Open access peer-reviewed chapter

OAM Modes in Optical Fibers for Next Generation Space Division Multiplexing (SDM) Systems

By Alaaeddine Rjeb, Habib Fathallah and Mohsen Machhout

Submitted: April 10th 2021Reviewed: April 18th 2021Published: November 24th 2021

DOI: 10.5772/intechopen.97773

Downloaded: 48

Abstract

Due to the renewed demand on data bandwidth imposed by the upcoming capacity crunch, optical communication (research and industry) community has oriented their effort to space division multiplexing (SDM) and particularly to mode division multiplexing (MDM). This is based on separate/independent and orthogonal spatial modes of optical fiber as data carriers along optical fiber. Orbital Angular Momentum (OAM) is one of the variants of MDM that showed promising features including the efficient enhancement of capacity transmission from Tbit to Pbit and substantial improvement of spectral efficiency up to hundreds (bs-1 Hz-1). In this chapter, we review the potentials of harnessing SDM as a promising solution for next generation global communications systems. We focus on different SDM approaches and we address specifically the MDM (different modes in optical fiber). Finally, we highlight the recent main works and achievements that have been conducted (in last decade) in OAM-MDM over optical fibers. We focus on main R&D activities incorporating specialty fibers that have been proposed, designed and demonstrating in order to handle appropriates OAM modes.

Keywords

  • Space Division Multiplexing (SDM)
  • Mode Division Multiplexing (MDM)
  • Orbital Angular Momentum (OAM)
  • Specialty optical fibers

1. Introduction

Bandwidth-hungry applications and services, such as HDTV, big data, quantum computing, 5G/6G communication, industry 4.0 and game streaming, in addition to the exponential increase of users and connected devices (Internet of Things: IOT), may cause a capacity crunch in near future [1, 2, 3]. While other physical limitations behind the capacity crunch are based on the nonlinear Shannon limit and the scalability of actually deployed devices. The cited emerging applications (i.e. paradigms) has pushed telecommunications community (researchers & industries) to grow through multiple stages by developing higher capacity optical networks in optical fiber based links targeting to deal with the evolution of the market need for telecoms and Internet data services and paving the road to surpass the upcoming capacity limit challenges [4].

Recently, the capacity and the spectral efficiency of optical fibers have been substantially improved (i.e. scaling by several orders of magnitude) by using different multiplexing techniques and advanced optical modulation formats. These multiplexing techniques are based on the exploitation of degrees of freedom of the optical signal to encode data information. The time, as time division multiplexing (TDM: interleaving channels temporally), the polarization, Polarization division multiplexing (PDM), the wavelength, as wavelength division multiplexing (WDM: using multiple wavelength channels) and the phase (quadrature) are examples of such techniques [5].

Research and industrial community had recently oriented their effort towards Space Division Multiplexing (SDM) techniques that is based on the exploitation of the spatial structure of the light or the physical transmission medium to encode information. Simply, SDM consists of increasing the number of data channels available inside an optical fiber. Two attractive embodiments of SDM are core division multiplexing (CDM) and mode division multiplexing (MDM) [6]. CDM is simply considered as the increasing of parallel single mode cores, carrying information, embedded in the same cladding of optical fiber (known as multicore fiber MCF) or single core fibers bundles [7]. Mode division multiplexing (MDM) is based on excitation and propagation of several spatial optical modes as individual/separate/independent data channels within common physical transmission medium targeting to boost the capacity transmission [8]. MDM is realized by multimode fibers generally over short haul interconnect transmission or few mode fibers as transmission medium for long haul transmission link. Numerous mode basis have been used for mode division multiplexing showing its effectiveness to scale up from Terabit to Petabit the capacity transmission and unleash from dozen to hundred (bit/s/Hz) the spectral efficiency over optical fiber.

It is well known that light can carry Angular Momentum (AM) that expresses the amount of dynamical rotation present in the electromagnetic field representing the light. The AM of light beam is divided into two distinct forms of rotation: Spin Angular Momentum (SAM) and Orbital Angular Momentum (OAM) [9]. The SAM is related to the polarization of light (e.g. right or left in circular polarization) while the OAM is related to the spiral phase front of exp. (jlφ) where l is a topological charge number (arbitrary unlimited integer), and φ is the azimuthal angle. Orbital angular momentum (OAM) of light, (known as twisted light), an additional degree of freedom, is arguably one of the most promising approaches that has recently deserved a special attention in optical fiber networks. Benefiting from two inherent features, which are:

(1) The orthogonality: where as a definition two signals are orthogonal, if data sent in these two dimensions can be uniquely separated from one another at the receiver without affecting each other’s detection performance. Two OAM modes with different charge number l do not interfere.

(2) The unlimitleness: the charge number l is theoretically infinite. Hence, Each OAM mode (each specifically l) is an independent data channels. OAM modes has been harnessed in multiplexing/de-multiplexing (OAM-MDM) or in increasing the overall optical channel capacity [10, 11].

As any promising technology, OAM-MDM through optical fibers is facing several key challenges, and lots crucial issues that it is of great importance to handle with it in order to truly realize the full potential of this technique and to paving the road to a robust transmission operation with raised performances in future communication systems.

In strict sense ‘Mode division multiplexing’, means that the modes (channels) are separate and should remain uncoupled and not interfere with each other (i.e. orthogonal). Hence, mode coupling (e.g. channels crosstalk) is the major obstacle for OAM-MDM. Channels crosstalk is obviated by either fiber design or multiple input multiple output digital signal processing (MIMO DSP) [9, 10, 11].

By carefully manipulating the fiber design parameters, it is possible to supervise the interactions between propagated modes and even control which modal basis is incorporated: LP-fibers where the separation between vector modes are inferior to 1 × 10–4, or OAM-fibers where the intermodal separation exceeds 1 × 10–4, since either LP or OAM modes are constructed from fiber eigenmodes themselves [9]. This better facilitates understanding each fiber parameter impact and smooth the way of transition from design stage to fabrication process. Adding to that, exploit MIMO DSP is considered as the extreme choice to decipher channels at the receiving stage since it is heavy and complex. Its complexity is came from its direct proportionality to the transmission distance and to the number of modes. This allow it to become impractical in real time and threats the scalability of MDM in next generation optical communication system. For OAM-MDM systems using optical fibers, the fiber design stage is considered as the most crucial part and there is still a lot of opportunities for improved designs. New fiber designs for OAM mode transmission over short/medium and longer distances or among higher number of modes or possess a high performance metrics have been proposed and examined.

With the different related key challenges, this chapter offers a review of the state-of-the-art of SDM advances especially on OAM-MDM over optical fibers. In the first section, we discuss the SDM approaches as a solution to the expected capacity limit. The different mode basis supported in optical fibers are presented and discussed as either cylindrical vector modes, LP modes or OAM modes. The second section acts as a survey on recent advances (over last ten years) in OAM-MDM over optical fibers. We review the research effort invested in harnessing OAM as a degree of freedom to carry data in optical fiber networks. We summarized the key obtained results in the main family of optical fibers (i.e. conventional fibers and OAM specialty fibers) using OAM modes.

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2. SDM over optical fibers

Space division multiplexing (SDM) has attracted high interest. It has revealed multiple directions of exploration and development. SDM consists of exploiting space-independent communication channels in both guided waves (e.g. optical fibers) or free space optical link (FSO). The channels’ type vary depending in which factor of SDM we are exploiting; diversified cores, multiplexed LP modes or modes carrying OAM, multiple cores each supporting few multiplexed LP modes and so on.

Two main subset in SDM could be explored: core division multiplexing (CDM) where information is transmitted through cores (or fibers) of multicore fibers or mode division multiplexing (MDM), where information is transmitted through propagating modes of few or multimode fibers.

2.1 Core division multiplexing (CDM)

In principle, two main schemes are used. The first is based on the use of Single-core Fiber bundle (i.e. fiber ribbon) where parallels single mode fibers are packed together creating a fiber bundle or ribbon cable. The overall diameter of these bundles varies from around 10 mm to 27 mm. Fiber bundles deliver up to hundreds of parallel links. Fiber bundles have been commercially available [12, 13] and deployed in current optical infrastructure for several years already. Fiber bundles are also commercially used in conjunction with several SDM transceiver technologies [14].

The second scheme is based on carrying data on single cores (each core supports single mode) embedded in the same fiber known as Multicore Fibers (MCFs). Hence, each core is considered as an independent single channel (Figure 1). The most important constraint in MCFs is the inter-core crosstalk (XT) caused by signal power leakage from core to its adjacent cores that is controlled by core pitch (distance between adjacent cores denoted usually as ʌ) [15]. There are in Principle, two main categories of MCF: weakly coupled MCFs (=uncoupled MCF) and strongly coupled MCFs (=coupled MCF) depending on the value of a coupling coefficient ‘K’ (used to characterize the intercore crosstalk) [16, 17, 18]. Using the so-called supermodes to carry data, the crosstalk in coupled MCF must be mitigated by complex digital signal processing algorithms, such as multiple-input multiple-output digital signal processing (MIMO-DSP) techniques [19]. On the contrary, due to low XT in uncoupled MCF, it is not necessary to mitigate the XT impacts via complex MIMO. In principle, three crosstalk suppression schemes in uncoupled MCF could be incorporated, which are trench-assisted structure, heterogeneous core arrangement, and propagation-direction interleaving (PDI) technique [7].

Figure 1.

SDM through MCF.

The first paper on communication using MCF demonstrate a transmission of 112-Tb/s over 76.8 km in a 7-cores fiber using SDM and dense WDM in the C + L ITU-T bands. The spectral efficiency was of 14 b/s/Hz [20]. The second paper [21] shows an ultra-low crosstalk level (≤ − 55 dB over 17.6 km), which presents the lowest crosstalk between neighboring cores value to date. Other reported works, show high capacity (1.01Pb/s) [22] over 52 km single span of 12- core MCF. In [23], over 7326 km, a record of 140.7 Tb/s capacity are reached.

2.2 Mode division multiplexing (MDM)

Carrying data on optical fiber modes known as mode division multiplexing. In that scenario, each propagating mode is considered as independent channel [5, 24]. Two types of fiber are dedicated to support that strategy. One is based on the use of multimode fibers (MMF) while the second exploits the known few-mode fibers (FMF). The main difference between both is the number of modes (available channels). Since MMF can support large number of modes (tens), the intermodal crosstalk becomes large as well as the differential mode group delay (DMGD), where each mode has its own velocity, reducing the number of propagating modes along the fiber becomes viable solution. This supports FMF as a viable candidate for realizing SDM [5]. The concept of mode division multiplexing over a few/multi-mode fiber is illustrated in Figure 2.

Figure 2.

The concept of mode division multiplexing over a FMF/MMF.

Other kinds of optical fiber that can be used in MDM such as photonic crystal fibers (PCFs). Based on the properties of photonic crystals, PCF confines light by band gap effects, using air holes in their cross-sections, or by a conventional higher-index core modified by the presence of air holes. The PCF is built of one material (SiO2, As2S3, Polymers, etc), and air holes are introduced in the area surrounding the core providing the change of the refractive index contrast between the core and the cladding. The transposition of air holes laid to form a hexagonal or circular lattice. Figure 3 recapitalizes the principle SDM approaches over optical fibers [25].

Figure 3.

Different approaches for SDM over optical fibers.

2.3 Guided modes of optical fibers

We look into the different modal basis that can be supported by optical fibers. Like all electromagnetic phenomena, the propagation of optical fields along optical fiber is governed by Maxwell’s equations. Several modal basis can describe the propagation in optical fibers. In this chapter, fiber guided modes that we will meet are vector modes (i.e. fiber eigenmodes), linear polarized modes (i.e. LP modes) and orbital angular momentum modes (i.e. OAM modes). In the following, we provide general notions including mathematical expressions of modes of each mode basis.

2.3.1 Cylindrical vector modes

In the absence of the current in the medium, Maxwell equations are reduced to two homogeneous vector wave equations given by the following expressions [26]:

2+k2n2E=E.lnn2E1
2+k2n2H=×H×lnn2E2

Where Eand Hare the electric and magnetic field respectively and n is the refractive index profile function. If we apply the boundary conditions according to the geometry and fiber refractive index, we get eigenvalues equation. Each solution of that equation is guided mode known by effective index neff. In cylindrical coordinates, for example, the electrical and magnetic fields are expressed as:

E=rEr+ϕEϕ+zEzexpjβzjωtH=rHr+ϕHϕ+rHzexpjβzjωtE3

Where Er, Hr are radial components, Eϕ and Hϕ are azimuthal components. r, ϕand zare unitary vectors. β = 2πneffis the propagation constant of guided mode, ω = 2πc/λ = kcis the pulsation; λ and c are the wavelength and light velocity both in vacuum, respectively. Guided modes in circularly symmetrical optical fiber are denoted as transverse electric (TE0,m) or transverse magnetic modes (TM0,m), if Ez = 0 or Hz = 0 respectively. Other kind of modes are HEν,m and EHν,m those where Ez ≠ 0 or Hz ≠ 0 (transverse components) are noted as hybrid modes. The designation HEν,mstands for a hybrid mode for which Hz is dominant compared to Ez, while for EHν,m, Ez is dominant compared to Hz. The indexes νand mare the azimuthal and radial indices. νis related to the number of symmetry axes in the azimuthal dependency of the fields, and mis related to the number of zeros in the radial dependency of the fields.

Because of the circular symmetry, the field must keep the same value after a full 2π azimuthal rotation, thus, the components Ez and Hz have a dependency according to cos(νϕ)or sin(νϕ).hence, in circularly symmetrical optical fiber, hybrid modes are composed by two modes: one evenwhile the other is odd. In the even mode, the radials components (Er) and azimuthal component (Hϕ)are with cos(νϕ)(i.e. Ox symmetry). The components Eϕ and Hr have dependency according to sin(νϕ)(i.e. Oy symmetry). The radial, azimuthal and longitudinal electrical field components of even and odd modes are given by the following expressions:

Ereven=errcosνϕEϕeven=eϕrsinνϕEzeven=ezrcosνϕE4
Erodd=errsinνϕEϕodd=eϕrcosνϕEzodd=ezrsinνϕE5

The modes HEν,meven/odd,HEν,meven/odd,TE0,mandTM0,mare usually denoted as vector modes, cylindrical vector modes or fiber eigenmodes.

2.3.2 Scalar modes: LP modes

Frequently, the refractive index difference between core and cladding in optical fiber is very small (ncore ≈ ncladding). We are then under the weakly guiding condition, and some approximations can be applied. The term “∇ln n2” is neglected in expression 1. The wave equation becomes scalar. The resulted modes are linearly polarized designated usually as LPlm modes. LP modes are quasi-TEM guided modes, and have negligible Ezand Hzcomponents. Therefore, they only have one component in the E field and one component in the H field (by convention, either Ex and Hy, or Ey and Hx in cartesien coordinates). This is why we call them scalar modes. The even modes are with cos(lϕ), while odd modes are varies with sin (lϕ). lis the azimuthal number while m has the same definition as in vector modes [26].The electric field components of even and odd modes (after variable separation: radial and azimuthal) are given by the next expressions:

Exeven=exrcosE6
Eyeven=eyrcosE7
Exodd=exrsinE8
Eyodd=eyrsinE9

Practically, the LP modes come from linear combination between cylindrical vector modes. The correspondence between the linearly polarized modes and the conventional cylindrical vector modes is shown below (Table 1).

Cylindrical vector modesLP modesCylindrical vector modesLP modes
HE1moddLP0myHE2mevenTM0mLP0meveny
HE1mevenLP0mxHEl+1modd+EHl1moddLPlmoddx
HE2modd+TE0mLP1moddxHEl+1moddEHl1moddLPlmoddy
HE2moddTE0mLP1moddyHEl+1meven+EHl1mevenLPlmevenx
HE2meven+TM0mLP0mevenxHEl+1mevenEHl1mevenLPlmeveny

Table 1.

The correspondence between LP modes and the CV modes.

2.3.3 OAM modes

Optical fiber can support OAM modes by correctly superposing the even and odd modes for each HEl,mand EHl,mvector mode with ± (π/2) phase shift [27, 28]. Taking into consideration the circular polarization of OAM states (spin); OAM modes are denoted as OAM±l,m±where ± superscript describes the spin angular momentum (circular polarization), l and m subscript denote the azimuthal and radial indices respectively. lis the topological number (number of twist in intensity profile), mdescribes the number of nulls radially (rings) in the intensity profile of the OAM mode. The magnitude of SAM equal ±sħwhere s = +1(left) or s = −1(right). The magnitude of OAM equals ±lħ. The total angular momentum AM is the sum of SAM and OAM with a magnitude of (±l ± s) ħ.

For the TM0,mand TE0,mmodes, the combination between them with a ± (π/2) phase shift, carries the same magnitude of SAM and OAM but with opposite sign, making the total angular momentum equal to zero. This mode is not stable and cannot propagate, because the propagation constants of TE0,mand TM0,mmodes are different. Therefore, we call this an unstable vortex. OAM modes made from HE1,mmodes would have a spin, but no topological charge (l = 0). Therefore, this is not a true OAM mode, but simply a vector mode with circular polarization. However, we will consider it as OAM0,m, in a more general definition.

OAM modes made from HEl,mmodes are rotating in the same direction as the spin (aligned spin-orbit modes), and OAM modes made from EHl,mmodes are rotating in the opposite direction as the spin (anti-aligned spin-orbit modes). If we take an even and an odd mode, with a π/2phase difference, and we sum the fields (expressions 1.5 and 1.6), we can get as a resulting field:

Er=errexp±jνϕEϕ=jeϕrexp±jνϕEz=ezrexp±jνϕE10

The synthetic formula are as given in the following expressions

HEl+1,meven±i×HEl+1,modd=OAM±l,mL/REHl1,meven±i×EHl1,modd=OAM±l,mR/LTM0m±jTE0m=OAM1m±E11

To summarize, for a given topological charge l, there are four possible OAMmodes: two different spin rotation, and two different phase rotation. This is illustrated in Figure 4. The only exceptions are for OAM±1,m, where spin and topological charge always have the same sign, and for OAM0,m, where there is no topological charge (only spin) [28].

Figure 4.

The four OAM mode degeneracies (reproduced from [28]).

Moreover, others OAM construction formulas are explored based on two spatially orthogonal linear polarized (LP) modes owning orthogonal polarization directions (with a ± π/2 phase shift) which can be obtained by solving the scalar version of Maxwell equation (the scalar Helmholtz (wave) equation) under the weakly guiding approximation [29]. The LP-OAM synthetic formula are as follows:

LPlmax±iLPlmbxLPlmay±iLPlmby=Fl,mr.xOAM±l,myOAM±l,mE12

where xand yare the linear polarization along the x-axis and y-axis respectively, Fl,mris the radial field distribution. The difference between OAMmodes generated from fiber vector modes (CV-OAM) possess circular polarization while those generated from LP modes (LP-OAM) are the linear polarization (has no SAM).

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3. OAM-MDM through optical fibers

OAM has seen application in optical communication due to the theoretically unprecedented quantities of data that can be modulated, multiplexed, transmitted and demultiplexed through either free space link (FSO as Free Space Optics), or optical fibers. Optical communications has exploited the physical dimension of optical signal to encode and transmit individual/separate/independent data stream through the same transmission medium (optical fiber or FSO). Since, the OAM is linked to the spatial phase distribution of light beam, it has been included under the space dimension as a subset or embodiment of SDM (space division multiplexing). In addition, since OAM is independent of wavelength, quadrature, and polarization, it provides an additional dimension for encoding information [30, 31]. The interest on OAM in communication (including optical, radio, underwater) has grown dramatically. Figure 5(a) and (b), which highlights the number of published papers (conferences paper, books, journal papers and patents), translates that huge interest. In Figure 5(a), we plot the number of published papers dealing with OAM in optical communication in last decade while Figure 5(b) shows the number of papers dealing with OAM in optical fibers, both are according to Google Scholar.

Figure 5.

Number of papers published dealing with (a) OAM in optical communication over ten years (ranging from 2011 to 2020), (b) OAM in optical fibers over the same period (according to Google scholar).

The worldwide backbone of high-capacity wired communications is optical fiber. The uses of OAM basis in optical fiber was a challenge to communication community. For a long time, optical fibers were only used for the generation or the transformation of OAM modes, and not for supporting their transmission [32]. The notion of transmitting OAM modes was demonstrated (theoretically, numerically, and experimentally) through conventional optical fibers (classical deployed fibers), or specialty fibers that have been specifically designed to transmit robust OAM modes. In the following, we present kinds of optical fibers based on the consideration of their refractive indexes, (e.g. graded, step, ring, etc.), geometrical features (MMF, SMF, and FMF etc.) and transmission caracteristics (MDM, CDM, PCF, kind of appropriate modes, etc.) and so on. We highlight the main design and principles results achievements.

3.1 Conventional fibers

Two examples of conventional optical fibers are multimode fiber MMF (e.g. OM1, OM2, OM3, OM4) where generally their refractive index are graded (GIF) and single mode fiber (e.g.G652) where the profile is step index (SMF). Conventional MMFs have large cores that are usually approximately 50 μm and can support hundreds of modes. Due to severe inter-modal dispersion limitations, MMF were replaced by single mode fibers (SMFs) that have a relatively small core radius (not exceeding 10 μm). The refractive indexes of both fibers (OM3, and G652 defined by ITU-T) are depicted in Figure 6(a) and (b).

Figure 6.

Refractive indexes of (a) graded index fiber (multimode fiber) and (b) step index fiber (single mode fiber).

The most commonly used modal basis for fibers are LP modes. LP modes are not exact fiber modes, and can be simply viewed as combinations of fiber eigenmodes transverse (TE, TM, HE and EH) as indicated above.

Other type of fibers are few mode fibers (FMF) which consist of an improved version of MMF. They support a limited number of modes, as one of the key components for SDM for optical networks. The first paper that mentioned the possibility of transmitting OAM modes through optical fiber is from Alexeyev et al. in 1998 [33]. The authors demonstrated that the solution for OAM modes could exist in optical fibers (MMF). Considering the propagation of OAM modes through the cited fibers, the analysis of OAM in conventional graded index multimode fiber was reported (theoretically and numerically) [34]. In that paper, Chen and his co-authors presented a comprehensive analysis of the ten-OAM modes groups supported in OM3, including mode coupling, chromatic dispersion, differential group delay, effective mode area and nonlinearities.

Later on, the same team demonstrated experimentally the transmission of four-OAM mode group in OM3 MMF using mode exciting and filtering elements at the 2-fiber extremity. Moreover, they demonstrated two OAM mode groups transmission over 2.6-km MMF with low crosstalk free of MIMO-DSP [35]. In 2018, Wang et al. reported the successful transmission of OAM modes over 8.8-km OM4 MMF [36]. Wang and co-workers demonstrates a 120-Gbit/s quadrature phase-shift keying (QPSK) signal transmission over 8.8-km OM 4 MMF with 2 × 2 and 4 × 4 MIMO-DSP. In second stage, they demonstrate the data-carrying two OAM mode groups (6 OAM states) multiplexing transmission over 8.8 km MMF without MIMO equalization.

The OAM in SMF (ITU-T G.652) was investigated, in [37]. The investigation was performed over 3 visible wavelengths (red at 632.8 nm, green at 532 nm, and blue at 476.5 nm) when G.652 becomes a few mode fiber. The synthetized OAM modes was investigated through effective mode area, nonlinearity, tolerance to fiber ellipticity and bending. The authors analyzed and estimated the fiber attenuation and bandwidth/capacity for OAM modes over six levels of wavelengths.

Few mode fibers (FMFs) with classical refractive index profile (step/graded), was used to transmit OAM modes. The transmission of OAM modes over FMF required a MIMO-DSP in combination with coherent detection to equalize the intermodal crosstalk. It was demonstrated in [38] the transmission of four OAM beams over 5-km FMF. Each transmitted OAM state carrying 20 Gbits/s QPSK data. MIMO DSP was used to mitigate the mode coupling effects. A graded index few mode fiber has been designed in [39] in order to support 10 OAM orders with high purity (≥ 99.9%) enabling low intermodal crosstalk (≤-30 dB). Later, in [40] Wang et al. demonstrated the viability of OAM modes transmission over both 50-km and 10-km FMFs. By adopting LDPC codes, the DMD and mode coupling was improved. In [41], Zhu et al. proposed and demonstrated a heterogeneous OAM based fiber by splicing 2 FMFs and MMF (OM3). Over 2 OAM modes, Zhu and co-workers transmit 20-Gbit/s QPSK data without MIMO-DSP. Recently, we proposed a family of graded index few mode fibers (four fibers) that supports 12 OAM states [42]. The evaluated differential group delay (DGD) and OAM purity demonstrate the viability of proposed fibers for short/medium haul connections.

3.2 OAM specialty fibers

OAM has changed the common features of optical fiber design guidelines. Cutting with the often-classical notion for imposing the center core to be the highest index of refractive (graded & step). In addition, the improvement of optical fibers fabrication technologies (materials & schemes) has made the fibers characterization no more challenging. New optical fibers with complicated shapes and high refractive index contrast have been experimentally characterized (demonstrated). The Modified Chemical Vapor Deposition (MCVD) is in principle one of the most fiber fabrication method that has been extensively used.

3.2.1 OAM-fibers recommendations and design guidelines

Mainly three common features between OAM specialty fibers are identified. The first consists of the high contrast between core and cladding refractive indexes (jumps/contrasts) increasing the mode effective indices separation (∆neff), hence enabling low induced crosstalk. The same feature involves the formation of OAM modes from cylindrical vector modes and avoid them to couple into LP modes. It is proved that minimum ∆neff of 10−4 is enough to keep robust OAM modes. This key value guarantees the minimum interaction between channels and prevents mode coupling inducing channels crosstalk XT. It has been demonstrated that through MCVD, a contrast of 0.14 is achievable with GeO2-SiO2 composition [43]. The second is about the refractive index profile that matches the donut shape of intensity profile of OAM mode (Ring shape: Figure 7). Thus, the Ring shaped (known also as depressed core fibers) has been extensively designed in OAM context instead of solid core fibers. Finally, the interfaces between fiber core and cladding preferred to be smoothed (instead of step (abrupt variation)) in order to eliminate the spin-orbit-coupling inducing OAM mode purity impairment and intrinsic crosstalk.

Figure 7.

OAM mode (a) phases pattern (e.g. OAM4,1), (b) normalized intensity, (c) fiber cross-section with ring shape.

3.2.2 Vortex fibers (VFs)

The first specialty FMF designed for OAM modes is vortex fiber [44]. The designed fiber possess a good separation between co-propagating modes. Vortex fiber was first introduced to create cylindrical vector beams represented by TE0,1and TM0,1modes (also known as polarization vortices). Proposed by Ramachandran and al., Vortex fiber has a central core able to transmit the fundamental mode, surrounded by a lower trench, and an outer ring able to transmit the first OAM mode group. In first experience, they reported a transmission through more than 20 m fiber. Two years later, transmission of OAM through a 1 km fiber was reported [45, 46, 47, 48, 49]. Figure 8 reported an optical microscope image of the end facet of the vortex fiber and the numerically calculated properties of the vortex fiber. All the experiments on OAM modes on the designed vortex fiber were summarized in [48].

Figure 8.

(a) Optical microscope image of vortex fiber, (b) numerically calculated properties [48].

3.2.3 Air Core fibers (ACFs)

Air core fiber (ACF) was proposed in [50]. 12 OAM modes were transmitted through 2 m of the fabricated ACF. Later on, 2 OAM modes were transmitted over 1 km of the fiber [51]. Among the main contributions, the authors demonstrated that OAM modes with higher l value are less sensitive to perturbations like bends and twists [52].

Within ROAM (revolution orbital angular momentum) project (EU H2020), Laval University (COPL) proposed and fabricated an ACF that achieved the record of OAM modes transmitted through an optical fiber. Benefiting from the high refractive index contrast (air/silica), the fabricated fiber supports the transmission of 36 OAM states [53]. Figure 9 shows the refractive index of ACF. Nevertheless, the designed fiber possess a very high loss (up to few dBs per meters) which make it unsuitable for communication. Recently, 10.56 Tbit/s has been demonstrated over 1.2 km ACF, without MIMO DSP, by carrying data over 12 OAM modes combined with wavelength division multiplexing (WDM) [54]. Latest air core ring fiber is designed to support more than 1000 OAM modes (using As2S3 as ring material) across wide wavelength band covering S, O, E, S, C, and L Bands [55].

Figure 9.

Refractive index profile of an air (hollow) core fiber (ACF).

3.2.4 Inverse parabolic graded index fibers (IPGIFs)

Ung et al. proposed the inverse parabolic graded index FMF (IPGIF) to support OAM modes [56, 57]. The refractive index of IPGIF is given by the following expression:

nr=n2(12NΔr2a20racoren3racladdingE13

Where a, n1, n2, n3 are the core radius, the refractive index at the core cladding interfaces, the refractive index at the core center and the refractive index of the cladding, respectively. The parameter N controls the shape of the IPGF. The refractive index of IPGF is presented in Figure 10. Based on a first-order perturbations, the authors highlighted the factors (refractive index, core radius and curvature shape) that directly related to enhance the intermodal separation in proposed IPGIF. Large refractive index gradient, high transverse field amplitude and large field variation are reasons of high intermodal separation enabling low crosstalk.

Figure 10.

Refractive index profile of inverse parabolic graded index fiber (IPGIF).

The designed IPG-FMF possess a good effective indices separation (∆neff > 2.1 × 10−4) between its supported vector modes, and the transmission of eight OAM states (OAM±0,1, OAM±1,1 and OAM±2,1) was demonstrated over 1 mwhich makes IPGIF suitable for short distances MDM transmission. On the other hand, the transmission of OAM±1,1 over more than 1 km was demonstrated by experiment, which makes the novel fiber as a promising candidate for long-distance OAM based MDM multiplexing system. Later on (2017), the multiplexing/transmission and demultiplexing of 3.36 Tbits/s was demonstrated over 10-meters inverse parabolic graded index fiber by using four OAM modes and 15 wavelengths (WDM) [58].

3.2.5 Ring Core fibers (RCFs)

Due to the emerging interest in OAM-guiding fibers, already designed fiber for LP modes was investigated through OAM. The Ring core fiber (RCF), which has been introduced to minimize the differential group delay between LP modes, was tailored to support and transmit OAM modes. This interest on ring core fiber come from its refractive index profile that closely matches the annular intensity profile of OAM beams (Figure 11). C. Brunet et al. present an analytic tool to solve the vector version of Maxwell equations in RCF [59]. A fully vectorial description was reported in order to better tailor the RCF to OAM context. Using the modal map developed in [59], the group designed and manufactured a family of RCF (five fibers) suitable for OAM transmission [60]. In [61] S. Ramachandran et al. demonstrated the stability of OAM modes in RCF.

Figure 11.

Examples of RCF refractive index profiles: (a) RCF (higher center) (b) RCF (lower center) and (c) RCF,a1anda2are inner and outer core radius respectively.

Recently, an RCF supported 50 OAM states divided into 13 mode groups (MGs) has been numerically investigated using small MIMO DSP blocks [62]. Experimentally, the transmission of two OAM mode-group is demonstrated over a 50 km ring core fiber without the use of MIMO DSP [63]. Emerging papers considering the design of RCFs and the propagation demonstration of OAM modes through it that we should mentions [64, 65].

3.2.6 Graded index ring Core fibers (GI-RCFs)

The ring notion touched the graded shape and a family of graded index ring core fibers (GI-RCF) has been proposed, designed and fabricated to support OAM mode group. Figure 12 shows the refractive index of GI-RCF. In [66], Zhu and co-workers designed and fabricated the GI-RCF for OAM modes. The fiber supports 22 OAM modes with low insertion loss (less than 1 dB/km). The crosstalk between the highest order mode groups is less than 14 dB after10-km propagation. With such fiber, a successful transmission of 32 Gbaud QPSk-data overall 80 channels is experimentally demonstrated. A transmission capacity of 5.12 Tbits/s and a spectral efficiency of 9 bit/s/Hz, over 10 km propagation was reported [67].

Figure 12.

Design of the GIRCF.

The second demonstration was performed over 18-km propagation. Recently, the same group demonstrate the transmission of 12 Gbaud (8QAM) over 224 channels (2 OAM × 112 wavelengths). A transmission capacity of 8.4 Tbits/s was achieved without MIMO DSP because of the large high-order mode group separation of the OAM fiber [68].

To increase even further the capacity of the fiber link, OAM transmission was reported over uncoupled multi core fibers. While a complete review on this topic exceed the scope of this chapter, we can nevertheless mention some contributions. Li and Wang designed seven-ring core fiber (MOMRF) supporting 154 data-channels in total (22 modes× 7 rings) [69]. The proposed fiber featuring low-level inter-ring crosstalk (−30 dB for a 100-km-long fiber) and intermodal crosstalk over a wide wavelength range (1520–1580 nm). Later, in [70], Li and Wang proposed a compact trench multi OAM ring fiber (TA-MOMRF) with 19 rings each supporting 22 modes (18 OAM states). The authors stated that such fiber is suitable for long distance OAM transmission enabling Pbit/s total transmission capacity and hundreds bit/s/Hz spectral efficiency. In [71], the authors proposed a coupled multi core fibers to support OAM modes (multi-orbital-angular-momentum (OAM) multicore supermode fiber (MOMCSF). The designed supermode fiber show favorable performance of low mode coupling, low nonlinearity, and low modal dependent loss.

3.2.7 Inverse raised cosine few mode fibers (IRC-FMFs)

Using IPGI fiber as a benchmark, we proposed a novel fiber that is based on inverse raised cosine function (IRCF). The standard raised cosine function (RCF) when applied to a wideband signal steeply removes the high out-of-band signals, making the filtered signal highly purified. Moreover, RCF is used in the same context because it eliminates intersymbol interference [72]. The IRCF profile is given by the following expression [73]:

nr=n2if0ra1α2Core12n2n31+cosπa×αra1α2ifa1α2ra1+α2Coren3ifra1+α2CladdingE14

where ais the core radius, n1 and n2 are respectively the maximum and the minimum refractive indices of the core, n3 is the refractive index of the cladding (r > a), and α is the profile shape. The refractive index of IRCF is shown in the Figure 13. The IRC profile is practically thinner (or more concentrated around the fiber axis) than the IPGI profile [73]. However, it is worthy to note that our profile becomes much smoother when reaching the maximum index value n1. When compared with IPGI-FMF, the inverse-raised-cosine function offers a large modal separation. The enhanced separation is likely to hinder mode coupling, reducing the system crosstalk and improving the transmission. Moreover, IRC-FMF has the potential to handle OAM modes with high purity hence low intrinsic crosstalk [73, 74].

Figure 13.

Index profiles of the IRC fiber (solid lines), with α ranging from 0 to 1 (reproduced from 73).

3.2.8 Hyperbolic tangent few mode fibers (HTAN-FMFs)

Based on hyperbolic tangent function (HTAN), we proposed and designed a ring core few mode fiber that we refer to as hyperbolic tangent few mode fiber (HTAN-FMF). The function HTAN was not common in optical fiber profiling. It is widely used in various fields/domains such as digital neural networks, image processing, digital filters, and decoding algorithms [75, 76, 77] but not common in waveguide and optical fiber designs. Intuitively, one of the most attractive criteria in hyperbolic tangent function, used as an activation function in neural network, is its strong gradient centered around the inflection point (switch point). This is the same criteria required from an optical fiber profile in order to enhance the intermodal separation. The refractive index of HTAN-FMF is given by the following expression [78]:

nr=n2if0ra1α2Coren1+n22+n2.Tanhπ×Tanhπ×ra1a1×αifa1α2ra1+α2Coren1ifa1+α2raCoren3ifraCladdingE15

Where n1, n2, n3 are the refractive index at the core-cladding interface, at the core center, and at the cladding region, respectively. a, a1and α are the core radius, the half of core radius (a1 = a/2) and the shape parameter respectively. ∆nis the actual refractive index difference (i.e. ∆n = n1-n2) which corresponds to the extent of hyperbolic tangent function inside the core. The shape parameter α controls the shape behavior of HTAN function. The refractive index of HTAN is illustrated in Figure 14. The proposed HTAN-FMF achieves a wide intermodal separation (between cylindrical vector modes) especially between TE0,1, HE2,1, and TM0,1 (≥3 × 10−4). This enables low-level crosstalk channels carrying data during propagation and outperforms what is existing in the literature [78]. On the other hand, even with an exterior abrupt variation, the inner smooth behavior of HTAN-FMF guarantees the enhancement of the obtained OAM mode purities (≥ 99.9%) leading to intrinsic crosstalk as minimum as −30 dB during propagation. Moreover, the obtained results in term of chromatic dispersion (max CD = −60 ps/(km.nm)), differential group delay (max DGD = 55 ps/m), and bending insensitivity, demonstrate that the HTAN-FMF could be a viable candidate for enhancing the transmission capacity and the spectral efficiency in next generation OAM mode division Multiplexing (OAM-MDM) systems [78].

Figure 14.

Refractive index profile of HTAN fiber for different values of profile shape α [78].

3.3 Photonic crystal fibers

Photonic crystal fibers (PCF) has shown its design flexibility to guide appropriate OAM modes. With adjustable parameters, PCF can offer more flexible design structures to provide unique fiber properties. Due to that, several kinds of OAM-PCF with various structures (hexagonal, circular, kagome…) and materials (As2S3, SiO2, polymer…), having promising features have been designed and even fabricated. PCF have been proposed and fabricated to ensure good transmission quality of OAM modes. While a review on this topic exceed the scope of this thesis, we can nevertheless mention some details and contributions. PCFs supporting one, 2, 10, 12, 14, 26, 34, 42 and 48, first order OAM modes have been proposed featuring good transmission properties [79, 80, 81, 82, 83, 84, 85, 86, 87, 88, 89].

The race is still ongoing to increase the number of OAM modes in PCF featuring good transmission proprieties. To the best of our knowledge, the most supporting OAM modes number in a circular PCF reaches 110 over C + L communication bands [90]. The designed fiber featured large effective indices separation (are at the order of 10−3), low nonlinear coefficient, low confinement loss (under 10−7 dB/m), and relatively flat chromatic dispersion. Such fiber could find potential application in high capacity OAM-MDM system. By analysis of these recent mosaic OAM-PCFs literature, we can come to the general requirements in PCF design that ensure good transmission quality of OAM modes in the following five points or guidelines [91, 92, 93, 94].

  • Fiber index profile that matches the intensity profile of OAM modes (ring shape).

  • The supported modes belonging to the same OAM mode family should possess a large index separation (≥10−4) to be free from complex and heavy multiple input multiple output digital signal processing (MIMO DSP) at the receiver side. This is achievable with high material contrast between the fiber core and the cladding. Instead of using pure SiO2 as a background material for the PCF-fiber, other available materials could be used such as Silicon (Si), As2S3, and Polymer.

  • Large core thickness is required targeting to increase the supported OAM mode number.

  • The excited OAM modes should be of the first order. Hence, it is preferable to avoid exciting the higher radial orders modes because it causes trouble in multiplexing and demultiplexing operations due to the intensity and phase variety distribution.

  • The guided OAM modes would possess good transmission features such as low confinement loss, flat dispersion, large effective mode area, and low nonlinear coefficient over a large wavelength range (at least covering C + L bands defined by ITU-T).

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4. Conclusion

In this chapter, we have attempted to provide recent advances in SDM based Optical fibers. We showed that SDM is currently the unexhausted technology that can deal with the capacity need and boost data traffic. Furthermore, an interesting embodiment of SDM, which is based on carrying data on fiber modes (MDM) has been presented and discussed. The different mode basis supported in optical fibers are presented and discussed. Furthermore, we reviewed the research activities that are based on harnessing OAM modes to encode data channels either in classical optical fibers (i.e. with classical refractive index profiles) or in special fibers with appropriate ring profiles. We presented the main research activities and recent trends in OAM-MDM over the last ten years.

© 2021 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution 3.0 License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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Alaaeddine Rjeb, Habib Fathallah and Mohsen Machhout (November 24th 2021). OAM Modes in Optical Fibers for Next Generation Space Division Multiplexing (SDM) Systems, Fiber Optics - Technology and Applications, Guillermo Huerta-Cuellar, IntechOpen, DOI: 10.5772/intechopen.97773. Available from:

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