A preliminary study of shaker-based optical coherence elastography for assessment of gingival elasticity
Introduction
Periodontitis, a chronic inflammatory disease occurring in the periodontal tissue, is considered as a major problem in the global burden of oral diseases due to its high frequency and non-ignorable impact on quality of life [1]. However, the pathogenesis of periodontitis is so complex that it has not been fully elucidated [2]. It has been acknowledged that during the occurrence and development of periodontitis, the primary pathological change is inflammation of gingival tissues (also termed as gingivitis) [3]. Therefore, early detection of gingivitis may provide accurate diagnosis of initial periodontal pathology. The gingiva is a collar of masticatory mucosa around the cervical portion of the teeth which serves as a major protective barrier between the environment of the mouth and the rest of the periodontium [4]. It is composed of two different stratified epithelia, and a densely collagenous lamina propria [5]. In the beginning of gingivitis, biomechanical properties of the gingiva may change with the hyperplasia or disappearance of collagen fibers before structural changes occur [5]. Therefore, knowledge of gingival elasticity is important for the early prevention and diagnosis of gingivitis and periodontitis. Additionally, the elastic information may be useful for a deeper understanding of the progression of periodontitis, which is of great significance for clinical treatment.
Several research groups have analyzed the gingiva through different methods [6], [7], [8], [9], [10], [11], [12], [13]. Chang SV et al. applied atomic force microscope to evaluate the structural and biomechanical properties of human free gingiva collagen fibrils, where the Young’s modulus was achieved by using mechanical stretching [6]. Goktas et al. carried out a study to explore biomechanical properties of the porcine attached gingiva and surrounding tissues by using tensile testing, dynamic compression, and stress relaxation analysis [13]. The resulting Young’s modulus indicated that the attached gingiva is significantly stiffer than regions of non-keratinized oral mucosa. Although the elastic modulus of the gingiva was obtained in both studies, drawbacks like the invasive nature and the requirement of thin sectioning limited their clinical application. Moreover, the localized quantification could not be realized by using the methods mentioned above, which is a key limitation to early diagnosis. Therefore, in order to achieve in vivo elasticity measurements of the gingiva, there is an urgent need for a noninvasive technology with localized sensitivities.
Elastography is an efficient way to evaluate biomechanical properties of biological tissues with features of noninvasive measurement and localized imaging, which includes an excitation mechanism and a detection system. The excitation unit is used to induce deformation, vibration, or vibration propagation, which are detected by an imaging unit [14]. In this area, ultrasound elastography and magnetic resonance elastography are the most widely used methods due to the advantages such as deep imaging [15], [16], [17], [18], [19]. However, the relatively low resolution limits their clinical application, particularly for detecting slight changes in tissue morphology and elasticity, which is important for early diagnosis [20].
Due to the limitations of the above-mentioned methods, alternative elastography techniques have been developed [21], [22], [23], [24], [25]. Among them, optical coherence elastography (OCE) is an emerging imaging modality for charactering tissue elasticity, which holds great potential for clinical application owing to its noninvasive nature, high resolution, high sensitivity, high acquisition speed, and real-time processing, which can be attributed to the advantages of optical coherence tomography (OCT) because OCE uses OCT to detect sample deformations [25]. Since the first introduction of the OCE technique in 1998, with the rapid development of system devices and detection algorithms, it has been widely applied in ophthalmology, cardiology and dermatology, and the related results have proved the significance of the biomechanical properties for disease diagnosis and treatment [26], [27], [28], [29], [30].
Based on the previous studies, the feasibility and reliability of the OCE technique for evaluating biomechanical properties of biological tissues have been confirmed. However, to date there is not much information available regarding the gingiva. In this paper, we performed a pilot study to quantitatively investigate gingival elasticity by using a shaker-based OCE system, where a shaker was used to mechanically induce the deformation in the gingiva because the shaker-based OCE can induce sufficient elastic wave propagation with high resolution and large field of view when compared with other excitation methods, such as acoustic radiation force [31], [32], [33], air puff [34], laser pulse [35], acoustic micro-tapping [36] and piezoelectric transducer [37], which is good for clinical translation [38]. Additionally, a spectral domain (SD) OCT system was used to track the mechanical deformations, on account of the higher resolution and better phase-stability when compared with the swept source OCT system [39].
To validate the feasibility of the proposed method, we first performed experiments on an agar phantom. The visualization of the elastic wave propagation enabled us to achieve the two dimensional (2D) and three dimensional (3D) elastic images and to quantify the elastic wave velocity and elastic modulus. Based on this, we applied our system to quantify biomechanical properties of an in vivo rabbit gingiva. As expected, the OCT structural images and elastic wave propagations were achieved, the corresponding shear modulus and Young’s modulus were also obtained, indicating that our system has the capability to evaluate gingival elasticity and may have the translational potential for clinical diagnosis.
Section snippets
System setup
The schematic diagram of the shaker-based OCE system is shown in Fig. 1, which includes the mechanical shaker excitation unit and the phase-resolved SD-OCT unit. In order to induce elastic wave in the gingiva, an arbitrary function generator (Tektronix AFG31102) was used to produce a modulated sinusoid wave signal which was then amplified by using a power amplifier (SPANAWAVE PAS-00023-25). Then the amplified signal drove the mechanical shaker (Bruel & Kjaer, mini-shaker type 4810; Duluth,
Phantom imaging
The phantom experiments were first carried out to verify the shaker excitation and OCT detection setups. Fig. 4(a) shows the 2D OCT image of the homogeneous phantom. According to the M-B mode protocol, the axial displacement can be mapped as a function of the propagation time. The 2D shear wave propagation imaged at five different time points are shown in Fig. 4(b)–4(f), in which different colors correspond to different vibration directions.
Based on the 2D Doppler OCT results, the 3D visual
Discussion
Medical studies indicated in recent years that the changes in biomechanical properties of the gingiva are closely related to the pathological process of gingivitis and periodontitis [42], thus providing a useful tool that enables us not only to early diagnose but also to better understand the progress of the disorders. Although several methods have been developed to evaluate biomechanical properties of the gingiva, such as mechanical stretching, tensile testing, dynamic compression, and stress
Conclusions
In this paper, we have developed a shaker-based OCE system for the detection of biomechanical properties of the gingiva. Quantitative elasticity measurements were first made on an agar phantom, and the reliable results verified the effectiveness of the proposed technique. Then experiments were carried out on an in vivo rabbit model, as a result, both of the structural and elastic images, as well as the corresponding elastic modulus were achieved. As the first in vivo elasticity imaging of the
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Funding
This work was supported by the National Key Research and Development Project, China [grant number 2018YFE0115700]; the National Natural Science Foundation, China [grant numbers 51863016, 51865040, 61865013, 41576033, 61177096]; Science and Technology Bureau of Nanchang City, China [grant number [2019] No.258]; and the Health Commission of Jiangxi Province, China [grant numbers 20184006, 2019B072].
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