Citation: | Wei X R, Liang Y Z, He Y J, et al. Tamm-surface plasmon hybrid mode for improving sensing figure of merit[J]. Opto-Electron Eng, 2022, 49(11): 220217. doi: 10.12086/oee.2022.220217 |
[1] | Singh P. SPR biosensors: historical perspectives and current challenges[J]. Sens Actuators B Chem, 2016, 229: 110−130. doi: 10.1016/j.snb.2016.01.118 |
[2] | Wen X M, Bi Y G, Yi F S, et al. Tunable surface plasmon-polariton resonance in organic light-emitting devices based on corrugated alloy electrodes[J]. Opto-Electron Adv, 2021, 4(8): 200024. doi: 10.29026/oea.2021.200024 |
[3] | Hu A Q, Liu S, Zhao J Y, et al. Controlling plasmon‐exciton interactions through photothermal reshaping[J]. Opto-Electron Adv, 2020, 3(1): 190017. doi: 10.29026/oea.2020.190017 |
[4] | Tong L M, Wei H, Zhang S P, et al. Recent advances in plasmonic sensors[J]. Sensors, 2014, 14(5): 7959−7973. doi: 10.3390/s140507959 |
[5] | Zhao Y, Tong R J, Xia F, et al. Current status of optical fiber biosensor based on surface plasmon resonance[J]. Biosens Bioelectron, 2019, 142: 111505. doi: 10.1016/j.bios.2019.111505 |
[6] | Shrivastav A M, Cvelbar U, Abdulhalim I. A comprehensive review on plasmonic-based biosensors used in viral diagnostics[J]. Commun Biol, 2021, 4(1): 70. doi: 10.1038/s42003-020-01615-8 |
[7] | Verma R, Gupta B D. Detection of heavy metal ions in contaminated water by surface plasmon resonance based optical fibre sensor using conducting polymer and chitosan[J]. Food Chem, 2015, 166: 568−575. doi: 10.1016/j.foodchem.2014.06.045 |
[8] | Li Y, Liu X, Lin Z. Recent developments and applications of surface plasmon resonance biosensors for the detection of mycotoxins in foodstuffs[J]. Food Chem, 2012, 132(3): 1549−1554. doi: 10.1016/j.foodchem.2011.10.109 |
[9] | Homola J, Yee S S, Gauglitz G. Surface plasmon resonance sensors: review[J]. Sens Actuators B Chem, 1999, 54(1–2): 3–15. doi: 10.1016/S0925-4005(98)00321-9. |
[10] | Kasani S, Curtin K, Wu N Q. A review of 2D and 3D plasmonic nanostructure array patterns: fabrication, light management and sensing applications[J]. Nanophotonics, 2019, 8(12): 2065−2089. doi: 10.1515/nanoph-2019-0158 |
[11] | Li D C, Wu J W, Wu P, et al. Affinity based glucose measurement using fiber optic surface plasmon resonance sensor with surface modification by borate polymer[J]. Sens Actuators B Chem, 2015, 213: 295−304. doi: 10.1016/j.snb.2015.02.039 |
[12] | Wu L M, Guo J, Wang Q K, et al. Sensitivity enhancement by using few-layer black phosphorus-graphene/TMDCs heterostructure in surface plasmon resonance biochemical sensor[J]. Sens Actuators B Chem, 2017, 249: 542−548. doi: 10.1016/j.snb.2017.04.110 |
[13] | Li C, Guo J J, Shafi M, et al. Optical fiber SPR biosensor complying with a 3D composite hyperbolic metamaterial and a graphene film[J]. Photonics Res, 2021, 9(3): 379−388. doi: 10.1364/PRJ.416815 |
[14] | Kumar S, Maji P S, Das R. Tamm-plasmon resonance based temperature sensor in a Ta2O5/SiO2 based distributed Bragg reflector[J]. Sens Actuators A Phys, 2017, 260: 10−15. doi: 10.1016/j.sna.2017.03.038 |
[15] | Wang X, Jiang X, You Q, et al. Tunable and multichannel terahertz perfect absorber due to Tamm surface plasmons with graphene[J]. Photonics Res, 2017, 5(6): 536−542. doi: 10.1364/PRJ.5.000536 |
[16] | Chang C C, Chen T Y, Lin T W, et al. Flexible and ultranarrow transmissive color filters by simultaneous excitations of triple resonant eigenmodes in hybrid metallic–optical Tamm state devices[J]. ACS Photonics, 2021, 8(2): 540−549. doi: 10.1021/acsphotonics.0c01550 |
[17] | Buzavaite-Verteliene E, Plikusiene I, Tolenis T, et al. Hybrid Tamm-surface plasmon polariton mode for highly sensitive detection of protein interactions[J]. Opt Express, 2020, 28(20): 29033−29043. doi: 10.1364/OE.401802 |
[18] | Afinogenov B I, Bessonov V O, Nikulin A A, et al. Observation of hybrid state of Tamm and surface plasmon-polaritons in one-dimensional photonic crystals[J]. Appl Phys Lett, 2013, 103(6): 061112. doi: 10.1063/1.4817999 |
[19] | Bužavaitė-Vertelienė E, Vertelis V, Balevičius Z. The experimental evidence of a strong coupling regime in the hybrid Tamm plasmon-surface plasmon polariton mode[J]. Nanophotonics, 2021, 10(5): 1565−1571. doi: 10.1515/nanoph-2020-0660 |
[20] | He X L, Yi H, Long J, et al. Plasmonic crystal cavity on single-mode optical fiber end facet for label-free biosensing[J]. Appl Phys Lett, 2016, 108(23): 231105. doi: 10.1063/1.4953413 |
[21] | Lei Z Y, Zhou X, Yang J, et al. Second-order distributed-feedback surface plasmon resonator for single-mode fiber end-facet biosensing[J]. Appl Phys Lett, 2017, 110(17): 171107. doi: 10.1063/1.4982625 |
[22] | Johnson P B, Christy R W. Optical constants of the noble metals[J]. Phys Rev B, 1972, 6(12): 4370−4379. doi: 10.1103/PhysRevB.6.4370 |
[23] | 侯艺博, 霍义萍, 姜雪莹, 等. 新月十字架纳米结构中多Fano共振的产生和高FOM共振(英文)[J]. 光电工程, 2020, 47(11): 200010. doi: 10.12086/oee.2020.200010. Hou Y B, Huo Y P, Jiang X Y, et al. Generation of multiple Fano resonance and high FOM resonance based on the crescent cross nanostructure[J]. Opto-Electron Eng, 2020, 47(11): 200010. doi: 10.12086/oee.2020.200010. |
Nanograting coupled multilayer stack structure for improving sensing figure of merit. (a) Three-dimensional schematic for biomolecule detection; (b) Cross-sectional view of the structure and corresponding material composition. The red arrows represent the propagation path of the TM polarized light, and the red curves represent the distribution characteristics of the electric field of SPP and TPP in the structure
The reflection spectra of the simplified structure. When the incident angle is equal to the first-order diffraction angle of the nanograting with a period of 536 nm and the thicknesses of the gold film on the top surface of the structure are (a) 400 nm and (b) 40 nm, respectively, the effect of the center wavelength of the photonic crystal on the reflection spectra of the gold film-photonic crystal multilayer structure; (c) The relationship between the wavevector and the energy of the incident light in the structure, and the dispersion curves excited separately by the SPP mode (yellow short dashed curve) and the low-order TPP mode (cyan short dashed line) ; (d) The reflection spectra of the structure that only excites TPP mode (yellow curve) and SPP mode (blue curve), and the reflection spectra corresponding to the strong coupling between TPP and SPP (red curve)
Reflection spectra and electric field distributions at the resonance positions of the grating-coupled multilayer stack structure. (a) Reflection spectra of three typical structures, in which there are TPP (yellow curve) and SPP (blue curve) modes and TPP-SPP hybrid mode (red curve) generated; The spatial electric field intensity distributions of (b) SPP mode, (c) TPP mode; (d) High-frequency and (e) low-frequency TPP-SPP hybridization modes. The curve in the right inset is the variation of electric field intensity at the dotted line position in the electric field intensity distribution diagrams
Quantitative evaluation of the sensing performance. Reflection spectra of structures with (a) TPP-SPP hybrid mode and (b) SPP mode at the ambient with different refractive indexes; (c) The amount of red-shift of the resonance wavelengths caused by the change of the external refractive index; (d) Sensing figures of merit of TPP-SPP hybrid mode (red mark) and SPP mode (blue mark) under the ambient surroundings with different refractive indexes
Reflection spectra of the structures corresponding to the excited high-frequency TPP-SPP hybrid mode structures at the wavelengths of (a) 631 nm and (b) 844 nm. The reflection spectra of the SPP mode are used as a reference; (c) Bulk refractive index sensitivity and (d) sensing figure of merit of TPP-SPP hybrid mode and SPP mode at different structural periods