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基于带宽匹配思想的SoC测试结构设计 被引量:6
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作者 邓立宝 乔立岩 +1 位作者 俞洋 彭喜元 《仪器仪表学报》 EI CAS CSCD 北大核心 2012年第8期1819-1825,共7页
IP(intellectual property)核复用的设计思想使得SoC(system-on-a-chip)成为当今集成电路设计的主流,但对其进行测试变得异常困难,这就是需要为SoC设计测试结构的主要原因。传统的测试结构功能是:根据自动测试设备(automatic test equip... IP(intellectual property)核复用的设计思想使得SoC(system-on-a-chip)成为当今集成电路设计的主流,但对其进行测试变得异常困难,这就是需要为SoC设计测试结构的主要原因。传统的测试结构功能是:根据自动测试设备(automatic test equip-ment,ATE)提供的某一频率,将测试数据通过测试结构依次施加到SoC内部的IP核,并获取测试响应传输到ATE中,以分析其功能正常与否。但是这种测试结构存在很多缺点,其中最主要的是未考虑测试设备提供的测试访问机制(test access mecha-nism,TAM)的宽度与SoC内各IP核的最佳测试带宽是否一致。对这一系列问题进行研究,提出一种基于带宽匹配思想的SoC测试结构设计方法,该方法主要通过一个带宽匹配转换模块,实现测试数据的宽度调整和施加频率的调整,在牺牲了芯片部分额外面积的前提下,很好地实现了测试带宽和测试频率的匹配,缩短了SoC的测试时间。最后将这种方法应用在ITC’02标准测试集上,实验结果验证了该方法的有效性。 展开更多
关键词 IP核复用 测试结构 测试访问机制 带宽匹配
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软X射线多层膜成像系统带宽匹配条件研究 被引量:1
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作者 王占山 曹健林 《光学精密工程》 EI CAS CSCD 1998年第1期12-17,共6页
从多层膜反射软X射线的特性出发,分析了两块多层膜组成系统的光强传输效率和位相变化关系,给出了成像系统带宽匹配条件。
关键词 软X射线 多层膜 成像系统 带宽匹配 薄膜
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基于可变带宽EFT滤波器的带宽匹配数字接收方法 被引量:1
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作者 吴伟 唐斌 《电子与信息学报》 EI CSCD 北大核心 2008年第11期2728-2731,共4页
该文提出了一种新的基于可变带宽EFT滤波器的带宽匹配数字接收方法。文中利用线性准时不变(LQTI)系统在扩展傅里叶变换(EFT)域的可变带宽频率特性来构建可变带宽滤波器(VBF),并将可变带宽EFT滤波器引入数字下变频(DDC),实现对不同带宽... 该文提出了一种新的基于可变带宽EFT滤波器的带宽匹配数字接收方法。文中利用线性准时不变(LQTI)系统在扩展傅里叶变换(EFT)域的可变带宽频率特性来构建可变带宽滤波器(VBF),并将可变带宽EFT滤波器引入数字下变频(DDC),实现对不同带宽信号的匹配接收。应用这种滤波器的优点在于只有一个直接决定带宽的可调谱参数,更新机制简单。文中还进一步给出带宽匹配接收数字下变频的多相高效结构,运算效率和工程可实现性大大提高。实验结果证明了该方法的正确性和有效性。 展开更多
关键词 扩展傅里叶变换 线性准时不变系统 可变带宽滤波器 带宽匹配接收 多相结构
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18.2nm Schwarzschild显微物镜用多层膜带宽匹配问题分析 被引量:1
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作者 王占山 《光学精密工程》 EI CAS CSCD 1999年第3期14-18,共5页
软X射线多层膜的进展使正入射高分辨率成像系统从红外、可见和紫外扩展到软X射线波段。由于软X射线多层膜的反射率还不能像其它波段反射镜反射率那样高,因此由两块同心球面反射镜组成的Schwarzschild物镜在软X射线波... 软X射线多层膜的进展使正入射高分辨率成像系统从红外、可见和紫外扩展到软X射线波段。由于软X射线多层膜的反射率还不能像其它波段反射镜反射率那样高,因此由两块同心球面反射镜组成的Schwarzschild物镜在软X射线波段得到了广泛的应用。本文从多层膜带宽匹配条件、Schwarzschild显微物镜的几何尺寸和多层膜镀制设备的性能出发,研究了实现Schwarzschild显微物镜带宽匹配条件的镀膜过程,为实际制备Schwarzschild显微物镜用多层膜提供理论指导。 展开更多
关键词 软X射线多层膜 带宽匹配 显微物镜
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自适应光学系统时间带宽和空间带宽的匹配
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作者 张德良 姜文汉 《光电工程》 EI CAS CSCD 1998年第4期13-21,共9页
自适应光学系统存在时间带宽和空间带宽。为了有效地利用自适应光学系统的系统资源,必须使这两种带宽匹配。本文通过经系统校正后的剩余波前扰动相位的均方差与系统时间带宽和空间带宽的关系,研究了在不同条件下系统时间带宽和空间带... 自适应光学系统存在时间带宽和空间带宽。为了有效地利用自适应光学系统的系统资源,必须使这两种带宽匹配。本文通过经系统校正后的剩余波前扰动相位的均方差与系统时间带宽和空间带宽的关系,研究了在不同条件下系统时间带宽和空间带宽的匹配问题。分析结果表明,在一定的系统时间延迟,探测噪声水平和大气条件下,自适应光学系统存在一个最佳时间带宽和最佳空间带宽。 展开更多
关键词 自适应光学 空间带宽 时间带宽 带宽匹配
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Construction of 1D Mn_(x)O_(y)/C@Fe_(3)O_(4) Heterostructure for Ultralight Broadband Electromagnetic Wave Absorption
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作者 SONG Zhiming LIU Bin +2 位作者 YI Peng HAN Xuhui LIU Xiaofang 《陶瓷学报》 北大核心 2025年第4期729-741,共13页
[Background and purposes]In recent years,there has been growing attention in academia and industry on the development of high-performance electromagnetic wave(EMW)absorbing materials.However,creating lightweight broad... [Background and purposes]In recent years,there has been growing attention in academia and industry on the development of high-performance electromagnetic wave(EMW)absorbing materials.However,creating lightweight broadband absorbers remains a challenge in terms of practical applications.EMW absorbing materials primarily rely on the magnetic loss of magnetic materials and/or the dielectric loss of dielectric materials to convert EMW energy into thermal energy for dissipation.Among various magnetic materials,Fe_(3)O_(4) plays an irreplaceable role in EMW absorption due to its high saturation magnetization,low cost and compatible dielectric loss in the gigahertz frequency range.Nevertheless,the high density,large matching thickness and narrow absorption bandwidth of Fe_(3)O_(4) pose significant challenges for practical applications.In contrast,one-dimensional(1D)structures not only retain the characteristic properties of lightweight,chemical stability and high dielectric loss,but also exhibit anisotropic structures and large aspect ratios.Additionally,researchers have found that the minimum reflection loss(RL)of hollow carbon materials with mesopores is nearly four times that of non-porous hollow carbon materials and nine times that of dense carbon materials.According to Maxwell's EMW theory,composites consisting of Fe_(3)O_(4) and one-dimensional(1D)mesoporous carbon materials can leverage their respective advantages by optimizing the composition and structure of the composites to balance u,and Er,thereby enhancing EMW absorption performance.Additionally,numerous studies have demonstrated that composites composed of multi-component heterostructures significantly enhance the EAB.This enhancement is primarily ascribed to the numerous interface polarization losses generated by the additional heterostructure interfaces,which also improve the overall impedance matching of the composites.In this study,we leverage the advantages of magnetic/carbon composites,one-dimensional(1D)mesoporous carbon and multi-component heterostructures to prepare a composite of 1D mesoporous carbon-coated manganese oxide(Mn_(3)O_(4) and MnO,denoted as Mn_(x)O_(y))embedded with Fe_(3)0_(4) nanoparticles(Mn_(x)O_(y)/C@Fe_(3)O_(4)).This composite was synthesized and its formation mechanism and microstructure were analyzed in detail.At the same time,the influence of this Mn_(x)O_(y)/C@Fe_(3)O_(4) structure on EMW properties and absorbing performance was further discussed.[Methods]Firstly,MnO_(2) nanowires were synthesized by using a simple hydrothermal method.Then,the MnO_(2) nanowires served as templates for the synthesis of MnO_(2)/PDA@Fe^(3+)composites through the in-situ polymerization of dopamine and Fe^(3+)adsorption.Finally,1D mesoporous carbon-coated manganese oxide composite embedded with Fe_(3)O_(4) nanoparticles(Mn_(x)O_(y)/C@Fe_(3)O_(4))composites were obtained after heat treatment at 550℃ in N_(2).The crystal structure of the samples was analyzed using X-ray diffractometer with Cu Ka irradiation.Scanning electron microscopy(SEM)and high-resolution transmission electron microscopy(TEM)were used to observe microstructure and morphology of the samples.Nitrogen sorption measurements were obtained at 77 K on a Quantachrome surface area and pore size analyzer to measure the specific surface area and pore size distribution.XPS analysis was performed on X-ray photoelectron spectrometer with monochromatic Al Ka radiation.Magnetization curves of the samples were recorded with a Quantum Design physical property measurement system(PPMS-9)at room temperature.The electromagnetic parameters of the Mn_(x)O_(y)/C@Fe_(3)O_(4) composites were measured using an Agilent N5230C network analyzer in the frequency range of 2-18 GHz.For electromagentic testing,the Mn,Oy/C@Fe34 composites and paraffin wax were mixed at 50°C according to the mass ratio of 15 wt.%,20 wt.%and 25 wt.%,and pressed in a special mold to make coaxial rings(inner diameter=3.04 mm,outer diameter-7 mm),which were denoted as S-1,S-2 and S-3,respectively.[Results]SEM images illustrate the preparation process of iD mesoporous carbon-coated manganese oxide embedded with Fe3O4 nanoparticles composites(Mn_(x)O_(y)/C@Fe_(3)O_(4)).Most of the manganese oxide(Mn,Oy)was reduced to granular after heat treatment,while the outer carbon layer remains its 1D morphology and the carbon layer is interspersed with Fe_(3)O_(4) nanoparticles.The diffraction peaks of MnO_(2) nanowires align well with the body-centered tetragonal a-MnO2.For the Mn_(x)O_(y)/C@Fe_(3)O_(4) composites,the signals of α-MnO_(2) disappears,followed by the emergence of Mn_(3)O_(4) and three prominent diffraction peaks for the cubic MnO.In addition,four weak diffraction peaks correspond to the magnetite Fe_(3)O_(4),consistent with the HRTEM results.The corresponding nitrogen adsorption-desorption isotherm and pore size distribution curve are presented to further analyze the mesoporous structure of composite.The surface composition and element valence states of the Mn_(x)O_(y)/C@Fe_(3)O_(4) composite were investigated by using XPS.The polarization relaxation processes were analyzed according to the Debye theory which describes the relationship between e'and e".Besides the polarization loss,the contribution of the conduction loss plays an important role for the overall dielectric loss.The magnetization curve of Mn_(x)O_(y)/C@Fe_(3)O_(4) exhibits typical ferromagnetic behavior.The permittivity parameter(Co),defined as Co=u"(u)^(-2)f^(-1) determine the contribution of eddy current effect to magnetic loss.The tand values are all larger than those of tand,for the three samples,indicating that the loss capacity of Mn_(x)O_(y)/C@Fe_(3)O_(4) composites is mainly derived from the dielectric loss.Although tand,is smaller,it plays an important role in improving the impedance matching of Mn_(x)O_(y)/C@Fe_(3)O_(4) composites.When the filler loading is 15 wt.%,the RL of sample S-1 is about-10.0 dB at the thickness of 1.5 mm with narrow EAB.As the filler loading increased to 20 wt.%,the RL of sample S-2 reached-62.0 dB at a thickness of 2.2 mm and the EAB was 6.4 GHz at a small thickness of 1.7 mm.When the filler loading is further increased to 25 wt.%,the microwave absorption performance of sample S3 decreased significantly with a little region of RL<-10.0 dB at the thickness of 5.0 mm.The values of[Zin/Zol of the three samples at thicknesses of 1.5-5.0 mm were calculated.Due to good impedance matching of S-2,the incident EMW can enter the material and then can be dissipated through dipole polarization loss,interface polarization loss,conduction loss,eddy current loss and natural ferromagnetic resonance loss.[Conclusions]1D Mn_(x)O_(y)/C@Fe_(3)O_(4) was synthesized via a process involving the coating of polydopamine,adsorption of Fe(ll)salts and heat treatment,using MnO_(2) nanowires as templates.The multi-component heterostructure of the Mn_(x)O_(y)/C@Fe_(3)O_(4) composite(Mn_(3)O_(4),MnO,Fe_(3)O_(4),and C)enhances the interfacial interactions between the different phases,providing increased interface polarization loss under the action of an alternating electromagnetic field.The numerous defects and terminal groups in the mesoporous carbon provide abundant dipole polarization centers.Additionally,the presence of mesopores reduces the weight of the material while increasing the multiple scattering losses of the electromagnetic waves within the material.The ID carbon structure in the matrix forms a conductive network between adjacent fibers,facilitating electron migration and transition,thereby enhancing conductive loss.The incorporation of magnetic Fe_(3)O_(4) nanoparticles introduces eddy current loss and natural ferromagnetic resonance loss,thus increasing magnetic loss.Moreover,the synergistic effect between dielectric and magnetic losses improves the impedance matching of the material,leading to excellent EMW absorption performance. 展开更多
关键词 electromagnetic wave absorbing materials impedance matching ultralight BROADBAND
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长段电缆中局部放电脉冲信号的传输特性及耦合研究 被引量:10
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作者 高旭泽 段然 +1 位作者 任明 谭笑 《电力工程技术》 2020年第5期2-9,共8页
对于交联聚乙烯(XLPE)电缆,通过局部放电的测量,可以检测到电缆本体或附件中多种潜在的绝缘缺陷。当局部放电脉冲在电缆中传播时,脉冲波形会发生畸变。文中针对局部放电脉冲在电缆本体传播时的脉冲波形变化进行分析,同时讨论不同耦合带... 对于交联聚乙烯(XLPE)电缆,通过局部放电的测量,可以检测到电缆本体或附件中多种潜在的绝缘缺陷。当局部放电脉冲在电缆中传播时,脉冲波形会发生畸变。文中针对局部放电脉冲在电缆本体传播时的脉冲波形变化进行分析,同时讨论不同耦合带宽对信号检测的影响,得出以下结论:当电缆发生局部放电时,脉冲信号幅值随着传播距离的增加迅速衰减,但脉冲视在放电量衰减幅度相对较小;宽带耦合具有较高的灵敏度,但是其电荷校准曲线误差较大,并且会导致信噪比降低,缺陷检出度下降;窄带耦合虽然能够获得较为准确的电荷校准曲线,却会导致脉冲波形发生叠加,影响故障点定位。 展开更多
关键词 长段电缆 局部放电 传输特性 高频衰减 匹配带宽
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