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Neural tube defects (NTDs) are severe birth defects of the central nervous system caused by failures in neural tube closure (NTC) during embryonic development1. The etiology of NTDs is complex. Studies have shown that NTC involves a sequence of morphogenetic processes, including convergent extension, bending of the neural plate (e.g., apical constriction), elevating the neural fold, and finally adhesion of the neural fold. These processes are regulated by multiple molecular and genetic mechanisms2,3, and any malfunction in these processes may result in NTDs4,5,6. As mounting evidence suggests that mechanical cues also play crucial roles during NTC3,7,8,9,10,11, and relationships have been found between genes and mechanical cues12,13,14, it becomes imperative to investigate the tissue biomechanics during neurulation.
Several techniques have been developed for measuring the mechanical properties of embryonic tissues, including laser ablation (LA)15, tissue dissection and relaxation (TDR)16,17, micropipette aspiration (MA)18, Atomic Force Microscopy (AFM)-based nanoindentation19, microindenters (MI) and microplates (MP)20, micro rheology (MR) with optical/magnetic tweezers21,22,23, and droplet-based sensors24. Existing methods can measure mechanical properties at spatial resolutions ranging from subcellular to tissue scales. However, most of these methods are invasive because they require contact with the sample (e.g., MA, AFM, MI, and MP), external material injection (e.g., MR and droplet-based sensors), or tissue dissection (e.g., LA and TDR). As a result, it is challenging for existing methods to monitor the mechanical evolution of neural plate tissue in situ25. Recently, reverberant optical coherence elastography has shown promise for non-contact mechanical mapping with high spatial resolution26.
Confocal Brillouin microscopy is an emerging optical modality that enables non-contact quantification of tissue biomechanics with subcellular resolution27,28,29,30. Brillouin microscopy is based on the principle of spontaneous Brillouin light scattering, which is the interaction between the incident laser light and the acoustic wave induced by thermal fluctuations within the material. Consequently, the scattered light experiences a frequency shift, known as the Brillouin shift ωR, following the equation31:
(1)
Here,
is the refractive index of the material, λ is the wavelength of the incident light, M' is the longitudinal modulus, ρ is the mass density, and θ is the angle between the incident light and the scattered light. For the same type of biological materials, the ratio of refractive index and density
is approximately constant28,32,33,34,35,36. Thus, the Brillouin shift can be directly used to estimate relative mechanical changes in physiological processes. The feasibility of Brillouin microscopy has been validated in various biological samples29,37,38. Recently, time-lapse mechanical imaging of a live chick embryo was demonstrated by combining a Brillouin microscope with an on-stage incubation system39. This protocol provides detailed descriptions of sample preparation, experiment implementation, and data post-processing and analysis. We hope this effort will facilitate the widespread adoption of non-contact Brillouin technology for studying biomechanical regulation in embryo development and birth defects.