共查询到20条相似文献,搜索用时 31 毫秒
1.
利用数值模型研究了完整深海声道中会聚区的水平偏移特性,根据折射定律和Lloyd镜效应推导了会聚区发生水平偏移时临界频率的表达式。研究结果表明:当声波频率低于临界频率时,会聚区的主导模态与频率相关,随着声波频率减小会聚区会向靠近声源的方向水平移动,同时传播损失明显增大,当声波频率大于临界频率时,会聚区的主导模态近似与频率无关,会聚区的位置和传播损失大小不会随频率改变而发生明显变化,声源深度不同时,临界频率也不同。通过临界频率可以确定在特定声源深度下,会聚区发生水平偏移时需要满足的频率条件,利用临界频率与声源深度之间的关系,可以被动估计深海浅层目标的深度。 相似文献
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基于不动点理论研究了多系统兼容接收机的频点选择问题,并引入遗传算法解决了这一问题.将Banach不动点理论引入频点空间,提出并证明了频点空间中频点集的遗传进化过程反映了频点空间呈现出的一种不动点物理特性;经过频点空间算子的足够多次的反复遗传进化作用,频点空间中的任一迭代序列源频点集都将最终收敛于唯一不动点目标频点集,而该不动点目标频点集中的目标频点即为该频点选择问题的最优解.完成了遗传算法应用于频点选择问题的理论研究与实现.仿真结果表明,该算法能够有效地解决多系统兼容接收机的频点选择问题.
关键词:
多系统
接收机
遗传算法
不动点 相似文献
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目前左手材料的负折射现象只发生在微波波段,通常把发生负折射现象的这个频率波段称为响应频段.由于左手材料的响应频段的频率很低,而常用的波源是太阳光或者是可见光,因此左手材料的应用受到极大的限制.如何使左手材料的响应频段从低频移到高频或者说从微波波段移到可见光波段是迫切需要解决的问题.在周期性结构的左手材料中影响响应频段的因素很多,例如周期性结构的单元形状、单元尺寸等等.文中通过改变周期性结构左手材料的单元尺寸实现了响应频段的移动,同时经实验和计算机模拟得到了单元尺寸和响应频段的关系即随着单元尺寸变小响应频段
关键词:
左手材料
周期性结构
单元尺寸
响应频段 相似文献
4.
时间频率基准装置——铯原子喷泉钟, 在标准时间产生和保持、基础物理研究中发挥了重要的作用. 介绍了铯原子喷泉钟的工作原理, 对影响其性能的各项噪声源和频移项给出了分析, 影响频率稳定度性能的主要因素为Dick 效应相关的原子团装载时间、微波激励源相位噪声和探测激光的频率噪声, 影响频率不确定性能主要频移项为: 黑体辐射频移、冷原子碰撞频移、腔相位分布频移和微波泄露频移; 总结和比较了当前具有先进性能的铯原子喷泉钟采用的技术; 介绍了铯原子喷泉钟的主要应用方向、空间冷原子铯钟的研制情况和光学频率原子钟进展. 相似文献
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双纵模稳频氦氖激光器的光谱与频率复现性分析 总被引:2,自引:0,他引:2
对双纵模稳频氦氖激光器的光谱及其频率复现性进行了理论估计,进行了633 nm碘稳定氦氖激光器的拍频实验,实验采用内腔激光器,并采用双纵模稳频的方法,通过观测激光器的两个偏振态互相垂直的相邻纵模的输出,并使二者稳定到功率相等的参考点处,获得激光稳定输出。实验通过观察双纵模稳定激光的模式输出,分析了影响激光频率复现性与频率稳定度的因素,测量了稳定激光的功率和频率稳定度。通过拍频测量,对激光器的频率复现性进行了分析,复现性用频差可以达到(1~2)×10-8量级。通过实验表明,双纵模稳频氦氖激光器的频率复现性完全符合用于长度精密测量的稳频激光器的要求,激光器可以很稳定地工作,稳定度用阿伦偏差表示可以达到10-10量级,可以作为实用的稳频激光标准。 相似文献
6.
Enhanced electron–positron pair production by frequency chirping in one-and two-color laser pulse fields
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Enhanced electron–positron pair production by frequency chirping in one- and two-color laser pulse fields is investigated by solving the quantum Vlasov equation. A small frequency chirp shifts the momentum spectrum along the momentum axis. The positive and negative frequency chirp parameters play the same role in increasing the pair number density. The sign change of the frequency chirp parameter at the moment t = 0 leads the pulse shape and momentum spectrum to be symmetric, and the number density to be increased. The number density of produced pairs in the two-color pulse field is much higher than that in the one-color pulse field and the larger frequency chirp pulse field dominates more strongly. In the two-color pulse fields, the relation between the frequency ratio of two colors and the number density is not sensitive to the parameters of small frequency chirp added in either a low frequency strong field or a high frequency weak field but sensitive to the parameters of large frequency chirp added in a high frequency weak field. 相似文献
7.
用一维流体模型研究了大气压双频氦气放电等离子体的特性。数值模拟的结果表明,在单、双频放电中,随着应用电压的增加,电子密度和放电电流都增加。相对于单频放电,双频放电中低频源的耦合效应使得放电中的电流以及电子密度降低。随着低频源电压峰值的增加,电子密度降低,离子通量,电子损失能量以及电子吸收能量均降低;但电子温度和电势随着低频源电压峰值的增加而增加。在相同低频源电压下,随着高频源电压的增加离子流非线性增加。 相似文献
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��һ�У�����������˧�ǣ��� Ө���� ��������ʯ���� 《核聚变与等离子体物理》2020,39(4):373-378
Based on one dimensional fluid model, the characteristics of helium plasma discharge driven by dual frequency at atmospheric pressure were studied. The results show that the electron density and discharge current increase with power voltage both in single frequency discharge and dual frequency discharge. In comparison with single frequency discharge, the discharge current and electron density in dual frequency discharge are lowered due to the coupling of low frequency source. As the voltage of low frequency source increases, the electron density, ion flux, electron energy dissipation, as well as electron heating decrease, whereas electron temperature and potential increase. As the voltage of high frequency source increases, the ion flux nonlinearly increases at the same voltage of low frequency source. 相似文献
9.
为了提高激光多普勒测速仪的测量精度,提出对激光多普勒信号先进行跟踪滤波,再进行频谱细化和频谱校正的信号处理方法,并利用信号处理系统对实测的多普勒信号进行了实验研究。实验结果表明:跟踪滤波器在滤除基底信号及系统的部分噪声的基础上,实时跟踪多普勒信号的频率,信噪比明显提高,所得结果与多普勒频率的真实值相一致;频谱细化技术大大提高了频谱分辨力,频谱校正技术使校正后的频率更接近真实值。 相似文献
10.
The double frequency method, where bubbles rising through a fluid are illuminated simultaneously with a ‘pump’ frequency swept through the resonance frequency range and a megahertz imaging frequency, is used to measure pressure changes in fluids non-invasively. The bubble echo spectrum is centred at the imaging frequency with side bands at separations equal to the pump frequency. If the ambient pressure is changed, the bubbles undergo changes in their sizes. This would alter the resonant frequency of the bubble and hence the peak of the echo at the sum (or difference) frequency. By observing shifts in the frequency of the peak amplitude of the side bands it is shown that fluid pressure changes can be measured accurately. 相似文献
11.
Yasuda K Torii T Yasui K Iida Y Tuziuti T Nakamura M Asakura Y 《Ultrasonics sonochemistry》2007,14(6):699-704
The ultrasonic reactor with dual frequency was used and the effect of frequency on the fluorescence intensity of terephthalate ion was experimentally investigated in the frequency range from 176 to 635 kHz. The sonochemical reaction fields were visualized by using sonochemical luminescence of luminol solution. Compared with the fluorescence intensity of terephthalate ion for single frequency, the fluorescence intensity for dual frequency increased. The fluorescence intensity ratio of dual frequency to single frequency had maximum value when the frequency of transducer attached at the bottom wall was comparable in magnitude to that at the side wall. In the case of dual frequency, the sonochemical reaction fields became more extensive in the reactor and more intensive around the center of the reactor. 相似文献
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Hidekatsu Yokoyama 《Applied magnetic resonance》2009,36(1):49-59
Coarse control and fine control of the resonant frequency of a loop-gap resonator (LGR) operating at an electron paramagnetic
resonance (EPR) frequency of ca. 650 MHz were achieved using a single-turn coil with a varactor diode attached (a frequency
shift coil). When the distance between the LGR and the frequency shift coil was changed from 15 to 10 mm under the condition
of constant voltage to the varactor diode (0 V), a shift of the resonant frequency of the LGR of ca. 20 MHz was observed (coarse
frequency control). When the voltage applied to the varactor diode was changed from 0 to 15 V at the same distance between
the LGR and the frequency shift coil (10 mm), a shift of the resonant frequency of the LGR of ca. 200 kHz was observed (fine
frequency control). There were no significant changes in sensitivity of EPR measurements of a phantom (comprised of agar with
a nitroxide radical and physiological saline solution) without and with the frequency shift coil. The EPR sensitivity did
not change discernibly when the resonant frequency was shifted by the frequency shift coil. Furthermore, radio-frequency phase
adjustment for homodyne detection could be performed by using the frequency shift coil without applying frequency modulation
to the carrier wave. 相似文献
15.
We discuss the correlations between the measured lasing-mode frequency difference and the mode polarization angle in an intracavity birefringent dual-frequency laser. The frequency difference and polarization are adjusted by rotating an intracavity quartz crystal through a large angular range. We propose two kinds of frequency difference: the equal-order frequency difference and the adjacent frequency difference. By measuring the equal-order frequency difference versus the quartz crystal rotation angle, the real physical process behind frequency splitting is revealed. Based on this, the adjacent frequency difference curve is also obtained. The emitted laser beam polarization angle is also measured for large rotations of the intracavity quartz crystal. These measurements reveal the complete process of optical activity in frequency splitting and allow us to predict the trends of frequency difference and polarization angle for large quartz crystal rotation angles. We analyze the correlations between the equal-order frequency difference and the polarization angle based on the experimental results, which show that the certain points on the two curves are inter-related. The principal results agree well with the optical theory of crystals. 相似文献
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《声学学报:英文版》2017,(3)
The two-dimensional nonlinear acoustic field of eleven exponential shaped resonators was simulated with a computational fluid dynamics software Fluent.The influence of driving frequency and driving intensity on pressure in resonator as well as its natural frequency was investigated.The relationship between natural frequency and theoretical calculation resonance frequency was also explored.It is found that beating phenomena can be observed in the resonator when the driving frequency deviates from the natural frequency.Moreover,the natural frequency of resonator increases with the increasing of driving intensity,which shows a hard spring effect.However,the driving intensity plays little effect on natural frequency and the natural frequencies are smaller than the theoretical calculation values in any driving intensity.Meanwhile,a formula between the natural frequency and its first-order resonance frequency from theoretical calculation was obtained by linear fitting for all these exponential shaped resonators under consideration.It is also found that the highest pressure amplitude and highest pressure ratio can be obtained from the exponential shaped resonator of m=2.8 under the same driving intensity.Moreover,the relation between natural frequency and the theoretical resonance frequency for m=2.8-tube is slightly different from other tubes in consideration. 相似文献
18.
频率是电磁波最重要的一个基本物理量,随着THz技术的发展,在光源研制、宽带通信、超精细光谱测量等领域都对THz频率的高精度侧量提出了要求.传统的Fabry-Perot干涉法与外差探测法难以实现THz频率的高精度测量,频率梳方法虽然测量精度很高,但测量系统复杂.本文提出一种利用重复频率自由漂移的飞秒激光器实现太赫兹频率精密测量的新方法.通过对非锁定的飞秒激光器的重复频率和THz拍频频率进行同时连续采集与计算,得到被测THz频率,测量精度可以达到10~(-10)量级无需对飞秒激光重复频率进行复杂的锁定控制,测量系统大大简化. 相似文献
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根据稳态损耗因子的定义, 推导了含多阶模态的频带稳态损耗因子公式, 得到结论: 稳态损耗因子不一定介于各阶模态损耗因子之间, 而是与各阶模态对振动响应的贡献程度有关. 提出了过程损耗因子的概念, 并给出了利用频带内各模态固有频率、损耗因子和振幅计算过程损耗因子的方法. 当时间趋于无穷时, 过程损耗因子趋于只由最小模态损耗因子贡献的稳态损耗因子. 传统衰减法测试稳态损耗因子在频带内仅有单个模态或模态密集的情况下精度较高, 但对于含有多阶模态且模态不密集的中频带, 采用传统衰减法准确获取稳态损耗因子存在困难. 根据过程损耗因子的特点, 提出了利用时域衰减曲线逐步分离频带内不同衰减特性分量及其响应幅度从而获取稳态损耗因子的方法. 仿真和实验均表明: 提出的利用时域衰减数据获取稳态损耗因子的方法具有很高精度, 可以弥补传统衰减法在中频段损耗因子实验确定中的不足. 相似文献
20.
对比研究了基频、二倍频和三倍频激光单独和同时辐照下熔石英光学元件的初始损伤和损伤增长规律, 重点研究了基频和二倍频的加入对三倍频诱导初始损伤和损伤增长的影响, 分析了基频和二倍频相对于三倍频的折算因子。研究结果表明: 当基频和二倍频能量密度较低时, 它们对三倍频损伤几率曲线的影响可以忽略, 但会引起损伤程度的增加; 在多波长同时辐照的损伤增长中, 损伤增长阈值主要取决于三倍频的能量密度, 而损伤增长系数与总的能量密度有关; 折算因子可以同时反映初始损伤和损伤增长的波长效应和波长间的能量耦合效应。 相似文献