石墨烯复合超材料多维超灵敏谷氨酸传感器

Graphene-composite metamaterials-based multi-dimensional ultra-sensitive glutamic acid sensor

  • 摘要: 提出一种石墨烯-金属超材料复合太赫兹传感器,充分利用石墨烯能带Dirac点附近费米能级对样品的灵敏响应结合超材料表面强局域电场实现了对谷氨酸溶液浓度的多维超灵敏传感。实验结果表明,传感器在频率f =0.58 THz处存在一个明显的透射峰,且该透射峰幅值随谷氨酸溶液浓度的增加先升高后降低。若以透射峰幅值作为传感指标,器件能够探测到的最低浓度在10−1 fg/mL量级。另外,从传感器的透射波相位差-频率关系曲线中提取的斜率与浓度具有类线性关联,这意味着相位差信息也可以作为有效的传感指标。结合透射幅值和相位差两个传感指标,器件可以实现对谷氨酸溶液浓度的超灵敏精确检测。文中提出的器件为发展基于太赫兹超材料的超灵敏氨基酸传感器提供了帮助。

     

    Abstract:
      Objective  The pursuit of ultra-sensitive amino acid sensors is of great significance for biomedicine and chemical industry. Due to their low energy, high permeability, and fingerprint, terahertz (THz, 1 THz = 1012 Hz) waves are excellent candidates for the nondestructive detection of biochemical substances or molecules. For metamaterials, the strong local electric field generated by surface plasmon polariton is conducive to reflect the subtle changes of the surrounding environment into the THz signal spectrum, which provides an excellent platform for the development of ultra-sensitive, nondestructive, and unlabeled amino acid sensors. Up to now, however, few researches have been reported on amino acid sensors based on THz metamaterial. Therefore, the development of ultra-sensitive sensors that can detect amino acid solutions with low concentrations is an important subject in the realm of THz functional devices.
      Methods  Taking full advantage of the sensitive response of the Fermi level (EF) around the Dirac point in the graphene energy band to the sample in conjugation with the electric field strongly confined on the surface of the metamaterial, a terahertz sensor composed of graphene and metal metamaterial is proposed to realize the multi-dimensional ultra-sensitive sensing for glutamic acid. The designed sensor (denoted Dev.1) consists of a SiO2 substrate, polyimide (PI), metal arrays, and single-layer graphene. The detailed structure parameters of each metal pattern are as follows: L1=180 μm, L2=150 μm, a=20 μm, b=5 μm, c=14 μm, d=5 μm, e=18.5 μm, f=30 μm (Fig.1). The thickness of the unit cell, PI, and the substrate are 0.2 μm, 8 μm, and 300 μm, respectively. THz transmission spectra of the sensors are measured by THz-time domain spectrometer, and glutamic acid solutions with seven different concentrations are prepared: C0=0 fg/mL, C1=1.25 \times 10−1 fg/mL, C2=2.50 \times 10−1 fg/mL, C3=1.08 \times 101 fg/mL, C4=4.32 \times 102 fg/mL, C5=3.63 \times 105 fg/mL, C6=1.03 \times 1012 fg/mL. The simulation part is implemented by the time domain solver.
      Results and Discussions   For Dev.1, there is a significant resonant peak at f = 0.58 THz in the transmission spectra, which is attributed to the coupling between two groups of electrical dipole resonance modes (Fig.2(b)-(c), Fig.3). More importantly, the peak amplitude first increases and then decreases with the rising solution concentration. It means that taking \Delta T ( \Delta T=T_C_i-T_C_0 , where T_C_i ( T_C_0 ) is transmittance for the sensor covered by Ci (C0) glutamic acid solution) as the sensing indicator, the proposed sensor can detect the minimum value in the order of 10−1 fg/mL. Such ultrasensitivity can be rationalized by the ultra-sensitive response of EF around Dirac point to the surrounding environment (Fig.4) in conjugation with the confined field induced by electrical dipole induced. In addition, one can find that the slope extracted from ΔP(f) ( ΔP(f)=P_C_i(f)-P_C_0(f) , where P_C_i(f) ( P_C_0(f) ) is the phase of transmitted THz for the sensor covered by Ci (C0) glutamic acid solution vs frequency also exhibits quasi-linear dependence on Ci, and holds monotonically increasing within the range C0-C5 (Fig.5). It demonstrates that the slope related to phase difference can be cross-verified with ∆T to realize multi-dimensional and ultra-sensitive detection of glutamic acid solution with the concentration of C0-C5.
      Conclusions  A multi-dimensional ultra-sensitive THz sensor composed of graphene and metal metamaterials is proposed for the detection of glutamic acid concentration. The experimental results show that there is a transmission peak at 0.58 THz in the THz transmission spectra, which originates from the coupling between two modes of electrical dipoles. With the increase of glutamic acid concentration, the transmission peak amplitude increases first and then decreases. Taking the peak amplitude as the sensing indicator, the limit of detection for the sensor can be as low as the order of 10−1 fg/mL. The strong confined electric field on the surface of the metamaterial together with the sensitive response of the EF in the graphene energy band to different solution concentrations causes significant changes in the electromagnetic properties of the device and the corresponding transmitted THz wave, which is the main reason for the ultra-sensitive sensing characteristics for the composite device. In addition, the effect of glutamic acid solution concentration on the phase of transmitted THz wave was also studied. The results show that the slope extracted from phase difference-frequency curves has a quasi-linear relationship with the concentration from C0 to C5. Therefore, it can also be utilized as an indicator to detect the concentration of the glutamic acid solution with 10−1 fg/mL. This work has contributed to the development of THz metamaterials in amino acid sensors.

     

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