Shulin Chen‡
ab,
Chen Ding‡b,
Yong Linb,
Xinzhou Wub,
Wei Yuan*b,
Xiuqing Meng*a,
Wenming Sub and
Ke-Qin Zhang*c
aZhejiang Provincial Key Laboratory of Solid State Optoelectronic Devices, Zhejiang Normal University, Jinhua 321004, China. E-mail: xqmeng@zjnu.cn
bPrintable Electronics Research Centre, Suzhou Institute of Nano-tech and Nano-bionics, Chinese Academy of Sciences, Suzhou 215123, China. E-mail: wyuan2014@sinano.ac.cn
cNational Engineering Laboratory for Modern Silk, College of Textile and Clothing Engineering, Soochow University, Suzhou 215123, China. E-mail: kqzhang@suda.edu.cn
First published on 8th June 2020
Here we demonstrate a novel SERS-active substrate assembled by silver nanowire (Ag NW)-embedded porous polystyrene (PS) fibers. Ag NWs are synthesized through a glycerol-mediated solvothermal method firstly, then electrospun into PS porous fibers. The as-synthesized Ag NWs are embedded in PS fiber and aligned orderly along the axial direction. Porous structure appears in PS fiber due to the phase separation induced by rapid evaporation of solvents. Large amounts of holes not only greatly improve the sample collection efficiency of the SERS-active substrate, but also significantly facilitate the adsorption of target molecules on the surface of Ag NWs, thus increasing the probability of enhancement of target molecules. In addition, compared with polyvinyl alcohol (PVA) and polyvinyl pyrrolidone (PVP), PS has better solvent resistance. The detection limit of 4-aminothiophenol (4-ATP) on our fabricated electrospun fiber mats is 10−7 M, and the electrospun fiber mats showed good reproducibility of SERS signal detection. This study proposes a feasible strategy for the large-scale preparation of flexible SERS-active substrate assembled by Ag NW-embedded porous PS fibers. The produced flexible SERS substrates may have potential application in wearable sensors for the trace detection of chemical and biological molecules.
Recently, more and more efforts have been employed to explore the flexible SERS-active substrates. Compared with the traditional rigid metal substrates, flexible SERS-active substrates can attach to the surface of human skin or irregularly shaped objects to realize the in situ and real-time measurement of analytes. Therefore, the flexible SERS-active substrate is regarded as a promising candidate for the next generation of wearable and portable sensing devices.14–17
Among the various flexible substrates, electrospun polymer nanofibers have been shown to be one of the most promising templates to pack noble metal nanostructures with great precision due to their advantages of high mechanical flexibility, large specific surface and good permeability.18 Table S1† summarizes the recently reported papers on flexible SERS substrates based on metallic nanomaterials and electrospun polymer fibers. Many polymers, such as polyvinyl alcohol (PVA),19 polyvinyl pyrrolidone (PVP),20 polyacrylic acid (PAA),21 poly(ε-caprolactone) (PCL),22 polyacrylonitrile (PAN)23 and poly(L-lactic acid) (PLLA),24 have been utilized to combine with different Au and Ag nanostructures to fabricate various flexible substrates for SERS.15,25,26 In general, there are two different composite modes for metal nanomaterials and electrospun fibers: one is embedding into the fiber by directly electrospinning the pre-mixed polymer solution, and the other is immobilization on the fiber surface by surface modification or in situ synthesis.23,24 It is obvious from Table S1† that the electrospun fiber substrates with metal nanoparticles immobilized onto the fiber surface have lower detection limit and higher enhancement factor than the electrospun substrates with metal nanoparticles embedded into the fibers. However, these exposed metal nanoparticles are vulnerable to water vapor oxidation and mechanical damage, which seriously weakens the enhancement effect for SERS substrates.22,27 For the embedded mode of metal nanoparticle or nanowires, it is true that the polymer outside the metal nanomaterials can protect them from contamination and surface oxidation, especially for Ag nanostructures, which gives the composite a long lifetime.17 However, the encapsulated polymer also prevents the target molecules from adsorbing on the surface of metal nanostructures quickly and accurately, which will seriously reduce the efficiency of sample collection. Therefore, in this work, we designed a new SERS substrate based on electrospun fibers, which not can only protect the metal nanomaterials from oxidation and mechanical damage, but also enable the target molecules to easily access the enhancement region and significantly improve the collection efficiency of target samples. Furthermore, PVA and PVP are popular polymer materials for electrospinning, and they are usually used as supporting materials for metal nanostructures for SERS (see in Table S1†). Nevertheless, these biocompatible polymers are water soluble, which greatly limits the applications of these metal/nanofiber composites as SERS-active substrates because these polymer host matrixes have weak resistance to some common and green solvents, such as ethanol or water.
Herein, we describe a novel SERS-active substrate assembled by Ag NW-embedded porous PS fibers. Highly SERS-active Ag NWs are synthesized firstly and then electrospun into PS porous fibers. During the process of electrospinning, as-synthesized Ag NWs are embedded in PS fiber and aligned along the axial direction; at the same time, an interconnected porous structure appears in the PS fiber due to the phase separation induced by rapid evaporation of solvents.28–30 The formation of pore structures not only greatly improves the sample collection efficiency of SERS-active substrate but also significantly facilitates the adsorption of target molecules on the surface of Ag NWs, thus increasing the enhancement probability of target molecules. In addition, compared with PVA and PVP, PS has better solvent resistance. This study proposes a feasible strategy for the large-scale preparation of flexible SERS-active substrate assembled by Ag NW-embedded porous PS fibers. The produced flexible SERS substrates may have potential application in wearable sensors for the trace detection of chemical and biological molecules.
Fig. 1 Schematic illustration of (a) Ag NWs/PS composite porous fiber preparation process and (b) target molecules permeating into the surface of Ag NWs from the holes for SERS testing. |
Ag NWs were synthesized with reference to the existing reports of Yu's group.31 As shown in Fig. 2a, it is a high-throughput method, and the synthesized Ag NWs–ethanol dispersion presents a uniform grey colour. A typical SEM image (Fig. 2b) shows the synthesized Ag NWs have a high aspect ratio, with 70–130 nm diameter and 10–20 μm length. The XRD pattern in Fig. 2c confirms that the synthesized Ag NWs are highly crystalline and exist purely in a face-centered cubic (FCC) structure.16,20 Furthermore, the UV-Vis absorption spectrum of the Ag NWs–ethanol dispersion (Fig. 2d) displays typical two surface plasmon resonance (SPR) peaks at 353 and 384 nm. The SPR peak at 384 nm corresponds to the transverse plasmon resonance of nanowires,36 and the weaker peak at 353 nm is attributable to the quadrupole resonance excitation of nanowires.37,38
Fig. 3a shows the prepared electrospun fiber mat with a large area of 10 × 10 cm2. The disordered fibers were stacked on the collector to form a nonwoven mat, whose thickness depends on the electrospinning time, as shown in Fig. S2.† Compared with the pure PS fiber mat, the Ag NWs/PS composite fiber mat is more fluffy with the same electrospinning time. The thickness of the composite fiber mat collected for 20 min is about 400 μm, which is enough for the subsequent SERS experiments. The obtained Ag NWs/PS composite fiber mat presents uniform yellowish-brown color, which is similar to the color of the electrospun solution (inset picture in Fig. 3a). The typical SEM image in Fig. 3b shows that the composite fibers have uniform shape and size. The diameter distribution (Fig. S3†), measured through the statistics of SEM images by ImageJ, confirms that the fibers have a uniform diameter of 2.06 ± 0.25 μm. The surface and cross-sectional morphology of the composite fiber were observed using SEM. As we expected, there are large amounts of holes on the surface and inside of the composite fiber (Fig. 3c). The inset shows direct evidence that Ag NWs are embedded into the porous PS fibers. Observing by SEM, there are few Ag NWs on the fiber surface, which means most of the Ag NWs are embedded inside the matrix. Through distorting and stretching the composite fibers, Ag NWs come out of the broken fibers, as shown in Fig. 3d. In addition, the UV-Vis absorption spectrum of the Ag NWs/PS composite fiber mat was measured as shown in Fig. S4,† which indicates an obvious SPR peak at 359 nm.
Fig. 4a shows a photograph of the electrospun fiber mats with different contents of Ag NWs. From left to right, the Ag NWs content are 10 mg, 25 mg, 35 mg and 50 mg, respectively. It is obvious that greater the content of Ag NWs, the deeper the color of the electrospun mat is. Furthermore, the electrospun Ag NWs/PS composite fiber was observed by TEM, as shown in Fig. 4b–e. From these images, we can clearly see that the Ag NWs are embedded in the PS matrix and arranged parallel to each other along the length of the fibers. When the Ag NW content is 10 mg (Ag NWs:PS:DMF = 10 mg:1.8 g:7.2 g), only one or two discontinuous nanowires are assembled within a single fiber (Fig. 4b). With increasing content of Ag NWs in the electrospun solution, more nanowires were embedded in PS fibers (Fig. S5†). By increasing the Ag NW content to 50 mg (Ag NWs:S:DMF = 50 mg:1.8 g:7.2 g), there are about eight nanowires assembled within one single fiber (Fig. 4e). It is true that the more Ag NWs in the fiber, the more “hot spots” it can provide for SERS effect.20 However, if the amount of Ag NWs is further increased, the viscosity of the electrospun solution will be too high to spin fibers.
The solvent resistance of the host matrix for metal nanostructures is very important for practical SERS application. The existing literature reports that PVA and PVP are popular polymer materials for electrospinning, and they are usually used as supporting materials for metal nanostructures. However, these polymers have weak resistance to some common and green solvents, such as ethanol or water. As shown in Fig. 5, once immersed into ethanol and water, PVP-based fiber mats dissolve instantly, while PS-based fiber mats can stably exist in ethanol and water. Obviously, the poor solvent resistance of the polymer matrix will greatly limit the application scenarios of these composite fibers for SERS. However, because of the chemically hydrophobic nature of PS polymer,28,30 the water contact angle of the composite fiber mat is larger than 120°, as shown in Fig. S6,† which means that the obtained Ag NWs/PS fiber mat is not suitable for the collection and detection of molecules in aqueous solution, but it can still detect probe molecules in alcohol solution.
Fig. 5 Photographs of (a) 10 mg-Ag NWs/PVP and (b) 50 mg-AgNWs/PS electrospun fiber mats before and after immersion in ethanol or water. All scale bars are 1 cm. |
In order to understand the sample collection process of the Ag NWs/PS porous composite fiber, we conducted a penetration experiment with fluorescent solution (0.1 mol FITC in 10 ml ethanol). The detailed experimental process is briefly described as follows: firstly, a single porous fiber and a single solid fiber were respectively fixed on a glass substrate. Secondly, the FITC solution was dropped on one end of the porous fiber and the solid fiber, respectively, as shown in the inset of Fig. 6. Thirdly, the optical (Fig. 6a and c) and fluorescent (Fig. 6b and d) images were captured by laser confocal microscope. It should be noted that all the images were taken immediately after dropping the FITC solution on the end of the fibers. Obviously, the fluorescence solution permeated into the holes of the composite fiber quickly and was transported along the fiber's longitudinal direction (Fig. 6b), which confirms that target molecules can easily access the surface of Ag NWs. For comparison, the Ag NWs/PS solid composite fibers (Fig. S7†) were also fabricated by electrospinning of Ag NWs/PS/THF mixed solution (10 mg Ag NWs, 1.8 g PS, 7.2 g THF). As expected, the FITC/ethanol solution did not permeate the solid fiber at all (Fig. 6d). In addition to the fibers, the Ag NWs/PS porous and solid composite films were also prepared by spin-coating, shown in Fig. S8.† As expected, the fluorescent solution is unable to permeate the solid film, while the porous film showed a similar solution permeation phenomenon as porous fibers. These results reveal that porous structure greatly improves the sample collection efficiency of the SERS-active substrate and facilitates the adsorption of target molecules on the surface of Ag NWs.
The prepared Ag NWs/PS porous fibers can be used as SERS substrates. Herein, we used 4-ATP as the probe molecule for the SERS measurement to study the enhancement effects of the Ag NWs/PS porous fiber mats because 4-ATP has distinct Raman features. Another very important reason for choosing 4-ATP as probe molecule is that it can be used as a Raman active molecule by attaching onto Ag NWs, and this structure is then used to capture and detect the target biomolecules through their specific binding sites,39,40 which means we can anchor the 4-ATP molecule onto our prepared SERS substrates as a linker to capture and detect some biomolecules in our follow-up study.41 To prepare the SERS substrates, large-sized electrospun fiber mats were cut into strips (1.0 × 0.5 cm2) firstly, and then these strips were immersed into 4-ATP/methanol solutions with different concentrations for only 10 seconds. Finally, these infiltrated strips were taken out quickly and dried in a culture dish naturally at ambient temperature prior to the measurement. When the substrate was immersed into the 4-ATP/ethanol solution, the probe molecule can permeate the fiber quickly and access the surface of Ag NWs efficiently because of the large amount of holes. Fig. 7a shows a set of SERS spectra for 0.1 M 4-ATP adsorbed on the Ag NWs/PS porous fibers with different Ag NW contents. It is obvious that the higher the content of Ag NWs in the PS fiber, the higher the intensity of the Raman signal. When more Ag NWs are embedded in the fiber, the spacing between adjacent nanowires is smaller, which can generate more electromagnetic fields for adsorbed 4-ATP molecules and result in the Raman signal enhancement.20,35 Six characteristic 4-ATP peaks can be seen at 1077, 1147, 1175, 1396, 1446, and 1573 cm−1 when the Ag NW content was 50 mg. Three intense vibrational bands are found around the wavenumbers of 1077, 1175, and 1573 cm−1, which arise from the C–S stretching, C–H bending and C–C stretching modes of 4-ATP, respectively.42–45 The bands at 1396 and 1446 cm−1 are assigned to the NN stretching vibrations of 4,4′-dimercaptoazo-benzene (DMAB), which are generated from the interactions between two adjacent 4-ATP molecules.39 When the content of Ag NWs is lower than 50 mg, only the 1077 and 1573 cm−1 vibration peaks are identical and become weaker and weaker. Therefore, the electrospun mats obtained from 50 mg-Ag NWs/PS/DMF solution were used as SERS substrate in subsequent experiments.
Fig. 7b shows the SERS spectra of different 4-ATP concentrations (1.0 M, 10−2 M, 10−4 M, 10−6 M and 10−7 M) adsorbed on the 50 mg-Ag NWs/PS porous fibers. As the concentration of probe molecule becomes lower and lower, the number of detected peaks becomes less and less, and the peak values are weaker and weaker. However, the wavenumbers of 1077 and 1573 cm−1 still could be detected clearly, but the width of these bands became wider. We suppose this unusual phenomenon is caused by the fluorescence enhancement effect, implying a non-distinct Raman property.46 Herein, the electrospun SERS substrate was able to detect 4-ATP at a low concentration of 10−7 M. The reproducibility of Raman signals for the Ag NWs/PS substrate was evaluated by collecting the SERS spectra of 4-ATP molecules from 5 randomly selected positions on the same strip. As shown in Fig. 7c, the number of peaks and their wavenumbers were almost the same, which demonstrated good reproducibility of the SERS signals. Relative standard deviation (RSD) is always used to evaluate the quality of reproducibility. The RSD indicating reproducibility of signal intensity has been calculated and is shown in the inset of Fig. 7c. The SERS peaks basically locate at 1047 and 1573 cm−1, and their intensity RSD are 10.8% and 8.7%, respectively.
Fig. 7d shows the Raman spectra of 10−4 M 4-ATP adsorbed on the 50 mg-Ag NWs/PS porous fibers and pure PS porous fibers without Ag NWs. It is obvious that the signal intensity of Raman spectrum is greatly enhanced by the addition of Ag NWs. The enhancement factor (EF) was calculated by using the following equation:47 EF = (ISERS/Inon-SERS) × (Cnon-SERS/CSERS), where ISERS and Inon-SERS are the intensities of the SERS and the non-SERS signal of the peak in consideration, respectively, and CSERS and Cnon-SERS are the concentrations of the target molecule on the SERS and non-SERS surfaces, respectively. The EF was ∼105 for the case of 4-APT when calculated using the peak at 1573 cm−1.
In order to highlight the advantage of the prepared Ag NWs/PS porous fibers in terms of sample collection efficiency, the SERS spectra of 10−4 M 4-ATP adsorbed on different substrates (including electrospun porous/solid fibers and casted porous/solid films) with same collection time were measured as shown in Fig. 8. For comparability, the content of Ag NWs in all substrates is the same at 50 mg, and the concentration of 4-ATP is 10−4 M. All the substrates were cut into small strips of the same area, and then immersed into 4-ATP solution for the same amount of time (only 10 seconds). Finally, these infiltrated strips were taken out and dried at room temperature for SERS measurements. As expected, 4-ATP molecules adsorbed on the porous fibers show the strongest Raman signal (Fig. 8a), and the intensity of the peak at 1573 cm−1 was up to 1.3 × 104. This is mainly because the large number of pores can adsorb more 4-ATP solution in a unit of time, which leads to more 4-ATP molecules adsorbed on the surface of Ag NWs. For comparison, 4-ATP molecules adsorbed in the solid fibers show very weak Raman signal, as shown in curve 4 of Fig. 8a, and the intensity of the peak at 1573 cm−1 was only 286. There are two main reasons for the weak Raman signal of 4-ATP adsorbed in solid fibers. On the one hand, the adsorption capacity of solid fibers for 4-ATP solution is small, resulting in less 4-ATP molecules adsorbed on its surface; on the other hand, Ag NWs were embedded into PS fibers, and the encapsulated polymer can prevent the 4-ATP molecule access to the surface of Ag NWs. There are similar phenomena in the casted films, and the SERS spectra of 4-ATP molecules adsorbed on porous film (Fig. S9a†) and solid film (Fig. S9b†) are shown in curves 2 and 3 in Fig. 8a, with the intensity of the peak at 1573 cm−1 being 3272 and 627, respectively. The large amount of holes in the fibers greatly improve the sample collection efficiency of the SERS-active substrate and facilitate the adsorption of analyte on the surface of Ag NWs.
Fig. 8 (a) SERS spectra of 10−4 M 4-ATP collected on different substrates; (b) peak intensity of 1573 cm−1 in different SERS spectra in (a). |
Footnotes |
† Electronic supplementary information (ESI) available: Photograph of the synthesized Ag NWs in flask; diameter distribution of electrospun Ag NWs/PS composite fibers; number of Ag NWs in electrospun fiber as faction of Ag NWs content in electrospun solutions; surface and cross-section SEM images of Ag NWs/PS solid composite fiber; transport of FITC/ethanol solution in Ag NWs/PS porous and solid composite films. See DOI: 10.1039/d0ra01454k |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2020 |