首页> 外文期刊>American Journal of Neuroradiology >Candidate Biomarkers of Extravascular Extracellular Space: A Direct Comparison of Apparent Diffusion Coefficient and Dynamic Contrast-Enhanced MR Imaging--Derived Measurement of the Volume of the Extravascular Extracellular Space in Glioblastoma Multiforme
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Candidate Biomarkers of Extravascular Extracellular Space: A Direct Comparison of Apparent Diffusion Coefficient and Dynamic Contrast-Enhanced MR Imaging--Derived Measurement of the Volume of the Extravascular Extracellular Space in Glioblastoma Multiforme

机译:血管外细胞间隙的候选生物标志物:表观扩散系数和动态对比增强MR成像的直接比较-胶质母细胞瘤中血管外细胞间隙的体积测量

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摘要

BACKGROUND AND PURPOSE: ADC measurements have been shown to have an inverse relationship with tumor cell density. DCE-MR imaging modeling techniques can produce a measurement of the ve, which would also be expected to have an inverse relationship with cell density. The objective of this study was to test the hypothesis that areas of increased cellularity, and therefore low ADC, would be expected to have a small EES (low ve). MATERIALS AND METHODS: Nineteen patients with GBM were recruited. All imaging was performed before surgery on a 3T MR imaging scanner. Imaging included diffusion tensor imaging, T1-weighted DCE-MR imaging, and anatomic sequences. Tumor VOIs were defined on the anatomic images and modified to contain only enhancing voxels. Parametric maps of ADC and ve were generated. Statistical analysis of ADC and ve was performed on both a voxel-by-voxel basis and comparison of median values. RESULTS: No correlation was demonstrated between ADC and ve in either a voxel-by-voxel analysis or comparison of median values (P = .124). CONCLUSIONS: This study failed to demonstrate a correlation between ADC and ve. This is important because it suggests that though the mechanisms underlying these parameters are theoretically similar, they actually reflect different aspects of tumor microenvironment. Consequently ADC and ve should be considered to provide independent information about the properties of the EES. Abbreviations: ADC, apparent diffusion coefficient • DCE-MR, dynamic contrast-enhanced MR • DWI, diffusion-weighted imaging • EES, extravascular extracellular space • FFE, fast-field echo • FLIRT, FMRIB Linear Image Registration Tool • FSL, FMRIB Software Library • FMRIB, Functional Magnetic Resonance Imaging of the Brain • GBM, glioblastoma multiforme • IAUC, initial area under the concentration curve • max, maximum • min, minimum • NSF, nephrogenic systemic fibrosis • ve, volume of the extravascular extracellular space per unit volume • VOI, volume of interest GBM is the most common and most aggressive primary brain tumor of adulthood. These tumors are highly heterogeneous and characterized by varying degrees of hypercellularity, cytoplasmic and nuclear pleomorphism, mitoses, and endothelial proliferation within any given tumor. A number of MR imaging–based techniques have been developed to probe the tumor microenvironment. DWI allows quantification of the degree of motion of free water molecules, resulting from Brownian motion. ADC maps, which represent the freedom of water molecules to diffuse within tissue, can be generated. Although it has recently been demonstrated that it is possible to obtain estimates of cell packing and cell diameter in vivo,1 the values of ADC measured by using practical clinical data acquisitions are influenced by a number of factors. ADC is affected not only by the volume of the EES but also by its spatial configuration, intracellular diffusion coefficients, and membrane permeability. However, it has been proposed that ADC is predominantly affected by extracellular geometry.2 Thus water molecules will diffuse less freely in tissue characterized by narrow complex extracellular spaces, which might be seen in a tumor with large numbers of small cells, such as lymphoma, rather than in tissue with a smaller number of large cells in which the EES is less tortuous and in tissue in which the size of the EES is greater. Pharmacokinetic modeling analysis of DCE-MR imaging data allows estimation of a number of parameters that affect the delivery and local distribution of the contrast molecules. One of these is a direct estimate of the leakage volume available for contrast distribution outside the vascular space. This value (ve) is therefore a direct estimate of the volume of the EES.3 Both of these techniques have been applied extensively in glioma. Changes in ADC have been demonstrated early after radiation therapy and predict treatment response (following administration of corticosteroids).4–7 These changes are thought to reflect alterations in cellular structure due to apoptosis and/or necrosis.4,5 A number of investigators have shown an inverse linear relationship between ADC and cell density in cerebral tumors.5,8–10 In addition, several studies have noted an inverse relationship with malignancy and ADC, with increasing histologic tumor grade associated with low ADC values,8,9,11,12 including high-grade tumors that were indistinguishable from low-grade tumors on conventional imaging.13 Most DCE-MR imaging studies in glioma have evaluated vascular parameters such as blood volume and permeability, while ve has generally been overlooked. The few studies that have examined ve have shown it to be of value in distinguishing intra- from extra-axial tumors14,15 and have shown it to exhibit a tendency to increase with increasing tumor grade.14,16 In addition, ve demonstrated sensitivity in identifying changes in response to treatment with corticosteroids, with decreases in ve occurring following treatment, presumably reflecting a reduction in edema.17,18 A number of groups have performed both DCE-MR imaging and diffusion imaging in gliomas.14,18,19 However, to the authors' knowledge, no direct comparison of ADC and ve has been made in this tumor group. The objective of this study was to test the hypothesis that areas of increased cellularity, and therefore low ADC, would be expected to have low ve. Materials and Methods Patients The local research ethics committee approved the study, and all patients gave informed consent before recruitment. Patients with potential GBMs were identified via the neuro-oncology multidisciplinary team meetings at Salford Royal National Health Service Foundation Trust. Patients younger than 18 years of age, those unfit for surgery, and individuals in whom MR imaging was contraindicated were excluded from the outset. All imaging was performed before surgery. All tumors were histologically confirmed as GBM by either surgical debulking or biopsy, and patients in whom GBM could not be histologically confirmed postoperatively were excluded. Corticosteroids have previously been shown to alter the measurement of DCE-MR imaging parameters.6 Withholding corticosteroid treatment was deemed unethical; therefore, all patients received corticosteroid treatment for a minimum of 48 hours before imaging as part of their standard clinical treatment and to standardize treatment across all subjects. None received any other form of treatment at the time of imaging. Data Acquisition Imaging was performed at the University of Manchester Magnetic Resonance Imaging Facility (Hope Hospital, Salford, United Kingdom) by using a sensitivity encoding head coil on a 3T Achieva system (Philips Medical Systems, Best, the Netherlands). Conventional anatomic sequences were chosen according to those used in routine clinical practice and included the following: axial T1-weighted inversion recovery (TR, 8.4 ms; TE, 3.8 ms; TI, 1150 ms; section thickness, 1.8 mm; 256 x 256; FOV, 240 x 240 x 324 mm), axial T2-weighted (TR, 3000 ms; TE, 80 ms; section thickness, 3.0 mm; 1024 x 1024; FOV, 266 x 266 x 135 mm), coronal T2-weighted fluid-attenuated inversion recovery (TR, 11 000 ms; TE, 120 ms; TI, 2800 ms; section thickness, 3.0 mm; 512 x 512; FOV, 230 x 230 x 195 mm), and postcontrast T1-weighted 3D volume acquisitions (TR, 9.8 ms; TE, 4. 6 ms; section thickness, 1 mm; 256 x 256; FOV, 240 x 240 x 160 mm). A 6-direction axial diffusion tensor imaging sequence (TR, 2319 ms; TE, 68 ms; section thickness, 4 mm; 128 x 128; FOV, 230 x 230 x 100 mm; b-values 0 and 1000 s/mm2; , 33.5 ms) was acquired. For the DCE-MR imaging acquisitions, the orientation was altered to a sagittal-oblique plane to incorporate the internal carotid artery for measurement of an arterial input function. Four precontrast T1-FFE (radio-frequency-spoiled gradient echo) sequences (2°, 5°, 10°, 16°) were acquired in the same geometry for calculation of baseline T1 maps (TR, 3.5 ms; TE, 1.1 ms; section thickness, 4.2 mm; 128 x 128; FOV, 230 x 230 x 105 mm) with the standard variable flip angle method for T1 estimation being used.20 This was followed by a dynamic contrast-enhanced acquisition series (TR, 3.5 ms; TE, 1.1 ms; flip angle, 16°; section thickness, 4.2 mm; 128 x 128; FOV, 230 x 230 x 105 mm) consisting of 100 volumes with temporal spacing of approximately 3.4 seconds. Gadolinium-based contrast agent (gadopentetate dimeglumine bis-methylamide, Omniscan; GE Healthcare, Oslo, Norway) was injected as a bolus dose of 0.1-mmol/kg–1 of body weight, at a rate of 3 mLs–1, after acquisition of the fifth image volume. Pre- and postcontrast T1-weighted imaging sequences (TR, 9.3 ms; TE, 4.6 ms) were acquired in the same sagittal oblique geometry for definition of VOI of the whole tumor. Data Processing VOIs were defined for each tumor by an experienced radiologist (S.J.M.), before histologic diagnosis was confirmed. Analysis was performed by using in-house software (Manchester Dynamic Modeling) and the extended Tofts and Kermode pharmacokinetic model.21 Automated arterial input functions were generated from an appropriately chosen section that included the internal carotid artery.22 Parametric maps of the IAUC were produced. ADC maps were generated by using DTIStudio (Johns Hopkins University, Baltimore, Maryland).23 Tumor VOIs were modified to contain only voxels with contrast—that is with an initial IAUC during the first 60 seconds (IAUC60) e were generated. Axial ADC and sagittal oblique ve images were coregistered by using the FLIRT linear registration in the FSL package.24 The b = 0 image was used as the reference image, and the 2° T1-FFE was used as the input image. An affine 12-parameter registration with a normalized correlation (intramodal) cost function and nearest neighbor interpolation was applied. The derived transformation was then applied to the sagittal oblique ve parametric map. This generated an axially oriented ve map, which could be overlaid on the ADC for voxel-by-voxel analysis (Fig 1). View larger version (70K): [in this window] [in a new window] Fig 1. A and B, Sagittal oblique postcontrast T1-weighted image (A) depicting a left frontal GBM with ve (unitless) map overlaid (B). C, Axial postcontrast T1-weighted image. D, Axial ADC map with coregistered ve map overlaid and ve color scale bar. Statistical Analysis Scatterplots of ADC and ve were generated for both a voxel-by-voxel analysis and comparison of median values. In addition, a scatterplot of ADC versus ve, with low values of ve (<0.05) excluded, was generated. This was an attempt to overcome potential ve modeling problems, in which very low values of ve may be the result of underperfused tissue in which there is no leakage of contrast into the EES. Where appropriate, SPSS version 15.0 (SPSS, Chicago, Illinois) was used for bivariate Spearman correlation analysis to identify a relationship between the 2 parameters. Results Patients Nineteen patients (7 men, 11 women; age range, 18–77 years; mean age, 60 ± 12 years) with histologically confirmed GBM were included in the study. An additional 2 patients were excluded due to lack of histologic confirmation of GBM. Voxel-by-Voxel Analysis Figure 2 shows a typical sample scatterplot from 1 individual illustrating the voxel-by-voxel comparison of ADC and ve. These plots show no evidence of a linear relationship between ADC and ve in any case. Removal of very low values of ve (< 0.05) also showed no linear relationship between the 2 parameters (Fig 3). View larger version (25K): [in this window] [in a new window] Fig 2. Scatterplot of a voxel-by-voxel comparison of ADC and ve (no units) for 1 sample patient. No relationship is demonstrated between the 2 parameters. View larger version (24K): [in this window] [in a new window] Fig 3. Scatterplot of a voxel-by-voxel comparison of ADC and ve (no units) with low values of ve removed for 1 sample patient. Low values of ve may under-represent the EES because they may occur as a result of underperfusion and minimal contrast leakage into the EES. No relationship is demonstrated between the 2 parameters. Comparison of Median Values Figure 4 demonstrates the scatterplot of median values of ADC versus median values of ve. A Spearman bivariate correlation analysis showed no significant relationship between the 2 parameters (P = .124). View larger version (9K): [in this window] [in a new window] Fig 4. Scatterplot of a comparison of the median values of ADC versus ve (no units). Discussion There is a pressing requirement for imaging biomarkers that can provide information reflecting tumor cell numbers, cell size, and cell packing. In oncologic practice, there is an increasing need to monitor the effects of tumor phenotypes and novel therapeutics on cellular proliferation and cell death. Mapping the size and spatial characteristics of the EES is one of the most promising approaches, and a number of groups have already described relationships between diffusion and enhancement characteristics and cellular structure.14,15 Several groups have reported an inverse correlation of ADC with cell density in gliomas,5,8–10 and the measurement ve from DCE-MR imaging is thought to reflect EES volume. Indeed, similar changes were reported in both parameters following treatment with glucocorticoid steroids, with reductions in both ADC and ve.18 Both techniques, therefore, present us with promising candidate biomarkers for the study of cellular structure. In theory, these parameters are both heavily influenced by the volume of the EES, and we, therefore, hypothesized that these 2 measures should correlate. However, we were unable to identify any evidence of such a relationship on either a voxel-by-voxel basis or by comparison of median values. The negative results of this study are important because they indicate that our current conceptual understanding of these parameters is incomplete. This indicates the need for further evaluation of the features in the tumor microenvironment that affect each set of parameters if we are to use them as the basis for useful biomarkers of cellular structure. While no study has directly compared ve and ADC in glioma, a study of therapeutic response in breast carcinoma by Yankeelov et al25 reported a negative correlation between these 2 parameters, with ADC increasing and ve decreasing following treatment. They hypothesized that these findings may reflect a decrease in interstitial fluid pressure following treatment, aiding the elimination of cell debris and causing an increase in ADC but an overall decrease in ve.25 They also acknowledged the difficulties in measuring ADC accurately in breast tissue and how their findings differ from the those in the literature, in which studies of ADC values alone have reported decreases following treatment for breast cancer,26–31 which is in keeping with the changes in ADC values seen in glioma following treatment.4–7 There are potential methodologic problems with this study in the measurement of both parameters. A number of factors can influence measurements derived from DWI. The calculation of ADC is based on the difference in observed signal intensity, which occurs as a result of diffusion between temporally separated dephasing and rephasing gradients. The magnitude, duration, and temporal separation of these matched gradients will each have a separate effect on the magnitude of the resulting signal-intensity drop observed. Thus calculated ADC values will be affected not only by the volume of the EES but also by the complexity and absolute dimensions of the EES. Diffusion signal intensity can also be affected by capillary bed perfusion, intracellular diffusion coefficients, membrane permeability, and exchange times.32 The heterogeneous nature of GBMs with areas of microvascular proliferation, necrosis, cyst formation, edema, and increased cellularity will, therefore, have the potential to influence the ADC values in a number of different ways. Areas of microvascular proliferation and increased perfusion may influence the diffusion signal intensity, though a relatively high b-value of 1000 s/mm–2 was used in this study, so capillary perfusion should not have significantly contributed to the signal intensity.32,33 Necrotic cells, debris, and hemorrhage also can restrict movement of water in the EES and decrease measured ADC values. Cystic areas are reflected by high ADC values,34 while areas of increased cellularity are associated with low ADC values.5,8–10 Destruction of the blood-brain barrier and alterations in cell permeability will also affect the intra- and extracellular diffusion coefficients and exchange times, again influencing the ADC values. The heterogeneity of GBMs complicates analysis further. While attempts were made to overcome the problems of regional heterogeneity by performing a voxel-by-voxel analysis of the data and excluding voxels that contained no contrast (and therefore were likely to represent solely cystic or necrotic material), no correction could be made for heterogeneity beyond the resolution of the voxel. Recently, a study by Sadeghi et al35 found an inverse relationship between ADC values and microvessel density in bulk tumor, which was not present in peritumoral or infiltrated tissue. They hypothesized that the ADC values within the bulk tumor and peritumoral tissue were influenced by different factors, with edema and components of the extracellular matrix having a more predominant effect on ADC values in the peritumoral tissue than either cell or vessel density. Unlike a number of previous studies,5,8–10 Sadeghi's group failed to find a significant relationship between ADC values and cell density. There are also potential modeling problems associated with the calculation of ve. By definition, ve can only be measured when contrast medium leaks from the vessels into the EES. Thus ve cannot be estimated in tissue that is unperfused or when no extravascular contrast leakage occurs. This means that there may be a significant number of voxels within each tumor that show very low/unmeasureable ve and a wide range of possible ADC values. Figure 2 provides some evidence that this may indeed be the case. However, if the low values of ve are removed from Fig 2, there is still no clear relationship between ve and ADC (Fig 3). One final limitation of the study is the use of Omniscan contrast agent, which has decreased dramatically as a result of its association with NSF.36 Agents that have a lower reported risk of NSF, such as gadolinium diethylene triamine pentaacetic acid (Magnevist; Bayer Schering Pharma, Berlin, Germany) and gadoterate meglunine (Dotarem; Guerbet, Paris, France), have T1 relaxivity properties similar to those of Omniscan (4.3 and 4.2 L/mmol/s respectively versus 4.6 L/mmol/s)37,38 and are, therefore, unlikely to have significant effects on the ve measurements if the study was repeated with an alternative contrast agent. Conclusions Although ADC and ve are believed to reflect the size of the EES, these measurements did not correlate in patients with GBM. These results suggest that the current interpretation of these parameters is oversimplistic and that they provide independent information about the tumor microenvironment. The lack of correlation may result from methodologic variations in either or both measurements. This study highlights the requirement for further development and evaluation of proposed biomarkers that describe aspects of the tumor microstructure.
机译:背景与目的:ADC测量结果已显示与肿瘤细胞密度成反比 。 DCE-MR成像建模技术 可以生成v e 的测量值,也可以期望 与细胞密度成反比关系。这项研究的目的 是为了检验以下假设:期望增加 细胞的面积,从而降低ADC的预期EES较小。 (低v e )。 材料和方法:招募了19名GBM患者。所有成像均在手术前在3T MR成像扫描仪上进行。成像包括 扩散张量成像,T1加权DCE-MR成像和解剖学 序列。肿瘤VOI在解剖图像上定义,并且 修改为仅包含增强体素。生成了 ADC和v e 的参数图。对ADC和v e 进行统计分析,是在逐个像素的基础上和中值的比较 上进行的。 sup>结果:在 逐像素分析或中位值比较(P )中,ADC和v e 之间均未显示相关性= .124)。 结论:这项研究未能证明ADC与 v e 之间的相关性。这很重要,因为它表明尽管这些参数背后的机制 在理论上是相似的,但它们实际上反映了肿瘤微环境的不同方面。 因此,ADC和v e 应该被视为提供有关EES特性的独立 信息。 缩写:ADC,视在扩散系数•DCE-MR,动态增强对比度的MR•DWI,弥散加权成像•EES,血管外空间•FFE,快速场回波•FLIRT,FMRIB线性图像配准工具•FSL,FMRIB软件库•FMRIB,大脑功能磁共振成像•GBM ,多形性胶质母细胞瘤•IAUC,浓度曲线下的初始面积•最大,最大•最小,最小•NSF,肾原性全身纤维化•v ,每单位体积的血管外细胞腔体积•VOI,体积感兴趣的GBM是最常见,最具攻击性的主要产品是成年后的肿瘤 。这些肿瘤具有高度异质性,并通过 在任何给定肿瘤内不同程度的超细胞性,胞质和核多态性,有丝分裂和内皮增殖来表征。已经开发了许多基于MR成像的技术 来探测肿瘤的微环境。 DWI 允许量化由于布朗运动而产生的自由水 分子的运动程度。 ADC映射,表示水分子自由运动可以在组织内产生 扩散。尽管最近 证明可以得到体内 细胞堆积和细胞直径的估计值,但 1 ADC的测量值< sup> 通过使用实际的临床数据,受许多因素影响 。 ADC不仅受EES的体积 的影响,还受其空间配置,细胞内 扩散系数和膜通透性的影响。但是,已经提出 ADC主要受细胞外 几何形状的影响。 2 因此,水分子在 中的扩散较少sup>以狭窄的复杂细胞外间隙为特征的组织, 可能出现在具有大量小细胞的肿瘤中,例如淋巴瘤,而不是数量较少的组织 EES弯曲较小的大细胞,以及EES大小较大的组织 DCE-的药代动力学建模分析MR成像数据允许 估计许多影响造影剂分子的递送和局部分布的参数。这些 之一是直接估计可用于血管空间外对比度 分布的泄漏量。这个值(v e )是 ,因此可以直接估算EES的体积。 3 技术已经在胶质瘤中得到广泛应用。 放疗 后很早就证实了ADC的变化,并预测了治疗反应(在皮质类固醇给药后)。 4-7 这些变化被认为反映了由于凋亡和/或坏死引起的 细胞结构改变。 4,5 许多研究者显示ADC与脑肿瘤细胞密度之间呈反线性关系。 5,8–10 此外,一些研究注意到 与恶性肿瘤和ADC呈反比关系,随着组织学肿瘤分级的增加( )与低ADC值相关, 8,9,11, 12 包括在 常规成像中无法与低度肿瘤区分开的高级 肿瘤。 13 大多数DCE-MR成像研究在神经胶质瘤中, 已评估了血管参数,例如血容量和 通透性,而v e 通常被忽略。少数对v e 进行了研究的研究表明,它对区分轴向外肿瘤 14具有重要的意义, 14 15 并具有 表明它具有随肿瘤 等级增加而增加的趋势。 14,16 另外,v e 在识别 皮质类固醇治疗反应的变化方面表现出敏感性,治疗后v e 下降,大概反映了 减少水肿。 17,18 许多小组既进行了DCE-MR成像又进行了扩散 成像 14,18,19 然而,据作者所知, 尚无ADC和v e 的直接比较。肿瘤 组。这项研究的目的是检验假设 ,即细胞流动性增加的区域,因此ADC低, ,应该具有低v e 材料和方法患者当地研究伦理委员会批准了该研究,并且 所有患者在征募前均已知情同意。通过Salford Royal National Health Service Foundation Trust的神经肿瘤学多学科小组会议确定了可能具有GBM的患者 。 18岁以下的患者,不适合 手术的患者以及禁忌MR成像的患者 从一开始就被排除在外。所有成像均在 手术之前进行。 通过外科手术切除或活检在组织学上均被确认为GBM,并且排除了不能在组织学上确认到术后的GBM 的患者。 糖皮质激素以前已经显示出可以改变DCE-MR成像参数的测量结果。 6 停用皮质类固醇激素治疗 被认为是不道德的;因此,所有患者均应在成像前接受皮质类固醇 治疗至少48小时,作为其标准临床治疗的一部分,并对所有受试者进行标准化治疗 。在成像时,没有人接受过任何其他形式的治疗。 数据采集成像是在曼彻斯特大学的磁共振成像设施(希望通过使用3T Achieva系统上的灵敏度编码磁头线圈 (荷兰,Best,菲利普斯医疗系统公司) 。根据常规 临床实践选择的常规 解剖序列,包括以下内容:轴向T1加权 反转恢复(TR,8.4 ms ; TE,3.8 ms; TI,1150 ms;截面 厚度,1.8 mm; 256 x 256; FOV,240 x 240 x 324 mm),轴向 T2加权( TR,3000毫秒; TE,80毫秒;截面厚度,3.0 mm; 1024 x 1024; FOV,266 x 266 x 135 mm),冠状T2加权 流体-衰减反转恢复(TR,11000 ms; TE,120 ms; TI,2800 ms;截面厚度,3.0 mm; 512 x 512; FOV, 230 x 230 x 195毫米),以及对比后T1加权的3D体积 采集(TR,9.8 ms; TE,4. 6 ms;截面厚度,1 mm; 256 x 256; FOV ,240 x 240 x 160毫米)。 6方向轴向 扩散张量成像序列(TR,2319 ms; TE,68 ms;截面 厚度,4 mm; 128 x 128; FOV,230 x 230 x 100毫米; b值 0和1000 s / mm 2 ;,33.5 ms)。 对于DCE-MR图像采集,将方向更改为矢状斜面,以合并颈内动脉以测量动脉输入功能。在相同的几何形状中获取了四个pre-contrast T1-FFE(射频损坏的梯度回波)序列(2°, 5°,10°,16°) > 用于计算基线T1图(TR,3.5 ms; TE,1.1 ms; 截面厚度,4.2 mm; 128 x 128; FOV(230 x 230 x 105 mm) ,并使用标准可变翻转角方法进行T1估计 。 20 之后是动态对比-enhanced 采集系列(TR,3.5 ms; TE,1.1 ms;翻转角,16°; 截面厚度,4.2 mm; 128 x 128; FOV,230 x 230 x 105毫米) 由100个体积组成,时间间隔约为 3.4秒。以0.1毫摩尔/千克的大剂量注射基于的造影剂(ado戊二酸酯 二聚甲胺双甲酰胺,Omniscan; GE Healthcare,奥斯陆, 挪威)。在获得第五个图像量的 之后,以3 mLs –1 的速度–1 体重。在 相同的矢状斜角几何中获取对比前和对比后T1加权的 成像序列(TR,9.3 ms; TE,4.6 ms) 整个肿瘤。 数据处理在确定组织学诊断之前,由经验丰富的放射科医生 (SJM)为每个肿瘤定义VOI。使用内部软件(Manchester Dynamic Modeling)以及扩展的Tofts和Kermode药代动力学 模型进行分析 。21 sup>从 适当选择的区域生成自动动脉输入功能,该区域包括颈内动脉 。 22 生成IAUC的参数图。 ADC映射 是使用DTIStudio(约翰霍普金斯大学, 巴尔的摩,马里兰州)生成的。 23 修改了肿瘤VOI仅包含具有对比度的体素-在最初的60秒内, 具有初始IAUC(IAUC 60 e 的参数图。 轴向ADC和矢状斜v e 图像通过 共同配准。 24 b = 0图像用作参考图像,而2° T1-FFE用作输入图像。仿射12参数配准 具有归一化的相关性(模态内)成本函数和 最近邻插值。然后将派生的变换 应用于矢状斜v e 参数图。 这将生成轴向取向的v e 映射,可以将其叠加在ADC上的 上以进行逐像素分析(图1)。 查看较大版本(70K):[在此窗口中] [在[新窗口]图1. A和B,矢状斜向对比后T1加权图像(A),其左前额叶GBM覆盖了v e (无单位)图(B)。 C,轴向对比后T1加权图像。 D,轴向ADC映射与共同注册的v e 映射重叠并且v e 彩色比例尺。统计分析ADC和v e 的散点图用于逐个体素 分析和中值比较。另外,ADC的散点图 与v e 的比较,排除了v e (<0.05)的低值, 已生成。这是为了克服潜在的v e 建模问题,其中v e 的极低值可能是 在EES中没有造影剂泄漏 的灌注不足组织的结果。在适当的情况下,使用SPSS 15.0 版本(SPSS,伊利诺伊州芝加哥)对双变量Spearman相关性进行分析,以识别两个参数之间的关系。 结果患者19名患者(男7例,女11例;年龄范围18-77岁;平均年龄 (±60±12岁),经组织学证实为 GBM。由于缺乏对GBM的组织学证实,另外2例患者被 排除。 Voxel-by-Voxel分析图2显示了来自1个人的典型散点图。 sup>说明了ADC与v e 的逐像素比较。这些 图在任何情况下都没有证据表明ADC 和v e 之间存在线性关系。移除非常低的v e (<0.05) 值也显示两个参数 之间没有线性关系(图3)。 观看大图(25K):[在此窗口中] [在新窗口中]图2. ADC和v e 的逐像素比较散点图(无单位) 1个样本患者。这两个参数之间没有关系。查看大图(24K):[在此窗口中] [在新窗口中]图3. ADC和v e (无单位)的低像素值的逐像素比较散点图移除了1位样本患者的v e 。 v e 的低值可能不足以代表EES,因为它们可能是由于灌注不足和造影剂泄漏到EES中的最小程度而发生的。这两个参数之间没有关系。中值的比较图4显示了ADC 的中值与v e 的中值的散点图。 Spearman双变量相关性 分析显示两个参数 之间没有显着相关性(P = .124)。 查看大图(9K):[在此窗口] [在新窗口中]图4. ADC与v e (无单位)的中位数比较的散点图。讨论对生物标志物成像的迫切要求是, 可以提供反映肿瘤细胞数量,细胞 大小和细胞堆积的信息。在肿瘤学实践中,越来越需要监测肿瘤表型和新型治疗方法对细胞增殖和细胞死亡的影响。 映射EES的大小和空间特征是最有前途的 方法之一,许多小组已经描述了扩散与扩散之间的关系 。增强特征和细胞 结构。 14,15 几个研究小组报告了胶质瘤中ADC的密度与细胞密度呈反相关, 5, 8–10 和DCE-MR成像的测量 v e 被认为反映了EES量。确实,糖皮质激素治疗 后,两个参数均报告了 相似的变化,ADC和 v e 。 18 因此,这两种技术为我们提供了用于细胞结构研究的有希望的 候选生物标记。在 理论中,这些参数都受到EES的 量的严重影响,因此,我们假设这两个 度量应该相关。但是,我们无法基于体素或基础值的比较来确定 这种关系的任何证据。 这项研究的负面结果很重要,因为它们 表示我们目前对这些 参数的概念性理解不完整。这表明如果要使用它们作为基础 ,则需要进一步 评估肿瘤微环境中影响 每组参数的特征。 虽然没有研究直接比较v e 和ADC在神经胶质瘤中的作用,但 对乳腺癌的治疗反应的研究Yankeelov 等人 25 报告了这两个参数之间的负相关性, 随着ADC的升高和v e 的降低而降低。他们 假设这些发现可能反映了治疗后间质液压力的降低,有助于消除 细胞碎片并导致ADC增加,但v e 中的总体下降 。 25 他们还认识到准确测量乳腺组织中 ADC的困难以及如何他们的发现与文献中的发现不同 ,其中仅ADC值 的研究报告了乳腺癌 癌症治疗后的减少, 26–31 与治疗后脑胶质瘤中ADC 值的变化保持一致。 4-7 这项研究在两个参数的测量中存在潜在的方法学问题。许多因素可以 影响从DWI得出的测量结果。 ADC的计算基于观察到的信号强度的差异, 是由于时间分离的 移相和移相梯度之间的扩散而产生的。这些匹配的梯度的大小,持续时间, 和时间间隔将分别对观察到的信号强度 drop的大小分别产生影响。 。因此,计算得出的ADC值不仅会受到EES的体积的影响,还会受到EES的复杂性和绝对尺寸的影响。扩散信号强度还可能受到毛细血管床灌注,细胞内扩散系数,膜通透性和交换时间的影响。 32 sup> GBMs具有微血管 扩散,坏死,囊肿形成,水肿和增加的 细胞性的异质性,因此有可能影响 < / sup> ADC值有许多不同的方式。尽管1000 s / mm –2 扩散和灌注增加的区域可能会影响扩散 信号强度。在本研究中使用了sup> ,因此毛细血管灌注不应显着影响信号强度。 32,33 坏死性 细胞,碎片和出血也可以限制EES中 水的移动并降低ADC的测量值。囊性区域 由较高的ADC值反映, 34 ,而 细胞增多的区域与较低的ADC值相关。 5,8– 10 血脑屏障的破坏和细胞 通透性的改变也将影响细胞内外扩散系数。 GBM的异质性进一步使分析复杂化。通过尝试对数据进行逐个体素分析并排除不包含 voxel的元素,从而尝试 来解决区域异质性 的问题。相反,(因此很可能 仅代表囊性或坏死性物质),无法对 体素分辨率超出范围的异质性进行校正 。最近,Sadeghi等人的 35 的一项研究发现ADC值与散装的 肿瘤中微血管密度之间的逆 关系,在肿瘤周围并不存在 他们假设大块肿瘤 和肿瘤周围组织中的ADC值受不同因素的影响, 具有水肿和食管癌的成分。细胞外基质对瘤周围组织中ADC值的影响主要大于细胞或血管密度。与许多先前的 研究不同, 5,8–10 Sadeghi的小组未能在ADC值与细胞密度之间找到显着的 关系。 > v e 计算也存在潜在的建模问题。根据定义,仅当 造影剂从血管泄漏到EES中时,才能测量v e 。因此,在未灌注或未发生 血管外造影剂泄漏的组织中,无法估算v e 。这意味着每个肿瘤中可能存在大量 的体素,其中 显示出非常低/无法测量的v e ,并且可能的范围很广。 sup> ADC值。图2提供了一些证据证明确实可能是 。但是,如果从 图2中删除了v e 的低值,则v e 和ADC 之间仍然没有明确的关系。 (图3)。 该研究的最后一个局限是使用Omniscan对比度 代理,由于其关联性,其使用量大大减少了。 与NSF。 36 报告的NSF风险较低的药物,如 ,如di二亚乙基三胺五乙酸(Magnevist; Bayer Ter弛豫特性 与Omniscan相似(4.3和4.2 L / mmol),具有蛇形的葡甲胺 (Dotarem; Guerbet,法国巴黎)。 / s分别为 和4.6 L / mmol / s) 37,38 ,因此,如果使用替代性造影剂重复该研究 ,则不太可能对v e 测量值产生显着影响。 结论尽管ADC和v e 被认为可以反映 EES的大小,但这些测量值与GBM患者无关。 这些结果表明这些 参数的当前解释过于简单,并且它们提供了有关肿瘤微环境的独立 信息。缺乏相关性 可能是由于两种方法之一或两者的方法学差异所致。 本研究强调了进一步开发和评估所提出的生物标志物的要求描述肿瘤微结构的各个方面。 < sup>

著录项

  • 来源
    《American Journal of Neuroradiology》 |2010年第3期|549-553|共5页
  • 作者单位

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Department of Neuroradiology (S.J.M., C.S., A.J.), Hope Hospital, Salford, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

    Department of Neuroradiology (S.J.M., C.S., A.J.), Hope Hospital, Salford, United Kingdom;

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

    From the Imaging Science and Biomedical Engineering Department (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), School of Cancer and Imaging Sciences, University of Manchester, Withington, Manchester, United Kingdom|Department of Neuroradiology (S.J.M., C.S., A.J.), Hope Hospital, Salford, United Kingdom|Biomedical Imaging Institute (S.J.M., C.J.R., S.C., S.Z., G.J.M.P., A.J.), University of Manchester, Manchester, United Kingdom.;

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