一种基于毛细管X光透镜的微型锥束CT扫描仪

周腊珍; 夏文静; 许倩倩; 陈赞; 李坊佐; 刘志国; 孙天希

doi:10.7498/aps.71.20212195

摘要

活体小动物成像系统是疾病研究、新药开发的重要组成部分. 其中, X射线微型锥束计算机断层成像(X-ray micro cone-beam computed tomography, Micro-CBCT)能实现数十至数百微米空间分辨率的解剖结构成像研究. Micro-CBCT成像仪的一个关键挑战是其空间和对比度分辨率主要取决于X射线源焦斑大小、探测器分辨率和系统几何结构等因素. 为提高Micro-CBCT的空间分辨率、对比度分辨率和成像均一性, 本文基于毛细管X光透镜研制了一款能够调控照射X射线束斑孔径的Micro-CBCT扫描仪, 用于小动物成像研究. 此系统由微焦斑X射线源、非晶硅平板探测器、旋转工作台和控制电脑组成, 并采用Feldkamp-Daivs-Kress算法重建投影图像. 对该系统的性能进行了测试, 结果表明, 系统在10%调制传递函数下的空间分辨率为9.1 lp/mm, 提高了1.35倍. 同时, 由于毛细管X光透镜对低能X射线的吸收和散射抑制作用, 实现了2倍以上的对比度增强, 减轻了多色X射线束硬化效应引起的图像均一性恶化问题. 应用该Micro-CBCT系统对麻醉小鼠进行了活体成像, 验证了该系统在小动物成像研究中的实用性.

关键词:

Abstract

In-vivo small animal imaging system is an important part of disease research and new drug development. It is essential for living small animal imaging system to be able to provide the anatomical structure, molecular and functional information. The X-ray micro cone-beam computed tomography (micro-CBCT) can perform longitudinal study with a resolution of tens-to-hundreds of microns in a short imaging time at a relatively low cost. Furthermore, it is easy to combine with other modalities to provide abundant information about small animals. A key challenge to the micro-CBCT scanner is that its spatial and contrast resolution determined primarily by the X-ray focal spot size, the detector element size, and the system geometry. Aiming to improve the spatial resolution, contrast resolution, and imaging uniformity of the micro-CBCT system, we use the X-ray polycapillary optics for adjusting the X-ray source. A micro-CBCT based on X-ray polycapillary optics with a large field of view is constructed for the small animal imaging study. The micro-CBCT system is composed of microfocus X-ray tube with an attached polycapillary focusing X-ray lens, amorphous silicon-based flat panel detector, rotation stage, and controlling PC. The Feldkamp-Daivs-Kress (FDK) algorithm is adopted to reconstruct the image. The system performances are evaluated. The magnification of this micro-CBCT system is 1.97. The results show that the spatial resolution of the system at 10% modulation transfer function (MTF) is 9.1 lp/mm, which is 1.35 times higher than that in the case of no optics. The image uniformity deterioration caused by hardening effect is effectively alleviated by filtrating the low energy X-rays with the X-ray polycapillary optics and the contrast enhancement is more than twice. The anesthetic rats are imaged with this micro-CBCT system in vivo and the practicability of the system in small animal imaging research is verified.

Keywords:

作者及机构信息

1.
赣南医学院医学信息工程学院, 赣州　341000

2.
赣南医学院, 组织工程材料与生物制造江西省重点实验室, 赣州　341000

3.
北京师范大学核科学与技术学院, 射线束技术教育部重点实验室, 北京　100875

通信作者: 李坊佐, lfz880920@163.com

基金项目: 国家自然科学基金(批准号: 11865003)、江西省自然科学基金(批准号: 20192BAB212008)和赣南医学院基金(批准号: QD201805)资助的课题

Authors and contacts

1.
School of Medical Information Engineering, Gannan Medical University, Ganzhou 341000, China

2.
Key Laboratory of Biomaterials and Biofabrication in Tissue Engineering of Jiangxi Province, Gannan Medical University, Ganzhou 341000, China

3.
Key Laboratory of Beam Technology Ministry of Education, College of Nuclear Science and Technology, Beijing Normal University, Beijing 100875, China

Corresponding author: Li Fang-Zuo, lfz880920@163.com

Funds: Project supported by the National Natural Science Foundation of China (Grant No. 11865003), the Natural Science Foundation of Jiangxi Province, China (Grant No. 20192BAB212008), and the Gannan Medicla University Foundation, China (Grant No. QD201805).

文章全文 : translate this paragraph

参考文献

[1]	Gregory S G, Sekhon M, Schein J, et al. 2002 Nature 418 743 Google Scholar
[2]	Ntziachristos V, Ripoll J, Wang L V, Weissleder R 2005 Nat. Biotechnol. 23 313 Google Scholar
[3]	Guerra A D, Belcari N 2007 Nucl. Instrum. Meth. Phys. Res. A 583 119 Google Scholar
[4]	Badea C T, Drangova M, Holdsworth D W, Johnson G A 2008 Phys. Med. Biol. 53 319 Google Scholar
[5]	Jan M L, Ni Y C, Chen K W, Ching H 2006 Nucl. Instrum. Meth. Phys. Res. A 569 314 Google Scholar
[6]	Biederer J, Mirsadraee S, Beer M, Molinari F, Puderbach M 2012 Insights Into Imaging 3 373 Google Scholar
[7]	Hoyer C, Gass N, Fahr W W, Sartorius A 2014 Neuropsychobiology 69 187 Google Scholar
[8]	Kunjachan S, Ehling J, Storm G, Kiessling F, Lammers T 2015 Chem. Rev. 115 10907 Google Scholar
[9]	Eghtedari M, Oraevsky A, Copland J A, Kotov N A, Conjusteau A, Motamedi M 2007 Nano Lett. 7 1914 Google Scholar
[10]	Taruttis A, Ntziachristos V 2015 Nat. Photonics 9 219 Google Scholar
[11]	Paulus M J, Gleason S S, Kennel S J, Hunsicker P R, Johnson D K 2000 Neoplasia 2 62 Google Scholar
[12]	罗召洋, 杨孝全, 孟远征, 邓勇 2010 物理学报 58 8237 Google Scholar Luo Z Y, Yang X Q, Meng Y Z, Deng Y 2010 Acta Phys. Sin. 58 8237 Google Scholar
[13]	魏星, 闫镔, 张峰, 李永丽, 席晓琦, 李磊 2014 物理学报 63 058702 Google Scholar Wei X, Yan B, Zhang F, Li Y L, Xi X Q, Li L 2014 Acta Phys. Sin. 63 058702 Google Scholar
[14]	Mazel V, Reiche I, Busignies V, Walter P, Tchoreloff P 2011 Talanta 85 556 Google Scholar
[15]	Sun T, Liu Z, Li Y, Lin X, Wang G, Zhu G, Xu Q, Luo P, Pan Q, Liu H 2010 Nucl. Instrum. Meth. Phys. Res. A 622 295 Google Scholar
[16]	Macdonald C A, Gibson W M 2003 X-Ray Spectrom. 32 258 Google Scholar
[17]	Albertini V R, Paci B, Generosi A, Dabagov S B, Kumakhov M A 2007 Spectrochim. Acta B 62 1203 Google Scholar
[18]	Huang R, Bilderback D H 2006 J. Synchrotron Radiat. 13 74 Google Scholar
[19]	Balaic D X, Barnea Z, Nugent K A, Garrett R F, Wilkins S W 1996 J. Synchrotron Radiat. 3 289 Google Scholar
[20]	MacDonald C A, Owens S M, Gibson W M 1999 J. Appl. Crystallogr. 32 160 Google Scholar
[21]	Bjeoumikhov A, Bjeoumikhova S, Langhoff N, Wedell R 2005 Appl. Phys. Lett. 86 144102 Google Scholar
[22]	Sun T, Liu Z, Ding X 2007 Nucl. Instrum. Meth. Phys. Res. B 262 153 Google Scholar
[23]	Sun T, Peng S, Liu Z, Sun W, Ma Y, Ding X 2013 J. Appl. Crystallogr. 46 1880 Google Scholar
[24]	Sun T, Macdonald C A 2013 J. Appl. Phys. 113 053104 Google Scholar
[25]	Lamb J S, Bilderback D H, Pollack L, Kwok L, Smilgies D M 2007 J. Appl. Crystallogr. 40 193 Google Scholar
[26]	Barrea R A, Huang R, Cornaby S, Bilderback D H, Irving T C 2009 J. Synchrotron Radiat. 16 76 Google Scholar
[27]	Zeng X, Duewer F, Feser M, Huang C, Lyon A, Tkachuk A, Yun W 2008 Appl. Opt. 47 2376 Google Scholar
[28]	Li F, Liu Z, Sun T, Jiang B, Zhu Y 2016 J. Chem. Phys. 144 104201 Google Scholar
[29]	Li F, Liu Z, Sun T 2016 J. Appl. Crystallogr. 49 627 Google Scholar
[30]	Li F, Liu Z, Sun T 2016 Rev. Sci. Instrum. 87 093106 Google Scholar
[31]	Li F, Liu Z, Sun T 2016 Food Chem. 210 435 Google Scholar
[32]	Li F, Liu Z, Sun T, Ma Y, Ding X 2015 Food Control 54 120 Google Scholar
[33]	Abreu C C, Kruger D G, MacDonald C A, Mistretta C A, Peppler W W, Xiao Q F 1995 Med. Phys. 22 1793 Google Scholar
[34]	Goertzen A L, Nagarkar V, Street R A, Paulus M J, Boone J M, Cherry S R 2004 Phys. Med. Biol. 49 5251 Google Scholar
[35]	Kim H K, Min K C, Achterkirchen T, Lee W 2009 IEEE Trans. Nucl. Sci. 56 1179 Google Scholar
[36]	Feldkamp L A, Davis L C, Kress J W 1984 J. Opt. Soc. Am. A 1 612 Google Scholar
[37]	Flannery B P, Deckman H W, Roberge W G, D'Amico K L 1987 Science 237 1439 Google Scholar
[38]	Sun T, Ding X 2005 J. Appl. Phys. 97 124904 Google Scholar
[39]	Kai Y, Kwan A L C, Miller D W F, Boone J M 2006 Med. Phys. 33 1695 Google Scholar
[40]	Kwan A L C, Boone J M, Yang K, Huang S Y 2007 Med. Phys. 34 275
[41]	余晓锷, 占杰, 李萍, 李婵娟 2006 第四军医大学学报 27 978 Google Scholar Yu X E, Zhan J, Li P, Li C J 2006 J. Fourth Mil. Med. Univ. 27 978 Google Scholar

施引文献

图 1 X射线源焦斑大小、SOD和SDD共同决定了Micro-CBCT的有效探测器孔径大小　(a) 焦点大小与有效探测器孔径α成正比; (b) SOD/SDD比值与有效探测器孔径α成正比

Fig. 1. X-ray tube focal spot size, SOD and SDD jointly determine the effective detector aperture size of the micro-CT system: (a) Focal spot size is proportional to the effective detector aperture (α); (b) ratio of SOD/SDD is proportional to the effective detector aperture (α).

下载: 全尺寸图片幻灯片

图 2 X射线焦斑大小的半影效应

Fig. 2. Penumbra effect of X-ray focal spot size.

下载: 全尺寸图片幻灯片

图 3 Micro-CBCT系统, 该系统由一个结合PFXRL的微聚焦X射线源、一个旋转样品台和一个非晶硅平板探测器组成　(a) Micro-CBCT原理图; (b) Micro-CBCT实物图; (c) 采用的PFXRL实物图

Fig. 3. Micro-CBCT system. The system consists of a microfocus X-ray source combined with a PFXRL, a rotating sample stage and an amorphous silicon-based FPD: (a) Micro-CBCT schematic diagram; (b) desktop micro-CBCT system; (c) the PFXRL.

下载: 全尺寸图片幻灯片

图 4 PFXRL的出口焦斑尺寸和收敛度随X射线能量的依赖关系

Fig. 4. Energy dependence of the output focal spot size and convergence for the PFXRL, respectively.

下载: 全尺寸图片幻灯片

图 5 PFXRL的传输效率和能量密度增益随X射线能量的依赖关系

Fig. 5. Energy dependence of transmission efficiency and gain in power density of the PFXRL, respectively.

下载: 全尺寸图片幻灯片

图 6 使用和不使用PFXRL两种条件下的Micro-CBCT图像和对应的MTF　(a)使用PFXRL; (b)不使用PFXRL; (c) MTF曲线

Fig. 6. Measured images and corresponding MTF of the micro-CBCT system with and without PFXRL: (a) With PFXRL; (b) without PFXRL; (c) MTF curves.

下载: 全尺寸图片幻灯片

图 7 对于测量的水模, 在使用和不使用PFXRL下的Micro-CBCT系统对比度分辨率与管电压的关系

Fig. 7. Measured contrast resolution of Micro-CBCT system as a function of tube voltages for water phantom.

下载: 全尺寸图片幻灯片

图 8 水模的均匀性响应　(a) 不使用PFXRL, 重建的水模中平横断面图像及绿线对应的CT值; (b) 使用PFXRL, 重建的水模中平横断面图像及绿线对应的CT值; (c) 采用0.5 mm厚的铝片附加滤过, 重建的水模中平横断面图像及绿线对应的CT值. 空气和水的CT值分别归一化为0和50

Fig. 8. Uniformity response of the water phantom: (a) Reconstructed transaxial image of the uniformity phantom without using PFXRL and radial signal profile taken from the green line; (b) reconstructed transaxial image of the uniformity phantom with using PFXRL and radial signal profile taken from the green line; (c) reconstructed transaxial image of the uniformity phantom with a 0.5 mm thick aluminum sheet as filter and radial signal profile taken from the green line. The CT values of air and water are normalized to 0 and 50, respectively.

下载: 全尺寸图片幻灯片

图 9 水模的噪声响应　(a)不使用PFXRL (附加滤过: 0.5 mm Al); (b)使用PFXRL

Fig. 9. Noise response of the water phantom: (a) Without PFXRL (additional filtration: 0.5 mm Al); (b) with PFXRL.

下载: 全尺寸图片幻灯片

图 10 小鼠Micro-CBCT成像　(a)使用PFXRL; (b)不使用PFXRL

Fig. 10. CT images of rats: (a) With PFXRL; (b) without PFXRL.

下载: 全尺寸图片幻灯片

图 11 麻醉小鼠横断面图像比较　(a)使用PFXRL; (b)不使用PFXRL

Fig. 11. Comparison of axial images of the anesthetized mice: (a) With PFXRL; (b) without PFXRL.

下载: 全尺寸图片幻灯片

图 12 麻醉小鼠肺、肾和下脊柱区域的基于PFXRL的Micro-CBCT图像. 每个图像的窗宽窗位设置不同以呈现出感兴趣的结构. 横断面((a), (d), (g))、冠状面((b), (e), (h))和矢状面((c), (f), (i))切片展示了各向同性的空间分辨率和好的软组织对比度. 肺内支气管结构、肾脏与周围的肌肉和脂肪、椎骨和椎间隙都清晰可见. 图像中的垂直比例尺显示1 cm的间距

Fig. 12. PFXRL-based Micro-CBCT images of the lung, kidney and lower spine of the anesthetized mice. The window and level settings are varied in each image to allow visualization of the structures of interest. Axial ((a), (d), (g)) , coronal ((b), (e), (h)) , and sagittal ((c), (f), (i)) slices qualitatively demonstrate isotropic spatial resolution, with excellent soft-tissue contrast in each case. Bronchial structure within the lungs is clearly identifiable, the kidney is well delineated from surrounding muscle and fat, and fine detail in the vertebrae and intervertebral spaces is demonstrated. The vertical scale in the images shows 1 cm spacing.

下载: 全尺寸图片幻灯片

表 1 PFXRL的基本参数

Table 1. Parameters of the PFXRL.

	PFXRL
Length /mm	69.4
Input focal distance /mm	76.3
Output focal distance /mm	20.1
Diameter of IFS at 17.4 keV /${\mu }\mathrm{m}$	169.2
Diameter of OFS at 17.4 keV /${\mu }\mathrm{m}$	46.7
Channel inner diameter of capillary at input/output /μm	10.4

下载: 导出CSV

[1]	Gregory S G, Sekhon M, Schein J, et al. 2002 Nature 418 743 Google Scholar
[2]	Ntziachristos V, Ripoll J, Wang L V, Weissleder R 2005 Nat. Biotechnol. 23 313 Google Scholar
[3]	Guerra A D, Belcari N 2007 Nucl. Instrum. Meth. Phys. Res. A 583 119 Google Scholar
[4]	Badea C T, Drangova M, Holdsworth D W, Johnson G A 2008 Phys. Med. Biol. 53 319 Google Scholar
[5]	Jan M L, Ni Y C, Chen K W, Ching H 2006 Nucl. Instrum. Meth. Phys. Res. A 569 314 Google Scholar
[6]	Biederer J, Mirsadraee S, Beer M, Molinari F, Puderbach M 2012 Insights Into Imaging 3 373 Google Scholar
[7]	Hoyer C, Gass N, Fahr W W, Sartorius A 2014 Neuropsychobiology 69 187 Google Scholar
[8]	Kunjachan S, Ehling J, Storm G, Kiessling F, Lammers T 2015 Chem. Rev. 115 10907 Google Scholar
[9]	Eghtedari M, Oraevsky A, Copland J A, Kotov N A, Conjusteau A, Motamedi M 2007 Nano Lett. 7 1914 Google Scholar
[10]	Taruttis A, Ntziachristos V 2015 Nat. Photonics 9 219 Google Scholar
[11]	Paulus M J, Gleason S S, Kennel S J, Hunsicker P R, Johnson D K 2000 Neoplasia 2 62 Google Scholar
[12]	罗召洋, 杨孝全, 孟远征, 邓勇 2010 物理学报 58 8237 Google Scholar Luo Z Y, Yang X Q, Meng Y Z, Deng Y 2010 Acta Phys. Sin. 58 8237 Google Scholar
[13]	魏星, 闫镔, 张峰, 李永丽, 席晓琦, 李磊 2014 物理学报 63 058702 Google Scholar Wei X, Yan B, Zhang F, Li Y L, Xi X Q, Li L 2014 Acta Phys. Sin. 63 058702 Google Scholar
[14]	Mazel V, Reiche I, Busignies V, Walter P, Tchoreloff P 2011 Talanta 85 556 Google Scholar
[15]	Sun T, Liu Z, Li Y, Lin X, Wang G, Zhu G, Xu Q, Luo P, Pan Q, Liu H 2010 Nucl. Instrum. Meth. Phys. Res. A 622 295 Google Scholar
[16]	Macdonald C A, Gibson W M 2003 X-Ray Spectrom. 32 258 Google Scholar
[17]	Albertini V R, Paci B, Generosi A, Dabagov S B, Kumakhov M A 2007 Spectrochim. Acta B 62 1203 Google Scholar
[18]	Huang R, Bilderback D H 2006 J. Synchrotron Radiat. 13 74 Google Scholar
[19]	Balaic D X, Barnea Z, Nugent K A, Garrett R F, Wilkins S W 1996 J. Synchrotron Radiat. 3 289 Google Scholar
[20]	MacDonald C A, Owens S M, Gibson W M 1999 J. Appl. Crystallogr. 32 160 Google Scholar
[21]	Bjeoumikhov A, Bjeoumikhova S, Langhoff N, Wedell R 2005 Appl. Phys. Lett. 86 144102 Google Scholar
[22]	Sun T, Liu Z, Ding X 2007 Nucl. Instrum. Meth. Phys. Res. B 262 153 Google Scholar
[23]	Sun T, Peng S, Liu Z, Sun W, Ma Y, Ding X 2013 J. Appl. Crystallogr. 46 1880 Google Scholar
[24]	Sun T, Macdonald C A 2013 J. Appl. Phys. 113 053104 Google Scholar
[25]	Lamb J S, Bilderback D H, Pollack L, Kwok L, Smilgies D M 2007 J. Appl. Crystallogr. 40 193 Google Scholar
[26]	Barrea R A, Huang R, Cornaby S, Bilderback D H, Irving T C 2009 J. Synchrotron Radiat. 16 76 Google Scholar
[27]	Zeng X, Duewer F, Feser M, Huang C, Lyon A, Tkachuk A, Yun W 2008 Appl. Opt. 47 2376 Google Scholar
[28]	Li F, Liu Z, Sun T, Jiang B, Zhu Y 2016 J. Chem. Phys. 144 104201 Google Scholar
[29]	Li F, Liu Z, Sun T 2016 J. Appl. Crystallogr. 49 627 Google Scholar
[30]	Li F, Liu Z, Sun T 2016 Rev. Sci. Instrum. 87 093106 Google Scholar
[31]	Li F, Liu Z, Sun T 2016 Food Chem. 210 435 Google Scholar
[32]	Li F, Liu Z, Sun T, Ma Y, Ding X 2015 Food Control 54 120 Google Scholar
[33]	Abreu C C, Kruger D G, MacDonald C A, Mistretta C A, Peppler W W, Xiao Q F 1995 Med. Phys. 22 1793 Google Scholar
[34]	Goertzen A L, Nagarkar V, Street R A, Paulus M J, Boone J M, Cherry S R 2004 Phys. Med. Biol. 49 5251 Google Scholar
[35]	Kim H K, Min K C, Achterkirchen T, Lee W 2009 IEEE Trans. Nucl. Sci. 56 1179 Google Scholar
[36]	Feldkamp L A, Davis L C, Kress J W 1984 J. Opt. Soc. Am. A 1 612 Google Scholar
[37]	Flannery B P, Deckman H W, Roberge W G, D'Amico K L 1987 Science 237 1439 Google Scholar
[38]	Sun T, Ding X 2005 J. Appl. Phys. 97 124904 Google Scholar
[39]	Kai Y, Kwan A L C, Miller D W F, Boone J M 2006 Med. Phys. 33 1695 Google Scholar
[40]	Kwan A L C, Boone J M, Yang K, Huang S Y 2007 Med. Phys. 34 275
[41]	余晓锷, 占杰, 李萍, 李婵娟 2006 第四军医大学学报 27 978 Google Scholar Yu X E, Zhan J, Li P, Li C J 2006 J. Fourth Mil. Med. Univ. 27 978 Google Scholar

[1]	廖可梁, 何其利, 宋杨, 李荣刚, 宋茂华, 李盼云, 赵海峰, 刘鹏, 朱佩平. 基于实验室光源的透射X射线纳米分辨显微镜研制. 物理学报, 2024, 73(17): 178701. doi: 10.7498/aps.73.20240727
[2]	陈子涵, 宋梦齐, 陈恒, 王志立. 双三角形相位光栅X射线干涉仪的条纹可见度. 物理学报, 2023, 72(14): 148701. doi: 10.7498/aps.72.20230461
[3]	邓文娟, 朱斌, 王壮飞, 彭新村, 邹继军. 变掺杂变组分Al_xGa_1–xAs/GaAs反射式光电阴极分辨力特性. 物理学报, 2022, 71(15): 157901. doi: 10.7498/aps.71.20220244
[4]	鞠晓璐, 李可, 余福成, 许明伟, 邓彪, 李宾, 肖体乔. 电解池电化学反应过程的运动衬度X射线成像. 物理学报, 2022, 71(14): 144101. doi: 10.7498/aps.71.20220339
[5]	刘尚阔, 王涛, 李坤, 曹昆, 张玺斌, 周艳, 赵建科, 姚保利. 光源光谱特性对空间相机调制传递函数检测的影响. 物理学报, 2021, 70(13): 134208. doi: 10.7498/aps.70.20201575
[6]	刘俊, 姜其立, 帅麒麟, 李融武, 潘秋丽, 程琳, 王荣. 一种点光源的自适应束斑X射线衍射仪的研制. 物理学报, 2021, 70(1): 010701. doi: 10.7498/aps.70.20201228
[7]	张美, 李奎念, 李阳, 盛亮, 张艳红. 一种新型的液闪阵列成像屏空间分辨特性. 物理学报, 2020, 69(6): 062801. doi: 10.7498/aps.69.20191545
[8]	郝未倩, 梁忠诚, 刘肖尧, 赵瑞, 孔梅梅, 关建飞, 张月. 分形结构稀疏孔径阵列的成像性能. 物理学报, 2019, 68(19): 199501. doi: 10.7498/aps.68.20190818
[9]	戚俊成, 刘宾, 陈荣昌, 夏正德, 肖体乔. X射线光场成像技术研究. 物理学报, 2019, 68(2): 024202. doi: 10.7498/aps.68.20181555
[10]	姜其立, 段泽明, 帅麒麟, 李融武, 潘秋丽, 程琳. 一种毛细管聚焦的微束X射线衍射仪. 物理学报, 2019, 68(24): 240701. doi: 10.7498/aps.68.20190497
[11]	郑鑫, 武鹏飞, 饶瑞中. 天光背景下混浊大气中成像质量的分析方法. 物理学报, 2018, 67(8): 088701. doi: 10.7498/aps.67.20172625
[12]	张敏睿, 贺正权, 汪韬, 田进寿. 偏振双向衰减对光学成像系统像质影响的矢量平面波谱理论分析. 物理学报, 2017, 66(8): 084202. doi: 10.7498/aps.66.084202
[13]	段亚轩, 刘尚阔, 陈永权, 薛勋, 赵建科, 高立民. Bayer滤波型彩色相机调制传递函数测量方法. 物理学报, 2017, 66(7): 074204. doi: 10.7498/aps.66.074204
[14]	杜杨, 刘鑫, 雷耀虎, 黄建衡, 赵志刚, 林丹樱, 郭金川, 李冀, 牛憨笨. X射线光栅微分相衬成像视场分析. 物理学报, 2016, 65(5): 058701. doi: 10.7498/aps.65.058701
[15]	刘鑫, 易明皓, 郭金川. 线焦斑X射线源成像. 物理学报, 2016, 65(21): 219501. doi: 10.7498/aps.65.219501
[16]	陈晓虎, 王晓方, 张巍巍, 汪文慧. 相位型波带板应用于大尺度X射线源成像的分析与模拟. 物理学报, 2013, 62(1): 015208. doi: 10.7498/aps.62.015208
[17]	王晓方, 王晶宇. 菲涅耳波带板应用于聚变靶的高分辨X射线成像分析. 物理学报, 2011, 60(2): 025212. doi: 10.7498/aps.60.025212
[18]	邹继军, 常本康, 杨智, 张益军, 乔建良. 指数掺杂GaAs光电阴极分辨力特性分析. 物理学报, 2009, 58(8): 5842-5846. doi: 10.7498/aps.58.5842
[19]	戚巽骏, 林斌, 曹向群, 陈钰清. 基于调制传递函数的光学低通滤波器评价模型与实验研究. 物理学报, 2008, 57(5): 2854-2859. doi: 10.7498/aps.57.2854
[20]	田进寿, 赵宝升, 吴建军, 赵卫, 刘运全, 张杰. 飞秒电子衍射系统中调制传递函数的理论计算. 物理学报, 2006, 55(7): 3368-3374. doi: 10.7498/aps.55.3368

计量

文章访问数: 5750
PDF下载量: 98
被引次数: 0

姓名
邮箱
手机号码
标题
留言内容
验证码

搜索

留言板