Fig. 1. (a) Lens for quasi-nondiffractive OAM waves, and the picture is quoted from Ref. [
11], (b) nondiffractive Bessel beam launcher, and the picture is quoted from Ref. [
21], (c) flat-top beam shaper, and the picture is quoted from Ref. [
12], (d) Luneburg lens, and the picture is quoted from Ref. [
22], (e) LP-CP converter, and the picture is quoted from Ref. [
24], (f) polarization beam splitter, and the picture is quoted from Ref. [
25]
![(a-ⅰ) 3-D near-field focus-scanning lens, (a-ⅱ) power densities on the three focal planes (S = 0.5, 4.5, and 8.5 mm) at 300 GHz by combining synchronous co-rotation and counter-rotation of the lenses, and the picture is quoted from Ref. [10], (b) multi-focus lens, and the picture is quoted from Ref. [43], (c-ⅰ) stretchable Fresnel flat zone plate, (c-ⅱ) Fresnel flat zone plate at stretching degrees of 0 and 21%, (c-ⅲ) E-field of the zone plate at stretching degrees of 0 and 21%, and the picture is quoted from Ref. [44], (d) two-layered cascaded discrete dielectric lens, and the picture is quoted from Ref. [17], (e-ⅰ) high numerical aperture metalens, (e-ⅱ) the schematic diagram of processing flow of metalens, and the picture is quoted from Ref. [45], (f) measurement setup of the time domain spectrometer , and the picture is quoted from Ref. [55], (g) measurement setup of the Field-effect transistors, and the picture is quoted from Ref. [18]](/richHtml/hwyhmb/2023/42/6/806/img_03.jpg)
Fig. 2. (a-ⅰ) 3-D near-field focus-scanning lens, (a-ⅱ) power densities on the three focal planes (S = 0.5, 4.5, and 8.5 mm) at 300 GHz by combining synchronous co-rotation and counter-rotation of the lenses, and the picture is quoted from Ref. [
10], (b) multi-focus lens, and the picture is quoted from Ref. [
43], (c-ⅰ) stretchable Fresnel flat zone plate, (c-ⅱ) Fresnel flat zone plate at stretching degrees of 0 and 21%, (c-ⅲ) E-field of the zone plate at stretching degrees of 0 and 21%, and the picture is quoted from Ref. [
44], (d) two-layered cascaded discrete dielectric lens, and the picture is quoted from Ref. [
17], (e-ⅰ) high numerical aperture metalens, (e-ⅱ) the schematic diagram of processing flow of metalens, and the picture is quoted from Ref. [
45], (f) measurement setup of the time domain spectrometer , and the picture is quoted from Ref. [
55], (g) measurement setup of the Field-effect transistors, and the picture is quoted from Ref. [
18]
Fig. 2. (a) Bullet shaped ceramic composite lens, and the picture is quoted from Ref. [
26], (b) hyperhemispherical Si lens, and the picture is quoted from Ref. [
27], (c) hemicylindrical PTFE lens
[16], (d) hemispherical TPX, and the picture is quoted from Ref. [
13], (e) cylindrical sapphire-fiber lens, and the picture is quoted from Ref. [
29], (f) 3D printed planar lens, and the picture is quoted from Ref. [
30]
参考文献 | 结构 | 技术 | 材料 | 工作频率 | 功能 |
---|
[11] | 离散介质 | 3D打印 | 聚乳酸 | 140 GHz | 产生偏转准非衍射OAM波 | [12] | 双曲面 | - | 聚四氟乙烯 | 100 GHz | 产生平顶波束 | [21] | 离散介质 | 3D打印 | 耐高温树脂 | 300 GHz | 发射非衍射贝塞尔波束 | [22] | 超半圆+圆柱 | 3D打印 | 金属+聚苯乙烯 | 130~180 GHz | 扫描和接收广角波束 | [24] | 离散介质 | 3D打印 | 耐高温树脂 | 300 GHz | 高增益线极化转圆极化 | [25] | 离散介质 | 3D打印 | 聚乳酸 | 140 GHz | 极化分束 |
|
Table 1. THz lens antennas for beam control in references
参考文献 | 形状 | 材料 | 工作频率 | 应用 |
---|
[13] | 半球形 | 聚甲基戊烯 | 220~320 GHz | CMOS 超宽带调频连续波雷达 | [16] | 半圆柱 | 聚四氟乙烯 | 280~330 GHz | 漏波天线 | [26] | 子弹形 | 氧化钼锂空心玻璃微珠陶瓷复合材料 | 220-330 GHz | - | [27] | 半球形 | 硅 | 670 GHz | 振荡器辐射源阵列 | [28] | 半球形 | 硅 | 100~600 GHz | 光导脉冲源 | [29] | 圆柱形 | 蓝宝石纤维 | - | 光导天线 | [30] | 平面超材料 | 聚合物和金属增材3D打印 | 140 GHz | 调频连续波雷达 |
|
Table 2. High gain THz lens antennas in references
参考文献 | 结构 | 材料 | 工作频率 | 功能 |
---|
[10] | 离散介质 | 耐高温树脂 | 300 GHz | 三维近场聚焦扫描 | [17] | 离散介质 | 耐高温树脂 | 300 GHz | 动态全息成像 | [18] | 商用曲面透镜 | 聚四氟乙烯 | 490~645 GHz | 准直、预聚焦 | [43] | C形槽超表面阵列 | 二氧化钒 | 800 GHz | 热可切换多聚焦 | [44] | 平面 | 可拉伸单壁碳纳米管薄膜 +可拉伸聚合物 | 0.3~1.2 THz | 径向拉伸变焦 | [45] | 超透镜 | 硅 | 30 THz | 成像 | [55] | 商用曲面透镜 | 聚甲基戊烯 | 0.25~1 THz | 准直 |
|
Table 3. THz lens antennas for focus and collimation