In our study, we have confirmed that the permeability changes after a single dose of anti-VEGF treatment are correlated with survival measures. We extend these earlier findings by exploring the performance of DSC-MRI rather than DCE-MRI, and by using automatic postprocessing routines. This more streamlined, T
2*-based approach appears capable of predicting patient outcome after 1 day of anti-VEGF therapy, just as the dual T
1- and T
2*-based approach described earlier. As in the original
VNI work (
Sorensen et al, 2009), including circulating collagen IV levels further improved the correlation to
PFS. With the potential to exclude DCE imaging and blood sampling from the analysis, however, MRI (DSC imaging ~2

minutes) and postprocessing (~seconds) times are reduced considerably.
Ktrans from DCE imaging is extensively used as an imaging marker for the characterization of glioma type and treatment effect (
Tofts and Kermode, 1991;
Roberts et al, 2000;
Batchelor et al, 2007;
Sorensen et al, 2009;
Beaumont et al, 2009;
Lacerda and Law, 2009). Furthermore, it has also been shown that cerebral perfusion, blood volume, and permeability can be simultaneously acquired from the DCE first-pass response and used to characterize gliomas (
Li et al, 2003;
Larsson et al, 2009). In one study (
Li et al, 2003), this was performed by iterative separation of the intravascular and extravascular components of the contrast agent concentration contribution to the first-pass curves. In our study using a fully automated approach, DSC imaging was selected over DCE because optimal assessment of brain tissue hemodynamics from DCE imaging is dependent on correct estimates of T
1 and reduction of T
2* effects on the AIFs. Also, compared with DSC, DCE usually suffers from lower temporal resolution and spatial coverage. Nevertheless, contrary to DCE imaging, DSC-based measures of permeability have not received as much attention for tumor classification. Reasons for this might be the complexity of the analysis and that DSC-based permeability values are hard to quantify. Consequently, permeability estimates using DSC in the literature vary. One study reported differences in a
Ktrans parameter between glioblastomas, meningiomas, and lymphomas by using first-pass pharmacokinetic modeling on the DSC images (
Johnson et al, 2004). Using the same method, a second study reported good correlation between
Ktrans from DCE and DSC in gliomas, whereas a third study reported poor correlation between
Ktrans and glioma grade (
Law et al, 2004;
Cha et al, 2006). When comparing
Ktrans from DCE and DSC in meningiomas, the correlation was poor (
Cha et al, 2006). Furthermore, another study used the same method to successfully predict high glioma grade based on a combination of
Ktrans and
CBV (
Law et al, 2006). Using method I, one study showed that the DSC-based
K2 parameter could successfully differentiate between high- and low-grade gliomas, whereas another study did not observe this effect (
Donahue et al, 2000;
Provenzale et al, 2002). Also, similar to our study,
K2 has been shown to be unsuccessful in predicting response (time to progression) of antiangiogenetic therapy in glioblastomas (
Sawlani et al, 2010).
Results from the simulations in Part I and the patient data in Part II suggest a similar relationship between the DSC-derived
Ka permeability parameter and
Ktrans from DCE imaging. Using linear mixed model analysis on the patient data, median
Ka values were found to increase significantly for increasing
Ktrans cohorts. Furthermore, our results showed the
Ka data tended to converge at higher values of
Ktrans, resulting in a borderline significantly higher goodness of fit when using a quadratic polynomial function compared with that of a linear function. Thus, although the assumption of a linear relationship to
Ktrans will be valid for most
Ka values, care should be taken with high
Ka values as our proposed DSC leakage correction model assumes a negligible reflux (
KtranstN−1/
ve![[double less-than sign]](/corehtml/pmc/pmcents/x226A.gif)
1), which is not reasonable for high values of permeability. As discussed in more detail in Part I, this leads to an underestimation of
Ka. Our group is currently working on a method that will assess and correct for this effect by applying a second linear fit to the tail of the residue function. Furthermore, even with the use of a 0.1-mmol/kg predose to minimize T
1-dominant extravasation effects (
Paulson and Schmainda, 2008;
Hu et al, 2010), 10 of 30 patients showed a negative ‘dip' in the
Ka values at low
Ktrans. As discussed in Part I, this might be explained by the predose not being able to remove all T
1 effects in the MR signal in all patients. Here, it has been previously shown that the size of the loading dose needs to be sufficiently high (
![[gt-or-equal, slanted]](/corehtml/pmc/pmcents/ges.gif)
0.1

mmol/kg) for optimal tissue saturation (
Donahue et al, 2000). Consequently, for the range of
Ka (
K2) values reported in our study, care should be taken when evaluating values close to zero. Potentially, at the cost of lower SNR, using a lower flip angle in the DSC imaging protocol should minimize this effect.
Nevertheless, our results showed
Ka to be sensitive to anti-VEGF treatment effects and predictive of both
PFS and
OS. Thus, the
Ka values obtained in our patient data suggest that DSC imaging can form the basis for a pseudo-leakage parameter that scales with tumor permeability and consequently patient prognosis. Using a histogram-based method (
Emblem et al, 2008), more homogenous distributions of
Ka values (comparable to a greater reduction in mean values) were seen at day +1 in patients with increased
PFS and
OS. Compared to using mean values (assuming T
2*-dominant leakage only), a higher correlation with
PFS and
OS was observed for both methods when using the histogram method (data not shown). Furthermore, compared to the reference study (
Sorensen et al, 2009), a higher correlation with
PFS and
OS was observed for
CBV using both methods. This is probably due to the use of a fully automated, user-independent analysis method including automatic AIF selection and partial volume correction (
Bjornerud and Emblem, 2010). Interestingly, although the resulting
CBV maps of the two methods can have clearly visible differences, our results suggest that the influence of the leakage correction method on predictive values of
CBV to survival is relatively limited. Hence, when using
CBV as the only parameter to assess tumor response to therapy, the choice of leakage correction method seems relatively unimportant. While this argument may not hold true for preoperative tumor grading, the high prognostic value of the
CBV parameter to progression and survival during anti-VEGF treatment in our study seem to suggest that the dramatic changes in microvasculature blood volume reduce the influence of the leakage correction error. When including the
Ka (
K2) parameter in the analysis, however, choosing an
MTT insensitive correction method can prove important as studies have shown that
MTT increases with the higher vascular complexity associated with tumor angiogenesis (
Bastin et al, 2006;
Jain et al, 2007). This may be especially critical when assessing therapy-induced vascular normalization properties as anti-VEGF therapy in combination with radiation and chemotherapy kills or suppress cancer cells thereby normalizing tumor vascularity and potentially restoring impaired blood flow (
Griffon-Etienne et al, 1999;
Batchelor et al, 2007;
Sorensen et al, 2009;
Jain et al, 2009). Furthermore, the Kaplan–Meier curves suggest that the
VNI parameter derived using method II is able to consistently identify patients that respond to anti-VEGF therapy and subsequently have longer
PFS and
OS. Using method I, however, the survival distributions for
OS were not different for the ‘poor responding' and ‘good responding' groups. Although these results should be used with care and there may be more than one choice of survival distribution groups, our results indicate that the
VNI parameter of method II holds a higher sensitivity to potential treatment effects to that of method I.
Whether the higher predictive values of the Ka parameter over K2 is because Ka is closer to a true measure of the permeability surface area product remains to be explored, but the correlation between the logarithmic differences in Ka and K2 and MTT suggests that K2 deviate from Ka at higher MTT values resulting in an overestimation of the K2 leakage effect, an argument also supported by the results from Part I of our study. This effect was observed for both T1- and T2*-dominant contrast agent extravasation. Contrary to Part I, however, there was no correlation between the logarithmic differences in CBV and MTT. This result is in line with the survival analysis discussed above, in that the Ka (K2) seem to hold a higher sensitivity towards changes in MTT compared with CBV. A reason for this might be that relative changes in CBV are modest compared with relative changes in Ka (K2). Nevertheless, it should be noted that this discrepancy between Parts I and II may in part also be explained by differences in sampling sizes between the two studies.
A potential limitation to method II is that an AIF needs to be identified. Although this is the focus of much research and debate (
Rausch et al, 2000;
Kiselev, 2001;
Knutsson et al, 2004) selecting an optimal AIF with correct tissue density and large/small vessel hematocrit values can be difficult and further complicates the analysis compared with method I. However, to improve stability, we applied a recently published fully automatic method for AIF selection and partial volume correction (
Bjornerud and Emblem, 2010). Furthermore, we minimized unwanted oscillations in the residue functions by employing a heavy computational iterative Tikhonov regularization-based SVD deconvolution method. Results from Part I of our study showed that the estimation of
Ka is rather insensitive to oscillations and the use of a much faster truncated SVD approach should potentially have little influence on our results. Also, contrary to our simulations, an offset in
Ka values for
Ktrans values equal to zero was observed in our patient data. This may be explained by an incorrect nonzero estimation of
Ka for low leakage values due to noise limitations. Thus, a better estimation of the residue function by fitting a Lorentzian function and a linear component to the data may reduce this systematic error. This relatively small error, however, should be uniform across patients and have minimal influence on our results.
In conclusion, we have shown that prognostic values of progression and survival in brain tumor patients undergoing anti-VEGF therapy can be assessed using a single MRI acquisition and automatic postprocessing routines insensitive to variations in MTTs. Our results are comparable to previous studies using more input data. The reduced complexity of the proposed method brings MRI one step closer to providing clinically feasible imaging biomarkers for monitoring early tumor response to treatment.