A Simple overview on Hollow Core Fiber

in Zero to Infinity3 years ago

Hollow core fibers (HCFs) are a form of fiber with an air core surrounding by dielectric layer cladding components that restrict light [1]. In comparison to the embodiment of traditional fiber, it can direct light at a very rapid propagation speed through hollow regions and has a number of unique properties such as reduced nonlinearity, lower material absorption, and a higher damage threshold [2-5]. Various designs of HCFs have caught the interest of researchers all around the world due to their exceptional features and design flexibility [2]. HCFs have several uses, such as laser sources [3], ultrashort pulse delivery [6], optical fiber communication [7,8], terahertz guiding [9], and so on. Hollow-core photonic bandgap fibers (HC-PBGFs) are implemented by having a periodic refractive index in the cladding that guides light using the photonic bandgap effect [1], and hollow-core photonic bandgap fibers (HC-PBGFs) are implemented by having a periodic refractive index in the cladding that guides light using the photonic bandgap effect. Hollow-core antiresonant fibers (HC-ARFs), on the other hand, guide light by observing antiresonant reflection and wavenumber mismatch in the core and cladding regions [4]. The cladding geometry of HC-ARFs is relatively simple, resulting in very low loss, low group velocity dispersion (GVD), decreased nonlinearity, and so on [5].

Antiresonant fibers (ARFs) mainly focus on the cladding elements responsible for confining light in the core by applying antiresonant reflection through it [10]. The cladding geometry maintains a gap between neighboring cladding antiresonant tubes (ARTs) that leads to attenuating the resonance happening in the nodes [4].


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Furthermore, several studies have been conducted using nested cladding tubes to reduce light leakage by augmenting anti-resonant reflection [4,5,10,11]. Aside from that, various studies on various cladding configurations have been reported, such as single-ring (SR) ART elements [12], double-ring (DR) ART elements [13], nested ring elements [4, 5, 14], elliptical shape ART elements [15], ice-cream cone shape ART elements [16], conjoined tube elements [7, 17–19], and so on. Pryamikov et al. [12] presented and manufactured an ARF based on the SR platform with six ARTs and demonstrated a reduced loss in the mid-IR region with broad bandwidth. Furthermore, as compared to circular tube architectures, elliptical capillary structures showed a loss of less than one order of magnitude [15]. In addition, Poletti et al. proposed a layered nodeless ARF with six ART that outperformed SR-ARFs and PBGFs in terms of fiber performance [4].

Multilayer based ARFs have a new research focus that aims to improve confinement loss (CL) and bending loss (BL) performance. For example, a conjoined tube fiber (CTF) structure with six tubes was reported to have a 2 dB/km loss at 1.512 m and a higher BL of 1 dB/km for telecommunication applications [7]. Adding a silica layer in the radial direction greatly lowered the CL [6, 18, 19, 20]. With state-of-the-art manufacturing, however, CTFs must be improved and updated to present a revolutionary design with amazing low losses and single mode (SM) performance, which will accelerate the advancement of ARFs in optical fiber communication systems.

REFERENCES

[1] R. Cregan et al., “Single-mode photonic band gap guidance of light inair,” science, vol. 285, no. 5433, pp. 1537–1539, 1999.
[2] F. Yu et al., "Negative curvature hollow-core optical fiber," IEEE J.Sel. Top. Quantum Electron., vol. 22, no. 2, pp. 146–155, 2016.
[3] M. R. A. Hassan et al., "Cavity-based mid-ir fiber gas laser pumped bya diode laser," Optica, vol. 3, no. 3, pp. 218–221, 2016.
[4] F. Poletti, "Nested antiresonant nodeless hollow core fiber," Opticsexpress, vol. 22, no. 20, pp. 23807–23828, 2014.
[5] W. Belardi, "Design and properties of hollow antiresonant fibers for507 the visible and near infrared spectral range," J. LightwaveTechnol., vol. 508, no. 33, pp. 4497–4503, 2015.
[6] P. S. J. Russell et al., "Hollow-core photonic crystal fibres for gasbased nonlinear optics," Nature Photonics, vol. 8, no. 4, pp. 278–286,2014.
[7] Poletti et al., "Towards high-capacity fibre-optic communications atthe speed of light in vacuum," Nature Photonics, vol. 7, no. 4, pp. 279-284, 2013.
[8] S. f. Gao et al., "Hollow-core conjoined-tube negative-curvature fibrewith ultralow loss," Nature communications, vol. 9, no. 1, pp. 1–6,2018.
[9] A. L. Cruz et al., "3d printed hollow-core terahertz fibers," Fibers, vol.6, no. 3, p. 43, 2018.
[10] K. S. R. Shaha et al., "Low loss double cladding nested hollow coreantiresonant fiber," OSA Continuum, vol. 3, no. 9, pp. 2512–2524,2020.
[11] G. T. Jasion et al., "Hollow core NANF with 0.28 db/km attenuation inthe C and L bands," in Optical Fiber Communication Conference(Optical Society of America, 2020), paper Th4B–4.
[12] A. D. Pryamikov et al., "Demonstration of a waveguide regime for asilica hollow-core microstructured optical fiber with a negativecurvature of the core boundary in the spectral region < 3.5 µm," Opticsexpress, vol. 19, no. 2, pp. 1441–1448, 2011.
[13] K. S. R. Shaha et al., "Nested antiresonant hollow-core fiber withultralow loss," in 2020 11th International Conference on Electrical and Computer Engineering (ICECE). IEEE, 2020, pp. 29–32.
[14] M. S. Habib, J. E. Antonio-Lopez, C. Markos, A. Schülzgen, and R.Amezcua-Correa, "Single-mode, low loss hollow-core anti-resonantfiber designs," Opt. Express, vol. 27, no. 4, pp. 3824-3836, 2019.
[15] M. S. Habib et al., "Low-loss single-mode hollow-core fiber withanisotropic anti-resonant elements," Optics express, vol. 24, no. 8, pp.8429–8436, 2016.
[16] F. Yu et al., "Low loss silica hollow core fibers for 3–4 µm spectralregion," Optics express, vol. 20, no. 10, pp. 11153–11158, 2012.
[17] M. A. Mollah et al., "Novel hollow-core asymmetric conjoined-tubeanti-resonant fiber for low-loss thz wave guidance," OSA Continuum,vol. 3, pp. 1169–1176, 2020.
[18] K. S. R. Shaha and A. Khaleque, "Low-loss single-mode modifiedconjoined tube hollow-core fiber," Appl. Opt., vol. 60, no. 21, pp.6243– 6250, Jul 2021.
[19] S. f. Gao et al., "Conquering the rayleigh scattering limit of silica glassfiber at visible wavelengths with a hollow-core fiber approach," Laser& Photonics Rev., vol. 14, pp. 1900241, 2020.
[20] Y. Wang, and W. Ding, "Confinement loss in hollow-core negativecurvature fiber: A multi-layered model," Optics Express, vol. 25, no.26, pp. 33122-33133, 2017.

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