• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

噪声在正电子发射断层扫描的全蒙特卡罗最大似然期望最大化算法及双矩阵重建中的影响。

The influence of noise in full Monte Carlo ML-EM and dual matrix reconstructions in positron emission tomography.

作者信息

Rehfeld Niklas, Alber Markus

机构信息

Sektion für Biomedizinische Physik, Universitätsklinikum Tübingen, Hoppe-Seyler-Str 3, 72076 Tübingen, Germany.

出版信息

Med Phys. 2006 Sep;33(9):3498-507. doi: 10.1118/1.2239165.

DOI:10.1118/1.2239165
PMID:17022246
Abstract

Monte Carlo (MC) simulations in positron emission tomography (PET) play an important role in detector modeling and algorithm testing. Whereas the simulations are widely used in a forward projection manner to accomplish this task, ideally they should be included into the reconstruction process itself. It is therefore desirable to investigate the convergence properties and the propagation of MC noise of these kinds of reconstruction algorithms. MC simulations were integrated into the maximum likelihood expectation maximization (ML-EM) algorithm in two different ways. In the full matrix approach the system matrix was calculated by running MC simulations, including scatter. This matrix was used in both the projector and the backprojector. In the dual matrix (DM) approach, MC simulations were used to incorporate scatter in the projector, whereas the backprojector only comprised attenuation. Repeated reconstructions with different MC seeds allowed a statistical analysis of the error at each iteration step and made it possible to investigate separately the propagation of the MC noise that was introduced by the sinogram, by the projector, and by the matrix. Both approaches resulted in similar images, but the DM approach with unmatched projector and backprojector yielded a faster initial convergence when compared to the ideal full matrix approach. The analysis of the noise sources for the modeled single ring scanner in full matrix reconstruction showed that the noise introduced by the matrix became comparable to the noise introduced by the sinogram when using a matrix that was simulated with 10,000 emissions/voxel.

摘要

正电子发射断层扫描(PET)中的蒙特卡罗(MC)模拟在探测器建模和算法测试中发挥着重要作用。虽然这些模拟广泛用于前向投影方式来完成此任务,但理想情况下,它们应纳入重建过程本身。因此,研究这类重建算法的收敛特性和MC噪声的传播是很有必要的。MC模拟以两种不同方式集成到最大似然期望最大化(ML-EM)算法中。在全矩阵方法中,通过运行包括散射的MC模拟来计算系统矩阵。该矩阵用于投影仪和反投影仪。在双矩阵(DM)方法中,MC模拟用于在投影仪中纳入散射,而反投影仪仅包含衰减。使用不同的MC种子进行重复重建,可以对每个迭代步骤的误差进行统计分析,并能够分别研究由正弦图、投影仪和矩阵引入的MC噪声的传播。两种方法都得到了相似的图像,但与理想的全矩阵方法相比,投影仪和反投影仪不匹配的DM方法产生了更快的初始收敛。对全矩阵重建中建模的单环扫描仪的噪声源分析表明,当使用以10,000次发射/体素模拟的矩阵时,矩阵引入的噪声与正弦图引入的噪声相当。

相似文献

1
The influence of noise in full Monte Carlo ML-EM and dual matrix reconstructions in positron emission tomography.噪声在正电子发射断层扫描的全蒙特卡罗最大似然期望最大化算法及双矩阵重建中的影响。
Med Phys. 2006 Sep;33(9):3498-507. doi: 10.1118/1.2239165.
2
Reconstruction of 2D PET data with Monte Carlo generated system matrix for generalized natural pixels.使用蒙特卡罗生成的系统矩阵对广义自然像素进行二维正电子发射断层扫描(PET)数据重建。
Phys Med Biol. 2006 Jun 21;51(12):3105-25. doi: 10.1088/0031-9155/51/12/008. Epub 2006 May 31.
3
Noise properties of the EM algorithm: II. Monte Carlo simulations.期望最大化算法的噪声特性:II. 蒙特卡罗模拟
Phys Med Biol. 1994 May;39(5):847-71. doi: 10.1088/0031-9155/39/5/005.
4
A residual correction method for high-resolution PET reconstruction with application to on-the-fly Monte Carlo based model of positron range.一种适用于基于飞行时间蒙特卡罗的正电子射程模型的高分辨率 PET 重建的残差校正方法。
Med Phys. 2010 Feb;37(2):704-13. doi: 10.1118/1.3284980.
5
Noise characterization of block-iterative reconstruction algorithms: II. Monte Carlo simulations.块迭代重建算法的噪声特性:II. 蒙特卡洛模拟
IEEE Trans Med Imaging. 2005 Jan;24(1):112-21. doi: 10.1109/tmi.2004.836876.
6
Direct reconstruction of kinetic parameter images from dynamic PET data.从动态PET数据直接重建动力学参数图像。
IEEE Trans Med Imaging. 2005 May;24(5):636-50. doi: 10.1109/TMI.2005.845317.
7
A parallelizable compression scheme for Monte Carlo scatter system matrices in PET image reconstruction.正电子发射断层扫描(PET)图像重建中用于蒙特卡罗散射系统矩阵的可并行压缩方案。
Phys Med Biol. 2007 Jun 21;52(12):3421-37. doi: 10.1088/0031-9155/52/12/007. Epub 2007 May 17.
8
Noise and signal decoupling in maximum-likelihood reconstructions and Metz filters for PET brain images.PET脑图像最大似然重建和梅茨滤波器中的噪声与信号解耦
Phys Med Biol. 1994 Apr;39(4):735-50. doi: 10.1088/0031-9155/39/4/006.
9
Efficient fully 3-D iterative SPECT reconstruction with Monte Carlo-based scatter compensation.基于蒙特卡洛散射补偿的高效全三维迭代单光子发射计算机断层显像重建
IEEE Trans Med Imaging. 2002 Aug;21(8):867-77. doi: 10.1109/TMI.2002.803130.
10
Iterative image reconstruction for positron emission tomography based on a detector response function estimated from point source measurements.基于从点源测量估计的探测器响应函数的正电子发射断层扫描迭代图像重建。
Phys Med Biol. 2009 Jun 21;54(12):3709-25. doi: 10.1088/0031-9155/54/12/007. Epub 2009 May 28.