Apparent diffusion coefficient measurement of the parotid gland parenchyma
Review Article

Apparent diffusion coefficient measurement of the parotid gland parenchyma

Maja Bruvo1^, Faisal Mahmood2,3^

1Radiography, Department of Technology, Faculty of Health, University College Copenhagen, Copenhagen, Denmark; 2Laboratory of Radiation Physics, Department of Oncology, Odense University Hospital, Odense, Denmark; 3Research Unit for Oncology, Department of Clinical Research, University of Southern Denmark, Odense, Denmark

^ORCID: Maja Bruvo, 0000-0002-9939-6337; Faisal Mahmood, 0000-0002-7270-7967.

Correspondence to: Maja Bruvo. Birkevaenget 6, 4621 Gadstrup, Denmark. Email: majl@kp.dk.

Abstract: The measurements of apparent diffusion coefficient (ADC) with diffusion weighted magnetic resonance imaging (DW-MRI) is becoming a popular diagnostic and research tool for examination of parotid glands. However, there is little agreement between the reported ADC values of the parotid gland in published literature. In this review 43 studies on ADC measurement of the parotid glands were included. The analyses indicated several possible culprits of the observed ADC discrepancies. For example, DW-MRI examinations under gustatory stimulation gives higher ADC values compared to the unstimulated parotid gland (P=0.003). The diffusion weighting factors (b-values) can either increase (b-value <200 s/mm2) or decrease ADC values (b-values >1,000 s/mm2). The timing of follow-up DW-MRI after radiotherapy (RT) indicates correlation to the found ADC values (R2 =0.39). Interestingly, the choice of regions of interest (ROI) appears not to affect the measurements of ADC (P=0.75). It can be concluded that there is a critical need for standardization of ADC measurement of the parotid glands to allow valid inter-study comparisons and eventually to reach consensus on the use of ADC as biomarker.

Keywords: Diffusion weighted magnetic resonance imaging (DW-MRI); apparent diffusion coefficient; parotid gland parenchyma


Submitted Oct 21, 2020. Accepted for publication Mar 18, 2021.

doi: 10.21037/qims-20-1178


Introduction

Diffusion weighted magnetic resonance imaging (DW-MRI) is a popular diagnostic tool in radiology, and in radiotherapy (RT) it is becoming a standard supplementary technique for outlining the extent of the tumor for treatment planning. In research, its potential as a non-invasive biomarker of treatment response is being studied extensively (1,2). DW-MRI provides image contrast based on differences in the Brownian diffusion of water molecules within the tissue. The diffusion can in a post-processing step be quantified in terms of the so-called apparent diffusion coefficient (ADC).

In parotid glands, DW-MRI is commonly used in clinical evaluation, for example with information about localization of the tumor within the parotid gland and differentiation of malignancy from benignity (3). It has also been investigated for the diagnosis of xerostomia, Sjögren’s syndrome, Kimura disease and other non-neoplastic disorders affecting the parotid glands. More recently (since 2001) there has been a growing interest in using ADC to investigate functional and structural changes in the parotid glands in patients treated with RT for cancer in the head and neck region to diagnose or predict side effects like xerostomia (4-6).

Furthermore, it may be expected that with the recent clinical release of the hybrid MRI linear accelerator (7) ADC may be studied even more intensively in the coming years in different anatomies including the parotid gland.

A quick search of the published studies revealed that there is a substantial variation in the study designs, DW-MRI acquisition protocols and post processing steps, including definition of the region of interest (ROI) and ADC calculation methods. This is problematic since there is a potential risk that the reported ADC values are correlated to technical differences of the studies rather than biological differences within patient subgroups. This has in fact been indicated in a few previous studies of for example DW-MRI protocols (8), ROI definition (9), and timing of DW-MRI following gustatory stimulation and RT (5,10).

The lack of standardization of ADC measurement in the parotid gland is a potential limitation for valid inter-study comparison, and in the end to reach valid clinical consensus for the use of ADC as a biomarker. This review includes all currently published DW-MRI studies where ADC has been used for evaluation of parotid glands, to provide a comprehensive overview of the potential covariates. It is organized into introductory sections about DW-MRI and the parotid gland including an overview of radiation toxicity and ROI selection. This is followed by a discussion of possible factors affecting the ADC of the parotid gland based on the reviewed publications.

Throughout this review the term normal parotid parenchyma is used to designate the disease-free parotid parenchyma. Studies examining normal parotid parenchyma and irradiated normal parotid parenchyma in head and neck cancer patients treated with RT are included to discuss the ADC values in relation to trial design, DWI-MRI acquisition and post processing. Studies examining the diseased parotid gland (parotid tumors, Sjögren’s syndrome and Kimura disease) are included to survey acquisition parameters only. Conclusions based on current studies and recommendations for future studies are provided.

Technical introduction

The biophysical basis of DW-MRI

In DW-MRI, the MRI signal is sensitized to the diffusion of water (hydrogen nuclei) within the tissue. Free diffusion is characterized by a Gaussian displacement distribution, the width of which at a given temperature is proportional to the diffusion coefficient and the time during which diffusion has taken place (diffusion time), i.e., in this framework, the diffusion coefficient can be defined as the proportionality constant between the mean squared displacement of a particle and the time allowed for diffusion. At body temperature (310.15 K or 37 °C) and at typical diffusions times (~5 ms) of the DWI-MRI sequence the mean squared displacement of free water (within an imaging voxel) is about 10 micrometers, the order of magnitude of a human cell. In the tissue the cellular environment delimits the degree of free diffusion, and therefore a structural change in the cellular environment (for example due to pathology) may result in an altered displacement distribution and reflected in the diffusion coefficient. The term apparent diffusion coefficient (ADC) was coined for DW-MRI to underline that it reflects the average diffusivity of water in a heterogeneous cellular environment.

DW-MRI acquisition

In DW-MRI the challenge is to measure very small and short-lived signals. That requires speed and repetition. The initial development of DW-MRI was done specifically in the subfield of neuroimaging, and focusing the technique on other parts of the body and relevant clinical issues has seen challenges from physiological aspects, such as movement, and anatomical differentiation, posting sudden changes in the signal from tissues or indeed voids, all leading to problems in acquiring the signal and assigning it properly. The increase in field strength in clinically available scanners, moving typically from 1.5 tesla (T) to 3 T, yields an immediate boost in neuroimaging, but often presents a less straightforward advantage in other parts of the anatomy, as not only the signal is increased, but also the attendant artifacts.

In the case of parotid imaging, the initial approach has been to apply the readily available neuroimaging techniques without much alteration. As new hardware, such as specialized coils, and imaging sequences less prone to artifacts have become available, an approach tailored to the specific organ is beginning to appear. In coil design, proximity to the tissue is key, and moving from head coils, designed primarily for brain imaging, to dedicated head and neck (HN) or neurovascular (NV) coils has been a step forward. A shift away from the standard clinical acquisition protocol of two b-values towards an investigation of whether other values would be more appropriate is also beginning to appear.

The DW-MRI sequence consists of a diffusion sensitization part, in which the diffusion gradients are applied, and an imaging part where imaging gradients are applied. Diffusion sensitization is achieved by the key physical concept that magnetic gradients accumulate a phase difference in water hydrogen nuclei (protons). In the standard DW-MRI a pair of diffusion gradient pulses is used with a 180 refocusing RF pulse in between (pulsed field gradient spin-echo technique) (11). The first gradient labels the protons by inflicting a certain position dependent phase change. In case of static protons, the second gradient will rewind the phase change completely. Diffusing protons on the other hand will not be phase refocused which will result in a decreased signal. The diffusion sensitized signal decays as a function of the amount of diffusion-weighting applied through the use diffusion sensitizing gradients expressed as b-values. For the imaging part most frequently echo planar imaging (EPI) with fat saturation is used since it is fast. Sometimes, fast spin echo (FSE) is preferred because it is less prone to geometrical distortions (12). This is however at the expense of longer imaging time or lower signal-to-noise (SNR). With longer scan times collateral effects such as motion artifacts can further deteriorate image quality.

The optimal choice of b-values is not clearly defined and depends upon system performance (field strength, gradient strength and slew rate), number of signal averages and the clinical application. The usual range of b-values in clinical practice is about 1,000 s/mm2, usually from 0 to 1,000 s/mm2, with some anatomical site dependent variations. The upper limit is basically dictated by the hardware capability of clinical systems. If the b-value is set too high the SNR can decrease too much and introduce a bias (13). At b-values below about 200 s/mm2 the signal attenuation is sensitive to signal loss from capillary perfusion (14,15) (Figure 1). This can be useful if adequately modelled in the postprocessing step, otherwise a bias towards too high ADC estimates should be expected. User-defined number of excitations of individual b-value images is often used to achieve homoscedasticity and sufficient precision.

Figure 1 Diagram showing how apparent diffusion coefficient (ADC) is related to the MRI signal at different b-values. Modified from Mahmood and Hansen, 2015 (15). In the low b-values region the signal from capillary blood flow contributes to the total signal. In the high b-value region the noise floor can constrain the recorded signal to stay higher than can be attributed to the underlying diffusion process. ADC should be measured from mid-range b-values.

ADC calculation

In the simplest interpretation of ADC, tissue with high cell density will have a low ADC (more hindered diffusion) whereas low cell density (e.g., due to necrosis or extracellular oedema) will have higher ADC (less hindered diffusion). This implies that DW-MRI quantifies predominantly diffusion taking place in the extracellular space (16,17). DW-MRI can also provide additional information about tissue microstructure, especially about cell count (18).

To calculate the ADC at least two b-values are required. In a clinical setting the ADC is almost exclusively calculated on the MRI workstation assuming a mono exponential model (free diffusion in a single compartment):

ADC=ln( S1/S2 )( b2b1 )

Here, S1 and S2 are the signal values in a single voxel or average signal value of a region of interest at two different b-values, b1 and b2, respectively (11). This shows that the ADC becomes the slope of the line connecting the two points [b1, ln(S1)] and [b2, ln(S2)]. If more b-values (or repetitions of the same b-values) are acquired a better estimate of ADC (the slope) can be achieved. Also, with more b-values (typically 5 or more) within the same b-value range (typically 0–1,000 s/mm2) it is possible to use a model that describes the signal better than the mono exponential model. The bi-exponential intravoxel incoherent motion (IVIM) model (19) is a popular alternative.

Voxel-by-voxel calculation of ADC better appreciates the heterogeneity of the tissue, for example by extracted histogram descriptors (e.g., minimum and maximum ADC). On the other hand, by averaging the signal within a given ROI before calculating the ADC is an approach less sensitive to bulk motion. The choice of analyses may depend on the quality of the DW-MRI scans available, and in general, it is not clear which of these two approaches should be used in clinical investigations.

Physiology of parotid glands

The parotid glands are the largest salivary glands located in the retromandibular fossa. They are purely serous glands containing an abundant amount of adipose tissue that occupies about a half of the gland parenchyma. The parotid glands are secretory organs, where various molecules are conveyed into the saliva-producing cells (acinar cells) via the capillary network, and the saliva is moving in the small ductal termination surrounded by acinar cells and is then secreted into the lumen of the excretory ductal system (20). These movements of molecules and water represent the main function of the parotid glands.

Human unstimulated salivary flow rates display circadian variation that is a cyclic event controlled by the body’s biological clock, with a peak level in the afternoon and a time span of 12 hours between highest and lowest secretory rates (21,22). The parotid gland mainly secretes saliva in stimulated conditions like chewing, when it secretes 50–60% of total whole mouth saliva (23,24). Within the gland, alterations in blood perfusion also occur in response to various stimuli. Therefore, such a process is altered in the diseased states of the parotid glands, for example, in sialoadenitis and Sjögren’s syndrome.

Irradiation and parotid glands

Parotid and other salivary glands are highly sensitive to ionizing radiation, which can lead to irreversible loss of gland function, xerostomia and reduced quality of life in patients after RT (25). Mechanisms of radiation-induced damage of salivary glands have previously been investigated, suggesting selective damage of plasma membrane of the secretory cells immediately after radiation exposure, followed by damage of DNA, death of acinar progenitor cells and finally lysis of acinar cells (26,27). Loss of acinar cells and glandular shrinkage occurs during the acute phase, 0–10 days after radiation exposure (28). Affected individuals display a 50–60% loss of salivary flow in this first week of RT (25,29). The chronic effects of radiation (more than 240 days after radiation exposure) may be the consequence of acute damage to salivary glands (30). Chronically, affected individuals continue to display significant decreases in salivary flow and are diagnosed with xerostomia for several months or years following RT (25,29,30). Patients receiving low dose (<25 Gy mean dose) to their salivary glands can experience recovery of salivary function within 12–24 months (25,30,31). A mean dose above 39 Gy to the parotid gland inflicts high risk of irreversible damage of parotid gland tissue and permanent xerostomia (32).

Regions of interest (ROI) in parotid glands

In the parotid glands, ROIs are usually manually drawn, as a reader-based circular ROIs or as an outline of as much of the gland parenchyma as possible, excluding the regions containing large vessels such as the retromandibular vein and external carotid artery. Each method has its intrinsic advantages and disadvantages. Reader-based circular ROI on selected slices may lead to inter-reader variability during ROI placement and may not reflect tissue heterogeneity. While whole-volume ROI overcomes the above-mentioned problem, it is a time-consuming process, which limits its application in routine clinical practice (9). Mahmood et al. 2015 (33) concluded in a study of brain metastases patients treated with whole brain irradiation that the effect of ROI strategy is significant for the ADC calculation. This indicates that ROI methods should be considered in studies where ADC is used.


The studies

The literature search was conducted in PubMed and Web of Science databases and resulted in 43 DW-MRI studies where ADC has been used for evaluation of parotid glands (Table 1). All studies were written in English and published from 2001 to 2019. They are sorted by their population size, from 4 to 149 study subjects. Additionally, Table 1 contains details regarding scanner manufacturer, acquisition method and ADC calculation. Study 13 (4) uses only b-values below 150 s/mm2 for calculation of ADC and may therefore be considered an outlier.

Table 1
Table 1 Included studies with the clinical condition of focus, population size, details about scanner manufacturer, acquisition method and ADC calculation
Full table

Factors affecting measurments of ADC

ADC of normal parotid parenchyma

The reported mean ADC values derived from 25 studies reporting ADC values of the normal parotid parenchyma are illustrated in Figure 2. The ADC values for parotid glands range from 0.28×10−3 to 2.42×10−3 mm2/s.

Figure 2 Mean apparent diffusion coefficient (ADC) of normal parotid parenchyma. Numbers indicate study id.

The effect of gustatory stimulation

Nine studies are using gustatory stimulation during DW-MRI examinations of the normal parotid parenchyma. Since the parotid glands produce only about one-thirds of the total saliva at rest and about two-thirds of the total saliva during gustatory stimulation, more valuable information regarding secretory function of parotid glands can be acquired by DW-MRI during gustatory stimulation (39,44). The nine studies using gustatory stimulation during DW-MRI examinations are listed in Table 2 together with the stimulating agent applied during the stimulation. The mean ADC values from those nine studies vary from 0.92×10−3 to 1.49×10−3 mm2/s (Figure 3).

Table 2
Table 2 Studies using gustatory stimulation under DW-MRI scans
Full table
Figure 3 Mean apparent diffusion coefficient (ADC) of normal parotid parenchyma under gustatory stimulation. Numbers indicate study id.

All the studies where parotid glands were scanned both at rest and under gustatory stimulation observed a significant increase in ADC values after stimulation (at rest, 1.08±1.14×10−3 mm2/s, stimulated, 1.22±1.19×10−3 mm2/s, matched pairs t-test (Excel 2019, ver. 16.0, Microsoft Corporation, Washington, USA), P=0.003 (Figure 4), but the pattern of response to gustatory stimulation and the stimulating agent used varied considerably. In the studies 5 and 8 a 500 mg tablet of ascorbic acid was used as the stimulating agent. The patients were advised to let the tablet dissolve in their mouths, not to chew on it. This resulted in an initial decrease and subsequent increase in the ADC values. On the other hand, studies 15, 30 and 39, having used lemon juice as a stimulant, and 11, 14, and 16, who performed the gustatory stimulation with six tablets and two instantly bitten tablets of 100 mg of ascorbic acid, reported an initial increase and subsequent fluctuation in the ADC values. This may be explained by the quicker saliva production as a response to more immediate stimulation such as lemon juice, higher number of tablets or instantly bitten tablets of ascorbic acid are likely to stimulate simultaneously more receptors than a single slowly dissolving tablet of ascorbic acid does.

Figure 4 Mean apparent diffusion coefficient (ADC) of parotid glands from nine studies using gustatory stimulation under DWI-MR examinations, first at rest and then under stimulation. T-test-Matched pairs t-test.

There are also differences in when and how frequent DW-MRI were acquired during gustatory stimulation (Table 2). Some of the studies (Study id: 15, 37, 39) performed only one DW-MRI scanning 30 seconds after stimulation, while the others repeated the sequence 7–10 times during stimulation (Study id: 5, 8, 11, 12, 14, 16). There seems to be no difference in mean ADC values between these two groups of studies (One DW-MRI scanning 30 seconds after stimulation, three studies, mean ADC =1.19±0.02×10−3 mm2/s; Repeated sequence 7–10 times during stimulation, six studies, mean ADC =1.29±0.27×10−3 mm2/s).

The effect of b-values

Figure 5 shows the distribution of b-values used for ADC measurement in the 43 studies included in this review.

Figure 5 Overview of the variation in b-values in all 43 included studies.

The most frequent individual choices are b=0 s/mm2 and b=1,000 s/mm2 (Figure 6), and the combination of these two which is present in 33% of the studies. The use of b=500 s/mm2 in combination with b=0 s/mm2 and b=1,000 s/mm2 is reported in 11 studies (24%). The overall most frequent range is b=0 s/mm2 to b=1,000 s/mm2 which is reported in 60% of the studies. Furthermore, only three studies exceed b=1,000 s/mm2 (Study id: 3, 18, 21), of which one extended to b=2,000 s/mm2 (Study id: 21). In the latter study a higher field strength (3 T) was used compared to the other two studies (1.5 T), which might explain the choice of the much higher b-value (diffusional kurtosis was also reported which also requires high b-values). Multiple b-values (b>3) are used in 11 studies, 5 of which acquire most of their b-values up till b=300 s/mm2. Six studies avoid the use of low b-values (Study id: 3, 5, 8, 29, 31, 35).

Figure 6 The distribution of reported b-values. The most popular individual choices of b-values: b=0 s/mm2 (35 studies), b=500 s/mm2 (16 studies), b=800 s/mm2 (12 studies), b=1,000 s/mm2 (32 studies).

The b-value profiles shown here (Figure 5) reflects that the typical radiology DWI-MRI protocol is acquired with two b-values only, a high b-value, typically 800 or 1,000 s/mm2, and 0 s/mm2 (i.e., without diffusion weighting).

In the high end of the b-value range (typically above 1,000 s/mm2 for most clinical systems), there is a risk that the measurement has very low SNR. For this reason, it is advised to assess the SNR at the highest b-value planned for the study with the intended coil setup. A generally valid way of increasing the SNR is by increasing the number of signals averaged. This however does not remove the bias from the measurement if the initial SNR is too low (13) and results in an underestimated ADC value if not properly dealt with in the post-processing step (71).

For the examination of the effect of choice of different b-values on ADC measurements of normal parotid parenchyma 25 studies are selected. Figure 7 shows how the choice of different b-values affect calculation of ADC. It is seen that if only low b-values are used (<300 s/mm2), like in study 13, it will lead to higher ADC values. This was in particular demonstrated in study 6, study of the influence on b-values on the ADC of the parotid gland. When lower b-values were included in a mono-exponential model higher ADC was obtained. This increase in ADC is related to the signal contribution of the so-called IVIM which stems from capillary perfusion (14). This means that if two exponentials are required to model data properly, and if the ADC is calculated from all acquired b-values using a mono exponential model, it will be overestimated (72). Studies 10 and 19 acquired DW-MRI with both lower and higher b-values but accounted for capillary perfusion with the IVIM formalism and arrived at lower ADC values. In the other hand, the use of high b-values in absence of b=0 s/mm2 will lead to low ADC values. This is also indicated in this overview where six studies avoided use of low b-values (Figure 7).

Figure 7 Reported mean apparent diffusion coefficient (ADC) values of the normal parotid parenchyma and the corresponding b-values configurations. Horizontal lines indicate that b-values belong to the same acquisition.

The effect of ROI definition method

From the examined literature, region of interest (ROI) selection methods can be divided into four groups: whole-gland ROI, ROI on the slice with largest parotid gland cross section, ROI selected on 3 contiguous slices, and reader-based circular ROI in selected slices (Figure 8).

Figure 8 Number of studies divided into the different delineation strategies.

Table 3 shows an overview of ROI selection methods in the 25 studies describing delineation of normal parotid parenchyma. There is no significant difference in mean ADC values between the four ROI selection methods (reader-based circular ROI in selected slices, mean ADC =1.08±0.60×10−3 mm2/s, whole-gland ROI, mean ADC =0.90±0.30×10−3 mm2/s, ROI on the slice with largest parotid gland cross section, mean ADC=0.93±0.18×10−3 mm2/s, ROI selected on 3 contiguous slices, mean ADC =1.06±0.26×10−3 mm2/s, The one-way analysis of variance (ANOVA) (Excel 2019, ver. 16.0, Microsoft Corporation, Washington, USA, P=0.75).

Table 3
Table 3 ROI definition methods from 25 studies describing delineation of normal parotid parenchyma
Full table

Study 20 performed ROC analysis based on whole-gland ROI, selected slice ROI on the largest slice and reader-based circular ROI. This analysis relived no significant difference in ADC values between the three ROI selection methods. On the other hand, the same study showed that the best inter- and intra-reader agreement during ROI placement, and the best diagnostic ability in detecting parotid gland abnormality was achieved using whole-gland ROI method. The study pointed out that whole-gland ROI method is significantly more time consuming which might be a distinct obstacle to its routine application in clinical practice. In contrast, it points out that the selected slice ROI approach significantly reduce the delineation time while showing comparable diagnostic performance and is recommended for routine clinical practice. Reader-based circular ROI was not recommended because of the relatively lower inter-reader agreement and diagnostic performance.

Study 38 performed ADC measurements with defined 12 concentric round ROIs (areas: 9, 28, 34, 50, 60, 82, 93, 98, 115, 130, 136, and 149 mm2). This study revealed that there were no significant differences in mean ADCs with the 12 ROIs for normal parotid parenchyma.

Irradiated normal parotid parenchyma

For the examination of the effect of irradiation on ADC measurements of normal parotid parenchyma 10 studies that report both mean dose to the parotid glands and mean ADC values are selected (Study id: 4, 5, 7, 10, 11, 13, 14, 16, 17, 21). Study 13, using only low b-values, which therefore more likely is a measure of so-called pseudo diffusion from perfusion and saliva flow, rather than true diffusion, was also excluded, leaving nine studies to be examined.

The effect of radiation dose

There is a significant difference between pre-RT ADC and post-RT ADC values based on the nine studies examined (pre-RT, mean ADC =0.92±0.21×10−3 mm2/s, post-RT, mean ADC =1.31±0.28×10−3 mm2/s, matched pairs t-test (Excel 2019, ver. 16.0, Microsoft Corporation, Washington, USA), P<0.001). The changes in mean ADC values were all positive, i.e., post RT ADC were higher than pre-RT ADC. A very early in-treatment transient reduction in ADC followed by a steady increase can be indicative of good response (73). This can be attributed to cell swelling (cytotoxic edema) followed by necrosis and lysis resulting in reduced cellularity (1,18).

There was a weak correlation between the change in ADC and the mean dose to the parotid glands (R2 =0.17) (Figure 9).

Figure 9 The change in apparent diffusion coefficient (ADC) from pre-RT to post-RT as a function of mean dose (28.4–53.9 Gy). R2-correlation coefficient. Numbers indicate study id.

The relationship between the mean dose to the salivary glands and changes in ADC in the unstimulated state has been investigated by studies 4, 7, 11, 21 and 24. Study 24 found no significant correlation between ADC changes and mean dose to the parotid glands. Meanwhile, study 4 found a slight correlation (r =0.33) between mean dose to the salivary glands and changes of ADC at 2 to3 months after end of the RT course. Study 11 was the first study to confirm a dose-response relationship in ADC changes in a longer term follow up. The increase in ADC was evident in irradiated salivary glands, and correlated with mean dose (at rest, r=0.61, P<0.001; under stimulation, r=0.48, P<0.01). Study 7 found that the parotid gland ADC was positively associated with the radiation dose (R2 =0.212, P=0.0001). Study 21 showed no correlation between ADC values and mean radiation dose.

The effect of post radiotherapy timing of DW-MRI

Post RT treatment timing vary from 7 days (Study id: 14) to 270 days (Study id: 5) in the nine included studies. This wide range in the timing of the DW-MRI can influence changes in mean ADC considerably, since the radiation induced damage of salivary gland is most pronounced in the acute phase (0–10 days) and early phase (10–60 days) after RT dye to loss of acinar cells and glandular shrinkage (28), and after that a partial restitution of parotid gland function can appear during the first two years after RT (74). Therefore, the largest changes in mean ADC values are expected within the first 60 days after end of the RT course (10). This is indeed seen in the reviewed data (Figure 10), as a slight negative correlation between changes in mean ADC pre-post values and time point of post treatment (R2 =0.39).

Figure 10 Apparent diffusion coefficient (ADC) change from pre-RT to post-RT plotted as function of post treatment time in days (7–270 days). R2-correlation coefficient. Numbers indicate study id.

Study 7 reported longitudinal evaluation of parotid glands after DWI-MR examinations 51.2±15.9 days (time point 1), 240.3±54.6 days (time point 2), and 489.3±99.2 days (time point 3) after RT. The ADC post-RT was highest at time point 1 and decreased through time point 2 and 3. At time point 3, although the ADC post was still higher than pre-RT ADC, the difference was not significant (P=0.153) while the post-RT ADC was significantly higher at time point 1 (P<0.005) and 2 (P<0.005) than pre-RT ADC, respectively. Similar results were obtained from study 14 where parotid ADC values showed an increase one week after RT (pre RT, mean ADC =1.26±0.10×10−3 mm2/s, one week after RT, mean ADC =1.75±0.16×10−3 mm2/s, P<0.001), followed by a decrease at one year after RT (one year post-RT, mean ADC= 1.57 ± 0.15×10−3 mm2/s, P<0.001).

Other factors influencing ADC

During the review process other potential ADC modulating factors were disclosed.

It is known that saliva flow rates display circadian variation (21,22), and thus ADC may show a similar rhythm. Only one study (Study id:16) performed all DW-MRI examinations around the same time of day. In this study patients were also asked not to eat or drink at least one hour prior to examination to secure that parotid glands were at rest at time of the examination. Examinations performed under the same physical conditions and at the same time of day are crucial for reproducibility of examinations (75).

The negative association between parotid ADC of healthy volunteers and age has been shown in previous studies (76). The age-related changes in the parotid glands is therefore another factor that can influence ADC measurements but has not been separately analyzed in any of the included studies.

Different diets and nutritional states by the time of examination, different seasons and temperatures, smokers vs. non-smokers, medications, certain medical conditions, and differences in race may also influence the saliva production and therefore changes in the ADC (77-80). Further, there is a high inter-individual variability of saliva production (up to 40–50%) in healthy volunteers (80,81). This suggests that ADC variability could be considerable due to this natural difference in parotid function. One way to mitigate this effect is by conducting longitudinal studies to assess the individual changes in ADC allowing for linear mixed effect analyses.


Conclusion

The review analyses revealed a discrepancy in the reported ADC values of the parotid gland based on 43 clinical studies. The analysis indicates that technical differences related to trial design, MRI acquisition and post-processing can be potential culprits but may not explain all of the variation in measured ADC values.

Lack of standardization of ADC measurement potentially restricts inter-study comparisons and hampers the effort towards validation of ADC as a biomarker in the parotid gland. Conclusions based on the reviewed studies and recommendations for the future studies are listed in Table 4.

Table 4
Table 4 Summary of conclusions and future recommendations
Full table

Acknowledgments

The authors wish to acknowledge Dr. Rasmus Hvass Hansen for his ideas on the outline of this review, and for providing writing and language editing assistance.

Funding: None.


Footnote

Conflicts of Interest: Both authors have completed the ICMJE uniform disclosure form (available at http://dx.doi.org/10.21037/qims-20-1178). The authors have no conflicts of interest to declare.

Ethical Statement: The authors are accountable for all aspects of the work in ensuring that questions related to the accuracy or integrity of any part of the work are appropriately investigated and resolved.

Open Access Statement: This is an Open Access article distributed in accordance with the Creative Commons Attribution-NonCommercial-NoDerivs 4.0 International License (CC BY-NC-ND 4.0), which permits the non-commercial replication and distribution of the article with the strict proviso that no changes or edits are made and the original work is properly cited (including links to both the formal publication through the relevant DOI and the license). See: https://creativecommons.org/licenses/by-nc-nd/4.0/.


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Cite this article as: Bruvo M, Mahmood F. Apparent diffusion coefficient measurement of the parotid gland parenchyma. Quant Imaging Med Surg 2021;11(8):3812-3829. doi: 10.21037/qims-20-1178