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Cardiac Imaging |
1 From the University of Oxford Centre for Clinical Magnetic Resonance Research and Department of Cardiovascular Medicine, University of Oxford, John Radcliffe Hospital, Headley Way, Headington, Oxford OX3 9DU, England. Received February 16, 2006; revision requested April 20; revision received May 15; final version accepted July 7. Supported by grants from the British Heart Foundation and Medical Research Council. A.S.H.C. supported by a grant from the Oxfordshire Health Services Research Committee. J.B.S. supported by an intermediate research fellowship from the British Heart Foundation. Address correspondence to J.B.S. (e-mail: joseph.selvanayagam{at}cardiov.ox.ac.uk).
| ABSTRACT |
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Materials and Methods: The institutional research ethics committee approved the study. Participants gave written informed consent. Sixteen male patients (mean age, 66 years ± 13 [standard deviation]) with myocardial infarction were imaged with the same sequence by the same operator at 1.5 and 3.0 T. After cine imaging, a bolus of gadodiamide was administered. Short-axis images of entire left ventricle (LV) were acquired with a breath-hold T1-weighted segmented inversion-recovery turbo fast low-angle shot (FLASH) sequence. Agreement for myocardial hyperenhancement (HE) mass between field strengths was assessed with Bland-Altman method; agreement for detection and transmural extent of HE was assessed with
statistics. Intra- and interobserver reproducibility of mass and transmural extent of HE were assessed at 1.5 and 3.0 T.
Results: Bland-Altman analysis revealed no systematic bias (mean difference, 0.2 g; 95% confidence interval: 0.7 g, 1.2 g) and acceptable limits of agreement (3.3 to 3.8 g) between field strengths for HE mass. HE mass measurements were strongly correlated (R2 = 0.99); there was no significant difference in measurements at 1.5 and 3.0 T (28.1 g ± 15.7 [22.6% ± 10.9 of LV mass] vs 27.8 g ± 15.7 [22.3% ± 10.7 of LV mass], respectively; P = .599). For all segments, there was a high degree of agreement for HE detection (
= 0.90) and transmural grade (
= 0.79) between field strengths. Intra- and interobserver variability were low between both field strengths. Initial inversion time selected to null the signal of normal myocardium at 3.0 T was 57 msec ± 20 longer than at 1.5 T (P < .01).
Conclusion: By using the same turbo FLASH MR pulse sequence, there was strong agreement in mass and transmural extent of myocardial HE between 1.5 and 3.0 T.
© RSNA, 2007
| INTRODUCTION |
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Three-tesla MR systems that have been approved for clinical use are expected to provide an increased signal-to-noise ratio that may improve applications, such as perfusion imaging and spectroscopy, that are currently limited by low temporal and spatial resolution at 1.5 T (1218). Assessment of myocardial viability plays an important role in the clinical interpretation of the results derived from such applications. For example, a current strategy to improve the accuracy of cardiac MR imaging for depiction of coronary disease incorporates rest and stress cardiac MR perfusion results with DE MR imaging findings (19).
We hypothesized that there would be strong agreement in the mass and transmural grade of myocardial hyperenhancement (HE) between 1.5 and 3.0 T. Hence, the purpose of our study was to prospectively compare the visualization and quantification of irreversible myocardial injury in patients with confirmed chronic myocardial infarction at 1.5- and 3.0-T MR imaging.
| MATERIALS AND METHODS |
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Cardiac MR Imaging Protocol
For each patient, images were acquired by the same operator (A.S.H.C. or J.B.S.) at both 1.5 (Sonata; Siemens Medical Solutions, Erlangen, Germany) and 3.0 T (Trio; Siemens Medical Solutions) in random order, such that eight patients underwent imaging at 1.5 T first, followed by imaging at 3.0 T an hour later, and vice versa for the other eight patients.
Images were acquired with the patient in the supine position by using anterior phased-array surface coils and either posterior phased-array surface coils (at 3.0 T) or two elements of the integrated spine coil (at 1.5 T). A standard electrocardiographic lead set (Siemens) was used; four leads were positioned over the anterior chest wall. From standard pilot images, short-axis cine images covering the entire left ventricle (LV) were acquired by using a retrospectively electrocardiographically gated steady-state free precession sequence (Table 1) to aid delineation of the subendocardial border by matching these images with contrast materialenhanced images. At 3.0 T, the protocol included a postacquisition delay of 3 seconds and a steady-state free precession frequency pilot (single-shot acquisition per cardiac cycle with a trigger delay of 350 msec; section thickness, 7 mm; repetition time, 3.1 msec; frequency offsets from 200 to 200 Hz in 40-Hz increments; breath-hold time, 11 cardiac cycles) to select the optimal frequency offset.
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Imaging at both field strengths was well tolerated by all patients, and all images acquired were of sufficient quality for analysis, despite sternal wires in two (13%) of 16 patients, coronary stents in eight (50%) patients, and atrial fibrillation in one (6%) patient. In eight (50%) patients, we were able to trigger image acquisition to every other cardiac cycle. The remaining eight patients could not hold their breath long enough to enable triggering of image acquisition to every other cardiac cycle, and in these patients, image acquisition was triggered to every cardiac cycle. No problems with electrocardiographic gating were encountered.
Image Analysis
By using software (Argus, version 25A; Siemens Medical Solutions), LV end-diastolic and end-systolic volume, ejection fraction, and mass were calculated for each patient in the standard way by manually tracing the endocardial and epicardial contours on end-diastolic and end-systolic images at 1.5 T (A.S.H.C.).
By using computer software (Matlab, version 6.5; MathWorks, Natick, Mass), the mass of myocardial HE in the LV on each image was quantified by an experienced observer (J.B.S.), who was blinded to patient information and field strength and who was separate from the observer who calculated the volume and mass. Hyperenhanced pixels were defined as those with SI greater than 2 standard deviations above the mean SI in a remote, nonenhanced myocardial region on the same image (3). On each short-axis image, computer-assisted planimetry was used to delineate the area of HE, which was multiplied by the section thickness and the myocardial density of 1.05 g/mL to obtain the infarct mass. The infarct mass also was expressed as a percentage of LV mass by dividing the infarct mass by the total LV mass measured at 1.5 T. Image intensity settings were kept constant for each patient.
Furthermore, to assess agreement between both field strengths for detection and transmural grade of HE, quantitative analysis (J.B.S.) as per Kim et al (23) and blinded to patient information and field strength was performed by using the 17-segment model recommended by the American Heart Association (24) and the following scoring system: no HE, grade 0; 1%25% HE, grade 1; 26%50% HE, grade 2; 51%75% HE, grade 3; and more than 75% HE, grade 4 (5,23). Because the most apical segment can be affected by partial volume effects, it was excluded from the analysis.
To assess inter- and intraobserver reproducibility of measurements, two observers (A.S.H.C., J.B.S.) blinded to the previous results independently quantified the mass and transmural extent of HE 6 months later with a random selection of 50% of the images.
For each cardiac MR examination, the short-axis image showing the largest hyperenhanced region of myocardium was selected by an observer (A.S.H.C.) blinded to patient information and field strength. On each selected image, the observer measured SIs in the myocardial region of elevated SI (hyperenhanced myocardium) and in a remote myocardial region (nonenhanced myocardium), as well as the standard deviation of the noise in a circular region outside the body and anterior to the chest wall. The percentage SI elevation in the myocardium was calculated as follows: (mean SIHM mean SINM)/(mean SINM) · 100. The image contrast-to-noise ratio was calculated as follows: (mean SIHM mean SINM)/(1.5 · standard deviation of noise), where HM is hyperenhanced myocardium and NM is nonenhanced myocardium.
Statistical Analysis
Data analysis was performed with software (SPSS, version 13.0 for Windows; SPSS, Chicago, Ill). All results are expressed as mean ± standard deviation. The Shapiro-Wilk test of normality and z scores for skewness and kurtosis were used to assess whether the data for mass of myocardial HE and for TI conformed to the normal distribution. Agreement for mass of HE between field strengths was assessed by using the method proposed by Bland and Altman (25) and correlation coefficients, and agreement for detection and transmural extent of HE was assessed by means of
statistics. The
categories were as follows: less than 0.21, poor agreement; 0.210.40, fair agreement; 0.410.60, moderate agreement; 0.610.80, substantial agreement; more than 0.80, almost perfect agreement (26). Intra- and interobserver reproducibility of measurements of mass and transmural extent of HE were assessed by using the Bland-Altman method and
statistics. Paired t tests were used to compare the effect of field strength on measured mass of HE, initial and mean TI, percentage SI elevation, and contrast-to-noise ratio and to assess whether the order of imaging affected measurement of mass of HE or initial TI. Multilevel models were fitted to the data to allow for the correlation between repeated measurements across myocardial segments. Statistical tests were two tailed, and a P value of less than .05 was considered to indicate a statistically significant difference.
| RESULTS |
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Mass of Myocardial HE
The data for measured mass of myocardial HE conformed to the normal distribution. The mass of HE ranged from 2 g (1% of LV mass) to 57 g (40% of LV mass). There was a strong correlation between the measurements (Fig 1), and Bland-Altman analysis (Fig 2) revealed no systematic bias (mean difference, 0.2 g; 95% confidence interval: 0.7 g, 1.2 g) and acceptable limits of agreement (3.3 to 3.8 g) between both field strengths for mass of HE. The difference between mass of HE at 1.5 and at 3.0 T was not statistically significant (28.1 g ± 15.7 [22.6% ± 10.9 of LV mass] vs 27.8 g ± 15.7 [22.3% ± 10.7 of LV mass], respectively; P = .599). Further analysis confirmed that the difference between mass of HE measured at 1.5 T and that at 3.0 T did not reach significance, irrespective of the order of imaging. In patients who underwent 1.5-T imaging first, the mass of HE was 31.7 g ± 15.3 (23.4% ± 12.6 of LV mass) at 1.5 T versus 31.7 g ± 14.1 (23.4% ± 12.0 of LV mass) at 3.0 T (P > .99). In patients who underwent 3.0-T imaging first, the mass of HE was 23.4 g ± 16.2 (20.8% ± 7.3 of LV mass) at 1.5 T versus 22.8 g ± 17.3 (20.1% ± 8.5 of LV mass) at 3.0 T (P = .462).
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= 0.90), with exact agreement in 243 (94.9%) of 256 myocardial segments. Of a total of 256 myocardial segments in all 16 patients, 127 (49.6%) were graded as showing some degree of HE at 1.5 T, and 128 (50.0%) were graded as showing some degree of HE at 3.0 T (Fig 3).
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= 0.79), with exact agreement in 221 (86.3%) of 256 myocardial segments (Fig 4). These associations remained strong and highly significant (both, P < .01) after adjusting for the correlation between multiple segments in multilevel models.
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= 0.78 and 0.74 at 1.5 T and 3.0 T, respectively) and interobserver agreement (
= 0.70 and 0.67 at 1.5 T and 3.0 T, respectively).
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| DISCUSSION |
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There are two critical elements in the clinical performance of the DE technique at 1.5 T (27). First, its ability to help quantify small areas of myocardial necrosis (with a resolution almost 30-fold greater than that at SPECT) allows visualization of microinfarcts that cannot be depicted with other imaging techniques (7). Second, by providing direct depiction of both nonviable and viable myocardium, DE MR imaging gives information about the transmural extent of irreversible injury, which makes it a powerful tool for the prediction of myocardial viability (23). In our study, we assessed both of these elements at 3.0 T and compared them with the already validated 1.5-T sequence. We found that both the measurement of volume (with computer-assisted planimetry) and transmural grade of HE were virtually identical at 1.5 and 3.0 T, despite sternal wires and coronary stents in a substantial proportion of patients and despite theoretic concerns of reliable R-wave triggering (amplified magnetohydrodynamic effects) at 3.0 T.
Furthermore, our study results demonstrated good intra- and interobserver agreement for measurements of mass and transmural extent of HE at both field strengths. This indicates that DE MR imaging with a turbo FLASH pulse sequence is a reproducible technique at either field strength. The mass of HE quantified in our study cohort was over a wide range, representing very small (2 g; 1% of LV mass) to large (57 g; 40% of LV mass) areas of myocardial injury. Some of the variability in measurements of mass of HE can be accounted for by intra- and interobserver variability, although observer variability was 5% or less at both field strengths. There was less agreement for transmural grade of HE than for detection of HE. The principal reasons were the inherently greater variability in scoring transmural grade from 0 to 4 when compared with that of the binary decision as to whether HE is present or absent and some variability in registration of segments between 1.5- and 3.0-T imaging.
Injured myocardium demonstrates greater shortening of the T1 after contrast material administration than does normal myocardium. Inherent to the higher field strength at 3.0 T, myocardial T1 is longer than that at 1.5 T. Results of our study demonstrate that optimal TI to null the signal of normal myocardium needs to be longer at 3.0 T at the same time after contrast material injection. This is to be expected because the TI chosen to provide maximal SI difference between infarcted and normal myocardium is directly related to myocardial T1.
The percentage SI elevation and contrast-to-noise ratio obtained in our study at 1.5 T compared favorably with those reported by Simonetti et al (1) in their work in canine hearts. However, we found no significant differences in the percentage SI elevation or contrast-to-noise ratio between both field strengths, which is consistent with the findings of Hackenbroch et al (28). Results of other studies demonstrate higher percentage SI elevation at 3.0 T than we found (1107% [21] and 1230% [28]), which might be explained by the use of double the contrast agent dose (0.2 mmol/kg) in these studies when compared with ours (0.1 mmol/kg). Theoretically, one might expect that the signal-to-noise ratio would double when the static magnetic field strength is doubled and that the increase in T1 would make the effects of contrast agents more pronounced. There may be several reasons for our findings. In practice, the increased T1 may have decreased our signal-to-noise ratio because of saturation effects, which counteracted the signal-to-noise ratio increase caused by the higher field strength. Second, different radiofrequency coil configurations were used with each system. Third, the sequence parameters at 1.5 T have been thoroughly optimized and one would expect 3.0-T data to improve with optimization, and contrast agent dose, repetition time, and flip angle are likely to play an important role.
Our study had limitations. The number of patients was small, and, to keep the patient cohort uniform, we excluded patients with acute myocardial infarction or nonischemic cardiomyopathy. Hence, we could not assess the phenomena of microvascular obstruction (8) (zone of hypoenhancement surrounded by hyperenhanced myocardium on images) or myocardial fibrosis seen in dilated or hypertrophic cardiomyopathy (29,30). Nevertheless, we suspect 3.0-T DE MR imaging to be similar to 1.5 T for these indications, provided the TI is appropriately lengthened.
Residual contrast material at acquisition of the second set of DE images in each patient may have affected the TI and/or mass of HE measured. However, in healthy human volunteers, Weinmann et al (31) demonstrated that the plasma concentration of gadolinium-based contrast material declines according to a biexponential function, with a distribution phase with a mean half-life of 12 minutes ± 7.8, and concluded that its efficiency to enhance SI will last up to only about 1 hour after intravenous injection of 0.1 mmol/kg. Accordingly, in our cardiac MR protocol, the time interval between acquisition of the sets of images with each system was 1 hour for each patient, the operator adjusted TI during each examination to maintain optimum nulling of the signal of the normal myocardium, and the randomization of the order of imaging was perfectly balanced to avoid bias. Furthermore, our data indicate that the order of imaging had no influence on the initial TI selected by the operator or the mass of HE measured.
The results of our study demonstrate that DE MR imaging at 3.0 T is a reproducible technique that can be applied for the identification of irreversible injury and myocardial viability. We envisage that DE MR imaging can be included as part of the comprehensive cardiac MR protocol at 3.0 T with applications such as myocardial perfusion and spectroscopy that are likely to be improved by the increased signal-to-noise ratio associated with the higher field strength.
| ADVANCES IN KNOWLEDGE |
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| FOOTNOTES |
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Abbreviations: DE = delayed enhancement FLASH = fast low-angle shot HE = hyperenhancement LV = left ventricle SI = signal intensity TI = inversion time
Authors stated no financial relationship to disclose.
Author contributions: Guarantors of integrity of entire study, A.S.H.C., S.N., J.B.S.; study concepts/study design or data acquisition or data analysis/interpretation, all authors; manuscript drafting or manuscript revision for important intellectual content, all authors; approval of final version of submitted manuscript, all authors; literature research, A.S.H.C., M.D.R., J.B.S.; clinical studies, A.S.H.C., J.B.S.; statistical analysis, A.S.H.C., M.D.R., J.B.S.; and manuscript editing, all authors
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