Figure 2a illustrates the working principle of the proposed NFPSU. When skin deformations relating to finger movements occur, the pressure applied to the bottom of the attached soft liquid sac changes. According to Pascal’s principle, the pressure applied to any point within an incompressible liquid can be transmitted to every point of the liquid in real time.
[35] Therefore, the pressure applied to the bottom of the soft-liquid-sac base is transmitted to the top surface, causing the contact filmy optical-nanofiber sensor to deform. In this way, the external mechanical signals related to finger movements captured at any point of the soft liquid sac base are transmitted to the optical-nanofiber sensor with high fidelity, eliminating the impact of position drift on the sensing signals. As shown in
Figure 2b, when the optical nanofiber is slightly bent under pressure, the well-confined symmetric mode of an 800-nm-diameter nanofiber at the input port evolves into an asymmetric profile with clear optical leakage, making it highly sensitive to mechanical stimuli.
The model between the nanofiber deformation and optical intensity is provided in Supporting Information. As shown in Figure S1, the bending radius decreases with the increase of the applied normal force.
On the other hand, when an 800-nm-diameter nanofiber is embedded in PDMS, it will be not sensitive to the change of temperature based on our previous studies.[36,37] In this study, the optical nanofiber was fabricated by heating and stretching a standard silica single-mode fiber (SMF).[38] The as-fabricated optical nanofiber showed excellent flexibility, significantly exceeding the performance of standard silica or polymer optical fibers. For example, the bending radius could be made less than 10 µm, as shown in Figure 2c. Owing to its smooth surface and geometric uniformity (Figure 2c), the as-fabricated fiber offered a transmission greater than 99%[38] and a tensile strength higher than that of spider silk.[39]
Figure 2d shows a U-shaped nanofiber guiding 633-nm-wavelength laser light. The bright red light along the fiber indicates the presence of an evanescent field outside the optical nanofiber. Generally, with the decrease of the fiber diameter, the fractional power of the light outside the optical fiber increases exponentially and a stronger evanescent field results in a higher sensitivity. However, a thinner optical nanofiber loses mechanical stability when it is manipulated to form a U shape structure. In this work, an 800-nm-diameter optical nanofiber was chosen for the trade-off between high sensitivity and mechanical stability. For high compactness, the curved end of the U-shaped optical-nanofiber sensor was intentionally positioned slightly over the edge of the liquid sac to ensure that deformation would occur in the sensitive area of the nanofiber.
To investigate the sensor’s pressure response, we used a mechanical testing system (Figure S2). Figure 2e shows the wavelength-dependent transmittance response to applied static pressure in the range 0-31.8 kPa. With increasing wavelength, the transmittance of the nanofiber decreases and the sensitivity increases as a result of the increasing fractional power of the evanescent field.[19] By defining the sensitivity as S=ΔT/ΔP, where ΔT is the change of transmittance and ΔP is the change of pressure, the sensor shows a lower sensitivity of -0.01 kPa-1 when the applied pressure is less than 6.4 kPa. In the high-pressure range (6.4-31.8 kPa), the sensor achieves a higher sensitivity of -0.03 kPa-1 (inset of Fig. 2e).