Thyroid nodules are frequently detected with the widespread application of sonography (
15). However, the malignancy rate of palpable nodules is less than 5% (
2). The primary goal of imaging is to determine the malignant nodules. MRI diffusion characteristics of thyroid lesions may help us to differentiate different types of thyroid nodules.
Diffusion is a random microscopic movement of water molecules. Measurement of diffusion in vivo is now possible with diffusion-weighted MRI and ADC measurements. The hypercellularity within malignant tumors leads to reduction in the diffusion space of water molecules in the extracellular and intracellular space (
16-
18). In recent years, DWI in the head and neck region and the thyroid gland has gained importance (
2,
8-
10,
13,
19-
21). The malignant thyroid nodules when compared with the benign ones have larger nuclei and an increased number of cell counts resulting in a decreased extracellular matrix (
22). Due to these tissue characteristics, there is restriction in movement of water molecules in malignant nodules resulting in findings of restricted diffusion, and low ADC values on DWI (
2,
8,
10,
13). The difference in ADC values between benign and malignant nodules on 1.5 Tesla magnets has been demonstrated by other authors. Most of the studies demonstrated that the ADC values of benign thyroid nodules are significantly greater than those of malignant nodules (
2,
8,
10). The b value has an impact on image quality and ADC measurement. A high b value image provides valuable diffusion data with restricted perfusion and T2-weighted effects. However, as the b value increases, the noise increases leading to distortion of the images (
23). Image distortion due to susceptibility artifacts is prominant at higher field strength magnets. However, these limitations can be overcome by using parallel imaging, smaller voxel size and shorter echo times (
11,
24,
25). In our study, to improve image quality, we performed DWI with parallel imaging (GRAPPA factor: 2), 4 mm slice thickness and 128 × 128 matrix size and obtained images without degradation. In literature, there are limited number of studies about thyroid nodules that have been performed on 3 Tesla magnets (
13,
14). In a recent study conducted by Ilica et al., they used six b values, with the highest b value of 1500. The mean ADC values for benign and malignant nodules were 1.548 × 10
-3 mm
2/s, and 0.814 × 10
-3 mm
2/s respectively. The ADC values were significantly different among these groups (P < 0.001). Similarly in our study, we used high b values (b:500, b:1000) and the ADC values of 63 benign nodules were significantly higher than the 13 malignant nodules at both b levels (P < 0.000). The mean ADC value of the benign nodules was 2.022 × 10
-3 mm
2/s and the mean ADC of the malignant nodules was 1.027 × 10
-3 mm
2/s for b:1000 in the present study. Ilicaet al. reported the mean ADC value of the normal thyroid tissue as 1.323 ± 210 (× 10
-3 mm
2/s) in the healthy control group. This finding is similar with the ADC values of our healthy control group at b:1000 (1.350 ± 150 × 10
-3 mm
2/s) (
13).
Despite the new automated measurement techniques, ADC values can vary between patients and within patients. For this reason, ADC measurements from unaffected tissues of patient groups were compared with each other and with the control group. Calculation of the normalized ADC values can eliminate the imaging related variability (
21,
26). Bozgeyik et al. checked the normal looking parenchyma of patients with thyroid nodules. There were no significant difference between the ADC values of thyroid tissue in healthy subjects and the patient group with nodules (
10). They reported that the thyroid parenchyma ADC values of the patient group can be regarded as a reference as control group (
10). We could evaluate the average parencyhmal ADC value in 25 patients. ADC values obtained from the parenchyma fields were confirmed histopathologically as normal in these patients. Therefore, we think that the parenchyma ADC values of this patient group can be accepted as a reference for thyroid gland parenchyma. Similar to the study carried out by Bozgeyik et al. (
10) in our study, no statistically significant difference was found between the normal parenchyma ADC
MEAN of the patient and control group at b: 500 and b:1000. When we compared the parenchyma ADC
MEAN values of the malignant, benign and control groups, we also found no difference between the three groups (
Table 1). In our study, nodal ADC
MEAN/thyroid parenchyma ADC
MEAN ratios of malignant nodules were significantly lower than benign nodules in both b: 500 and b:1000 values and there was no overlap between these groups. In the analysis of the ROC curve showing the power of the ADC
MEAN/thyroid parenchyma ADC
MEAN ratio to differentiate benign and malignant nodules, the area under the curve was 0.99 for b:500 and 1 for b:1000. Sensitivity at thresholds determined by the curve was found to be 100% for both b:500 and b:1000 values. That is, the ADC ratio of all malignant nodules is below 0.98 at b:500 and below 0.95 at b:1000 and the specificity is 92% and 100% respectively at b:500, b:1000. According to these results, the use of the nodal ADC
MEAN/thyroid parenchyma ADC
MEAN ratio in distinction of malignant-benign thyroid nodules appears to be a very sensitive and specific method. The limitation of this method is multinodular goiter cases in which measurement of intact thyroid parenchyma may be difficult. Mutlu et al. normalized their measurements using the spine as a reference (
21). However, the spinal cord is surrounded by spinal osseous elements, which can lead difficulty in measurements. According to our findings, the intact thyroid tissue of the patient can be used for normalization issues. Therefore, combination of normalized ADC values might be helpful in the interpretation of thyroid nodules and might determine the optimal ADC ratio for quantitative evaluation.
There are several limitations of the study. First, evaluation of nodules below 1 cm was not included in the study. Therefore, it is necessary to determine the accuracy of 3 Tesla diffusion MRI findings in this group of patients as well. Second, the sample size of malignant nodules was relatively small in our study group. A larger population would probably strengthen these findings and provide more information.
In conclusion, the findings of our study show that ADC values obtained with high b values at 3 T are beneficial in differentiation of benign and malignant thyroid nodules. Measurement of nodule ADCMEAN/thyroid parenchyma ADCMEAN ratio is a valuable adjunctive tool. Further large scale studies are mandatory to predict the clinical impact of 3 T DWI.