Differentiation of spinal lesions using monoexponential, biexponential, and gamma distribution diffusion-weighted MR Imaging: Initial clinical results
Miyuki Takasu1, Yuji Akiyama1, Chihiro Tani1, Yoko Kaichi1, Takayuki Tamura1, Koichi Oshio2, and Kazuo Awai1

1Diagnostic Radiology, Hiroshima University Hospital, Hiroshima-shi, Japan, 2Department of Diagnostic Radiology, Keio University School of Medicine, Tokyo, Japan

Synopsis

The purpose of this study was to quantitatively compare various diffusion parameters obtained from monoexponential, biexponential, and gamma distribution models in differentiating vertebral lesions in human subjects. All MR parameters, except for ADCfast and frac > 3, were significantly different between normal bone marrow and lesions. Water molecular diffusion parameters may provide additional information and improve the differentiation of spinal lesions compared with conventional diffusion parameters. This also refers to differentiation of malignant lesions from acute spinal fracture, in which both PG (D) calculated from gamma distribution model and perfusion fraction f of the biexponential model proved to be useful.

Intruduction

An isotropic apparent diffusion coefficient (ADC) obtained from diffusion-weighted imaging (DWI) with a monoexponential model may not be able to accurately reflect water molecular diffusion in vivo due to influence by the microcirculation of blood in capillaries1. The purpose of this study was to quantitatively compare the potential of various diffusion parameters obtained from monoexponential, biexponential, and gamma distribution models in differentiating vertebral lesions in human subjects.

Materials and Methods

Theoretical Background:

The ADC value was calculated using a monoexponential model as follows:

S(b)/S(0) = exp(-b·ADC),

where S(b) represents the signal intensity in the presence of diffusion sensitization, b, and S(0) represents the signal intensity in the absence of diffusion sensitization.

Three parameters: perfusion fraction (f), pseudo-ADC (ADCfast), and true ADC (ADCslow), were calculated using biexponential intravoxel incoherent motion analysis1:

S(b)/S(0)= [f·exp (-b·ADCfast)] +[(1 - f )·exp(-b·ADCslow)].

The GDM assumes a continuous distribution of diffusion coefficients, P(D). The DW signal can be written as follows:

(1) $$S(b)=\int P(D)exp(-bD)dD$$

The gamma distribution function, PG(D) has been suggested recently2:

(2) $$PG(D,\kappa,\theta)=D^{\kappa-1}\frac{exp(-D/\theta)}{Γ(\kappa)\theta^{\kappa}}$$

where Γ is the gamma function, θ is the scale parameter of the same dimensionality as the diffusivity, and κ is the shape parameter. Replacing P(D) in Eq. (1) by PG(D) in Eq. (2), gives the following expression for the DW signal attenuation:

S(b)=(1+bθ)

The excess kurtosis K of the diffusion probability distribution function (PDF) can be calculated as:

(3) $$K=\frac{\mu_{4}}{\mu_{2}^{2}}-3=\frac{12t^{2}(\kappa^{2}\theta^{2}+\kappa\theta^{2})}{4t^{2}\kappa^{2}\theta^{2}}-3=\frac{3}{\kappa}$$

where μn is nth moment of the PDF.

MRI examination:

DW images of the 73 subjects’ lumbar spines were categorized as follows: patients with normal bone marrow (n=43), patients with acute spinal fracture (n=11), and patients with malignant spinal tumor (n=19; multiple myeloma, 8; lymphoma, 3; chordoma, 2; acute lymphocytic leukemia, 2; metastatic tumor from lung cancer, 4). MRI examinations were performed on a 3T system (Ingenia; Philips Healthcare) equipped with the anterior coil and the integrated posterior coil. Single-shot DW EPI with 9 values (0, 40, 80, 140, 200, 500, 1000, 1500, 2000) on 3 orthogonal axes were performed with the following acquisition parameters: TR/TE =8000/84 ms, FOV= 35×35 cm2, matrix size 192×192, in-plane voxel size 1.8×1.8 mm2, slice thickness 4 mm, number of slices 11, slice gap 1 mm, factor of 3 SENSE on the phase direction, and 1 average.

Image data analysis:

Mean signal intensity was calculated by placing operator-determined regions of interest (ROIs) within the malignant spinal lesions or within the bone marrow (BM) of an acute vertebral fracture or within normal BM for each b-value in each subject. Signal intensity values for BM were calculated as the mean value obtained from the L1 to L3 vertebral bodies for normal subjects. For each of subject, ADC, f, ADCfast, ADCslow, scale parameter θ, scale parameter κ, the area fraction of D < 1.0mm2/s (frac <1), the area fraction of D > 3.0 mm2/s (frac >3), PG(D) and K, calculated from the GDM, were measured using equations (1-3).

Statistical analysis:

Parameters of the 3 groups (i.e., normal-, fracture-, and malignant groups) were compared by the Kruskal-Wallis test. Multiple regression analysis was performed to identify the potential association of diffusion model parameters for differentiating BM diseases and receiver operating characteristic analyses were then performed.

Results and discussion

Table 1 summarizes the MR parameters for the 3 groups. All MR parameters, except for ADCfast and frac > 3, were significantly different between normal BM and lesions. Perfusion fraction f, scale parameter θ, and PG (D) proved to be useful for the differentiation of malignant lesions from acute spinal fractures.

Multiple regression analysis demonstrated that the perfusion fraction f (P=0.03) and and PG(D) (P=0.02) contributed to the risk for malignant spinal lesions. Areas under the curve (AUCs) were 0.727 for PG(D) (sensitivity: 84.2%, specificity: 63.6%), and 0.703 for perfusion fraction f (sensitivity: 68.4%, specificity: 81.8, Fig. 1).

A meta-analysis in 2008 concluded that the capability of ADC to distinguish benign fractures from pathologic fractures was dependent on signal intensity in a fractured vertebra on DWI3. In this study, perfusion fraction f and PG(D) were shown to be useful for differentiating benign fractures from malignant spinal lesions. They had similar AUCs for differentiation, but these 2 parameters might be regarded as complementary regarding sensitivity and specificity.

Conclusion

Water molecular diffusion parameters may provide additional information and improve the differentiation of spinal lesions compared with conventional diffusion parameters, which would be helpful in improving therapy strategies and prognoses. This also refers to differentiation of malignant lesions from acute spinal fracture, in which both PG (D) calculated from GDM and perfusion fraction f of the biexponential model proved to be useful.

Acknowledgements

No acknowledgement found.

References

1. Le Bihan D, Breton E, Lallemand D, et al. Separation of diffusion and perfusion in intravoxel incoherent motion MR imaging. Radiology 1988;168(2):497–505.

2. Oshio K, Shinmoto H, Mulkern RV. Interpretation of diffusion MR imaging data using a gamma distribution model. Magn Reson Med Sci. 2014 13:191-195.

3. Karchevsky M, Babb JS, Schweitzer ME. Can diffusion-weighted imaging be used to differentiate benign from pathologic fractures? A meta-analysis. Skeletal Radiol. 2008 Sep;37(9):791-795.

Figures

Table 1 MR parameters for the 3 groups.

Note. Values represent the means ± standard deviation.

**P < 0.01, normal bone marrow vs. acute fracture or malignant lesion.

*P < 0.05, normal bone marrow vs. acute fracture or malignant lesion.

+P < 0.05, acute fracture vs. malignant lesion.


With the cutoff value derived from ROC analysis, PG(D) could be used to differentiate malignant spinal lesions from acute spinal fractures with 84.2% sensitivity and 63.6% specificity. PG (D), gamma distribution function; f, perfusion fraction.



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
4472