies, 1 and 6 kHz. The modulation waveform was quasitrapezoidal. Within each modulation period, P, a time Tss was spent at each extreme of frequency or amplitude. The transitions between the extremes, with duration Ttrans had the form of a half-cycle of a cosine function. The modulation rate was 2, 5, 10, or 20 Hz, giving values of P of 500, 200, 100, and 50 ms. TSS varied from 0 ms (sinusoidal modulation) up to 160, 80, 40, or 20 ms, for rates of 2, 5, 10, and 20 Hz, respectively. The detectability of AM was not greatly affected by modulation rate or by the value of TSS, except for a slight improvement with increasing TSS for the lowest modulation rates; this was true for both carrier frequencies. For FM of the 6-kHz carrier, the pattern of results was similar to that found for AM, which is consistent with an excitation-pattern model of FM detection. For FM of the 1-kHz carrier, performance improved markedly with increasing TSS, especially for the lower FM rates; there was no change in performance with TSS for the 20-Hz modulation rate. The results are consistent with the idea that detection of FM of a 1-kHz carrier is partly mediated by a sluggish temporal mechanism. That mechanism benefits from greater time spent at frequency extremes of the modulation cycle for rates up to 10 Hz.     

Effect of amplitude and frequency of ultrasonic irradiation on morphological characteristics control of calcium carbonate

We have previously reported on the morphological control of calcium carbonate by changing synthetic conditions such as temperature, pH and degree of supersaturation in liquid reaction. The present study reports the effect of amplitude and frequency of ultrasonic irradiation on the particle size of calcium carbonate using a horn type ultrasonic apparatus at two different frequencies. The calcium carbonate precipitated by mechanical stirring had a particle size of about 20 μm. By contrast, the particle size of vaterite formed under ultrasonic irradiation was about 2 μm, with a specific surface area of 25–30 m²/g. The major polymorph of calcium carbonate formed by ultrasonic irradiation was vaterite with some calcite present. For 40 kHz ultrasonic irradiation, the specific surface area of the calcium carbonate increased with increasing amplitude. The particle size of vaterite formed at this frequency was about 2 μm, and its distribution was sharper than that obtained at 20 kHz. The mode diameter of the synthesized vaterite was found to decrease with increasing amplitude at 40 kHz.     

混凝土材料声发射信号的频率特征及其与强度参量的相关性试验研究

混凝土材料声发射信号频率特征与强度指标的关系是混凝土材料声发射检测技术的重要基础。通过实验,对声发射信号频率特征与混凝土强度指标的相关关系进行了探讨。研究结果表明,在较低的应力水平上,不同强度等级混凝土声发射信号大都是低频信号。而在较高应力水平时,随着强度等级的增加,声发射信号的优势频率则逐渐升高。     

全新的电导率特征矩阵方法及其在石墨烯THz频率光学特性上的应用

基于麦克斯韦方程组所要求的电磁场边界条件首次从理论上严格推导得到超薄导电体及其复合多层介质结构光学特性的一般计算方法及其特征矩阵公式, 其优点在于只要借助于导电体的电导率而无需知道其介电常数和磁导率即可计算得到反射、透射和吸收等光学特性, 克服了传统的传输矩阵方法必需知道组成材料的介电常数和磁导率才能获得其光学性质的问题, 并利用此方法获得了石墨烯及其复合多层结构在THz频率范围内反射、透射和吸收等光学行为.     

一种S波段磁绝缘线振荡器的高频特性研究

 用数值计算的方法计算了S波段磁绝缘线振荡器（S-MILO）的主慢波结构谐振腔的π/4模、π/2模、3π/4模和π模的谐振频率,分别为1.40,2.21,2.46和2.51 GHz;计算出S-MILO封闭腔中的谐振频率依次为1.26,2.04,2.42和2.53 GHz,并计算了本征π模时的Q值。通过监测宽带激励源响应计算出S-MILO开放腔的谐振频率为2.43 GHz。对S-MILO开放腔传输特性研究表明：频率为2.25～3.05 GHz的微波,在第一腔内得到了有效抑制,输出微波的频率范围为2.2～2.5 GHz。通过对其传输特性进行研究,验证了S-MILO的高频电磁结构的合理设计。     

一种演示RLC电路相频特性的物理实验仪

介绍一种利用两个简谐振动的合成原理来演示RLC电路相频特性的物理实验仪．     

光谱分辨率对黑土有机质预测模型的影响

高光谱遥感以其高光谱分辨率适于反射光谱特征复杂的地物识别与参数反演,但对于反射光谱特征平滑的地物,高光谱数据可能存在数据冗余问题。本研究对实验室测定的黑土高光谱反射率进行重采样,基于统计分析方法研究了光谱分辨率对黑土有机质预测模型精度的影响,结果表明:黑土有机质含量高,土壤有机质的光谱作用范围宽(445～1 380nm);黑土有机质光谱预测模型精度随光谱分辨率降低,呈现先增后减的趋势,最优模型的光谱分辨率为50nm,低于高光谱遥感波段设置,略高于多光谱传感器波段设置;黑土有机质光谱预测最优模型以倒数对数微分为自变量,模型决定系数R2=0.799,RMSE=0.439,研究成果为土壤有机质遥感反演、光谱速测仪器的研制,以及传感器波段设置提供理论基础与技术支持。     

振幅和相位涨落对锁模脉冲列特性的影响

用傅里叶变换的方法分析了锁模激光器中模式间的相位和振幅涨落对锁模脉冲列特性的影响。将锁模激光器中各模式的相位和振幅涨落作傅里叶展开,再通过增益谱抽样的傅里叶变化得到其时域行为。分析结果表明振幅系统涨落及随机涨落均不引起脉宽的明显变化,只引起脉冲间背景的加大,但相位涨落随机会使脉冲列强度产生波动。所用物理图像简明,结果对获得稳定的锁模脉冲列的实验研究有参考意义。     

太湖不同叶绿素a浓度水体荧光特征分析

利用2008年太湖蓝藻爆发的5-8月实测的27个站点水体光谱反射率和水质参数,分析了不同叶绿素a浓度等级下太湖水体光谱的荧光特征.结果表明,荧光峰位置和荧光峰高度都与叶绿素浓度呈显著正相关,且荧光峰峰值位置和半宽度与叶绿素a浓度的拟合度要高于基线荧光峰高度和归一化荧光峰高度.荧光峰特性用于二类水体中高浓度叶绿素探测较传...     

磁绝缘线振荡器谐振腔的高频特性研究

 利用数值方法计算了磁绝缘线振荡器(MILO)主慢波结构谐振腔和扼流腔的谐振频率和场分布。结果表明：当主慢波结构腔内半径为4.6 cm,扼流腔内半径为4.2 cm,阴极半径为3 cm时,MILO工作在3.6~4.4 GHz频率范围,扼流片可以阻止微波功率向脉冲功率源泄漏,这有利于提高器件微波输出的功率;4.5~4.9GHz频段为慢波结构的阻带,微波在该频段截止。计算了C波段MILO开放腔的谐振频率,当模式分别为3π/8,π/2,5π/8,3π/4时,其谐振频率分别为3.18,3.76,4.00,4.11 GHz;并通过实验测出了开放腔的谐振频率,其相应的值分别为3.80,3.94,4.08.4.18 GHz, Q分别为194,143,231,468。数值计算的谐振频率与实验测出的频率基本一致。     

环形激光陀螺仪机械抖动参数的选定

抖动参数的正确选择直接影响抖动偏频效果。为了有效地进行抖动偏频 ,抖动角速度幅度应远大于 RL G的闭锁阀值。当抖动角幅度增大至一定值后 ,再增大抖动角幅度对抖动偏频效果影响不大 ,而局部调整抖动角幅度却可能使动态锁区降为 0 ,实现完全解锁。同时抖动角幅度的对称性控制对减小由抖动而产生的偏置误差具有重要的意义。为了适应高速数字采集和处理 ,抖动频率应尽可能地提高