There are a lot of linear polarization (LP) light in nature, and many LP light are harmful in photography. They will introduce reflection light into the camera to reduce the clarity and bright-dark contrast of the photo. Polarizer can filter out these harmful LP light, making the color of the photo more saturated and clear. Ordinary cameras usually use a linear-polarizing lens and rotate it to reduce LP light incidence. However, there is still an ignorable remnant of LP light within camera, which still cause some harmful results. In some advanced cameras with auto focus (AF) and automatic exposure (AE), the residual LP light inside the camera will make AF invalid and AE inaccurate. In this case, camera has to depend on the circular-polarizing lens (CPL), which can directly convert the incident LP light into circular polarization (CP) light. For most optical devices, the CP light has no difference with the non-polarized light. Theoretically, the CPL can be used in any camera, including advanced terahertz (THz) camera. However, the preparation of the traditional CPL still depends on manual polishing and sanding, so that the CPL is expensive, low yields and generally large body that is difficult to integrate.

In recent years, researchers have devoted themselves to developing a novel polarization conversion device with lower cost, smaller size, higher integration degree and mutifunctions. Metamaterials/metasurfaces provide a good solution for these new devices^1-6. The THz CP conversion devices based on metasurfaces have been developed⁷. Further, to give full play to the advantages of the metasurfaces, the wavefront control devices combined with phase operation are realized, such as metalens^8-21. By arranging different structure units according to a certain phase distribution, the metalens can realize not only the focusing function similar to the traditional convex lens, but also the polarization conversion function^22-26. In general, THz metalens widely uses all-dielectric silicon (Si) material with transmission structure so as to meet the practical applications²⁷. If THz metalens can also achieve CP conversion, they can replace both traditional CPL and focus lens, and are used in advanced THz camera, further reducing the camera volume. A very important performance index is that metalens must perfectly convert incident LP light into single-handed CP light, which means the converted CP light can not contain both the left-handed and the right-handed. In the aspect of polarization conversion, the existing THz metalenses have realized the LP rotation^{22, 25}, but the polarization conversion of LP to single-handed CP is not realized. Using the chiral optics and the spin decoupling mechanisms to construct THz metalenses may obtain the conversion and focusing of LP to CP^28-30. However, the physical principles of these techniques involves the separation of left-handed circular polarization (LCP) and right-handed circular polarization (RCP) from incident LP, which does not allow the clean and efficient conversion of LP to single-handed CP. In other words, CP conversion in those THz metalenses contains both LCP and RCP components, and it is impossible to completely eliminate one CP but retain the opposite one. As a result, a part of LCP and RCP waves may combine into harmful LP waves again, so that those metalenses cannot still be applied in advanced THz camera.

The metalens must depend on several different structure units those phase can cover 0-2π. Traditionally, the principle of Pancharatnam-Berry (PB) phase is in whole or in part introduced in the phase design of the THz metalens, even for those THz metalenses containing chiral optics and spin decoupling mechanisms^28-30. For instance, the general operation is that several basic structures with different structural parameters are firstly designed to meet the phase change of 0-π, and then the phases of the remaining π-2π are obtained by rotating these structures at 90°. Assuming that a basic structure unit can realize the conversion of LP to single-handed CP, the helix of CP will be opposite direction after this structure being rotated by 90° due to the spin dependence of PB phase, which eventually results in the failure of conversion and focusing of LP to single-handed CP in whole metalens. Hence, these intrinsic shortcomings of PB phase in physical principle lead to that the THz metalens integrating the polarization conversion function of LP to single-handed CP has not been realized yet.

Meanwhile, the polarization conversion of the existing metalenses is usually not reversible. Although a LP THz wave through those metalenses is converted into other polarization states and focused, THz wave with other polarization states through those metalenses can no longer be converted into the original LP and focused. These shortcomings also limit the multifunctional applications of the THz metalens to some extent.

To overcome mentioned shortcomings in polarization conversion of the existing THz metalenses and expand their multifunctional applications, we designed an all-dielectric Si based THz metalens, which was assembled using dynamic phase (relating to the structural parameters of structure units) and getting rid of the PB phase (relating to rotation of structure units). Some new features appear and are described in Fig. 1. (i) The LP THz wave through metalens will be completely converted into a single-handed CP and then focused at a certain time. Next, we only need to rotate this metalens with ±45° and ±90° to achieve arbitrary switching among LP, LCP and RCP, as shown in Fig. 1(a-b). This feature shows it can be used in advanced THz camara, as a candidate to replace the group of traditional CPL and focusing lens. (ii) The polarization conversion is reversible, as shown in Fig. 1(c). When a single-handed CP THz wave passes through the metalens, it will be completely converted into LP and focused. Moreover, incident RCP and LCP correspond to two transmission LP waves which are always perpendicular to each other. When this property is used for polarization imaging, the incident RCP and LCP THz waves can be distinguished easily by monitoring transmission LP waves in the image plane, as shown in Fig. 1(d). The polarization imaging function may has a potential application in some fields such as chiral material studies.

The metalens model was built in commercial CST Microwave Studio software, and all numerical simulation results were obtained by time-domain solver. The simple silicon (Si) rectangular bar is used as basic structure to construct the metalens, and the structural parameters (height, length and width of Si rectangular bar) of units are selected from a large number of parameter scanning results. The metalens sample used high resistance Si wafer (conductivity δ<0.05 S m^–1) with 500 μm thickness, and was prepared using plasma etching method (ICP ion etching machine with SF₆ etching gas). The characterization system is shown as Fig. 2. A femtosecond laser outputs a 50 fs duration pulse with 800 nm central wavelength, and it goes through the beam splitter L1 to be separated into a probe beam and a pump beam. The slender pump beam reflected by the mirror L2 is firstly expanded via a concave lens L3 to cover enough the surface (1 cm × 1 cm) of <110> ZnTe crystal, and then induces optical rectification effects to radiate the linear polarization THz wave ³¹. Using a metallic parabolic mirror L4 collimate the THz beam before sample being irradiated by THz wave. THz wave through sample is received by a ZnTe detection crystal. At the same time, the slender probe beam is also expanded by a beam expanding system consisting of a series of lenses, and then adjust probe polarization through a half wave plate (HWP) and a polarizer. The probe beam will be reflected onto the detection crystal by the beam splitter L5. Subsequently, the received THz field excites Pockels effect in ZnTe detection crystal to modulate the polarization of probe beam. Then, the probe beam with polarization modulation through L5 is acquired by CCD camera to form eventually a THz image based on a balanced electro-optics detection technique³². This detection process is essentially the electro-optical sampling³³, and this system includes two convex lenses L6 and L7, a quarter wave plate (QWP) and a Wollaston prism (PBS). Besides, it is required to synchronously control the mechanical chopper and CCD camera for using a dynamics subtraction method to eliminate the background intensity of the probe beam.

The simple Si rectangular bar is used as basic structure to design metalens. Started by a feature that the incident x-LP THz wave through metalens is converted into LCP and focused, we discuss firstly the design process of metalens and then deduce other features.

At the first, let us see the polarization conversion property of a rectangular bar. After incident electric field through Si rectangular bar, the universal formation of transmission electric field is as follow:

1(ExtEyt)=(txxtxytyxtyy)(ExiEyi)=T(ExiEyi),

where Exi,Eyi are incident electric field at x-axis and y-axis, respectively, and Ext,Eyt are transmission electric field at x-axis and y-axis, respectively. T is the transfer Jones matrix and consists of transmission coefficients t_ab (a, b∈{x, y}, t_ab means the coefficient of transmission a-LP under incident b-LP). To obtain LCP conversion under incident x-LP wave (electric field vector (10)T), the initial site of Si rectangular bar is deduced to 45° deviated from x-axis, as shown in Fig. 3(a). The deduction process is shown in Section 1 of Supplementary Information in detail. The transmission LCP wave E0t and transfer Jones matrix T₀ is expressed as follow:

2T0=β(1−i−i1),

3E0t=T0(10)=β(1−i),

where β is a coefficient (see section S1). The Si substrate is h₁=300 μm, the height of Si bar is h₂=200 μm, and the side length of square unit cell is P=160 μm. An x-LP wave through this unit cell will split into a co-polarization component (T_x) and a cross-polarization component (T_y). The two transmission components (T_x and T_y) perpendicular to each other have a phase difference of π/2 and the same amplitude (about 0.5), which composes eventually a LCP wave. If the geometric parameters at length and width of Si bar are changed, which will obtain the phase variations of 0–2π. Five basic structures are found, and their shapes and parameters are as shown in Fig. 3(a). The phases (based on T_x) of five basic structures vary generally from 0 to 2π, as shown in Fig. 3(b). Further, using five basic structures to construct an array meeting phase profile in Eq. (4) can obtain THz metalens, as shown in Fig. 3(c).

4ϕ=2πλ(f−x2+y2+f2),

where the wavelength λ corresponds to 0.96 THz, (x, y) belongs to the coordinates of any point in this metalens with setting the origin point (0, 0) at center of metalens, and f=8 mm is the focal length of metalens. Meanwhile, to realize complete and stable LCP conversion, almost the same amplitude and stable phase difference of π/2 are required for two components (T_x and T_y) of every Si bar, as shown in Fig. 3(d–f).

Since the phase variations of 0–2π in metalens are achieved by changing structural parameters of Si bars and do not depend on rotation operation of Si bars, this is a dynamic phase assembled THz metalens. Obviously, if any PB phases is introduced in metalens (i.e., traditionally, the phase variations of 0–π in metalens are achieved by changing structural parameters of Si bars, but the phase variations of π–2π are got by 90° rotation operation of the existing Si bars), the polarization conversion of metalens will be complex so that the focusing with pure LCP conversion fails.

Next, we deduce other features of the THz metalens based on Jones matrix (Eq. (2)) of conversion from x-LP to LCP. When the metalens is rotated as a whole, with angles of θ=0°, 45°, 90°, 135°, respectively, every unit cell will be rotated correspondingly as shown in Fig. 4(a). Respectively, new transfer Jones matrices are deduced in Section 2 of Supplementary Information and shown as follows:

5For θ=45∘,T1=2β(1+i001−i).

6For θ=90∘/−90∘,T2=β(1ii1).

7For θ=135∘/−45∘,T3=2β(1−i001+i).

Correspondingly, the electric field of transmission waves under incident x-LP are expressed as:

8For θ=45∘,E1t=T1(10)=2β(1+i)(10).

9For θ=90∘/−90∘,E2t=T2(10)=β(1i).

10For θ=135∘/−45∘,E3t=T3(10)=2β(1−i)(10).

Equations (8) and (10) mean that when the metalens is rotated with ±45°, the transmission waves are still x-LP without polarization conversion. Also, five basic structures show almost the same transmission amplitude, as shown in Fig. 4(b, d). At this moment, the metalens will focus x-LP without polarization conversion. When the metalens is rotated with ±90°, formula (9) show that the transmission RCP conversion will appear. Obviously, the transmission amplitude of two components (T_x and T_y) are same as that before rotating metalens, but two components (T_x and T_y) will have a phase difference of Δφ=−π/2 as shown in Fig. 4(c), meaning the metalens will convert incident x-LP into RCP and then focus.

The above analyses indicate that we only need to rotate this metalens with ±90° to focus an incident x-LP with arbitrary single-handed CP conversion, respectively. In fact, it is easy to understand that arbitrary LP in x-o-y plane through metalens can also be focused with arbitrary single-handed CP conversion. For instance, if the incident LP has an angle ϕ to x-axis, we can rotate this metalens with an additional angle ϕ on basis of θ rotation angle. Then, this will have the same meaning as the above. Hence, the focusing and conversion of arbitrary LP to arbitrary single-handed CP can be obtained. Here, we can give their general forms. The incident LP with arbitrary direction in x-o-y plane can be obtained by rotating x-LP at an angle of ϕ, thus incident arbitrary LP wave EAi in x-o-y plane can be expressed via a base matrix H as follow:

11EAi=H(10)=(cosφ−sinφsinφcosφ)(10)=(cosφsinφ).

Further, the metalens should be rotated with an additional angle ϕ on basis of θ rotation angle, and new transfer Jones matrix is:

12Tn'=TnH−1=(cosφ−sinφsinφcosφ)Tn(cosφsinφ−sinφcosφ),n=0,1,2,3.

At this moment, this situation is equivalent to the an x-LP through the metalens without additional rotation angle ϕ. Eventually, the transmission electric field is expressed:

13Ent'=Tn'EAi=(cosφ−sinφsinφcosφ)Ent=HEnt,n=0,1,2,3.

It can be seen from formula (13) that the final transmission electric field Ent' is equivalent to rotating the previous transmission electric field Ent with an additional angle ϕ. The detailed deduction process for Eqs. (11–13) can be seen in Section 3 of Supplementary Information.

The SEM of original metalens is shown in Fig. 5(a). And Fig. 5(b) shows simulative and experimental results in focal plane for focusing and conversion of incident x-LP to transmission CP. In general, these experimental results are well agreement with the simulative results. The original metalens without any rotation (θ=0°) possesses a function of converting x-LP into pure LCP. When metalens is rotated at θ=±90°, x-LP to pure RCP conversion and focusing can be obtained. Further, if we want to keep x-LP focusing without polarization conversion, the metalens can be rotated at θ=±45°, as shown in Fig. 5(c). Overall, the metalens we designed has some practical values, including simple operation, high integration, and easily obtaining arbitrary single-handed CP.

The reversible polarization conversion is another characteristic of this metalens, that is, the metalens can convert not only incident LP into single-handed CP, but also incident single-handed CP into LP. For original metalens without any rotation (θ=0°), the incident RCP and LCP are transferred by Jones matrix T₀, and transmission fields Ent (n=4, 5) as follows:

14E4t=T0(1i)=β(1−i−i1)(1i)=2β(10).

15E5t=T0(1−i)=β(1−i−i1)(1−i)=−2β(01).

The above two formulas show that RCP through original metalens will be converted into an x-LP and focused, while LCP through this metalens will be converted into a y-axis LP (y-LP) and focused.

Further, we can rotate the metalens to change direction of transmission LP. Here, we have also deduced their general forms in Section 5 of Supplementary Information, and results are given as follows. Assuming that metalens is rotated with an angle θ, then RCP through metalens will be converted into a LP having an angle θ to x-axis with an additional phase shift θ, as shown in Fig. 6(a), and the general form is expressed as follow:

16E4t'=2βeiθ(cosθsinθ).

While LCP through metalens will be converted into a LP having an angle θ to y-axis with an additional phase shift (π/2−θ), as shown in Fig. 6(b), and the general form is expressed as follow:

17E5t'=−2βei(π2−θ)(−sinθcosθ).

In other words, to obtain conversion and focusing of arbitrary CP to arbitrary LP, we only need to rotate the metalens at a corresponding angle of target LP. Meanwhile, it is easy to understand that no matter how many angles the metalens rotates, the transmission LP waves corresponding to incident RCP and LCP are always perpendicular to each other. To verify the mentioned theory analyses, Fig. 6(c) shows simulative and experimental results for focusing and conversion of incident CP to transmission LP. Because the transmission LP before and after metalens rotation has a corresponding relationship, we only need to present the results in term of original metalens (θ=0°) here. It can be seen from Fig. 6(c) that the original metalens has the function of converting RCP into y-LP and converting LCP into x-LP, which verifies the mentioned theory analyses well.

The imaging results of THz focusing metalens are simulated. As long as a certain object-image relationship is satisfied, the ‘TJU’ pattern can be presented in image plane. As shown in Fig. 7(a), the object-image relationship is 1/f=1/u+1/v, where f=8 mm is focal length, and u=v=16 mm are object distance and image distance, respectively. We simulate firstly the CP imaging properties of metalens under incident x-LP, as shown Fig. 7(b). Due to LCP conversion, the original metalens possesses LCP imaging property well while there is no RCP imaging property. In contrast, since the RCP conversion appears as rotating metalens at ±90°, the metalens will present well RCP imaging property while there is no LCP imaging property. These results reveal that this metalens can be used in advanced THz camera, as a great candidate of traditional CP conversion and focusing device group.

In some fields, it is necessary to distinguish RCP and LCP. For instance, many natural and artificial materials such as chiral molecules can emit LCP wave (or induce LCP conversion), which are called left-handed materials, and vice versa are called right-handed materials. If the spin direction of these CP waves cannot be detected, the chiral properties of materials can not be distinguished. Here, this metalens we designed may provide a useful idea to distinguish LCP and RCP. It has been proposed in conversion and focusing of arbitrary single-handed CP to LP section that no matter how to rotate metalens, two transmission LP waves under incident RCP and LCP are always perpendicular to each other, which means two transmission LP waves have no overlapping components at all. Hence, incident RCP and LCP can be distinguished completely in polarization states by monitoring different transmission LP states. As shown in Fig. 7(c), the simulation show the original metalens under incident RCP can obtain x-LP imaging property well but no y-LP imaging property. Further, y-LP imaging property can be obtained under incident LCP, without any x-LP imaging property. These results indicate that this metalens may also be applied in polarization imaging field with LCP and RCP discrimination.

In this paper, to construct a metalens integrating single-handed CP conversion, an all-dielectric Si based THz metalens was designed using dynamic phase, without any PB phase. Simulative and experimental results show that LP THz wave through metalens can be converted into arbitrary single-handed CP THz wave and then focused. As a fixed incident x-LP, when this metalens is rotated with ±45° and ±90°, three transmission polarization states can be obtained, including LP without conversion, LCP and RCP. Meanwhile, the polarization conversion is reversible. The arbitrary single-handed CP THz wave through the metalens can also be converted into LP THz wave and then focused. Respectively, RCP and LCP through the metalens are converted into x-LP and y-LP. And no matter how many angles the metalens rotates, the corresponding two transmission LP waves under incident RCP and LCP are always perpendicular to each other. Further, the THz imaging properties of the metalens are also verified by simulation. Results show that the metalens can be expected to become a great candidate of CP conversion and focusing device in advanced THz camera. Moreover, the metalens can be used in polarization imaging field requiring LCP and RCP discrimination, such as chiral material studies, in which the incident RCP and LCP will be distinguished easily by monitoring transmission LP states in the image plane.