Generation of multiple Fano resonance and high FOM resonance based on the crescent cross nanostructure

Hou Yibo, Huo Yiping, Jiang Xueying, Zhou Chen, Guo Yiyuan,Niu Qiqiang, He Qian, Hao Xiangxiang

Generation of multiple Fano resonance and high FOM resonance based on the crescent cross nanostructure

Hou Yibo, Huo Yiping*, Jiang Xueying, Zhou Chen, Guo Yiyuan,Niu Qiqiang, He Qian, Hao Xiangxiang

School of Physics and Information Technology,Shaanxi Normal University, Xi’an, Shaanxi 710062, China

Metal surface plasmon has many novel optical properties and important applications, and it is also a research hotspot. In this paper, a crescent cross (CC) nanostructure composed of a crescent and a crossis studied by the finite element method. New plasmon magnetic mode and multiple Fano resonancecan be induced by breaking structure symmetry through changing structure parameters. Meanwhile, by changing the angle between the two rods symmetrically, the figure of merit (FOM) can reach 61. Our structure has important applications in the fields of multi-wavelength sensor, ultra-sensitive biosensor, surface enhanced spectroscopy, and slow light transmission.

multiple Fano resonance; surface plasmon; figure of merit

1 Introduction

In recent years, great progress has been made in the research based on surface plasmons (SPs). SPs has been widely used in nano-optoelectronic integration, optical imaging, biosensor, data storage, and has attracted great attention of researchers[1-2]. SPs is collective charge oscillation existing at the interface between conductor and dielectric. SPs is an electromagnetic wave in essence[3], and it can be divided into twotypes: one is propagating surface plasmon polaritons (SPPs),which can propagate along the interface between metal anddielectric;the other is limited by metal nanostructure and canonly be confined to the surface of metal nanoparticles, whichiscalledlocal surface plasmons (LSPs). SPs are favored by researchers for it canmanipulate and integrate photons at micro-nanoscale[4]. SPs not only can enhance the local electromagnetic field on the metal surface, but also break the optical diffraction limit, thus realizing the nanometer-scale regulation of light field[5]. SPs have extremely important application value in related aspects due to their novel optical properties, such as plasmon waveguides[6], surface enhanced Raman scattering[7], electromagnetic induced transparency, and Fano resonance effect[8-9].

Fano resonance comes from the quantum system originally. When the discrete and the continuous energy level are superimposed, quantum interference occurs and low absorption happens at a specific optical frequency, which results in an asymmetric linetype. U Fano explained the mechanism of asymmetric linetype by using strict theory[10-11]. In the SPs system, Fano resonance can be formed by the coupling between the bright mode (superradiant) and the dark mode (subradiant), which results in the asymmetric spectrum[12]. Fano resonance is characterized by asymmetric linetype. A spectral dip is formed through coupling of bright mode and dark mode, where scattering is suppressed and absorption is enhanced[13-14]. The bright mode has a large net dipole moment, which can be excited directly by incident light and exhibits a wider line-width spectrum[14-15]. The net dipole moment of dark mode is almost zero, so it has a small radiation damping and shows a narrow line width[14-16]. Different from the bright mode, dark mode can only be excited by near-field coupling or symmetry breaking[13,17]. For example, Zhu's team studied the structure of silver nanorods with wedge-shaped parts, the Fano line shape arises from the coupling between a hybridized plasmon resonance of the disk and a narrower quadrupolar mode supported by the edge of the missing wedge slice. Fang's team made the structure of heptamer graphene type light probe, where the structure of heptamer is intermingled in the middle of monolayer graphene and Fano resonance is formed through the coupling of heptamer and graphene[13-14]. The radiation loss of Fano resonance is small, and the energy of the incident field can be better confined to the structure surface[18-20]. Based on these optical properties, Fano resonance effect can be widely used in biosensors[21], electromagnetic induction absorption[22], optical switches[23], photodetectors[24-25], etc.

Due to the lack of natural magnetism, people initially focused on electric Fano resonance. However, the magnetic Fano resonance has advantages that the electrical Fano resonance does not have. A closed-loop current can be formed, which can limit the energy more locally, reduce the scattering loss, and strengthen the response of the magnetic field[26-27]. In nanostructures, artificial optical magnetism can be obtained by breaking the symmetry of nanostructure to form magnetic Fano resonance. The obvious characteristic of magnetic Fano resonance is a closed current loop. These features and advantages make magnetic Fano resonances have great potential application in metamaterials, stealth, and high-resolution lithography[28]. When the structure symmetry is destroyed, due to the generation of high order dark state, multiple Fano resonance effect can be induced[29]. Compared with single Fano resonance, multiple Fano resonance effects can adjust multiple waveband spectrum simultaneously[30-31]. The nanostructure parameter effects the modulation depth and resonance frequency of multiple Fano resonance greatly[32]. In addition, the spectrum of Fano resonance varies with the refractive index of environment, which is very suitable for sensing applications[32-33]. Many studies have been carried out to improve the figure of merit (FOM), which can measure the sensing properties of the structure. For example, the maximum FOM of the T-type nanorod dimer structure proposed by Feng team is 9.5[34]; the FOM value of Hu team's I-type trimer structure with two rods can reach 25.9[35]; the FOM value of the H-type nanostructure designed by Goncalves team is 30[36].

The split ring is one of the most common structure in the study of plasmon. A cross is added on the split ring nanostructure, and the cross can be rotated, so the structure asymmetry degree can be adjusted conveniently in various ways. In theory, the cross and the crescent are coupled to form a magnetic pattern and generate magnetic Fano resonance. New plasmon modes and multiple Fano resonance can be induced by breaking structure symmetry through changing structure parameters. In addition, the FOM value can be modulated by changing the angle between two rods symmetrically and the maximum FOM value reaches 61. These optical properties make our structure have broad application prospects in surface enhanced Raman scattering, plasmon scale, multi-band sensing, etc.

2 Structure and simulation method

Figure 1 shows 2-D and 3-D views of the CC nanostructure. The cross is composed of bar1and bar2. The centers of the inner ring and the outer ring are1and2, respectively. The radius of the inner ring and outer ring areand0, respectively. The width and half length of the nanorods areand, respectively. The thickness of the whole nanostructure is. Figs. 1(c)~1(e) are the rotation angles of the cross, rod2and the whole structure around1, which are,andrespectively. The light incident along the negativeaxis and the polarization direction is alongaxis. Compared with other metal materials, silver has the lower loss in the visible light, so silver is selected as the material of the CC nanostructure. The dielectric constant of silver is taken from Johnson and Christy (JC), and the surrounding medium is air.

Fig. 1 (a) 2-D structure and geometric parameters of the CC nanostructure; (b) 3-D schematic diagram of the CC nanostructure; The rotation angles of the cross (c), rod a2 (d)and the whole structure (e) around O1 are θ, α and β degrees respectively

In this paper, a commercial software COMSOL Multiphysics based on the finite element method is used to calculate the optical response of the CC nanostructure. The extinction cross section of the CC nanostructure is calculated, which is equal to the sum of the absorption cross section and the scattering cross section. The total scattering cross section is calculated by integrating the scattered power flux on the outer closed surface of the CC nanostructure. A spherical perfect matching layer (PML) was designed to eliminate the interference of boundary reflections and absorb all of the emitted radiation.

3 Results and discussion

3.1 Optical response characteristic of the CC nanostructure

Fig. 2(a) shows the extinction spectrum of the CC nanostructure, where=80 nm,0=100 nm,=60 nm,=20 nm and=20 nm. From the left to the right, there are three resonance peaks, which are named￠,and. A Fano dipis formed betweenand. In order to explore the formation of this Fano dip, we give the charge distributions, surface current density and magnetic field enhancement distributions of peak￠,,and dip. Figs. 2(b)~(e) show the charge distributions of￠,,and, and Figs. 2(f)~(i) show the surface current density and the magnetic field enhancement distributions of￠,,and. In Fig. 2(b), the charges of the crescent and the cross oscillate in phase, so￠is a bright electric mode. Similarly, modeis also a bright electric mode. Therefore, modes￠andhave a wide linewidth. In Fig. 2(e), the charges of crescent and cross oscillate out phase and the electric dipole moment is small.Two opposite current loops and magnetic hot spots are formed in the gap, sois a dark magnetic mode. Destructive interference between the bright electric modeand the dark magnetic modeforms the magnectic Fano dip. Fig. 2(d) and 2(h) show the charge distribution, magnetic field enhancement and surface current density distribution of dip.

3.2 New magnetic mode generation by rotating the cross

The optical properties of the CC with clockwise rotating cross are further studied. Fig. 3(a) is the extinction spectra when the cross rotate angle is0° , 10°, 20° and 30° respectively.Whenis 10°, a new modeappears near 950 nm, whose charge distributionis shown in Fig.3(b).It can be seen that it is a quadrupole-quadrupole mode and the electric dipole moment is large. Fig. 3(c) shows the magnetic field enhancement and surface current density distributions of mode. It can be seen that three circulations0,1,2and three hot spots are formed between the crescent and the cross. Therefore, modeis bright magnetic mode, which is induced by the symmetry breaking of the CC nanostructure. The region of circulation2can be seen as a series of inductance and capacitance, the magnetic resonance at modeis similar to LC resonance. The resonance frequency formula is showed by equation (1),

Fig. 2 (a) Extinction spectrum of the CC nanostructure; (b)~(e) The charge distributions; (f)~(i) The magnetic field enhancement and surface current density distributions of modeE￠, E, m and M. Here, H represents the local magnetic field, and H0 represents the background magnetic field, where R=80 nm, R0=100 nm, L=60 nm, w=20 nm and T=20 nm

hereis the resonance frequency,is the inductance andis the capacitance. As the rotating angle of the cross increases, the gap between the rod and the crescent is enlarged. The capacitancedecreases, and the resonance frequencyincreases, so modeblue shifts.

3.3 Double Fano resonance generation by rotating rod a2

Rotating the rod2anticlockwise by 15, 30, 45and 60,the optical property of the CC nanostructure were further studied. For the symmetry breaking, a new modeis created near 950 nmwhenis 15. According to LC resonance frequency formula, as the rod2rotates anticlockwise, angleincreases and the inductancedecreases, so the resonance frequencyincreases and modeblue shifts. At the same time, the distance between the two rods decreases, so the coupling between the two rods becomes stronger and the intensity of modeis enhanced. Fig.4(b) shows the charge distribution of mode, which is a quadrupole-quadrupole mode with a small electricdipole moment and can be judged as a dark mode.It’s magnetic field enhancement and current distributions are shown in Fig.4(c). Three hotspots and three circulations are formed between the crescent and the bars,so modeis a dark magnetic mode. The dark magnetic modeand the original bright electric modeare coupled to form a Fano dip. Fano dipandare called double Fano resonance.

3.4 Multiple Fano resonance generation by breaking structure symmetry

3.4.1 Reducing the length of rod1

Fig. 5(a) showsthe extinction spectra of the CC nanostructure when the half length of bar1reduces from 60 nm to 35 nm with 5 nm intervals. Whenis 55 nm, a new modeappears. Whenis 50 nm, another new mode￠is induced, and whenis 45 nm, the third new modeappears. Figs. 5(b)~5(d) showthe charge distributions of the new modes,￠,. Figs. 5(e)~5(g) are magnetic field enhancements and surface currentdensity distributions of the new modes,￠,. Fig.5(d)shows that modeis a dipole-quadrupole mode with a large electric dipole moment,which is a bright state. In Fig.5(g), there are three current loops with opposite rotating directions and three magnetic hotspots in the gap betweenthe crescent and the cross, so modeis a bright magnetic mode. From Figs. 5(c) and 5(f), it can be seen that mode￠is a quadrupole-quadrupole mode, and the electric dipole moment is small, so it can be judged as dark mode. There isno circulation in the current distribution, so mode￠is a dark electric mode. The coupling of modesand￠induces the first Fano dip2near 850 nm.Mode￠coupledwith modeto form the second electric Fano resonance dip1near 800 nm. From Figs. 5(b) and 5(e), it can be judged that modeis also a dark mode. Modeandare coupled to form the third electric Fano resonancedipat 680 nm.So,,1and2are the multiple Fano resonance.

Fig. 3 (a) Extinction spectra of the CC nanostructure with rotating cross; (b) The charge distribution of the new mode D when θ=10°; (c) The magnetic field enhancement and surface current density distribution of the new mode D when θ=10°

Fig. 4 (a) Extinction spectra of the CC nanostructure with rotating rod a2; (b) The charge distribution of mode G when α=15°; (c) The magnetic field enhancement and current density distributions of mode G when α=15°

3.4.2 Rotating the whole structure

The optical properties of the rotating CC nanostructure were studied. Fig. 6(a) shows the extinction spectra of the entire CC nanostructure with different rotating angle. It can be seen that whenis 15°, new modesis generated. Continue to rotate the whole structure to 30°, new mode￠appears. Then, rotate the whole structure to 45°, new modeappears. Figs. 6(b)~6(d) are charge distributions of new modes￠,and. Figs. 6(e)~6(g) are magnetic field enhancement and surface current density distributions of new modes￠,,. As shown in Figs. 6(b) and 6(e), a high-order quadrupole-octupole mode￠is excited by rotating the overall structure, which can be judged as a bright electric mode. It can be seen from Figs. 6(c) and 6(f) that modeis a quadrupole-quadrupole mode and the electric dipole moment is small. There is no current loop in the structure, so it is judged to be a dark electric mode. Figs. 6(d) and 6(g) show that modeis a quadrupole-quadrupole mode with a small electric dipole moment and three current loops, so modeis a dark magnetic mode. Thus, the coupling of modesandinduces the first magnetic Fano dip2at 900 nm. The coupling of modes Eandproduces the second Fano dip1at 700 nm. And the coupling of modesand￠forms the third Fano dipnear 600 nm.2,1andare multiple Fano resonance.

Asincreases, the intensity of modedecreases continuously until the modedisappears whenis 90°. This interesting phenomenon can be explained by Fig. 7. The black and red solid lines represent the symmetry axis of the CC nanostructure and the polarization direction of the electric field, respectively.is the angle between the symmetry axis of the CC naostructure and the polarization direction of the electric field. The polarization direction of the electric field can be decomposed along the symmetry axis () of the CC structure and decomposed perpendicular to the symmetry axis () (Fig. 7(b)). Ifincreases, the intensity of modewill be reduced, which can be interpreted as the decrease of the parallel component. Whenis 90°, the modedisappears because there is no parallel component(Fig. 7(c)).

Fig. 5 (a) Extinction spectra of the CC nanostructure when bar a1 decreases; (b)~(d) The charge distributions of mode B, V', V when L=40 nm; (e)~(g) The magnetic field enhancement and surface current density distributions of modes B, V', V when L=40 nm

Fig. 6 (a) The extinction spectra of the CC nanostructure with rotating the whole structure from 0°to 90°with 15°intervals; (b)~(d) The charge distributions of mode Z', Z and H when β= 60°; (e)~(g) The magnetic field enhancement and surface current distributions of mode Z', Z and Hwhen β = 60°

Fig. 7 Schematic diagram when the angle between the polarization direction of the electric field and the symmetry axis of the CC nanostructure β is (a) 0°; (b) 45° and (c) 90° respectively. Ex and Ey are the parallel component and the vertical component of symmetry axis, respectively

3.5 High FOM by changing the angle between the two bars

The Fano resonance peak changes with the refractive index of the surrounding environment. As shown in Fig. 8(a), the extinction cross section and the resonance peak position of the CC nanostructure with different refractive index environments are simulated. The inset is the 2-D diagram of the structure, the angle between the two rods is 150°, and other parameters are the same as above. In order to study the sensitivity of the CC nanostructures to the surrounding environment, the position of modewith different refractive index environments are calculated. Whenis 1, modeis at 1090 nm, and whenis 1.05, modeis red shifted to 1140 nm, which is due to the influence of environmental change on far-field interference between different scatter paths. As we all know, device sensitivity is an important indicator for the performance of a sensor, which is calculated by the formula (2),

theFWHMis the full width at half maximum of the resonance mode, theFOMof the CC nanostructure is 61.

The FOM was studied when change the angle between two rods in a metal nanostructure. Fig. 8(b) shows that, as the angle between the two rods changes from 90° to 180° with 15° intervals, the FOM value increases firstly and then reduces sharply to 35 at 165° and finally increases to 48 at 180o. It can be found that the highest FOM value is 61. Compared with other plasma metal nanostructures, the FOM value of the CC metal nanostructures studied in this paper is relatively high, and it has applications in biosensors, optical switches, photodetectors, etc.

4 Conclusions

We designed a CC nanostructure to achieve multiple Fano resonance with high FOM magnetic resonance. Breaking the symmetry of the structure by rotating the cross and the single rod, a new magnetic mode can be created. The multiple Fano resonance can be generated by rotating the whole structure and reducing the length of rod1. High FOM can be implemented by changing the angle between the two rods in the structure. These excellent optical properties make the CC nanostructures have potential application prospects in ultra-sensitive biosensors, surface enhanced spectroscopy and so on.

Fig. 8 (a) The extinction cross-section of the CC nanostructures varies with the refractive index of the surrounding environment. The angle between the two rods is 150o; (b) The FOM value of the structure changing with the angle between the two rods

[1] Zhang J X, Zhang L D. Nanostructures for surface plasmons[J].2012, 4(2): 157–321.

[2] Gao W T, Chen C Y, Sun Z J. Local field enhancement and its wavelength tuning in metal nanoparticle arrays[J].2019, 58(3): 030910.

[3] Garcia M A. Surface plasmons in metallic nanoparticles: fundamentals and applications[J]., 2011, 44(28): 283001.

[4] Lodewijks K, Ryken J, Van Roy W,Tuning the fano resonance between localized and propagating surface plasmon resonances for refractive index sensing applications[J]., 2013, 8(3): 1379–1385.

[5] Newman D M, Wears M L, Matelon R J,. Magneto-optic behaviour in the presence of surface plasmons[J]., 2008, 20(34): 345230.

[6] Liu L, Han Z H, He S L. Novel surface plasmon waveguide for high integration[J]., 2005, 13(17): 6645–6650.

[7] Dong J, Qu S X, Zheng H R,. Simultaneous SEF and SERRS from silver fractal-like nanostructure[J]., 2014, 191: 595–599.

[8] Ooi C H R, Tan K S. Controlling double quantum coherence and electromagnetic induced transparency with plasmonic metallic nanoparticle[J]., 2013, 8(2): 891–898.

[9] Luk'Yanchuk B, Zheludev N I, Maier S A,. The fano resonance in plasmonic nanostructures and metamaterials[J]., 2010, 9(9): 707–715.

[10] Kobayashi K, Aikawa H, Sano A,. Fano resonance in a quantum wire with a side-coupled quantum dot[J]., 2004, 70(3): 035319.

[11] de Guevara M L L, Claro F, Orellana P A. Ghost fano resonance in a double quantum dot molecule attached to leads[J]., 2003, 67(19): 195335.

[12] Hajebifard A, Berini P. Fano resonances in plasmonic heptamer nano-hole arrays[J]., 2017, 25(16): 18566–18580.

[13] Fang Z Y, Liu Z, Wang Y M,. Graphene-antenna sandwich photodetector[J]., 2012, 12(7): 3808–3813.

[14] Fang Z Y, Cai J Y, Yan Z B,. Removing a wedge from a metallic nanodisk reveals a fano resonance[J]., 2011, 11(10): 4475–4479.

[15] Frimmer M, Coenen T, Koenderink A F. Signature of a fano resonance in a plasmonic metamolecule’s local density of optical states[J]., 2012, 108(7): 077404.

[16] Chen S, Meng L Y, Hu J W,. Fano interference between higher localized and propagating surface plasmon modes in nanovoid arrays[J]., 2015, 10(1): 71–76.

[17] Li J, Zhang Y, Jia T Q,. High tunability multipolar fano resonances in dual-ring/disk cavities[J]., 2014, 9(6): 1251–1256.

[18] Kuznetsov M, Haus H. Radiation loss in dielectric waveguide structures by the volume current method[J]., 1983, 19(10): 1505–1514.

[19] Huo Y Y, Jia T Q, Zhang Y,. Spaser based on fano resonance in a rod and concentric square ring-disk nanostructure[J]., 2014, 104(11): 113104.

[20] Zhao Q, Yang Z J, He J. Fano resonances in heterogeneous dimers of silicon and gold nanospheres[J]., 2018, 13(3): 137801.

[21] Lee K L, Wu S H, Lee C W,. Sensitive biosensors using fano resonance in single gold nanoslit with periodic grooves[J]., 2011, 19(24): 24530–24539.

[22] Lee E, Zhou K, Gwon M,. Surface plasmon-induced absorption enhancement of silicon nanowire array[J]., 2012, 8457: 84572C.

[23] Tasolamprou A C, Zografopoulos D C, Kriezis E E. Liquid crystal-based dielectric loaded surface plasmon polariton optical switches[J]., 2011, 110(9): 093102.

[24] Gong X, Tong M H, Xia Y J,. High-detectivity polymer photodetectors with spectral response from 300 nm to 1450 nm[J]., 2009, 325(5948): 1665–1667.

[25] Berini P. Surface plasmon photodetectors and their applications[J]., 2014, 8(2): 197–220.

[26] Bao Y J, Hu Z J, Li Z W,. Magnetic plasmonic fano resonance at optical frequency[J]., 2015, 11(18): 2177–2181.

[27] Bao Y J, Zu S, Zhang Y F,. Active control of graphene-based unidirectional surface plasmon launcher[J]., 2015, 2(8): 1135–1140.

[28] Bao Y J, Zhu X, Fang Z Y. Plasmonic toroidal dipolar response under radially polarized excitation[J]., 2015, 5: 11793.

[29] Zhang Q, Wen X L, Li G Y,. Multiple magnetic mode-based fano resonance in split-ring resonator/disk nanocavities[J]., 2013, 7(12): 11071–11078.

[30] Yang L, Wang J C, Yang L Z,. Characteristics of multiple fano resonances in waveguide-coupled surface plasmon resonance sensors based on waveguide theory[J]., 2018, 8(1): 2560.

[31] Kong Y, Cao J J, Qian W C,. Multiple fano resonance based optical refractive index sensor composed of micro-cavity and micro-structure[J]., 2018, 10(6): 6804410.

[32] Li C, Li S L, Wang Y L,. Multiple fano resonances based on plasmonic resonator system with end-coupled cavities for high-performance nanosensor[J].2017, 9(6): 4801509.

[33] Zhang Y Y, Li S L, Zhang X Y,. Evolution of fano resonance based on symmetric/asymmetric plasmonic waveguide system and its application in nanosensor[J].2016, 370: 203–208.

[34] Yun B F, Hu G H, Cong J W,Fano resonances induced by strong interactions between dipole and multipole plasmons in t-shaped nanorod dimer[J].2014, 9(3): 691–698.

[35] Wang J Q, Fan C Z, He J N,. Double fano resonances due to interplay of electric and magnetic plasmon modes in planar plasmonic structure with high sensing sensitivity[J].2013, 21(2): 2236–2244.

[36] Gon?alves M R, Melikyan A, Minassian H,. Strong dipole-quadrupole coupling and fano resonance in h-like metallic nanostructures[J].2014, 22(20): 24516–24529.

Generation of multiple Fano resonance and high FOM resonance based onthe crescent crossnanostructure

Hou Yibo, Huo Yiping*, Jiang Xueying, Zhou Chen, Guo Yiyuan,Niu Qiqiang, He Qian, Hao Xiangxiang

School of Physics and Information Technology, Shaanxi Normal University, Xi’an, Shaanxi 710062, China

(a) 2-D structure and geometric parameters of the CC nanostructure; (b) 3-D schematic diagram of the CC nanostructure

Overview:In recent years, great progress has been made in the research based on surface plasmons (SPs). SPs has been widely used in nano-optoelectronic integration, optical imaging, biosensor, data storage, and has attracted great attention of researchers. Fano resonance comes from the quantum system originally. When the discrete and the continuous energy level are superimposed, quantum interference occurs and low absorption happens at a specific optical frequency, which results in an asymmetric linetype. U Fano explained the mechanism of asymmetric linetype by using strict theory. In the SPs system, Fano resonance can be formed by the coupling between the bright mode (superradiant) and the dark mode (subradiant), which results in the asymmetric spectrum. Fano resonance is characterized by asymmetric linetype. A spectral dip is formed through coupling of bright mode and dark mode, where scattering is suppressed and absorption is enhanced. In order to explore the optical characteristics and application of surface plasmon resonance modes of composite metal nanostructures, a crescent cross (CC) nanostructure composed of a crescent and a cross is designed. A commercial software COMSOL Multiphysics based on the finite element method is used to calculate the optical response of the CC nanostructure. The direction of incident light is perpendicular to the surface of the nanostructure, and the polarization of light propagates parallel to the structure. By changing the structural parameters to break the symmetry of the nanostructure, rich optical properties can be obtained. The rotating cross can excite the surface plasmon resonance magnetic mode, and the electric mode and the magnetic mode are coupled to form the magnetic Fano resonance. The magnetic Fano resonance has advantages that the electrical Fano resonance does not have. A closed-loop current can be formed, which can limit the energy more locally, reduce the scattering loss and strengthen the response of the magnetic field. By rotating and shortening the single rod2, the structural symmetry is broken to generate multiple Fano resonance effects. Meanwhile, the optical characteristics of the plasmon resonance mode on the surface of the nanostructure are tuned by changing the polarization direction of light (rotating the entire structure) without changing the basic structure, and it is found that new Fano resonances occur continuously during the rotation process, thus forming multiple Fano resonances. In order to explore the application potential of crescent cross nanostructure in sensing field, we calculated its sensitivity. By changing the angle between the two rods symmetrically, the figure of merit (FOM) can reach 61. Our structure has important applications in the fields of multi-wavelength sensor, ultra-sensitive biosensor, surface enhanced spectroscopy and slow light transmission.

Citation: Hou Y B, Huo Y P, Jiang X Y,. Generation of multiple Fano resonance andhigh FOM resonance based onthe crescent crossnanostructure[J]., 2020,47(11): 200010

新月十字架納米結(jié)構(gòu)中多Fano共振的產(chǎn)生和高FOM共振

侯藝博，霍義萍*，姜雪瑩，周 辰，郭懿圓，牛啟強(qiáng)，何 倩，郝祥祥

陜西師范大學(xué)物理學(xué)與信息技術(shù)學(xué)院，陜西 西安 710062

金屬表面等離激元具有許多新穎的光學(xué)特性和重要的應(yīng)用，并且也是當(dāng)今研究的熱點(diǎn)。本文采用有限元方法研究了由新月和十字架組成的新月十字架納米結(jié)構(gòu)。通過改變結(jié)構(gòu)參數(shù)來打破結(jié)構(gòu)對(duì)稱性，可以產(chǎn)生新的等離激元磁模式和多重Fano共振。同時(shí)，通過對(duì)稱地改變兩棒之間的夾角，F(xiàn)OM值可以達(dá)到61。我們的結(jié)構(gòu)在多波長傳感器、超靈敏生物傳感器、表面增強(qiáng)光譜和慢光傳輸?shù)阮I(lǐng)域有著重要的應(yīng)用。

多Fano共振；表面等離激元；品質(zhì)因數(shù)

TP212

A

侯藝博，霍義萍，姜雪瑩，等. 新月十字架納米結(jié)構(gòu)中多Fano共振的產(chǎn)生和高FOM共振[J]. 光電工程，2020，47(11): 200010

2020-01-06；

2020-03-31

國家自然科學(xué)基金資助項(xiàng)目(11604198)

侯藝博(1995-)，男，碩士，主要從事表面等離激元光子學(xué)的研究。E-mail：hou994682946@qq.com

霍義萍(1977-)，女，博士，副教授，主要從事表面等離激元光子學(xué)的研究。E-mail：yphuo@snnu.edu.cn

: Hou Y B, Huo Y P, Jiang X Y,Generation of multiple Fano resonance andhigh FOM resonance based onthe crescent crossnanostructure[J]., 2020, 47(11): 200010

10.12086/oee.2020.200010

Supported by National Natural Foundation of China (11604198)

* E-mail: yphuo@snnu.edu.cn