Direction-finding device based on coupled and detuned spoof localized surface plasmons

12405340 ยท 2025-09-02

Assignee

Inventors

Cpc classification

International classification

Abstract

A direction-finding device based on coupled and detuned spoof localized surface plasmons, comprising a dielectric substrate with a metal coating at the bottom and two evenly-grooved metal discs with different sizes or materials. The two grooved metal discs represent two spoof localized surface plasmonic resonators, i.e., SLSP1 and SLSP2, with different resonance frequencies due to their different sizes or materials. SLSP1 and SLSP2 are distributed on the dielectric substrate along the diagonal of the dielectric substrate, with the center of the dielectric substrate as a symmetrical center, to form a coupled and detuned spoof localized surface plasmonic system. In response to the incoming waves from different directions, SLSP1 and SLSP2 support spoof localized surface plasmonic modes with different phase differences. According to the phase difference, the incident angle of the incoming waves can be determined uniquely.

Claims

1. A direction-finding device based on coupled and detuned spoof localized surface plasmons, comprising: a dielectric substrate with a metal coating at a bottom; two evenly-grooved metal discs with different sizes or materials, representing a first spoof localized surface plasmonic resonator SLSP1 and a second spoof localized surface plasmonic resonator SLSP2 that have different resonance frequencies, wherein the first spoof localized surface plasmonic resonator SLSP1 and the second spoof localized surface plasmonic resonator SLSP2, are distributed on the dielectric substrate along a diagonal of the dielectric substrate, with a center of the dielectric substrate as a symmetrical center, to form a coupled and detuned spoof localized surface plasmonic system; a first probe and a second probe respectively provided adjacent to the first spoof localized surface plasmonic resonator SLSP1 and the second spoof localized surface plasmonic resonator SLSP2, and configured to detect electric fields of the first spoof localized surface plasmonic resonator SLSP1 and the second spoof localized surface plasmonic resonator SLSP2; and a signal processing circuit connected to the first probe and the second probe and configured to obtain an electric-field phase difference between the first spoof localized surface plasmonic resonator SLSP1 and the second spoof localized surface plasmonic resonator SLSP2 under an illumination of an incident wave; and determine directions of incoming waves based on a monotonous correspondence between the electric-field phase difference and an incident angle of the incoming waves.

2. The direction-finding device according to claim 1, wherein the two evenly-grooved metal discs with different sizes, refer to differences in an outer radius, an inner radius, or a thickness of the evenly-grooved metal discs, and the outer radius denotes a radius of each of the evenly-grooved metal discs, while the inner radius denotes an internal-circle radius of each of the evenly-grooved metal discs without grooves.

3. The direction-finding device according to claim 1, wherein a material of the evenly-grooved metal disc is selected from a group consisting of copper, gold, and silver.

4. The direction-finding device according to claim 1, wherein a material of the dielectric substrate is determined according to a permittivity parameter, enabling a structure of the evenly-grooved metal discs on the dielectric substrate to support spoof localized surface plasmonic resonance mode, and the metal coating at the bottom of the dielectric substrate is copper, gold, or silver.

5. The direction-finding device according to claim 1, wherein the first spoof localized surface plasmonic resonator SLSP1 and the second spoof localized surface plasmonic resonator SLSP2 support spoof localized surface plasmonic modes with different phase differences, in response to the incoming waves from different directions.

Description

BRIEF DESCRIPTION OF DRAWINGS

(1) The attached figures, which are incorporated in and constitute a part of this specification, serve to explain the principles of the present application together with the description.

(2) FIG. 1 is a schematic view of the direction-finding device structure based on coupled and detuned spoof localized surface plasmonic resonators according to an exemplary embodiment.

(3) FIG. 2 is a transmission spectrum diagram and dipole-mode profile supported by a spoof localized surface plasmon according to an exemplary embodiment.

(4) FIG. 3 is a spectral evolution of spoof localized surface plasmonic resonators with different inner radii according to an exemplary embodiment.

(5) FIG. 4 is a comparison of the spectral intensities before and after utilizing spoof localized surface plasmonic resonators according to an exemplary embodiment.

(6) FIG. 5 shows a monotonically increasing relationship between the measured phase difference of the spoof localized surface plasmons and the incident angle of the incoming waves, according to an exemplary embodiment.

DESCRIPTION OF EMBODIMENTS

(7) Reference will now be made in detail to exemplary embodiments, examples of which are illustrated in the accompanying drawings. When the following description refers to the drawings, unless otherwise indicated, the same numbers in different drawings indicate the same or similar elements. The embodiments described in the following exemplary embodiments do not represent all embodiments consistent with the present disclosure. Rather, they are merely examples of devices and methods consistent with some aspects of the present disclosure as detailed in the appended claims.

(8) The terminology used in the present disclosure is to describe specific embodiments only and is not intended to limit the present disclosure. The singular forms a, said and the used in the present disclosure and the appended claims are also intended to include the plural forms, unless the context clearly indicates other meaning. It should also be understood that the term and/or as used herein refers to and includes any or all possible combinations of one or more associated listed items.

(9) The present disclosure provides a direction-finding device based on coupled and detuned spoof localized surface plasmons (SLSPs). As shown in FIG. 1, the direction-finding device is composed of two evenly grooved metal discs of different sizes or materials on the dielectric substrate with a metal coating at the bottom. The two evenly grooved metal discs, represent a first spoof localized surface plasmonic resonator SLSP1 and a second spoof localized surface plasmonic resonator SLSP2 with different resonance frequencies due to their different sizes or materials. The two SLSP resonators, i.e., SLSP1 and SLSP2, are distributed on the dielectric substrate along the diagonal of the dielectric substrate, with the center of the dielectric substrate as a symmetrical center, to form a coupled and detuned SLSP system.

(10) It should be noted that the different sizes of the two evenly grooved metal discs, specifically, refer to the differences in the outer radius, inner radius, or thickness of the discs, The outer radius denotes the radius of the metal disc, while the inner radius denotes the internal-circle radius of the metal disc without grooves.

(11) The following discussion will focus on an embodiment of the direction-finding device operating at 3.67 GHz.

(12) In the embodiment, the two metal discs are evenly grooved from the edge of the discs, with inner radii of r.sub.1 and r.sub.2, outer radii of R.sub.1 and R.sub.2, and thicknesses of h.sub.c1 and h.sub.c2, respectively. The number of grooves of a metal disc is N, and the duty ratio of the groove width to groove cycle is A. It should be noted that the material of the metal discs can be copper, gold, silver, etc, and two metal discs can be made of different materials. The nearest distance from edge to edge of the two metal discs is d. The material of the dielectric substrate is determined according to the permittivity parameter, such as Polytetrafluoroethylene (PTFE) F4BTMS220. The material permittivity of the dielectric substrate is e, while the length and thickness of the substrate are L and h.sub.d, respectively. The metal coating at the bottom of the dielectric substrate can be copper, gold, silver, etc, and the thickness of the metal coating is h.sub.b. In the embodiment, the above materials and parameters can be appropriately adjusted according to the application requirements. Also, it is necessary to ensure the structure of the metal discs on the dielectric substrate still supports the SLSP resonance modes after adjustment.

(13) In this embodiment, for the direction-finding device operating at 3.67 GHz, the two metal discs are all made of copper, the number of grooves is N=60, and the duty ratio is A=50% (i.e., groove width:non-groove width=1:1). The outer radii of SLSP1 and SLSP2 are R.sub.1=R.sub.2=R=12 mm, and thicknesses are h.sub.c1=h.sub.c2=h.sub.c=0.0175 mm. The inner radii of SLSP1 and SLSP2 are r.sub.1=6 mm and r.sub.2=6.2 mm, respectively, hence there is a resonance frequency detuning between the two SLSPs. And the distance between the two SLSPs is d=10 mm. The material of the dielectric substrate is PTFE F4BTMS220, with a permittivity =2.2, and the substrate is coated with copper. The length and thickness of the dielectric substrate are L=80 mm and h.sub.d=2 mm, and the thickness of the copper coating at the bottom is h.sub.b=0.0175 mm.

(14) FIG. 2 shows the transmission spectra and dipole-mode profile supported by SLSP1 and SLSP2. From the spectra of FIG. 2, the resonance peaks of the SLSP1 and SLSP2 with internal radii of 6 mm and 6.2 mm are .sub.1=3.655 GHz and .sub.2=3.685 GHz, respectively, existing a frequency detuning =0.03 GHz. The central resonance frequency of the SLSP1 and SLSP2 is .sub.0=(.sub.1+.sub.2)/2=3.67 GHz. Both two spoof surface plasmonic resonators support the dipole mode at resonance peaks.

(15) It should be noted that for incident waves of other frequencies, we can design the parameters of the two SLSP resonators, such as the inner radii, the outer radii, the thickness or the material of the substrate, to adjust the central resonance frequency .sub.0 to be consistent with the frequency of the incident waves. It provides a platform for direction-finding applications in different frequency bands. Taking the inner radius r as an example, FIG. 3 shows the spectral evolution of the SLSP resonator with different inner radii, which demonstrates that the resonance frequency of the SLSP resonator can be adjusted as the inner radius changes.

(16) As shown in FIG. 4, under the far-field incident waves from a horn antenna, the detected field intensity of the SLSP resonator is enhanced by about 33 times compared with that without SLSP resonators, thus greatly improving the direction-finding sensitivity.

(17) FIG. 5 shows the evolution of the phase difference between the SLSP1 and SLSP2 as the incident angle of incoming waves changes, for the direction-finding device with coupled and independent SLSP resonators, respectively. From FIG. 5, the phase differences increase monotonically with the incident angles. Compared with the direction-finding device with independent SLSP resonators, the detected phase difference of the direction-finding device with detuned and coupled SLSP resonators is obviously broadened, i.e., from 0 to 159.4. Therefore, it realizes the full-range direction finding with the incident angle of 0 90, and further improves the direction-finding sensitivity and accuracy.

(18) When in use, the direction-finding device is fixed first, and two identical probes are arranged at positions A and B (as shown in FIG. 1), which are connected to the signal processing circuit. Under the illumination of the incident waves, the two probes detect the electric fields of the two resonators at positions A and B as input to the signal processing circuit to calculate the phase difference. When incoming waves are incident from different directions, the phase difference between the two SLSP resonators evolves. Therefore, according to the phase difference, the incident angle of the incoming waves can be determined.

(19) It should be noted that the present disclosure is not limited to the specific structure described above and shown in the drawings, which means that appropriate modifications can be made based on the direction-finding mechanism stated above.