3.1. Characterization of FHS
In this work, we prepared MXene by etching with HF as shown in
Figure 1, and the SEM images of MAX phase and MXene are illustrated in
Figure 4 (a) and (b). It is seen that MAX phase comprises uneven and tightly packed blocks. In comparison, the MXene is composed of accordion-like multilayers with layer thickness in the range of nanoscale, which is expected to show high specific surface area and provide more active sites for the adsorption of water molecules.
Figure 4 (c-g) present the morphology of FHS with different concentration of MXene. SA alone exhibits smooth surface, while MXene debris are clearly observed on the surface of the composite of SA/MXene. With the increment of the concentration of MXene, the composite exhibits rougher surface with higher density of MXene debris. Furthermore, the composite film shows little change in the morphology after crosslinking of SA with CaCl
2 as evidenced by comparison of
Figure 4 (f) with (g).
Figure 4 (h) and (i) present the SEM images of IDEs constructed on PI film. The boundary of the area treated with LDW and without LDW treatment is clear, indicating high resolution of the patterned structure induced by LDW treatment. At high magnification, IDEs reveal rugged and porous surface, which is attributed to the conversion of PI to the conductive graphene by laser treatment and is in agreement with literature reports [
21].
The chemical structure of the samples has been examined by the analysis of FT-IR spectroscopy. In the FT-IR spectrum of MXene (
Figure 5 (a)), the absorption peaks at 3435 cm
−1 and 1625 cm
−1 are ascribed to hydrogen-bonded -OH or water molecules coordinated on the surface of MXene. Furthermore, the characteristic peak at 1257 cm
−1 is attributed to the stretching vibration of C-F [
22]. The FT-IR characterization indicates the existence of functional groups like -OH and -F attached to the surface of MXene.
Figure 5 (b) shows the ATR-FTIR spectra of SA, SA/MXene1 and c-SA/MXene1-30. In the spectrum of SA, the absorption peak at 1031 cm-1 represents the symmetric stretching vibration of C-O on C-O-C [
23]. The characteristic peak 1413 cm
-1 is attributed to symmetric stretching of –COO– on the polymer chain [
24]. In the spectrum of MXene, the peak at 1257 cm
-1 is ascribed to C-F in MXene [
22]. Both characteristic peaks of MXene and SA are clearly identified in the spectrum of SA/MXene1. In comparison, in the spectrum of c-SA/MXene1-30, the absorption peak corresponding to symmetric stretching of –COO– on SA is shifted from 1413 cm
-1 to 1417 cm
-1, which is attributed to the crosslinked structure between CaCl
2 and SA [
24]. The above results indicate the successful preparation of SA/MXene and c-SA/MXene.
The ATR-FTIR spectra of PI and PI-A are shown in
Figure 5 (c). Compared with PI, in the ATR-FTIR spectrum of PI-A, new absorption peaks appear at 1556 cm
-1 and 1650 cm
-1, which are assigned to the N-H bending vibration peaks and C=O stretching vibration peaks, respectively. The observation of such new functional groups proves the hydrolysis of imide group of PI by the treatment with NaOH [
25].
Figure 5 (d) shows the Raman spectrum of the IDEs formed by laser treatment in the PI substrate. Three prominent peaks in the spectrum are identified at 1350 cm
-1, 1580 cm
-1 and 2680 cm
-1, corresponding to the D band, G band and 2D band of graphene, respectively [
26] .The D band is related to the conversion of sp
2 hybridized carbon to sp
3 hybridized carbon, while the G band is related to the vibration of sp
2 hybridized carbon [
27]. Obviously, the Raman characterization reveals that the LDW-induced IDEs are composed of conductive graphene.
3.2. Humidity Sensing Properties of FHS
Figure 6 (a) presents the humidity sensing curves of SA/MXene FHS with different concentration of MXene. The impedance of the FHS based on SA varies from ~10
6 Ω to 10
7 Ω within the range of 90% RH to 10% RH, showing relatively low sensitivity and high impedance even under humid environment. It is well-known that SA is a kind of natural polyelectrolyte with a large number of hydrophilic functional groups. With the increase of RH, more water molecules are absorbed in SA film, which are decomposed to produce protons and also promote the dissociation of Na
+ in SA to improve ion conductivity, leading to the decrement of impedance. However, the sensitivity of SA is limited, which can be further improved by compositing with nanomaterials with large specific area and high conductivity. Herein, MXene was introduced into the sensitive film, and the resulting sensing curves are shown in
Figure 6 (a). The FHS based on the composite of SA/MXene exhibited much lower impedance than that bases on SA alone at every RH investigated. which is attributed to excellent conductivity of MXene. Moreover, the composite sensor revealed much higher sensitivity than the sensor of SA. As a typical 2D nanomaterial, MXene possesses large specific area and abundant hydrophilic groups (such as -OH), which could provide sufficient active sites for the adsorption of water molecules and therefore improve the sensitivity of composite film. Specifically, when the concentration of MXene in the composite solution reaches 2 mg/mL, the impedance of corresponding sensor decreased dramatically over the whole tested humidity range. It is proposed that conducting path was well established in the composite film at such a high concentration of highly conductive MXene, leading to greatly improved conductivity of the composite sensor. Therefore, the variation of adsorbed water molecules with the change of RH did not result in much change in the conductivity, and the sensor demonstrated lower sensitivity. In the work, 1 mg/mL of MXene is selected as the optimal formula for the fabrication of the composite FHS.
Figure 6 (b) shows the influence of crosslinking time on the humidity sensing properties of c-SA/MXene FHS. The FHS of SA/MXene exhibited quite large hysteresis of ~12.5% RH. In comparison, the FHS based on c-SA/MXene obtained by immersion in CaCl
2 solution showed much decreased hysteresis. Specifically, extending the immersion time of FHS in CaCl
2 solution leads to smaller hysteresis and higher sensitivity. It has been reported that SA could react with Ca
2+ to form a stable intermolecular cross-linking network structure [
28]. Apparently, such crosslinked structure is helpful to hinder the accumulation of water molecules and avoid the formation of water layer in the sensing film, resulting in smaller hysteresis of the FHS. When the cross-linking time reaches 60 min, the sensor exhibited relatively small hysteresis of ~5.0% RH. Further increasing the immersion time could lead to even smaller hysteresis, but the sensitivity of the FHS is decreased, too. Immersion time of 30 min is thus chosen as optimal formula by considering the sensitivity and hysteresis. The c-SA/MXene1-30 FHS exhibited impedance change of two orders of magnitude and good sensing linearity (R
2 = 0.992,
Figure 6 (d)) on a semi-logarithmic scale over a wide range of 11-98%RH. Moreover, it revealed fast response/recover time (4 s/11 s,
Figure 6 (f)), which might be ascribed to the high specific surface area of MXene and accelerated desorption of water molecules due to the formation of crosslinked structure.
Additionally, humidity sensing curve of the FHS based on c-SA/MXene1-30 with PI without hydrophilic treatment as the substrate is presented in
Figure 6 (e) to explore the effect of surface modification on the humidity response of the FHS. The sensor with unmodified hydrophobic PI as the substrate showed very high impedance of over 10
7 Ohm in the whole tested humidity range (10-90% RH) with slight variation in the impedance. It is proposed that the incompatibility between hydrophobic substrate and hydrophilic sensitive materials hindered the deposition of the sensitive film on the flexible substrate, leading to poor sensitivity of resulting FHS. Apparently, the results revealed the importance of NaOH treatment of PI film for the fabrication of high performance composite FHS.
As discussed before, the stability under humid environment is crucial for the practical applications of FHS. Herein, c-SA/MXene1-30 FHS was placed in 98% RH for over 9 h and the real-time impedance response is illustrated in
Figure 7 (a). Clearly, the FHS did not show any degradation in sensing performance during the storage in the highly humid environment. Furthermore, the FHS was placed in a bottle containing water at 40
oC for 24 h, and its humidity responses before and after the exposure to the humid environment changed little as shown in
Figure 7 (b). The results clearly demonstrated that the FHS exhibited good durability towards humid environment, which might relate to the formation of crosslinking structure of SA in the composite film. Additionally, the responses of c-SA/MXene1-30 FHS to organic gases (methanol, ethanol, ether, acetone and n-hexane) are presented in
Figure 7 (c). The FHS exhibited quite small response towards all the tested organic gases, demonstrating excellent selectivity of c-SA/MXene1-30 FHS.
Figure 7 (d) displays the real-time responses of c-SA/MXene1-30 FHS during quick switching between high and low humidity environment for 120 cycles at an internal of 30 s. Clearly, the early, middle and late stages of the sensing curves show almost the same impedance values at high and low humidity levels and unchanged shapes, suggesting good sensing repeatability and stability of FHS.
Nyquist plots of c-SA/MXene1-30 FHS under various humidity environment were measured to explore the humidity sensing mechanism. As shown in
Figure 8 (a), when the humidity is below 33% RH, the Nyquist plot of the sensor is composed of a semicircle. In comparison, the Nyquist plots are composed of a semicircle at high frequency and a straight line at low frequency under 59-98% RH. The semicircle represents the membrane impedance of the sensor, while the straight line is ascribed to Warburg impedance of the diffusion process [
29]. Under low humidity level, limited water molecules are adsorbed on the humidity sensing film, resulting in poor ion conductivity. Therefore, the Nyquist plots are composed of a semicircle with large radius. With the increase of humidity, more and more water molecules are adsorbed on the humidity sensing film, which are decomposed and also promote the dissociation of ion in the sensing film to result in high ion conductivity and thus much smaller semicircle radius. At high humidity level, a large number of adsorbed water molecules form a continuous water layer on the surface of the sensing film (
Figure 8b), significantly enhancing ion conduction and playing a dominant role in the overall conductivity of the sensor.
3.3. Applications of FHS
The exhaled air of human is highly humid, and could change the humidity in surrounding microenvironment [
30]. Therefore, the detection of breath-induced humidity change could be utilized to reflect the respiration status for non-invasive and non-contact early diagnosis [
31,
32]. Herein, the c-SA/MXene1-30 FHS was assembled in a mask and worn by a volunteer to verify its potentials for respiratory monitoring. The real-time responses of the FHS towards the respiration of the volunteer at different breathing modes are shown in
Figure 9 (a-c). It is seen that the response curves exhibit distinct amplitude and frequency towards three different breathing modes. Apparently, the response curves exhibited the largest amplitude and the lowest frequency towards the slow breathing mode, while the sensing curves with the smallest amplitude and the highest frequency indicated fast breathing mode. It is proposed that during the breathing process, exhaled gas carries a large amount of water molecules, which increases the humidity of the air around mouth and leads to the decrease of the impedance of the sensor. By contrast, the water vapor content is lowered during inhalation and the humidity around mouth decreases, resulting in higher impedance for the sensor. In slow breathing rate, the FHS could adsorb/desorb water molecules more efficiently and thus exhibit larger impedance change and greater amplitude in the sensing curve. Obviously, our FHS with fast response could well differentiate the respiratory patterns, revealing potentials in non-contact respiratory motoring.
Similarly, the exhaled airflow during speaking leads to the vibration of the vocal cords to produce sound, which is then modulated into different syllables through the mouth and nose to form specific words. Apparently, the process of speaking is accompanied by humidity change of air around the mouth. Therefore, the detection of the humidity change in the microenvironment could be utilized to distinguish different syllables. In this work, a volunteer said different words (monosyllabic (pen), disyllabic (pencil), and trisyllabic (tomato)) and the real-time response of the c-SA/MXene1-30 FHS assembled around the mouth of the speaker was recorded (
Figure 9 (d)). It is clear that the FHS exhibited characteristic and repeatable sensing curves towards various syllables, indicating the potentials of speech recognition by c-SA/MXene1-30 FHS.
There have been a number of reports on the application of humidity sensors in non-contact HMI [
33,
34,
35]. Herein, the real-time impedance response of c-SA/MXene1-30 FHS was recorded as the fingertip of a volunteer approached the sensor at different distances of 1 mm, 3 mm, and 8 mm, and the results are displayed in
Figure 9 (e). It is found that FHS exhibited sensitive, reversible and repeatable responses towards the change of the distance between the sensor and fingertip, proving its capability of detecting the delicate movement of fingertip in a non-contact way. Obviously, the results indicate that the c-SA/MXene1-30 FHS shows potentials for non-contact HMI, which can be used for reducing the risk of virus transmission such as COVID-19 during large-scale infectious disease outbreaks.