Mid-infrared vector beams in selenide photonic crystal fiber with small hollow core and its application on supercontinuum generation

Characteristics of vector beams in mid-infrared waveband are analyzed numerically in an As2Se3 photonic crystal fiber (PCF) with small central hollow core (SCHH), including the mode fields, confinement loss, effective refractive index and chromatic dispersion. In the PCFs with the SCHH diameter d0 of 0-1.5 μm, the confinement losses of the four vector beams (HE11, TM01, TE01, and HE21) are smaller than 1.0 dB/m for the wavelengths up to ~5 μm. For the SCHH diameter d0 of 0.5-1.5 μm, the field enhancement of the HE11 mode occurs in the SCHHs in the central area for the wavelengths ≤ 5 μm. This happens because the evanescent light penetrates into the SCHH. With d0 increasing, the effective refractive index separations (δneff) between the HE11 mode and high-order modes (TM01, TE01, and HE21) decreases, while the δneff among the high-order modes increases. At the wavelength of 5 μm, the δneff of HE11-TE01, TE01- HE21, and HE21-TM01 is 0.03098, 0.03960, and 0.06867, respectively, when d0 is 1.5 μm. The second ZDWs of TE01, HE21 and TM01 mode are blueshifted with the increase of d0, but they are longer than 5 μm. The negative dispersion regions of the high-order modes (TE01, HE21, and TM01) are much wider than the HE11 modes. With the increase of d0, the HE11 mode dispersion curves have no obvious change, while the high-order modes (TE01, HE21, and TM01) dispersion curves become steep at the longer wavelength, the TM01 mode changes most obviously, and the depression appears. To demonstrate the application of the PCF, super-continuum generation pumped by the four vector modes are simulated and analyzed. Our simulated results will be useful for the optical applications in mid-infrared waveband, such as the generation of cylindrical vector mode and orbital angular momentum (OAM) and the particle manipulation by optical fields.

[1]  Olga Korotkova,et al.  Generation and propagation of a partially coherent vector beam with special correlation functions , 2014 .

[2]  Michael R. Gardner,et al.  High-speed and high-sensitivity parallel spectral-domain optical coherence tomography using a supercontinuum light source. , 2016, Optics letters.

[3]  Lixin Xu,et al.  An all-fiber laser generating cylindrical vector beam. , 2010, Optics express.

[4]  Jianlin Zhao,et al.  Cylindrical vector beam generation in fiber with mode selectivity and wavelength tunability over broadband by acoustic flexural wave. , 2016, Optics express.

[5]  Hongdan Wan,et al.  Switchable Dual-Wavelength Cylindrical Vector Beam Generation From a Passively Mode-Locked Fiber Laser Based on Carbon Nanotubes , 2018, IEEE Journal of Selected Topics in Quantum Electronics.

[6]  Fetah Benabid,et al.  Field enhancement within an optical fibre with a subwavelength air core , 2007 .

[7]  Govind P. Agrawal,et al.  Nonlinear Fiber Optics , 1989 .

[8]  Y. Kozawa,et al.  Optical trapping of micrometer-sized dielectric particles by cylindrical vector beams. , 2010, Optics express.

[9]  Myriam Raybaut,et al.  Microsecond fiber laser pumped, single-frequency optical parametric oscillator for trace gas detection. , 2013, Optics letters.

[10]  Q. Zhan Cylindrical vector beams: from mathematical concepts to applications , 2009 .

[11]  Uriel Levy,et al.  Demonstration of nanofocusing by the use of plasmonic lens illuminated with radially polarized light. , 2009, Nano letters.

[12]  P. Russell Photonic Crystal Fibers , 2003, Science.

[13]  V. Niziev,et al.  Laser beams with axially symmetric polarization , 2000 .

[14]  Vector beam generation from vertical cavity surface emitting lasers. , 2018, Optics letters.

[15]  J. Dudley,et al.  Supercontinuum generation in photonic crystal fiber , 2006 .

[16]  Jianping Ding,et al.  Generation of arbitrary vector beams with a spatial light modulator and a common path interferometric arrangement. , 2007, Optics letters.

[17]  M. Harasek,et al.  Enhanced mid-infrared multi-bounce ATR spectroscopy for online detection of hydrogen peroxide using a supercontinuum laser. , 2018, Optics express.

[18]  S. Ramachandran,et al.  Stable transmission of 12 OAM states in air-core fiber , 2013, CLEO: 2013.

[19]  Siddharth Ramachandran,et al.  Optical vortices in fiber , 2013 .

[20]  D. Hall,et al.  Vector-beam solutions of Maxwell's wave equation. , 1996, Optics letters.

[21]  M. Liao,et al.  Stimulated Raman scattering in AsSe2-As2S5 chalcogenide microstructured optical fiber with all-solid core. , 2016, Optics express.

[22]  B. Eggleton,et al.  Widely tunable, acousto-optic resonances in Chalcogenide As2Se3 fiber. , 2006, Optics express.

[23]  Tonglei Cheng,et al.  Fabrication of all-solid AsSe2–As2S5 microstructured optical fiber with two zero-dispersion wavelengths for generation of mid-infrared dispersive waves , 2016 .

[24]  H. Ming,et al.  High efficiency all-fiber cylindrical vector beam laser using a long-period fiber grating. , 2018, Optics letters.

[25]  G Leuchs,et al.  Sharper focus for a radially polarized light beam. , 2003, Physical review letters.

[26]  A. Willner,et al.  Octave-spanning supercontinuum generation of vortices in a As2S3 ring photonic crystal fiber , 2012, 2012 Conference on Lasers and Electro-Optics (CLEO).

[27]  L A Rusch,et al.  Few-mode fiber with inverse-parabolic graded-index profile for transmission of OAM-carrying modes. , 2014, Optics express.

[28]  Siddharth Ramachandran,et al.  Generation and propagation of radially polarized beams in optical fibers. , 2009, Optics letters.

[29]  C. Menyuk,et al.  Optimization of the split-step Fourier method in modeling optical-fiber communications systems , 2003 .

[30]  Xianzhong Chen,et al.  Vector Vortex Beam Generation with a Single Plasmonic Metasurface , 2016 .

[31]  P. Russell,et al.  Twist-induced guidance in coreless photonic crystal fiber: A helical channel for light , 2016, Science Advances.

[32]  M. Katoh,et al.  Generation of vector beam with tandem helical undulators , 2018, Applied Physics Letters.

[33]  H. Ebendorff‐Heidepriem,et al.  Suspended Core Fibers for the Transmission of Cylindrical Vector Modes , 2016, Journal of Lightwave Technology.

[34]  R. J. Weiblen,et al.  Negative curvature fibers , 2017 .

[35]  Generation of elliptic perfect optical vortex and elliptic perfect vector beam by modulating the dynamic and geometric phase , 2018, Applied Physics Letters.

[36]  Amiel A Ishaaya,et al.  Wavelength conversion of nanosecond pulses to the mid-IR in photonic crystal fibers. , 2012, Optics letters.

[37]  T G Brown,et al.  Longitudinal field modes probed by single molecules. , 2001, Physical review letters.

[38]  Jian Wang,et al.  High-base vector beam encoding/decoding for visible-light communications. , 2015, Optics letters.

[39]  Hongdan Wan,et al.  High efficiency mode-locked, cylindrical vector beam fiber laser based on a mode selective coupler. , 2017, Optics express.

[40]  Knight,et al.  Single-Mode Photonic Band Gap Guidance of Light in Air. , 1999, Science.

[41]  S Spälter,et al.  Large Kerr effect in bulk Se-based chalcogenide glasses. , 2000, Optics letters.

[42]  Giovanni Volpe,et al.  Generation of cylindrical vector beams with few-mode fibers excited by Laguerre-Gaussian beams , 2004 .