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Cancer Research UK Clinical Magnetic Resonance Research Group, Institute of Cancer Research and Royal Marsden NHS Foundation Trust, Downs Road, Sutton, Surrey SM2 5PT, UK
Correspondence: Dr N M deSouza, Clinical Magnetic Resonance Research Group, MRI Unit, Institute of Cancer Research, Downs Road, Sutton, Surrey SM2 5PT, UK
| Abstract |
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| Introduction |
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30% of new cancer cases [1] and requires 68 tissue cores obtained under transrectal US (TRUS) guidance for diagnosis. T2 weighted magnetic resonance imaging (MRI) delineates prostate cancer as a region of low signal intensity (indicative of a shorter T2 relaxation time constant for tumour) surrounded by high signal intensity (longer T2) of normal peripheral zone tissue [2, 3]. However, although the sensitivity of T2 weighted images for tumour detection is high, specificity is poor [4]. Furthermore, the 30% of tumours that occur in the central gland cannot be detected on T2 weighted imaging because it is not possible to differentiate them from the low signal-intensity benign nodules of prostatic hyperplasia. Potential advantages of improved discrimination of malignant tissue in both the peripheral and central zones of the prostate include better local staging performance, increased accuracy in performing biopsy, improved focusing of irradiation for intensity-modulated radiotherapy, improved follow-up of therapy response and earlier detection of tumour recurrence.
An alternative to T2 weighted MRI is to develop image contrast through "apparent diffusivity" (tissue water incoherent displacement over distances of
120 µm). Diffusion-weighted magnetic resonance imaging (DW-MRI) has been used in both clinical and research settings for detecting cerebral [58] as well as cancer-related pathologies [913]. In cancer imaging, it has been used primarily in characterizing brain tumours [7] and in differentiating brain lesions based on diffusivity of peritumoural oedema [14]. However, there are a few recent reports of the utility of DW-MRI in prostate cancer [1519] where its role appears promising but has not been established. The extensive branching ductal structure of the normal prostate compared with the highly restricted intracellular and interstitial spaces encountered in prostate cancers produces a substantial differential in apparent diffusion coefficient (ADC), and thus the potential for high image contrast. The purpose of this study was to investigate the potential of DW-MRI in identifying malignant nodules by comparing apparent diffusion coefficients (ADCs) of malignant peripheral zone (PZ) nodules with values from non-malignant PZ and from the central gland (CG), which is primarily composed of benign nodules.
| Methods and materials |
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Imaging
Imaging was done on a 1.5-T Intera (Philips Medical Systems, Netherlands) using a balloon design endorectal coil inflated with 50 ml of air. Hyoscine butyl bromide 20 mg was administered intramuscularly to reduce peristalsis. Conventional T2 weighted fast spin-echo images were obtained transverse to the prostate and in the two orthogonal planes (FSE 2000/90 ms [TR/effective TE], echo train length 16, 2 signal averages, 20 slices) with a 256x512 matrix; 3 mm slice thickness and a 14 cm FOV (Figure 1a,b
). In addition, echo-planar diffusion-weighted sequences (DWI 2500/69 [TR/TE]) with b values of 0 mm2 s1, 300 mm2 s1, 500 mm2 s1 and 800 mm2 s1 in 3 directions were performed transverse to the prostate. This provided an approximately linear spacing of b values, and resulted in a better fit than using two points only. The phase-encoding gradient was from left to right in order to minimize motion artifacts in the prostate. Twelve 4 mm thick slices (20 cm FOV, matrix 128) provided coverage of the prostate with an image acquisition time of 1 min 24 s. Apparent diffusion coefficient (ADC) maps using the combined multidirectional diffusion data were generated using the system software (Figure 1c
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Statistical analysis
The data was tested for normality using a Shapiro-Francia test. As data was normally distributed, differences in ADC between malignant PZ, CG and non-malignant PZ were calculated using the independent samples t-tests and a p value of <0.05 was taken to be significant. A receiver operating characteristic (ROC) curve was also constructed using SPSS® (version 11.5 for Windows; SPSS, Inc., Chicago, IL) and used to examine whether the ADC could be used to differentiate between malignant PZ nodules, CG (predominantly benign nodules) and non-malignant PZ.
| Results |
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On the echo-planar diffusion-weighted images, the rigid body shift was only in the phase-encoding (left-right) direction (Figure 2a
); this bulk shift was below 1.5 mm in 70% of cases and in the range of 1.54.3 mm in 30% of cases. A bulk shift of 0.114.28 mm (median 1.10 mm) corrected for the co-registration error. After correction for these rigid body shifts, there was residual disagreement between echo-planar and T2 weighted prostate outlines of 1.2±0.5 mm due to susceptibility distortion (Figure 2b
). As these were small and variable in direction, it was considered unnecessary to attempt to further correction.
ADC values from malignant PZ were 1.30±0.30x103 mm2 s1 (mean±SD), from CG were 1.46±0.14x103 mm2 s1 and from non-malignant PZ were 1.71±0.16x103 mm2 s1 (Figure 3
). The differences between these regions were statistically significant (malignant PZ vs CG p<0.01, malignant vs non malignant PZ p<0.0001, non-malignant PZ vs CG p<0.0001).
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| Discussion |
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The mean ADC values of the malignant nodules obtained in this study correlates well with a previous report in which an endorectal coil was used [15], but not with data that was obtained with the use of a phased array coil alone [16]. This is likely to be related to the selection of ROIs, rather than to differences in data acquisition. However, poorer signal-to-noise and increased volume averaging with use of a phased array coil, may also have an impact on the ADC analysis. Compared with the previous reports, the ROI size we used was greater. This has the advantage of including the whole of a heterogeneous tumour or benign nodule and avoids bias from radiologist selected ROIs. For evaluation of non-malignant regions where ROI placement is less critical, there is good agreement between our values and those of others [15, 16]. In the six patients where contralateral tumours identified on biopsy did not correspond to low signal intensity nodules on the T2 weighted scans, foci of restricted diffusion were visually noted in two. It was not possible to obtain meaningful ADC values from these regions because of the likelihood of introducing bias in selecting ROIs on the ADC map. In order to obtain an accurate estimation of ADC from a region of tumour, registration of the ADC map with tumour ROIs drawn on whole-mount prostatectomy specimens is needed.
The prostate is composed of several regions of glandular and non-glandular tissue [21]. The non-glandular fibromuscular stroma lies anteromedially. The glandular region is divided into three zones (peripheral, transition, central). The transition and central zones comprise the central gland, which is easily distinguishable from the peripheral zone (which lies posteriorly and laterally) on T2 weighted MRI. Identification of the 30% of tumours that do not lie within the PZ is not possible on T2 weighting because of the normally low signal intensity of benign nodules and fibrous stroma in the transitional and central zones. We were therefore unable to include these tumours in our malignant ROIs. Furthermore, the inclusion of CG tumour within the CG ROI may have reduced the sensitivity of our results. Another limitation of this study is that malignant lesions not visible on T2 weighted images have not been included in the analysis. The error inherent in sampling with TRUS-guided biopsy would make it difficult to place ROIs over a biopsy-positive location where there was no identifiable MR abnormality with any degree of certainty. As it was not possible to separate benign and malignant nodules within the CG, or identify tumours not visible on T2 weighting without histological mapping of the whole-mount radical prostatectomy specimen, a further study to do this is warranted.
The glandular architecture of the normal prostate consists of small, round acini amid loosely woven, randomly orientated stroma. The epithelium is arranged in glands around a central lumen with intervening stroma made up of smooth muscle and fibrous tissue. Microscopically, BPH can involve both glands and stroma, although the former is usually more prominent. The glands are well-differentiated and still have some intervening stroma. In neoplasia, the glands of prostatic adenocarcinoma may still be recognizable as glands, but there is often little intervening stroma and the nuclei are hyperchromatic. These cellular and structural changes have a substantial impact on tissue water diffusion characteristics and on the diffusion-weighted image where image contrast is determined by the random microscopic motion of water protons. Apparent diffusion coefficients derived from these images thus reflect differences in water mobility and can potentially be used to separate nodules based on their cellularity. Malignant nodules are typically more cellular than the nodules of BPH, although there is significant heterogeneity in the latter where glandular BPH nodules, mixed BPH nodules and stromal BPH nodules with different cellularity may all co-exist. In this study, use of a threshold value of 1.6x103 for ADC could separate benign from malignant PZ with 86.7% sensitivity and 72.2% specificity. Our ADC measurements of tumour and prostate also may be overestimated because of perfusion weighting resulting from the inclusion of a b value of 0. However, we would expect the tumour ADC to be overestimated more than that of normal prostate given the greater blood flow rate and vascular volume of tumour [22]. Also, it was not possible to separately identify ADC values in regions of prostatitis, as there was only one patient in the study cohort with this histology.
In pelvic imaging, where fast acquisition to "freeze" bulk motion is of paramount importance, single-shot echo-planar sequences are favoured over turbo spin-echo sequences for diffusion-weighted imaging. The disadvantage of using single-shot turbo spin-echo sequences is the low signal-to-noise arising from long echo train length and long effective echo times. Echo-planar sequences also have their limitations and are prone to susceptibility-induced distortion, particularly in prostate imaging where air in the rectum or within the balloon of the endorectal coil causes significant local magnetic field inhomogeneity and susceptibility artefact. These susceptibility effects are greatly reduced when partially parallel acquisition methods (such as SENSE [23]) are used owing to the reduced echo-train length [24]. The measured distortion on our images was only 1.2±0.5 mm for the boundary of the whole prostate, which is less than the pixel size of the echo-planar diffusion-weighted images, and the distortion of soft-tissue lesions within the prostate would be expected to be less than this. Any inadvertent inclusion of normal tissue within the ROI transferred to the ADC maps would tend to reduce the difference in mean ADC values of tumour, rather than lead to spurious significance. This, together with the unfavourable signal-to-noise ratio in single-shot turbo spin-echo diffusion-weighted images, resulted in our preference for the echo-planar approach.
In this study we opted to use endorectal balloon coils rather than a phased array surface coil as their sensitivity for signal detection compared to a phased array coil is superior up to 5 cm from the coil surface. This provided an adequate signal-to-noise ratio on diffusion-weighted echo-planar sequences whilst also allowing higher spatial resolution for tumour identification on T2 weighted images. Previous data has shown a signal-to-noise advantage of endocavitary coils over phased array coils up to two coil diameters from the coil surface [25]. Unfortunately, endorectal coils are currently not commercially available in phased array versions to permit the use of parallel imaging. It is unlikely that the inflated endorectal coil had any significant influence on ADC values; any such effect would be symmetrical in the peripheral zone. Also, the degree of coil inflation (55 ml air) was identical in all patients reducing interpatient variability. Although it is possible to reduce susceptibility artefacts from air in the balloon by filling the balloon with perflurocarbon or water, this requires a double balloon design, and was not possible in the single balloon design endorectal coil used in our study. In our experience patient tolerance for the endorectal procedure is relatively good, particularly with short examination times (diffusion-weighted imaging 1.5 min, total examination time 17 min). In no case was the examination terminated or abandoned because of patient discomfort. Use of an endorectal coil in combination with a surface phased array coil would further improve signal detection, but this is currently not available on our system.
In future, it may be possible to use DW-MRI as an adjunct to T2 weighted sequences as a diagnostic tool for improving sensitivity of prostate cancer detection. It would complement techniques such as MR spectroscopy and dynamic contrast-enhanced imaging, which are increasingly used in tumour detection. It may also be valuable for characterization of highly cellular regions of tumours vs acellular regions, as well as for detecting treatment response, which is manifested as a change in cellularity within the tumour over time.
This work was supported by Cancer Research UK [CRUK] grant number C1060/A808.
This work was presented at the International Society of Magnetic Resonance in Medicine, FL, USA, May 2005.
| Acknowledgments |
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Received for publication February 8, 2006. Revision received June 14, 2006. Accepted for publication July 13, 2006.
| References |
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