同步辐射X射线衍射增强CT方法研究

本文将同步辐射硬X射线衍射增强成像方法应用于材料无损检测CT方法中（简称衍射增强CT法），并对自制样品进行投影成像重建，获得了非常清晰的样品内部结构图像,并与样品的单晶吸收成像CT重建结果进行对比.结果表明，对于吸收系数相近的结构材料,衍射增强CT法可得到更好的物质内部边界.     

卷积差技术在ESR和ESR成像中的应用

该文将卷积差技术应用于提高ESR谱的分辨率和在ESR成像过程中扣除固有线宽介绍了卷积差过程,对比了卷积差前后ESR谱的变化.     

X射线相衬成像应用于惯性约束核聚变多层球壳靶丸检测

随着惯性约束核聚变(ICF)研究的逐步深入,尤其是氘氚(DT)燃料层球壳梯度掺杂的广泛应用,对轻物质界面的诊断需求日益增长.在北京同步辐射形貌成像站的微米CT机上利用类同轴相衬成像方法获取了三层球壳靶丸的相衬图像,最佳空间分辨率达到了2μupm,衬度达到12%;通过分析边缘增强函数和衬度传递函数之间的关系,总结出一套完整的类同轴相衬成像方法,同时将相衬成像结果与吸收成像结果对比.实验结果表明,X射线相衬成像在轻物质界面的分辨中具有明显的优势,能够广泛应用于ICF研究、医学断层扫描CT装置和生物结构等前沿科学领域.     

深度学习在计算成像中的应用

近年来,深度学习被广泛应用于计算成像中,并取得了令人瞩目的成果,已成为该领域的研究热点。为了深入了解现有基于深度学习的方法是如何解决众多计算成像问题的,主要介绍了该方法的基本理论和实施步骤,然后以散射成像、数字全息及计算鬼成像中的应用为例具体介绍该方法的有效性和优越性。汇总对比了一些典型应用,并对基于深度学习的计算成像方法进行了总结和展望。     

同步辐射相位衬度成像医学应用初探

近年来,相位衬度成像技术医学领域应用的发展引人瞩目.同步辐射相位衬度成像无须使用对比剂就能显示传统X射线无法显示的肌腱、软骨、韧带、脂肪、血管及神经等软组织.文章作者应用包括类同轴相衬成像和衍射增强成像在内的相位衬度成像技术进行了肝胆、肺脏、肾脏、胃肠道、心脏、血管、骨关节组织与肿瘤成像,证实了同步辐射相位衬度成像较传统X射线成像图像清晰,分辩率明显提高,特别适用于软组织、血管等的成像.     

红外扫描过采样系统点目标检测性能分析与仿真EI北大核心CSCD

过采样是为提高遥感扫描图像分辨率而提出的一种新的成像体制,为将其应用于红外搜索与跟踪系统,需研究过采样对系统点目标检测性能的影响.从扫描成像原理角度对比分析常规采样和过采样的特点;基于高分辨率图像退化方式给出扫描图像仿真方法;通过仿真扫描图像进行单帧目标检测处理,对比分析两种采样体制下的系统点目标检测性能.结果表明,在相同条件下,过采样系统点目标检测性能优于常规采样;常规采样扫描图像中目标一般呈现1×1点状,而过采样扫描图像中目标呈现斑点状,利用该特性可进一步提升过采样系统目标检测性能.     

基于数字微镜器件的压缩感知关联成像研究

将数字微镜器件(DMD)应用于压缩感知(CS)关联成像,在该成像方案中,只需用无空间分辨能力的桶探测器,并结合相应的算法就能得到物体的像;将此成像方案应用于多光谱成像,仅需用线列探测器就能得到物体多光谱像,简化了多光谱成像探测的光电记录过程.通过对关联成像和CS理论的介绍阐明了成像原理.在实验平台上搭建演示装置,分别用...     

红外扫描过采样系统点目标检测性能分析与仿真

过采样是为提高遥感扫描图像分辨率而提出的一种新的成像体制,为将其应用于红外搜索与跟踪系统,需研究过采样对系统点目标检测性能的影响.从扫描成像原理角度对比分析常规采样和过采样的特点;基于高分辨率图像退化方式给出扫描图像仿真方法;通过仿真扫描图像进行单帧目标检测处理,对比分析两种采样体制下的系统点目标检测性能.结果表明,在相同条件下,过采样系统点目标检测性能优于常规采样;常规采样扫描图像中目标一般呈现1×1点状,而过采样扫描图像中目标呈现斑点状,利用该特性可进一步提升过采样系统目标检测性能.     

地面核磁共振反演导电层状模型

提出不同于常规线性规划的广义线性迭代反演成像技术,并将其应用于任意层状导电介质的地面核磁共振数据分析.在这种方法中,初始振幅强度的平方作为反演成像的对象,它可以表示为含水量分布的二次型形式,并且在反演成像迭代过程中,对应的Jacobian矩阵元素可以用解析形式显式表示出来.反演成像可以从均匀半空间模型开始迭代,理论上,2次迭代就可以完成成像过程.用实际数据对提出的反演成像理论进行了验证.与常规方法相比,新方法的成像结果与实际情况具有更好的一致性,证明了广义线性迭代反演成像不仅具有较好的稳定性和收敛性,还特别适合任意良导层状模型的地面核磁共振数据反演成像.     

强度涨落在热光鬼成像中的作用

热光鬼成像的图像质量在实际应用中具有重要作用. 通过理论分析和数值模拟, 发现光场的强度涨落程度会影响热光鬼成像的对比度, 基于此, 提出可以通过调节热光场的平均强度和强度波动的方差来提高成像对比度, 并且研究了这一方法对成像信噪比的影响. 将这种方法与另一种提高成像对比度的方法——高阶鬼成像进行了对比, 所得结果将有助于提高对热光鬼成像的理解. 关键词： 鬼成像 强度涨落 对比度 信噪比     

Efficiency of paramagnetic relaxation enhancement in off-resonance rotating frame

Transferring from laboratory frame to off-resonance rotating frame for the (1)H spin can compensate the relaxivity loss for paramagnetic agents at the magnetic field strength higher than 3 Tesla and enhance water relaxation rate constant significantly. A comprehensive theory for calculating the relaxation rate constants in the off-resonance rotating frame is described. This theory considers the contributions from both inner shell and outer shell water. The derived relaxation rate constants and relaxation enhancement efficiency as a function of the magnetic field strength and the effective field parameters are directly correlated to the structures, dynamics and environments of paramagnetic agents. To validate the theoretical predictions, we have measured the relaxation enhancement efficiency for a series of macromolecule conjugated gadolinium chelates at 9.4 Tesla. The experimental results confirmed the theoretical predictions. The theory also predicts the relaxation enhancement for T(2)-type paramagnetic agents at high magnetic fields. Promising fields of applications include situations where T(1)- or T(2)-type paramagnetic agents are used for labeling molecular/cellular events.     

The line shapes of the water proton resonances of red blood cells containing carbonyl hemoglobin, deoxyhemoglobin, and methemoglobin: implications for the interpretation of proton MRI at fields of 1.5 T and below

The 300 MHz (7 T) water proton resonances of suspensions of red blood cells containing paramagnetic deoxyhemoglobin or methemoglobin can be resolved into two broad lines assignable to intra- and extracellular water which undergoes rapid T2 relaxation by diffusion in magnetic field gradients induced by the intracellular paramagnets. The width of the resolved lines allowed an estimate of the maximum contribution that diffusion makes to T2 relaxation at 7 T. The dependence of the diffusion contribution on the square of the strength of the static magnetic field suggest that diffusion makes a small contribution to water proton T2 relaxation at 1.5 T compared to 7 T, and a negligible one at 0.5 T in early and intermediate hematomas containing deoxyhemoglobin or methemoglobin in intact red blood cells. At the lower field strengths, water proton T2 relaxation is apparently dominated by the rapid chemical exchange (mean lifetime tau = 10 msec) between the intra- and extracellular environments.     

Transverse relaxation mechanisms in articular cartilage

Relaxation rates in the rotating frame (R1rho) and spin-spin relaxation rates (R2) were measured in articular cartilage at various orientations of cartilage layer to the static magnetic field (B0), at various spin locking field strengths and at two different static magnetic field strengths. It was found that R1rho in the deep radial zone depended on the orientation of specimens in the magnet and decreased with increasing the spin locking field strength. In contrast, R1rho values in the transitional zone were nearly independent of the specimen orientation and the spin locking field strength. Measurements of the same specimens at 2.95 and 7.05 T showed an increase of R1rho and most R2 values with increasing B0. The inverse B0 dependence of some R2 values was probably due to a multicomponent character of the transverse magnetization decay. The experiments revealed that the dominant T1rho and T2 relaxation mechanism at B0 < or = 3 T is a dipolar interaction due to slow anisotropic motion of water molecules in the collagen matrix. On average, the contribution of scalar relaxation due to rapid proton exchange in femoral head cartilage at 2.95 T is about 6% or less of the total R1rho at the spin locking field of 1000 Hz.     

Determination of blood longitudinal relaxation time (T1) at high magnetic field strengths

In this study, a circulation system was used to measure T(1) values of bovine blood under physiological conditions at field strengths of 4.7, 7 and 9.4 T. Results show that T(1) increases linearly with magnetic field B(0) and can be described with the equation T(1)=129 ms/T B(0)+1167 ms for magnetic field strengths between 1.5 and 9.4 T.     

Solid-state S MAS NMR of inorganic sulfates

Solid-state (33)S MAS NMR spectra of a variety of inorganic sulfates have been obtained at magnetic field strengths of 4.7, 14.1, 17.6, and 18.8 T. Some of the difficulties associated with obtaining natural abundance (33)S NMR spectra have been overcome by using a high magnetic field strength and magic angle spinning (MAS). Multiple factors were considered when analyzing the spectral linewidths, including magnetic field inhomogeneity, dipolar coupling, chemical shift anisotropy, chemical shift dispersion, and quadrupolar coupling. In most of these sulfate samples, quadrupolar coupling was the dominant line broadening mechanism. Nuclear electric quadrupolar coupling constants (C(q)) as large as 2.05 MHz were calculated using spectral simulation software. Spectral information from these new data are compared with X-ray measurements and GAUSSIAN 98W calculations. A general correlation was observed between the magnitude of the C(q) and the increasing difference between S-O bond distances within the sulfate groups. Solid-state (33)S spin-lattice (T(1)) relaxation times were measured and show a significant reduction in T(1) for the hydrated sulfates. This is most likely the result of the modulation of the time-dependent electric field gradient at the nuclear site by motion of water molecules. This information will be useful in future efforts to use (33)S NMR in the compositional and structural analysis of sulfur containing materials.     

Solid-state 33S MAS NMR of inorganic sulfates

Solid-state (33)S MAS NMR spectra of a variety of inorganic sulfates have been obtained at magnetic field strengths of 4.7, 14.1, 17.6, and 18.8 T. Some of the difficulties associated with obtaining natural abundance (33)S NMR spectra have been overcome by using a high magnetic field strength and magic angle spinning (MAS). Multiple factors were considered when analyzing the spectral linewidths, including magnetic field inhomogeneity, dipolar coupling, chemical shift anisotropy, chemical shift dispersion, and quadrupolar coupling. In most of these sulfate samples, quadrupolar coupling was the dominant line broadening mechanism. Nuclear electric quadrupolar coupling constants (C(q)) as large as 2.05 MHz were calculated using spectral simulation software. Spectral information from these new data are compared with X-ray measurements and GAUSSIAN 98W calculations. A general correlation was observed between the magnitude of the C(q) and the increasing difference between S-O bond distances within the sulfate groups. Solid-state (33)S spin-lattice (T(1)) relaxation times were measured and show a significant reduction in T(1) for the hydrated sulfates. This is most likely the result of the modulation of the time-dependent electric field gradient at the nuclear site by motion of water molecules. This information will be useful in future efforts to use (33)S NMR in the compositional and structural analysis of sulfur containing materials.     

A field-sweep/field-lock system for superconducting magnets--Application to high-field EPR

We describe a field-lock/field-sweep system for the use in superconducting magnets. The system is based on a commercially available field mapping unit and a custom designed broad-band 1H NMR probe. The NMR signal of a small water sample is used in a feedback loop to set and control the magnetic field to high accuracy. The current instrumental configuration allows field sweeps of +/-0.4 T and a resolution of up to 10(-5) T (0.1 G) and the performance of the system is demonstrated in a high-field electron paramagnetic resonance (EPR) application. The system should also be of utility in other experiments requiring precise and reproducible sweeps of the magnetic field such as DNP, ENDOR or PELDOR.     

Nuclear magnetic resonance for cultural heritage

Nuclear magnetic resonance (NMR) portable devices are now being used for nondestructive in situ analysis of water content, pore space structure and protective treatment performance in porous media in the field of cultural heritage. It is a standard procedure to invert T(1) and T(2) relaxation data of fully water-saturated samples to get "pore size" distributions, but the use of T(2) requires great caution. It is well known that dephasing effects due to water molecule diffusion in a magnetic field gradient can affect transverse relaxation data, even if the smallest experimentally available half echo time tau is used in Carr-Purcell-Meiboom-Gill experiments. When a portable single-sided NMR apparatus is used, large field gradients due to the instrument, at the scale of the sample, are thought to be the dominant dephasing cause. In this paper, T(1) and T(2) (at different tau values) distributions were measured in natural (Lecce stone) and artificial (brick samples coming from the Greek-Roman Theatre of Taormina) porous media of interest for cultural heritage by a standard laboratory instrument and a portable device. While T(1) distributions do not show any appreciable effect from inhomogeneous fields, T(2) distributions can show strong effects, and a procedure is presented based on the dependence of 1/T(2) on tau to separate pore-scale gradient effects from sample-scale gradient effects. Unexpectedly, the gradient at the pore scale can be, in some cases, strong enough to make negligible the effects of gradients at the sample scale of the single-sided device.     

Correction of local B0 shifts in 3D EPSI of the human brain at 4 T

High-spatial-resolution acquisition (HR) was previously proposed for 3D echo-planar spectroscopic imaging (EPSI) in combination with a high-spatial-resolution water reference EPSI data set to minimize inhomogeneous spectral line broadening, allowing for local frequency shift (B(0) shift) correction in human brain metabolite maps at 1.5 T (Ebel A et al., Magn. Reson. Imaging 21:113-120, 2003). At a higher magnetic field strength, B(0), increased field inhomogeneities typically lead to increased line broadening. Additionally, increased susceptibility variations render shimming of the main magnetic field over the whole head more difficult. This study addressed the question whether local B(0)-shift correction still helps limit line broadening in whole-brain 3D EPSI at higher magnetic fields. The combination of HR and local B(0)-shift correction to limit line broadening was evaluated at 4 T. Similar to the results at 1.5 T, the approach provided a high yield of voxels with good spectral quality for 3D EPSI, resulting in improved brain coverage.     

Electric field measurements and computational modeling at ultrahigh-field MRI

While magnetic resonance images essentially contain a map of the both circularly polarized components of the RF transverse magnetic fields (B(1) field), the thermal heat and electromagnetic power deposition is generated by the associated electric fields. Measurement of electric field distributions/intensities across a sample yields an indirect indication of possible cause of heating within the sample and potentially enables the detection of "hot spots," which can be present within inhomogeneous radiofrequency (RF) fields, such as the case with magnetic resonance imaging at high field strength. As a result, establishing a valid technique for direct measurements of the electric field and its correlation, obtained using computational electromagnetics, is essential in assessing (1) the safety of the RF coil designs and (2) the validity of the calculations. In this work, a probe was built and used to measure the transverse electric field (E(1) field) distributions within an empty 8 T (tuned to 340 MHz) RF head coil and within a saline water phantom loaded in the same coil. The measured E(1) field distributions were favorably compared to the distributions obtained utilizing a finite difference time domain in-house package.