Design of terahertz metal-dielectric-metal waveguide with microfluidic sensing stub
Introduction
Terahertz spectroscopy, which covers radiation band ranging 100 GHz to 10 THz, has intrigued tremendous interests in the biological, chemical sciences as well as clinical research communities. Studies have shown that terahertz waves could identify intermolecular and intramolecular hydrogen bonds in biological materials such as amino acids [1], polypeptides [2], DNA [3], protein [4], sugars [5], pharmaceuticals [6]. Applications such as pathological examinations of tissues [7] and identification of drugs or explosives in postal packages can also be realized with this real-time, marker-free and non-ionizing technique 8, 9.
However, there are a few limitations for applying THz spectroscopy in biological detection in water solutions. Firstly, water has huge absorption of THz waves due to the excitation of both water dipolar moments and the hydrogen bond network. The method of using attenuated total reflection can partially solve the problem, but it will encounter the large signal loss from the in and out of the coupling prism [10]. Second, relatively larger volume of bio-samples would be needed for THz analyses based on transmission, since the wavelength of 1 THz is about 300 µm and the wrist of the correspondent Gaussian beam is therefore above 1 mm. Large quantities of samples to be studied may be hard to collect in reality. To overcome such difficulties in sample volume, microfluidic systems have been proposed for accurate volume control of the solutions to perform THz spectroscopy 11, 12, 13, 14.
Alternatively, to address the above limitations, different THz wave manipulation structures such as parallel plate waveguides (PPWGs) or similarly metal-dielectric-metal (MDM) waveguides were proposed, since they can support modes with deep sub-wavelength scale and high group velocity over a very wide range of frequencies extending from DC to visible scale. This is due to the formation of the dispersion-less transverse electro-magnetic (TEM) mode or the similarly MDM fundamental mode (TM0) considering surface plasmon polaritons(SPP) [15]. In THz domain, the highly localized field inside the PPWGs has been used to increase the sensitivity of a measurement 16, 17, 18. Furthermore the stub like resonator has been integrated in the THz PPWG as a refractive index sensor for liquids in a microfluidic platform 19, 20, but they did not use the TM0 mode and the influence of THz SPP at metal-dielectric interfaces had not been explored though the metals behave almost like a perfect conductor (PEC).
In this paper, we proposed a compact (several tens of micrometers width and several hundreds of micrometers length) and highly sensitive liquid refractive index sensor based on a two layers THz MDM stub structure. To make optimized designs, we not only employed the numerical technique such as the finite difference-time domain method (FDTD), but also generated the transmission line model (TLM) for the proposed sensing structure. TLM is a fast and reliable analytical approach investigated for optical bands 21, 22, 23, 24, but few applications are reported in the THz band. The characterization of the impedance of the MDM by TLM can be useful for a better understanding of the MDM based THz components. TLM analytical modal also provides a design tool to generate complex plasmonic structures since the amount of calculation will dramatically drop when the optimization is necessary compared with EM popular full wave numerical methods such as FDTD and FEM. The model allows us to rapidly and precisely simulate the transmission spectra of THz MDM stub sensor considering SPP. The sensing characteristics of the proposed THz MDM stub structure were analyzed in detail. The result show that THz MDM stub integrated with a microfluidic channel can be a very promising for both molecular and cellular analyses towards point-of-care type of biological sensing.
Section snippets
Structure and method
The proposed THz MDM wave guide with a two layers stub structure is schematically shown in Fig. 1(a) and (b), in which the stub includes a solid spacing dielectric layer and a liquid biomaterial sample layer. Consider the possible applied scenario in Fig. 1(a) where the thickness t of the structure is thick enough to simplify the sensor into a 2D scheme in Fig. 1(b). The channel () width is d. The two layers stub with width w includes a dielectric spacing layer () with height h1 and a
Results and discussion
To illustrate the developed transmission line model by comparing the metal models by PEC and Drude, we considered the THz stub waveguide with the following set of parameters L=200 , h2=w=d=20 , and h1=10. The metal is gold, the channel is filled with air, the spacing dielectric is Si, and the sample is water by the model in Eq. (8). The geometry parameters are typical in applications such as PCR [30] and circulation tumor cell (CTC) detection 31, 32, 33, 34, 35. We examined the accuracy of
Conclusion
In summary, we introduce the design of a compact THz MDM waveguide-coupled microfluidic stub structure for the detection of refractive index variations in liquid. TLM method is proved as an efficient and reliable analytical approach to design the sensor structure on deep THz sub-wavelength MDM waveguide. The resonant wavelength of the sensor has a linear relationship with the refractive index of the sample under investigation. The sensitivity of the sensor can be further optimized by narrowing
Acknowledgments
Our work has been financially supported by the Nonprofit Technology Research Programs of Zhejiang Province of China under Grant no. 2013C31088 (Li), National Science Foundation CAREER Award under Grant no. 0846313 and DARPA Young Faculty Award under N66001-10-1-4049 (Zhang).
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