Abstract
Objectives
To evaluate the added value of diffusion-weighted imaging (DWI) to perfusion-weighted imaging (PWI) for differentiating tumour progression from radiation necrosis.
Methods
Sixteen consecutive patients who underwent removal of a metastatic brain tumour that increased in size after stereotactic radiosurgery were retrospectively reviewed. The layering of the ADC was categorised into three patterns. ADC values were measured on each layer, and the maximum rCBV was measured. rCBV and the layering pattern of the ADC of radiation necrosis and tumour progression were compared.
Results
Nine cases of radiation necrosis and seven cases of tumour progression were pathologically confirmed. Radiation necrosis (88.9 % vs. 14.3 %) showed a three-layer pattern of ADC with a middle layer of minimum ADC more frequently. If rCBV larger than 2.6 was used to differentiate radiation necrosis and tumour progression, the sensitivity was 100 % but specificity was 56 %. If the lesions with the three-layer pattern of ADC with moderately increased rCBV (2.6–4.1) were excluded from tumour progression, the sensitivity and specificity increased to 100 %.
Conclusions
The three-layer pattern of ADC shows high specificity in diagnosing radiation necrosis; therefore, combined analysis of the ADC pattern with rCBV may have added value in the correct differentiation of tumour progression from radiation necrosis.
Key Points
•MRI follow-up often reveals increasing size of enhancing lesions after stereotactic radiosurgery
•Inflammation around tumour necrosis increases regional cerebral blood volume (rCBV), mimicking progression
•A three-layer apparent diffusion coefficient (ADC) pattern on diffusion-weighted MRI suggests radiation necrosis.
•The combined use of rCBV and DW MRI enables accurate differentiation.
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Introduction
An increase in the size of enhancing lesions on follow-up MRI after stereotactic radiosurgery (SRS) is well documented [1, 2]. This phenomenon causes management dilemmas for physicians who interpret any increase in lesion size as cancer progression based on the conventional concept of tumour treatment response evaluation [3, 4].
Patel et al. [3] reported that approximately one-third of SRS-treated lesions increased in size during follow-up. However, only 10 out of 120 patients (8 %) required salvage surgery for lesion progression, and the vast majority of lesion size increases were asymptomatic and required only observation. The increased size of enhancing lesions after SRS is often associated with an exaggerated immune response against radiation, and this exaggerated immune response may result in improved cancer survival and control [3, 5, 6].
Radiation-induced changes mostly result from injury to the small vessels, such as hyalinisation, fibrinoid necrosis and spontaneous thrombosis [7]. Other causes of radiation necrosis are direct injury to glial parenchymal elements and immunological reactivity secondary to allergic hypersensitivity [7, 8]. Central nervous system tissue is highly responsive to ionising radiation, and the induction of cytokines is prominent in radiation-induced cellular responses, resulting in local neuroimmune and inflammatory reactions [8]. An experimental study showed the induction of tumour necrosis factor (TNF)-α gene expression, which persisted for 2–3 months following mouse brain irradiation (25 Gy) and was followed by persistent gene overexpression for 6 months [9].
Radiation necrosis of the irradiated brain has various histological features, including coagulation necrosis and liquefaction necrosis [10]. The typical coagulation necrosis shows vascular changes such as fibrinoid necrosis, hyalinisation of the vessel wall and occlusion of the lumen by fibrin thrombi. In the area around typical coagulation necrosis, a zone of active inflammatory response is formed.
Radiation necrosis with markedly increased signal intensity on diffusion-weighted imaging (DWI) and a low apparent diffusion coefficient (ADC) value was reported in a previous study [11, 12]. This is caused by the development of intracellular oedema in the viable tumour cells during the transition to complete necrosis with liquefaction. Also, the low ADC values in radiation necrosis might reflect early necrosis with abundant polymorphonuclear leukocytes, as in purulent fluid, because the high viscosity and inflammatory cellular composition may restrict water diffusion.
Differentiating between tumour progression and radiation necrosis after SRS is often difficult with conventional MRI and even with perfusion-weighted imaging (PWI). The active inflammatory response area around the necrosis area may show increased cerebral blood volume (CBV) and can mimic tumour progression. Based on our clinical experience, we found that analysis of the layering pattern in DWI could help differentiate radiation necrosis and tumour progression. As coagulation necrosis may make a liquefied centre, with a peripheral active inflammatory zone and transition zone in between, the ADC value of the transition zone will be low because of the high viscosity.
Thus, the aim of this study was to evaluate whether DWI findings of radiation necrosis were distinctive compared to those of tumour progression and to evaluate the added value of DWI on PWI.
Materials and methods
Study population
Between January 2008 and January 2012, 21 consecutive patients underwent craniotomy and tumour removal for metastatic brain tumours that increased in size after SRS and preoperative MRI including DWI and PWI. Images with significant haemorrhage (n = 4) and motion artefacts (n = 1) that prevented image analysis were excluded from the study. Finally, 16 consecutive patients (9 men and 7 women with an age range from 38 to 71 years; mean age, 56 years) were included in the study. This retrospective study was approved by the institutional review board in the hospital, and the requirement for informed consent was waived.
The mean interval between SRS and increased size of the lesion was 134 ± 83.4 days with a range of 40 to 311 days. The origins of tumours were as follows: lung adenocarcinoma (n = 8), lung squamous cell carcinoma (n = 2), small cell lung cancer (n = 2), hepatocellular carcinoma (n = 1), breast cancer (n = 1), advanced gastric cancer (n = 1) and sebaceous carcinoma of the eyelid (n = 1).
MR imaging protocol
Magnetic resonance imaging was obtained at 3.0 T (Achieva, Philips Medical Systems, Best, The Netherlands) with an eight-channel sensitivity-encoding (SENSE) head coil.
Contrast-enhanced axial spin echo T1-weighted imaging was acquired after intravenous injection of contrast material [Dotarem (gadoterate meglumine), Guerbet, Aulnay-sous-Bois, France, 0.1 mmol/kg body weight by power injector] with the following parameters: repetition time/echo time (TR/TE) = 500/10 ms; slice thickness = 5 mm; acquisition matrix = 256 × 226.
Spin echo EPI DWI (TR/TE = 3,000/76 ms, slice thickness = 5 mm, acquisition matrix = 128 × 128, b value = 0, 1,000 s/mm2) and dynamic susceptibility contrast (DSC) MR perfusion imaging [TR/TE = 1,720/35 ms, flip angle (FA) = 40°, slice thickness = 5 mm, acquisition matrix = 128 × 128, 50 volumes, acquisition time = 1 min 30 s] were obtained with parameters as described above. All MR sequences were acquired with the same field of view (FOV; 240 × 240 mm).
ADC map analysis
The layering of ADC values was categorised into three patterns (Fig. 1). The outer boundary of the lesion was considered to be the outer margin of the enhancing area. The one-layer pattern showed matched areas of the decreased ADC value and increased regional cerebral blood volume (rCBV) with enhancement. The two-layer pattern showed a decreased ADC value on the inner layer surrounded by a larger enhancing portion. The three-layer pattern showed an inner layer of increased ADC value and a middle layer of decreased ADC value, which were not enhanced, surrounded by an enhancing portion with increased rCBV.
The ADC values were measured on each discernible layer. The minimum ADC was recorded from three regions of interest (ROI; size = 3 mm2).
rCBV map analysis
Dynamic susceptibility contrast perfusion images were processed using a dedicated software package (Nordic ICE; NordicNeuroLab, Bergen, Norway). An rCBV map was generated using an established tracer kinetic model applied to the first-pass data [13]. Gamma variate fitting was applied to avoid a recirculation effect. As described previously, the dynamic curves were corrected mathematically to reduce contrast agent leakage effects [14]. The rCBV maps were normalised by dividing the rCBV value in the ROI with an unaffected white matter rCBV value defined by a neuroradiologist (J.C.).The maximum rCBV was recorded from three ROIs (size = 3 mm2).
Statistical analysis
Statistical analyses were performed using IBM SPSS Statistics 20 (IBM Corporation, NY, USA). The ADC values and rCBV between the radiation necrosis group and the tumour progression group were compared using Fisher’s exact test and the Mann-Whitney test. A receiver operating characteristic (ROC) curve was constructed to determine the optimal threshold of rCBV for differentiating radiation necrosis and tumour progression. For all statistical values, a P value less than 0.05 was considered to indicate a statistically significant difference.
Results
Nine cases of radiation necrosis (Fig. 2) and seven cases of tumour progression (Fig. 3) were pathologically confirmed.
All patients in the radiation necrosis group showed the three-layer pattern of ADC (100 % of the radiation necrosis group); however, six patients (85.7 %) in the tumour progression group showed the one- or two-layer pattern (P = 0.001; Table 1). The minimum ADC was measured at the middle layer in the radiation necrosis group (88.9 %), but in the tumour progression group, the minimum ADC was measured at the inner layer (57.1 %; P = 0.012; Table 2). There was only one exception having the minimum ADC at the middle layer in the tumour progression group; however, in that patient, the rCBV was 7.8, which may suggest tumour progression (Fig. 4).
The minimum ADC was smaller in the radiation necrosis group than in the tumour progression group (655.7 ± 184.4 × 10−6 mm2/s versus 829.6 ± 224.5 × 10−6 mm2/s, respectively); however, it was not statistically significant (P = 0.138). rCBV was higher in the tumour progression group than in the radiation necrosis group (6.3 ± 3.2 versus 2.8 ± 1.0, respectively; P = 0.013; Table 3). There were no significant differences in terms of the mean values of each ADC layer (inner, middle, outer) in the radiation necrosis group and tumour progression group.
On the ROC curve analysis, the area under the curve (AUC) of rCBV for differentiating tumour progression from radiation necrosis was 0.873 (Fig. 5). If rCBV larger than 2.6 was used to differentiate radiation necrosis and tumour progression, the sensitivity was 100 % but specificity was 56 % owing to an overlapping portion (Fig. 6). If an rCBV larger than 4.1 was used to differentiate radiation necrosis and tumour progression, the sensitivity was 71.4 % and specificity was 100 %. If the diagnostic criterion was set to (1) the lesion with an rCBV larger than 2.6 that did not have the three-layer pattern of ADC or (2) the lesion with an rCBV larger than 4.1, the sensitivity and sensitivity were 100 %.
Discussion
Approximately one third of lesions treated with SRS increased in size during follow-up [3]. Increasing initial size is associated with a higher probability of a post-SRS increase in lesion size [3, 15]. Male sex and mean voxel dose <37 Gy are associated with a higher probability of a post-SRS increase in lesion size [3]. With regard to the timing of lesion growth, most lesions increase in size 3–6 months post-SRS. However, this enlargement can start as early as 6 weeks post-SRS and may not reach peak volume until 15 months post-SRS [3]. In this study, the time interval between SRS and increased size of the lesion was 134 ± 83.4 days (range from 40 to 311 days), which was consistent with previous reports.
Patel et al. [3] found that for those patients in whom all lesions increased in size, median survival was >18.4 months compared with 16.4 months for patients whose lesions showed mixed responses and 9.5 months for patients whose lesions all remained stable or decreased in size. They said the post-SRS lesional growth may not represent tumour regrowth at all but rather a brisk reactive immune response that is related to or causes apparent lesional growth on MR imaging; however, not all cases were pathologically confirmed.
Diffusion-weighted imaging has been used to differentiate brain abscess from necrotic tumour [12, 16]. Contrary to purulent fluid in the brain abscess, which shows diffusion restriction, necrotic areas in primary and metastatic tumours are usually more haemorrhagic, less viscous and less cellular, and therefore do not show diffusion restriction.
It is also well established that therapeutic radiation causes vasculopathy and necrosis in treated tissue. In cases of radiation necrosis of the brain, the necrotic areas show coagulation necrosis and liquefied softening necrosis [10]. In the area around the liquefied centre, more active inflammatory responses are formed with lymphocytes and macrophages as a partial rim of the reactive zone and surrounded by reactive gliosis and demyelination [3, 10]. Histologically, radiation-induced injury has been well-described as an area of necrosis surrounded by a robust inflammatory cell infiltrate that may also contain some tumour cells [17, 18]. Areas of sterile coagulation necrosis may contain creamy pus-like material with abundant polymorphonuclear leukocytes [19]; therefore, radiation necrosis may show diffusion restriction, that is, low ADC values. In previous reports of radiation necrosis of metastasis with low ADC values, the authors suggested that this low ADC value could be explained by the development of intracellular oedema in the viable tumour cells during the transition to complete necrosis with liquefaction [11, 12, 20, 21]. Therefore, mature radiation necrosis may show a three-layer pattern: an inner layer of complete necrosis with liquefaction that shows an increased ADC value, a middle layer of transition zone with a low ADC value and an outer layer of the active inflammatory zone with increased rCBV.
In previous studies, a lower ADC value was considered to indicate higher cellularity in a recurrent tumour [11, 22]. However, the range of the ADC values of a tumour is about 800–1,200 × 10−6 mm2/s. In their study, Toh et al. [23] showed that the mean ADC values of the enhancing rim in abscess, glioblastoma and metastasis were 691, 1,268 and 1,271 × 10−6 mm2/s, respectively. The ‘infarct-like’ extremely low ADC value of about 600 × 10−6 mm2/s may not be achieved by tumour and may only be achieved by infarction, abscess or radiation necrosis. Also, if the low ADC value portion was a viable tumour portion, the lesion should show contrast enhancement; however, in this study, the ‘infarct-like’ low ADC portion located in the middle layer did not show contrast enhancement.
The most widely used technique for a perfusion study is to evaluate the rCBV from DSC MR perfusion imaging [22, 24]. With an increment of vascularity in tumours, new vessels and damaged mature vessels are permeable to contrast agents, unlike vessels in the normal brain. Measurement of the rCBV reliably correlates with tumour grade and histological findings of increased tumour vascularity, particularly in gliomas [25]. rCBV can be used to differentiate between a radiation-induced change and tumour progression by estimating the regional CBV after radiosurgery. A decrease in rCBV values indicates a tumour response to therapy regardless of increases in tumour volume, which might be due to radiation-induced oedema and blood–brain barrier disruption, and necrosis as seen in a follow-up MRI study after radiosurgery. If an increment of rCBV in the enhancing component of the mass after radiosurgery appears on follow-up MRI, this finding may be considered indicative of tumour progression [26, 27].
In the area around the liquefied centre in radiation necrosis, there are more active inflammatory responses, resulting in some degree of increased rCBV. This results in a thin rim of increased rCBV on the peripheral portion of the necrotic area (Fig. 2); therefore, there is significant overlap of rCBV between radiation necrosis and tumour progression [28]. In our study, the specificity of rCBV > 2.6 for differentiating radiation necrosis and tumour progression was only 56 %. Also, the sensitivity of rCBV > 4.1 for differentiating radiation necrosis and tumour progression was 71.4 %. On the other hand, the three-layer pattern of ADC with a low ADC on the middle layer was highly specific for radiation necrosis. If the lesion with the three-layer pattern of ADC with moderately increased rCBV (2.6–4.1) was excluded from rCBV > 2.6, the sensitivity and specificity were increased to 100 %.
Our study has several limitations. Because of the small number of patients, a selection bias may have occurred. Next, pathological matching was not performed on each layer of the ADC. Also, the primary tumour site was heterogeneous; thus, the nature of the primary tumour may act as a bias.
In conclusion, the sensitivity and specificity of rCBV in diagnosing tumour progression is not high owing to an overlapping portion; therefore, the differentiation of tumour progression from radiation necrosis is often difficult. The presence of the three-layer pattern of ADC was highly specific for radiation necrosis. Therefore, a combination of ADC with rCBV may have added value in the correct differentiation of tumour progression from radiation necrosis.
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Cha, J., Kim, S.T., Kim, HJ. et al. Analysis of the layering pattern of the apparent diffusion coefficient (ADC) for differentiation of radiation necrosis from tumour progression. Eur Radiol 23, 879–886 (2013). https://doi.org/10.1007/s00330-012-2638-4
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DOI: https://doi.org/10.1007/s00330-012-2638-4