Ring-Core Photonic Crystal Fiber of Terahertz Orbital Angular Momentum Modes with Excellence Guiding Properties in Optical Fiber Communication

Abstract

The orbital angular momentum (OAM) of light is used for increasing the optical communication capacity in the mode division multiplexing (MDM) technique. A novel and simple structure of ring-core photonic crystal fiber (RC-PCF) is proposed in this paper. The ring core is doped by the Schott sulfur difluoride material and the cladding region is composed of fused silica with one layer of well-patterned air-holes. The guiding of Terahertz (THz) OAM beams with 58 OAM modes over 0.70 THz (0.20 THz–0.90 THz) frequency is supported by this proposed RC-PCF. The OAM modes are well-separated for their large refractive index difference above ${10}^{-4}$. The dispersion profile of each mode is varied in the range of 0.23–7.77 ps/THz/cm. The ultra-low confinement loss around ${10}^{-9}$ dB/cm and better mode purity up to 0.932 is achieved by this RC-PCF. For these good properties, the proposed fiber is a promising candidate to be applied in the THz OAM transmission systems with high feasibility and high capacity.

1. Introduction

Increasing the receptivity of optical fiber transmission links is an exigent task due to the swiftly growing necessity for information transmission capacity. For achieving communication capacity, the physical wave of the light beam—the frequency, wavelength, amplitude, phase, and polarization—has been used to convey information. This is done by using multiplexing techniques, such as polarization division multiplexing (PDM), wavelength division multiplexing (WDM), mode-division multiplexing (MDM), space division multiplexing (SDM) and some advanced modulation techniques [1,2,3]. The SDM exploits an unrecognized physical dimension space domain. This is the most plight, feasible, and effective way to enhance the capacity of the optical fiber link [4]. The orbital angular momentum (OAM) is one of the techniques of SDM, which has become a significant topic and also increases the applications field of optical communication [5,6], imaging [7], micro-manipulation [8], and quantum data technology [9,10]. Normally, OAM beams are linked with a helical front of $e^{\left(il\varphi \right)}$, where $\mathit{l}$ is an integer number named the topological charge, and $\varphi$ is the azimuthal angle. At present, OAM beams are generated by converting the Laguerre Gaussian beams [11], spiral plates [12], cylindrical lenses [13], and diffracted optical elements [14,15]. Nevertheless, by increasing the transmission distance, the OAM beams are slowly expanded in free space, which is exaggerated to their field of applications. Normally, step-index fibers [16,17], twisted fibers [18], grade index ring-based fibers [19], and fiber couplers [20] have been used to carry OAM states.

Nowadays, Terahertz (THz) systems are better for security inspection observation, imaging, and short-range ultra-bandwidth communication. The THz radiation is located between the microwave and infrared frequency, around 0.10 to 10 THz [21]. The OAM beams have scintillating, significant, and intriguing applications like optical microscopy, tweezing, and high-capacity optical transmission [22]. Recently, THz OAM has been a flourishing research topic concentrating on the spatial THz circulation generation [23,24,25,26]. It was found that doughnut-like OAM states are not very easy to start with the THz beams, which are linearly polarized from the THz source because of mode mismatch. Nonetheless, until now, the propagation of THz OAM is rarely analyzed and discussed but it has a great potential for a robust and stable THz transmission system depending on the OAM multiplexing technique.

For increasing the massive growth of information capacity, a huge number of OAM supported PCFs have been numerically analyzed and proposed at the optical communication waveband around 1550 nm [27]. The OAM supported optical fiber with a high indexed material doped ring is very advantageous because the OAM beams and the wave propagating region are doughnut-shaped [16]. Moreover, all solid step-indexed THz-supported PCFs are more challenging because the main problem is lacking transparent materials for the THz wave-guides. For the range of the THz spectrum, dry air is a more transparent and available medium. Many hollow-core THz wave demonstrators have been proposed, analyzed, and experimentally investigated such as all-dielectric wave-guides [28], metal-wire embedded dielectric wave-guides [29], and dielectric coated metallic wave-guides [30]. The most familiar guiding technique among these is the anti-resonant reflecting optical waveguide (ARROW) with a leaky behavior. The operating frequencies of ARROW with extreme loss regions are controlled through the thickness and refractive indices of the high indexed layer [31], whereas anti-resonant frequency sections are used for achieving low loss circulation. The ARROW technique with a hollow-core THz wave-guide is one of the best approaches to achieve a relatively low loss at the THz regime [32,33,34]. In 2016, J. Yang et al. [35] proposed and designed a hollow core Kagome PCF for THz wave-guide with a propagation loss of 0.002 cm${}^{-1}$ at 0.75 THz. In the same year, M. R. Hasan et al. [36] designed and analyzed a porous-core spiral PCF with confinement loss ${10}^{-3}$ dB/cm for THz wave guidance. Besides, OAM transmission with a large number of OAM states, low confinement loss, smooth dispersion variation, and better OAM quality are also considered. For developing those parameters of the PCF, some unique types of PCFs have been proposed and discussed before, such as the spiral PCF [37], circular PCF [38], chain PCF [39], quasi-crystal fiber [40], ring-based PCFs [41,42,43,44], and so forth. The ring-based material doped PCF is one of them for better quality and properties with efficient OAM transmission with fabrication possibilities. In 2019, H. Zhang et al. [41] designed a ring-core-based Erbium-doped circular PCF supporting 14 OAM modes. In 2020, M. F. Israk et al. [42] proposed, designed, and investigated a Schott sulfur Di-fluoride $\left(S{F}_2\right)$ doped ring based coil-shaped circular PCF supporting 56 OAM states with ultra-low confinement loss (1.7407 ×${10}^{-9}$ dB/cm) and smooth dispersion variation. Besides, S. H. Huang et al. [43] also designed a micro-structured high-indexed material doped (Schott $S{F}_2$ and phosphate glass) ring-based PCF with low confinement loss and a minimum dispersion variation of 2.92416 ps/nm/km at $H{E}_{31,1}$ mode. They also discussed the fabrication possibilities of high indexed ring based fiber and enabled support of 146 and 70 OAM modes for different materials. In addition, few of the essential parameters of optical communication are also discussed in that work. Recently, W. Wang et al. [44] proposed a dual guided Schott $S{F}_6$ doped ring-core based PCF with Schott LLF1 (very light flint) background material supporting 56 OAM modes and 4 LP modes with low crosstalk and confinement loss lower than 5 ×${10}^{-8}$ dB/m. Moreover, the THz-based OAM transmission is has rarely been discussed. In 2016, H. Li et al. [21] proposed a hollow core Kagome PCF for guiding THz OAM beams by following the ARROW-type THz waveguide. They analyzed the fiber characteristics over 0.20 THz to 0.90 THz for 2 groups of OAM modes with a confinement loss of around ${10}^{-3}$ dB/cm and OAM purity values beyond 0.90. A tabular and descriptive view is shown in

Table 1. THz guiding and material doped ring-core orbital angular momentum (OAM) fibers based on photonic crystal fiber (PCF) structures.

Year	Author	Lattice	Material	Number of OAM Modes	Operating Bandwidth	Reference
2016	H. Li et al.	Kagome	Polymer	3	700 GHz	[21]
2019	H. Zhang et al.	Circular	Erbium	14	560 nm	[41]
2020	M. F. Israk et al.	Coil	Schott $S{F}_2$	56	1900 nm	[42]
2019	S. H. Huang et al.	Circular	Schott $S{F}_2$ & phosphate glass	146 and 70	900 nm	[43]
2020	W. Wang et al.	Circular	Schott $S{F}_6$	56 + 4	300 nm	[44]

for some THz guiding and material doped ring-core OAM fibers based on PCF structures. So, from the above discussion, it can be said that we need to devise a new type of fiber for supporting THz OAM transmission with more performance analyses.

In this paper, we designed a light-guiding Schott $S{F}_2$ doped ring-based photonic crystal fiber for supporting Terahertz orbital angular momentum over a wide frequency range of 0.20–0.90 THz. The proposed circular PCF supported 58 OAM states. The PCF design and algorithm of the proposed PCF are represented in Section 2. The simulation results and discussion of the parameters are given in Section 3. The fabrication possibilities of the proposed PCF are discussed in Section 4. Finally, the conclusion is briefly summarized in Section 5.

2. PCF Design and Algorithm

Combining the benefits of the THz wave guidance and OAM transmission, we have designed a circular ring-core PCF (RC-PCF), supporting a large number of OAM modes, ultra-low confinement loss, flat dispersion, and better OAM quality in a broad THz frequency range. The cross-section of the proposed RC-PCF and the corresponding physical notation with description is shown in Figure 1a,b, respectively, with a list of size parameters, where $r_0$ and $r_1$ are the inner and outer radii of the light-guiding ring-core, respectively, and $t_1$ and $t_2$ are the thickness of the ring-core and perfectly matched layer (PML), respectively. The ∧ d are the pitch distance of air holes and the diameter of the air hole, respectively, and the ratio between them is the relative air diameter (d/∧). The PML is used outside the computation domain. The thickness of the PML $t_2$ is around 9% of the whole radius of the cross-section of the fiber. The $\rho$ is named as the ratio of the circular radii of ring-core and expressed through $r_0$/$r_1$. By changing this ratio, the number of the supported OAM modes and the quality of the OAM modes are varied. This ratio is used for measuring and comparing the OAM purity for different vector modes that are discussed later. The PCF is composed of a ring-core and a well-ordered layer of an air hole. The light-guiding and mode beam-bearing ring are doped through a high indexed material of Schott $S{F}_2$ with refractive index 1.62 [44] at 1550 nm wavelength. This high indexed ring-core contributes to the well-separated eigenmodes, although there are various types of glass material like LASF and SF11 for doping the light guiding path. But, for the high refractive index and relatively rough dispersion, these are not used for doping. On the other hand, $S{F}_2$ is better for dispersion and internal transmission, which was proved in References [42,43]. Besides, the background material of the proposed RC-PCF is fused silica with a relatively lower refractive index than Schott $S{F}_2$ of 1.446 [45]. The air holes outside the ring-core distribute the refractive index through the whole section of the fiber, which is favorable for tuning the wave-guide dispersion [46]. Since the THz OAM is a new concept of multiplexing system OAM in optical communication, so the structure of a fiber can be simple.

The proposed RC-PCF is designed and simulated through the COMSOL Multiphysics cross-platform software. For all the simulation results, except OAM purity, the values of the ratio of annular radii of ring-core and relative air diameter are fixed and these are $\rho$ = 0.71 and d/∧ = 0.83. For increasing the number of OAM modes, the radius of the inner diameter ($r_0$) of the proposed fiber is fixed at 0.45 mm. The simulation of the proposed PCF is done by the full-vector finite element method (FEM). The FEM and PML are used to calculate effective refractive indices for vector modes and electromagnetic mode field distributions. There are many methods for calculating the numerical values of PCF such as the plane wave, the supercell lattice method, the finite difference time domain method, and so forth. Nonetheless, FEM is a method for solving a partial differential equation with high precision. It also can combine multiple disciplines, such as mechanics, chemistry, acoustics, and optics. There are widespread application fields of FEM such as vehicle design, ship design and architectural structure. The effective refractive index, ring-core and total wave guiding power are calculated through the FEM method for the proposed PCF. The key steps are as follows—modeling the PCF geometry and doping material, select the values of $\rho$ and d/∧ considering the support of OAM transmission in the THz range frequency, select the operating frequency band, set the definitions and electromagnetic boundary conditions, pattern analysis, grid division, and setting expressions for derived values of global evaluations.

A large number of OAM modes ensure high capacity and secure data transmission. The OAM has become a robust multiplexing technique because of a huge number of OAM modes. For the proposed fiber, the supported OAM modes are expressed as $OA{M}_{\pm l,m}^{\pm }$ and they can be presented through $H{E}_{l+1,m}$ and $E{H}_{l-1,m}$. All the supported OAM and eigenmodes are mathematically expressed through the following Equations (1) and (2) [42].

$$\left\{\begin{array}{c}OA{M}_{\pm l,m}^{\pm }=H{E}_{l+1,m}^{even}\pm jH{E}_{l+1,m}^{odd}\\ OA{M}_{\pm l,m}^{\mp }=E{H}_{l-1,m}^{even}\pm jE{H}_{l-1,m}^{odd}\end{array}\right\};(l>1),$$

(1)

$$\left\{\begin{array}{c}OA{M}_{\pm l,m}^{\pm }=H{E}_{2,m}^{even}\pm jH{E}_{2,m}^{odd}\\ OA{M}_{\pm l,m}^{\mp }=T{M}_{0,m}\pm jT{E}_{0,m}\end{array}\right\};(l=1).$$

(2)

Here, the superscript ‘±’ is denoted as the polarization direction of spin angular momentum. From the above formulas, it can be seen that the rotation direction of HE modes with the direction of spin angular momentum, while the EH modes follow the opposite rotation direction [47,48]. Besides, even and odd modes are obtained after the $\pi$/2 phase shift and ‘±l’ denotes the rotation direction of the wavefront. The radial orders with m > 1 are not considered because of their disturbance in multiplexing and demultiplexing of OAM modes [44], thus we considered only m equal to 1. By following Equations (1) and (2), the 58 OAM and eigenmodes are supported through the proposed RC-PCF over the whole supported frequency band. These are – $OA{M}_{\pm 1,1}^{\pm }$$\left(H{E}_{2,1}\right)$, $OA{M}_{\pm 2,1}^{\pm }$$(H{E}_{3,1},E{H}_{1,1})$, $OA{M}_{\pm 3,1}^{\pm }$$(H{E}_{4,1},E{H}_{2,1})$, $OA{M}_{\pm 4,1}^{\pm }$$(H{E}_{5,1},E{H}_{3,1})$, $OA{M}_{\pm 5,1}^{\pm }$$(H{E}_{6,1},E{H}_{4,1})$, $OA{M}_{\pm 6,1}^{\pm }$$(H{E}_{7,1},E{H}_{5,1})$, $OA{M}_{\pm 7,1}^{\pm }$$(H{E}_{8,1},E{H}_{6,1})$, $OA{M}_{\pm 8,1}^{\pm }$$(H{E}_{9,1},E{H}_{7,1})$, $OA{M}_{\pm 9,1}^{\pm }$$(H{E}_{10,1},E{H}_{8,1})$, $OA{M}_{\pm 10,1}^{\pm }$$(H{E}_{11,1},E{H}_{9,1})$, $OA{M}_{\pm 11,1}^{\pm }$$(H{E}_{12,1},E{H}_{10,1})$, $OA{M}_{\pm 12,1}^{\pm }$$(H{E}_{13,1},E{H}_{11,1})$, $OA{M}_{\pm 13,1}^{\pm }$$(H{E}_{14,1},$$E{H}_{12,1})$, $OA{M}_{\pm 14,1}^{\pm }$$(H{E}_{15,1},E{H}_{13,1})$, $OA{M}_{\pm 15,1}^{\pm }$$(H{E}_{16,1},E{H}_{14,1})$.

All the supported OAM modes show a well limited intensity and phase distribution in the annular region. A well-structured mode field distribution is better for the OAM multiplexing technique. The intensity distribution of $H{E}_{1,1}$, $E{H}_{4,1}$, $H{E}_{9,1}$, $H{E}_{12,1}$, $H{E}_{16,1}$, $T{M}_{0,1}$, $T{E}_{0,1}$, and phase distributions of $H{E}_{4,1}$, $E{H}_{5,1}$, $H{E}_{10,1}$ are presented in Figure 2.

For enhancing the performance of the proposed PCF, we have discussed and analyzed some significant parameters of THz OAM transmission in a wide frequency band over 0.20 THz to 0.90 THz. The effective refractive index (ERI), effective refractive index difference (ERID), dispersion profile, confinement loss (CL) and OAM purity are numerically discussed and analyzed in this paper. The ERID of a group of OAM modes is always greater than ${10}^{-4}$. It is denoted through $\Delta n_{eff}$ and calculated by Equation (3) [48,49].

$$\Delta n_{eff}=|n_{ef{f}_{H{E}_{l+1,m}}}-n_{ef{f}_{E{H}_{l-1,m}}}|>{10}^{-4}.$$

(3)

The dispersion profile in the frequency domain is denoted by ${\beta }_2$ and evaluated through Equation (4) [50].

$$D=\frac{2}{c}\frac{d{n}_{eff}}{d\omega }+\frac{\omega }{c}\frac{d^2\left[n_{eff}\right]}{d{\omega }^2}[ps/THz/cm].$$

(4)

Here, $\omega$ is the radian frequency and the ps/THz/cm is the unit of dispersion measurement. The calculation of the CL is done by Equation (5) [51].

$$CL=\frac{4\pi f}{c}Im\left(n_{eff}\right)(dB/m)=4.187\times {10}^4\times Im\left(n_{eff}\right)(dB/cm).$$

(5)

Here, f and c are the operating frequency and speed of light in a vacuum. The Im($n_{eff}$) is a very small value, which is the imaginary part of the refractive index. The OAM purity of the proposed RC-PCF is calculated through Equation (6) [42].

$$\eta =\frac{I_r}{I_c}=\frac{{\int \int }_{rings}{\left|\overrightarrow{E}\right|}^{2}dxdy}{{\int \int }_{cross-section}{\left|\overrightarrow{E}\right|}^{2}dxdy}.$$

(6)

Here, $I_r$ is the normal mode of the ring area and $I_c$ is the intensity of the average mode in the total cross-view of the proposed PCF.

3. Simulation Results and Discussions

By following the previously discussed algorithm, the proposed ring-core fiber is simulated. The simulation results show a significant optical performance with supporting 58 OAM modes, good separation between eigenmodes, smooth dispersion profile, ultra-low confinement loss and better OAM quality. The properties of THz OAM transmission, like effective refractive index, effective refractive index difference, dispersion profile, confinement loss and OAM purity, are calculated, discussed and analyzed with necessary curves and applications. The THz OAM guiding fiber is large in structure, so the effective refractive area is high. Thus, the related parameters of the effective area are neglected in the simulation results and calculations section.

3.1. Effective Refractive Index

By following Equations (1) and (2), the effective refractive index of every OAM eigenmode is equivalent to the corresponding even and odd vector modes and these are dependent on the operating frequency. To evaluate the modal effective refractive index ($n_{e}ff$) of the proposed fiber, numerical simulations and calculations are done by the finite element solver, where a PML is accomplished adjacent to the cladding. The eigenmodes of $T{E}_{0,1}$, $T{M}_{0,1}$ and all of the supported HE modes are shown in Figure 3, besides all of the EH modes are shown in Figure 4. From both figures, the higher order of OAM modes is clearly represented, showing a lower refractive index, and by increasing the operating frequency, the refractive index is increased. It is known that resonant frequency is ascertained by the optical and geometrical characteristics of the first high-index layer. For guiding the THz OAM transmissions, in Reference [21], two resonant frequencies (0.45 THz and 0.88 THz) are used and analyzed as well as some OAM parameters within a certain frequency of 0.20 THz to 0.90 THz. In this proposed PCF, the refractive index of all the supported modes is calculated over ranges from 0.20 THz to 0.90 THz. The refractive index of all vector modes is between the cladding refractive index (1.446) and the light guiding refractive index (1.62). The dispersion characteristics (in Figure 6) are calculated by using the refractive index.

3.2. Effective Refractive Index Difference

Figure 5 shows the relationship between refractive index differences among all of the supported OAM groups and terahertz frequency. By using Equations (1) and (2), the groups are determined at the same topological charge of l. The difference is calculated through Equation (3) and the difference must be above ${10}^{-4}$. The large difference of OAM modes is confirmed, and that adjacent vector modes cannott couple with linear polarization (LP) over the supported frequency band. From Figure 5, it is noticed that the effective refractive index differences are gently decreased by increasing terahertz frequency and a higher-order group of OAM modes shows a higher value of differences. Most of the groups show a difference above ${10}^{-3}$ and some of them show ${10}^{-2}$ at 200 GHz and 300 GHz. Thus, the proposed PCF is reduced to the crosstalk threshold. The highest effective refractive index difference of 1.7606 × ${10}^{-2}$ is gained at 200 GHz frequency for |$H{E}_{16,1}$–$E{H}_{14,1}$|. This effective performance is obtained for the proposed well-designed PCF structure. So, it can be said that the proposed RC-PCF not only decreased the eigenmodes coupling with LP modes but also sustained the transmission with a single mode in the radial direction. For PCF guiding of OAM modes, large effective refractive index difference ($\Delta n_{eff}$) between near-degenerate eigenmodes (normally > ${10}^{-4}$) is highly suitable for long-haul optical transmissions [27].

3.3. Dispersion

Dispersion is an important property for THz OAM transmissions. It plays an important role to determine the transmission distance in optical fiber communication systems. It befell for the outpouring of light beams at the time of light propagation through fiber. Normally, there are two types of dispersion including material dispersion and waveguide dispersion. Material dispersion is not discussed here, because it is fixed and dependent on the material which is used for fiber design. On the other hand, the waveguide dispersion can be varied by changing operating wavelength or frequency. It is also adjusted by changing the shape of air holes, the spacing of air holes, the number of air holes, and the arrangements of air holes. For the proposed RC-PCF, we have calculated the dispersion by following Equation (4). Then, the evaluated values are plotted in Figure 6 over a broad range of operating frequencies of about 0.20 THz to 0.70 THz. In Equation (4), the dispersion is calculated by differentiating the refractive index in the second order with respect to frequency. The dispersion for the last two operating frequencies (0.80 THz and 0.90 THz) is neglected for its second-order derivation.

From Figure 6, it can be said that dispersion properties are softly decreased by increasing operating frequency and the lower order of OAM modes shows lower dispersion. The dispersion profile (Figure 6) shows an inverse characteristic with an effective refractive index (Figure 3 and Figure 4). The dispersion for all of the eigenmodes is varied from 0.23 ps/THz/cm to 7.77 ps/THz/cm. Dispersion variation is another important parameter for optical communication. It is calculated by determining the absolute difference between two end values of dispersion in the supported operating frequency. Maximum vector modes show a flattened dispersion profile. Besides, the lower dispersion variation is gained for the flattened dispersion. Some lower dispersion variations of 0.8881 ps/THz/cm, 0.9354 ps/THz/cm, 1.0049 ps/THz/cm, 1.0885 ps/THz/cm, 1.1735 ps/THz/cm are obtained for $T{E}_{0,1}$, $E{H}_{1,1}$, $E{H}_{2,1}$, $H{E}_{2,1}$, $H{E}_{3,1}$ modes. A comparative view for dispersion variation for this PCF and some prior PCFs are shown in

Table 2. Comparison of some THz OAM parameters of the operating bandwidth range, supported OAM modes, the lowest confinement loss, and the lowest dispersion variation for the proposed PCF with some prior PCFs.

Reference	Operating Bandwidth Range	Supported OAM Modes	The Lowest Confinement Loss (dB/cm)	The Lowest Dispersion Variation
[21]	0.20–0.90 THz	3	≈${10}^{-3}$	-
[37]	1.30–2.00 $\mathsf{\mu }$m	14	5.095 × ${10}^{-1}$	10.35 ps/km/nm
[38]	1.25–2.00 $\mathsf{\mu }$m	>42	9.52 × ${10}^{-7}$	-
[39]	1.20–1.95 $\mathsf{\mu }$m	26	3.19 × ${10}^{-8}$	3.8684 ps/km/nm
[42]	0.60–2.50 $\mathsf{\mu }$m	56	1.74 × ${10}^{-9}$	36.907 ps/km/nm
[43]	1.10–2.00 $\mathsf{\mu }$m	146	-	2.92 ps/km/nm
[44]	1.52–1.58 $\mathsf{\mu }$m	30	≈${10}^{-10}$	-
[48]	0.80–2.00 $\mathsf{\mu }$m	42	1.131 × ${10}^{-8}$	3.7980 ps/km/nm
[52]	1.40–1.70 $\mathsf{\mu }$m	56	<4.91 × ${10}^{-6}$	-
[53]	1.25–1.81 $\mathsf{\mu }$m	14	3.434 × ${10}^{-7}$	<46.38 ps/km/nm
[54]	0.80–1.80 $\mathsf{\mu }$m	26	1.030 × ${10}^{-8}$	7.8337 ps/km/nm
[55]	1.00–2.00 $\mathsf{\mu }$m	38	1.534 × ${10}^{-7}$	0.916 ps/km/nm
This work	0.20–0.90 THz	58	6.91 × ${10}^{-9}$	0.8881 ps/THz/cm

. The lower order of the vector modes obtained a lower dispersion variation because lower modes are confined to the light smoothly and outpoured the light slightly for the proposed RC-PCF. In Reference [43], the dispersion variation is greater than this proposed work although this work is investigated under the frequency domain. The RC-PCF is used in the multichannel communication link for its flattened dispersion profile. If the fiber shows a flattened dispersion profile, then multiple signals from the source reached the destination approximately simultaneously [50].

3.4. Confinement Loss

Confinement is the light restricting capability at the core of the PCF. Confinement loss (CL) has occurred for the structural imperfections of the fiber structure. Then it is incited through the interior components of the beam [48]. It is a harmful parameter for optical fiber communication. So, we need it to be as low as possible. For the well-structured PCF and the well-patterned air holes layer, the CL became very low. The CL was evaluated through Equation (5). The calculation of the CL is dependent on the unreal part of the effective refractive index, which is very low for the proposed PCF. It is also dependent on the size of the air holes, layers of the air holes, operating frequency, and the guiding mechanism of the fiber. The calculated values of CL for some of the vector modes of $H{E}_{1,1}$, $H{E}_{2,1}$, $E{H}_{5,1}$, $H{E}_{7,1}$, $E{H}_{10,1}$, $H{E}_{13,1}$, $H{E}_{16,1}$ are shown in Figure 7 with respect to operating frequency, ranging from 200 GHz to 900 GHz.

From Figure 7, it is indisputably shown demonstrated that CL for all modes is between 6.91 × ${10}^{-9}$ dB/cm to 8.21 × ${10}^{-9}$ dB/cm. The average CL of the proposed fiber is comparatively lower than the similarly designed fiber in Reference [43]. These ultra-low values of CL for the proposed PCF are attained for the high indexed material doped mode beam-bearing ring-core and well-patterned large air cavities. The lowest values of CL are obtained for the $H{E}_{1,1}$ mode. The robust transmission of optical communication and OAM transmission is ensured by this type of relatively lower confinement loss. A comparative view for dispersion variation, confinement loss, supported OAM modes for this PCF and some prior PCFs are shown in Table 2.

3.5. OAM Purity

OAM purity is one of the most important parameters for OAM transmissions. The OAM mode purity relates to how light beams are confined in the ring core of the fiber. When a fiber is supported by more numbers of OAM modes, then we should get attention on the purity or quality of OAM modes of this fiber because the high purity of modes ensures the stable transmission of fiber [38]. Mode quality depends on the number of vector modes, the width of ring core, pattern of air-holes, and layer numbers of air-holes. We have determined the values of mode purity for some of the vector modes with respect to the ratio of the annular radii of the ring core ($\rho$) and the relative air-hole diameter (d/∧) of the proposed RC-PCF. The inner diameter is fixed in Figure 1 for the increment of supported modes, so the outer diameter can change for determining mode purity. We also varied the relative air-hole diameter at the cladding region to evaluate the values of mode purity. It is evaluated through Equation (6).

The graphical representation of OAM purity for some vector modes is shown in Figure 8 with varying structural parameters. Here, two cases are presented with three phases for each case. Firstly, the annular radii of ring-core ($\rho$) are fixed at 0.71 and the relative air diameter (d/∧) is varied at 0.83, 0.78, and 0.73. Then, the relative air diameter (d/∧) is fixed at 0.83 and the annular radii of the ring-core ($\rho$) are varied at 0.68, 0.65, and 0.62. In these two cases, the values of $\rho$ and d/∧ are fixed at 0.71 and 0.83, respectively, in two cases, because these values are fixed at the proposed PCF for analyzing the other parameters of the OAM transmission. In Figure 8, it is plainly shown that the values of OAM purity vary from 0.9320 to 0.9599. This high value of OAM purity ensures the robust transmission of optical communication. All the above-discussed parameters with numerical values are summarized in

Table 3. Summary of key parameters for the proposed RC-PCF.

Key Parameters	Numerical Values
Number of Supported OAM modes	58
Operating Bandwidth	0.20–0.90 THz
Effective refractive index difference	>${10}^{-4}$
Dispersion	0.23–7.77 ps/THz/cm
Confinement Loss	6.91 × ${10}^{-9}$–8.21 × ${10}^{-9}$ dB/cm
OAM Purity	0.9320–0.9599

.

The simulation results and discussion section show some effective properties for THz OAM transmissions. Table 2 shows the confinement loss, dispersion variation and number of supported vector modes, which are better than the previously discussed fibers. The summary of Table 3 for the proposed PCF shows fruitful and feasible properties in the first time of THz OAM transmission with a simple and unique structure of the fiber. A circular design of a micro-structure ring-core fiber is designed and discussed by Huang et al. [43] in 2019. They just discussed some basic wavelength-based parameters of optical communication with the output of relatively high confinement loss and high dispersion. But, in the proposed work, some more special and essential parameters in optical communication are analyzed. Extremely low confinement loss, lower dispersion profile, and high OAM purity are obtained in a more bandwidth ranged THz domain. The main limitations of the proposed fiber are a limited number of OAM modes and a less concentrated light beam. Thus, it can be disclosed that the submitted PCF in the THz frequency band is the robust candidate for THz OAM transmissions and high-reliability optical fiber communication.

4. Fabrication Possibility

The proposed structure in Figure 1 is a robust candidate for guiding THz OAM transmissions. The summaries of characteristics for the proposed RC-PCF neatly show that the PCF maintained a better efficiency and ultra-feasible parameters. Thus, we have to discuss the fabrication procedure of this fiber. In Figure 1, it is displayed that in the cladding region there is a layer of air holes with 12 large air holes. The layer of the air hole is symmetrically patterned. A single layer of a circular air-hole can be easy to fabricate. Since the THz OAM is a new concept in optical communication, the simplicity of a fiber is not a big deal. Besides, the cladding region is doped by the fused silica with a refractive index of 1.446. Any kind of fused silica-based PCF structures can be fabricated by using a method—the ‘sol-gel’ method—which was proposed and analyzed by El et al. [56] in 2012. The proposed fiber has a very simple air holes pattern. Any type of fiber shape can be fabricated and the freedom to organize air-hole size, shape, and spacing are provided through this ‘sol-gel’ method. Nonetheless, the proposed fiber has a ring-core with a highly refractive index based material—Schott Sulfur Di-fluoride ($S{F}_2$)—with a refractive index of 1.62. This doped area is named the mode-covered ring-core region. The fabrication procedure has become complex for this material doped ring-core. Nowadays, the ring-core-based PCF of OAM transmission is common. Previously, highly indexed doped ring-core-based fibers are proposed and analyzed in References [41,42,43,44,57]. A material doped ring-core OAM transmission supported PCF is designed, analyzed and fabricated by C. Brunet et al. [57] in 2014. Consequently, in 2019, a micro-structure ring-core fiber is designed and the fabrication technique is discussed by Huang et al. [43]. The ring-core of this fiber is doped through the high indexed material of Phosphate glass and Schott sulfur di-fluoride with supporting 70 OAM modes. Moreover, the above-mentioned ring-core fibers of Reference [43] are followed by a fabrication method, which is discussed herein step by step. Firstly, the preform of the ring-core PCF is composed through the modified chemical vapor deposition (MCVD) [58] process. Then, they instrumentally and mechanically punched the preform or extrudes the preform through custom dyes to generate the piece of fiber [59]. At last, the preforms are compressed and drawn into the fiber. Then, these are put into a furnace at a suitable temperature. So, the proposed RC-PCF can be fabricated by following these processes. The proposed fiber is advantageous for guiding THz OAM with the multi-mode and wide-band transmission.

5. Conclusions

In conclusion, a ring-core circular photonic crystal fiber is proposed and analyzed in this paper. The ring core is doped by Schott $S{F}_2$ material. This PCF supports 58 OAM modes in a broad THz frequency spectrum from 0.20 THz to 0.90 THz. The supported OAM modes of the proposed PCF are well-separated for their unique design and high refractive index difference up to ${10}^{-4}$. The confinement loss is ultra-low for its ring-core and large air holes. The lowest confinement loss is 6.91 ×${10}^{-9}$ dB/cm. Moreover, the flat dispersion and smooth dispersion variation are obtained for this PCF. The lowest dispersion variation is 0.8881 ps/THz/cm. Besides, the supported modes of this fiber are well confined and the highest mode purity is 0.9599. By developing the manufacturing technique day by day, the proposed PCF can be fabricated successfully and applied in the THz OAM transmission. By evaluating the performances of the proposed fiber, it is a promising candidate for optical communications, especially in the fields of encoding, multiplexing, demultiplexing, sensing, supercontinuum generation, long-haul, and dense-capacity optical fiber transmissions, and other fields of applications.