Abstract

Atmospheric air-filled hollow core (HC) fibers, representing the simplest yet reliable form of gas-filled hollow core fiber, show remarkable nonlinear properties and have several interesting applications such as pulse compression, frequency conversion and supercontinuum generation. Although the propagation of sub-picosecond and few hundred picosecond pulses are well-studied in air-filled fibers, the nonlinear response of air to pulses with a duration of a few picoseconds has interesting features that have not yet been explored fully. Here, we experimentally and theoretically study the nonlinear propagation of ~6 ps pulses in three different types of atmospheric air-filled HC fiber. With this pulse length, we were able to explore different nonlinear characteristics of air at different power levels. Using in-house-fabricated, state-of-the-art HC photonic bandgap, HC tubular and HC Kagomé fibers, we were able to associate the origin of the initial pulse broadening process in these fibers to rotational Raman scattering (RRS) at low power levels. Due to the broadband and low loss transmission window of the HC Kagomé fiber we used, we observed the transition from initial pulse broadening (by RRS) at lower powers, through long-range frequency conversion (2330 cm−1) with the help of vibrational Raman scattering, to broadband (~700 nm) supercontinuum generation at high power levels. To model such a wide range of nonlinear processes in a unified approach, we have implemented a semi-quantum model for air into the generalized nonlinear Schrodinger equation, which surpasses the limits of the common single damping oscillator model in this pulse length regime. The model has been validated by comparison with experimental results and provides a powerful tool for the design, modeling and optimization of nonlinear processes in air-filled HC fibers.

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2017 (4)

2016 (4)

2015 (1)

2014 (7)

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

C. Li, K. P. Rishad, P. Horak, Y. Matsuura, and D. Faccio, “Spectral broadening and temporal compression of ∼ 100 fs pulses in air-filled hollow core capillary fibers,” Opt. Express 22(1), 1143–1151 (2014).
[Crossref] [PubMed]

M. A. Finger, N. Y. Joly, T. Weiss, and P. S. Russell, “Accuracy of the capillary approximation for gas-filled kagomé-style photonic crystal fibers,” Opt. Lett. 39(4), 821–824 (2014).
[Crossref] [PubMed]

B. Debord, M. Alharbi, L. Vincetti, A. Husakou, C. Fourcade-Dutin, C. Hoenninger, E. Mottay, F. Gérôme, and F. Benabid, “Multi-meter fiber-delivery and pulse self-compression of milli-Joule femtosecond laser and fiber-aided laser-micromachining,” Opt. Express 22(9), 10735–10746 (2014).
[Crossref] [PubMed]

A. Hartung, J. Kobelke, A. Schwuchow, K. Wondraczek, J. Bierlich, J. Popp, T. Frosch, and M. A. Schmidt, “Double antiresonant hollow core fiber--guidance in the deep ultraviolet by modified tunneling leaky modes,” Opt. Express 22(16), 19131–19140 (2014).
[Crossref] [PubMed]

F. Poletti, “Nested antiresonant nodeless hollow core fiber,” Opt. Express 22(20), 23807–23828 (2014).
[Crossref] [PubMed]

W. Ding and Y. Wang, “Analytic model for light guidance in single-wall hollow-core anti-resonant fibers,” Opt. Express 22(22), 27242–27256 (2014).
[Crossref] [PubMed]

2013 (6)

2011 (3)

2010 (1)

2009 (1)

X. Liu, “Adaptive higher-order split-step Fourier algorithm for simulating lightwave propagation in optical fiber,” Opt. Commun. 282(7), 1435–1439 (2009).
[Crossref]

2008 (4)

2007 (1)

2006 (1)

2003 (1)

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
[Crossref] [PubMed]

1999 (1)

M. E. Kooi, L. Ulivi, and J. A. Schouten, “Vibrational Spectra of Nitrogen in Simple Mixtures at High Pressures,” Int. J. Thermophys. 20(3), 867–876 (1999).
[Crossref]

1998 (1)

1997 (1)

1996 (1)

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
[Crossref]

1993 (1)

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

1989 (1)

K. J. Blow and D. Wood, “Theoretical description of transient stimulated Raman scattering in optical fibers,” IEEE J. Quantum Electron. 25(12), 2665–2673 (1989).
[Crossref]

1986 (2)

A. P. Hickman, J. A. Paisner, and W. K. Bischel, “Theory of multiwave propagation and frequency conversion in a Raman medium,” Phys. Rev. A Gen. Phys. 33(3), 1788–1797 (1986).
[Crossref] [PubMed]

L. A. Rahn and R. E. Palmer, “Studies of nitrogen self-broadening at high temperature with inverse Raman spectroscopy,” J. Opt. Soc. Am. B 3(9), 1164 (1986).
[Crossref]

1965 (1)

Y. R. Shen and N. Bloembergen, “Theory of Stimulated Brillouin and Raman Scattering,” Phys. Rev. 137(6A), A1787–A1805 (1965).
[Crossref]

Abdolvand, A.

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

K. F. Mak, J. C. Travers, N. Y. Joly, A. Abdolvand, and P. S. Russell, “Two techniques for temporal pulse compression in gas-filled hollow-core kagomé photonic crystal fiber,” Opt. Lett. 38(18), 3592–3595 (2013).
[Crossref] [PubMed]

Abokhamis Mousavi, S. M.

Agrawal, G. P.

Aldén, M.

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

Alharbi, M.

Amsanpally, A.

Baz, A.

Benabid, F.

B. Debord, A. Amsanpally, M. Chafer, A. Baz, M. Maurel, J. M. Blondy, E. Hugonnot, F. Scol, L. Vincetti, F. Gérôme, and F. Benabid, “Ultralow transmission loss in inhibited-coupling guiding hollow fibers,” Optica 4(2), 209 (2017).
[Crossref]

F. Guichard, A. Giree, Y. Zaouter, M. Hanna, G. Machinet, B. Debord, F. Gérôme, P. Dupriez, F. Druon, C. Hönninger, E. Mottay, F. Benabid, and P. Georges, “Nonlinear compression of high energy fiber amplifier pulses in air-filled hypocycloid-core Kagome fiber,” Opt. Express 23(6), 7416–7423 (2015).
[Crossref] [PubMed]

B. Debord, M. Alharbi, L. Vincetti, A. Husakou, C. Fourcade-Dutin, C. Hoenninger, E. Mottay, F. Gérôme, and F. Benabid, “Multi-meter fiber-delivery and pulse self-compression of milli-Joule femtosecond laser and fiber-aided laser-micromachining,” Opt. Express 22(9), 10735–10746 (2014).
[Crossref] [PubMed]

B. Debord, M. Alharbi, T. Bradley, C. Fourcade-Dutin, Y. Y. Wang, L. Vincetti, F. Gérôme, and F. Benabid, “Hypocycloid-shaped hollow-core photonic crystal fiber Part I: arc curvature effect on confinement loss,” Opt. Express 21(23), 28597–28608 (2013).
[Crossref] [PubMed]

F. Emaury, C. F. Dutin, C. J. Saraceno, M. Trant, O. H. Heckl, Y. Y. Wang, C. Schriber, F. Gerome, T. Südmeyer, F. Benabid, and U. Keller, “Beam delivery and pulse compression to sub-50 fs of a modelocked thin-disk laser in a gas-filled Kagome-type HC-PCF fiber,” Opt. Express 21(4), 4986–4994 (2013).
[Crossref] [PubMed]

Y. Y. Wang, N. V. Wheeler, F. Couny, P. J. Roberts, and F. Benabid, “Low loss broadband transmission in hypocycloid-core Kagome hollow-core photonic crystal fiber,” Opt. Lett. 36(5), 669–671 (2011).
[Crossref] [PubMed]

Bengtsson, P. E.

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

Ben-Yakar, A.

Bhagwat, A. R.

Bierlich, J.

Bird, D. M.

Birks, T. A.

Bischel, W. K.

A. P. Hickman, J. A. Paisner, and W. K. Bischel, “Theory of multiwave propagation and frequency conversion in a Raman medium,” Phys. Rev. A Gen. Phys. 33(3), 1788–1797 (1986).
[Crossref] [PubMed]

Bloembergen, N.

Y. R. Shen and N. Bloembergen, “Theory of Stimulated Brillouin and Raman Scattering,” Phys. Rev. 137(6A), A1787–A1805 (1965).
[Crossref]

Blondy, J. M.

Blow, K. J.

K. J. Blow and D. Wood, “Theoretical description of transient stimulated Raman scattering in optical fibers,” IEEE J. Quantum Electron. 25(12), 2665–2673 (1989).
[Crossref]

Bonamy, J.

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

Börzsönyi, A.

Bradley, T.

Bradley, T. D.

Bufetov, I. A.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Chafer, M.

Chang, W.

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

Chen, L.

Chen, Y.

Chichkov, B. N.

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
[Crossref]

Couny, F.

Debord, B.

Ding, W.

Do, B. T.

Druon, F.

Dupriez, P.

Dutin, C. F.

Emaury, F.

Faccio, D.

Ferhanoglu, O.

Finger, M. A.

Fokoua, E. N.

Fourcade-Dutin, C.

Franco, M. A.

Frosch, T.

Gaeta, A. L.

Georges, P.

Gerome, F.

Gérôme, F.

Giree, A.

Gladyshev, A. V.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Gorbach, A. V.

Gouveia, M. A.

Gray, D. R.

Grillon, G.

Guichard, F.

Hafizi, B.

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
[Crossref] [PubMed]

Hand, D. P.

Hanna, M.

Hartung, A.

Hayes, J. R.

Heckl, O. H.

Heiner, Z.

Hickman, A. P.

A. P. Hickman, J. A. Paisner, and W. K. Bischel, “Theory of multiwave propagation and frequency conversion in a Raman medium,” Phys. Rev. A Gen. Phys. 33(3), 1788–1797 (1986).
[Crossref] [PubMed]

Hoenninger, C.

Hölzer, P.

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

Hönninger, C.

Horak, P.

Hoy, C. L.

Hugonnot, E.

Husakou, A.

Jasion, G.

Jasion, G. T.

Jaworski, P.

Joly, N. Y.

Kalashnikov, M. P.

Keller, U.

Knight, J. C.

Kobelke, J.

Kolyadin, A. N.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Kooi, M. E.

M. E. Kooi, L. Ulivi, and J. A. Schouten, “Vibrational Spectra of Nitrogen in Simple Mixtures at High Pressures,” Int. J. Thermophys. 20(3), 867–876 (1999).
[Crossref]

Kosolapov, A. F.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Kovács, A. P.

Kröll, S.

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

Krylov, A. A.

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Li, C.

Liang, S.

Lin, Q.

Liu, X.

X. Liu, “Adaptive higher-order split-step Fourier algorithm for simulating lightwave propagation in optical fiber,” Opt. Commun. 282(7), 1435–1439 (2009).
[Crossref]

Liu, Z.

Machinet, G.

Maier, R. R.

Mak, K. F.

Mangan, B. J.

Martinsson, L.

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
[Crossref]

Matsuura, Y.

Maurel, M.

Mlejnek, M.

Moloney, J. V.

Momma, C.

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
[Crossref]

Mottay, E.

Mousavi, S. A.

Mysyrowicz, A.

Nibbering, E. T. J.

Nolte, S.

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
[Crossref]

Numkam Fokoua, E.

Okhrimchuk, A. G.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Osvay, K.

Paisner, J. A.

A. P. Hickman, J. A. Paisner, and W. K. Bischel, “Theory of multiwave propagation and frequency conversion in a Raman medium,” Phys. Rev. A Gen. Phys. 33(3), 1788–1797 (1986).
[Crossref] [PubMed]

Palmer, R. E.

Pearce, G. J.

Peñano, J. R.

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
[Crossref] [PubMed]

Petrovich, M. N.

Petrovich Marco, N.

F. Poletti, N. Petrovich Marco, and J. Richardson David, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 315 (2013).
[Crossref]

Piyawattanametha, W.

Pleteneva, E. N.

Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Poletti, F.

J. R. Hayes, S. R. Sandoghchi, T. D. Bradley, Z. Liu, R. Slavik, M. A. Gouveia, N. V. Wheeler, G. Jasion, Y. Chen, E. N. Fokoua, M. N. Petrovich, D. J. Richardson, and F. Poletti, “Antiresonant Hollow Core Fiber With an Octave Spanning Bandwidth for Short Haul Data Communications,” J. Lightwave Technol. 35(3), 437–442 (2017).
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N. V. Wheeler, T. D. Bradley, J. R. Hayes, M. A. Gouveia, S. Liang, Y. Chen, S. R. Sandoghchi, S. M. Abokhamis Mousavi, F. Poletti, M. N. Petrovich, and D. J. Richardson, “Low-loss Kagome hollow-core fibers operating from the near- to the mid-IR,” Opt. Lett. 42(13), 2571–2574 (2017).
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Y. Chen, Z. Liu, S. R. Sandoghchi, G. T. Jasion, T. D. Bradley, E. Numkam Fokoua, J. R. Hayes, N. V. Wheeler, D. R. Gray, B. J. Mangan, R. Slavik, F. Poletti, M. N. Petrovich, and D. J. Richardson, “Multi-kilometer Long, Longitudinally Uniform Hollow Core Photonic Bandgap Fibers for Broadband Low Latency Data Transmission,” J. Lightwave Technol. 34(1), 104–113 (2016).
[Crossref]

S. A. Mousavi, S. R. Sandoghchi, D. J. Richardson, and F. Poletti, “Broadband high birefringence and polarizing hollow core antiresonant fibers,” Opt. Express 24(20), 22943–22958 (2016).
[Crossref] [PubMed]

F. Poletti, “Nested antiresonant nodeless hollow core fiber,” Opt. Express 22(20), 23807–23828 (2014).
[Crossref] [PubMed]

F. Poletti, N. Petrovich Marco, and J. Richardson David, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 315 (2013).
[Crossref]

F. Poletti, M. N. Petrovich, and D. J. Richardson, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 4 (2013).
[Crossref]

Popp, J.

Prade, B. S.

Pryamikov, A. D.

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
[Crossref]

Ra, H.

Rahn, L. A.

Richardson, D. J.

Richardson David, J.

F. Poletti, N. Petrovich Marco, and J. Richardson David, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 315 (2013).
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Rishad, K. P.

Roberts, P. J.

Russell, P. S.

Russell, P. S. J.

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

Sandoghchi, S. R.

Saraceno, C. J.

Schmidt, M. A.

Schouten, J. A.

M. E. Kooi, L. Ulivi, and J. A. Schouten, “Vibrational Spectra of Nitrogen in Simple Mixtures at High Pressures,” Int. J. Thermophys. 20(3), 867–876 (1999).
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Schriber, C.

Schwuchow, A.

Scol, F.

Serafim, P.

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
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Setti, V.

Shen, Y. R.

Y. R. Shen and N. Bloembergen, “Theory of Stimulated Brillouin and Raman Scattering,” Phys. Rev. 137(6A), A1787–A1805 (1965).
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Skryabin, D. V.

Slavik, R.

Smith, A. V.

Solgaard, O.

Sprangle, P.

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
[Crossref] [PubMed]

Südmeyer, T.

Ting, A.

J. R. Peñano, P. Sprangle, P. Serafim, B. Hafizi, and A. Ting, “Stimulated Raman scattering of intense laser pulses in air,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 68(5), 056502 (2003).
[Crossref] [PubMed]

Trant, M.

Travers, J. C.

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
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K. F. Mak, J. C. Travers, N. Y. Joly, A. Abdolvand, and P. S. Russell, “Two techniques for temporal pulse compression in gas-filled hollow-core kagomé photonic crystal fiber,” Opt. Lett. 38(18), 3592–3595 (2013).
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B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
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Ulivi, L.

M. E. Kooi, L. Ulivi, and J. A. Schouten, “Vibrational Spectra of Nitrogen in Simple Mixtures at High Pressures,” Int. J. Thermophys. 20(3), 867–876 (1999).
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Vincetti, L.

von Alvensleben, F.

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
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Y. P. Yatsenko, E. N. Pleteneva, A. G. Okhrimchuk, A. V. Gladyshev, A. F. Kosolapov, A. N. Kolyadin, and I. A. Bufetov, “Multiband supercontinuum generation in an air-core revolver fibre,” Quantum Electron. 47(6), 553–560 (2017).
[Crossref]

Y. P. Yatsenko, A. A. Krylov, A. D. Pryamikov, A. F. Kosolapov, A. N. Kolyadin, A. V. Gladyshev, and I. A. Bufetov, “Propagation of femtosecond pulses in a hollow-core revolver fibre,” Quantum Electron. 46(7), 617–626 (2016).
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Yildirim, M.

Yu, F.

Zaouter, Y.

Zheltikov, A. M.

Appl. Opt. (2)

Appl. Phys., A Mater. Sci. Process. (1)

B. N. Chichkov, C. Momma, S. Nolte, F. von Alvensleben, and A. Tünnermann, “Femtosecond, picosecond and nanosecond laser ablation of solids,” Appl. Phys., A Mater. Sci. Process. 63(2), 109–115 (1996).
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K. J. Blow and D. Wood, “Theoretical description of transient stimulated Raman scattering in optical fibers,” IEEE J. Quantum Electron. 25(12), 2665–2673 (1989).
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M. E. Kooi, L. Ulivi, and J. A. Schouten, “Vibrational Spectra of Nitrogen in Simple Mixtures at High Pressures,” Int. J. Thermophys. 20(3), 867–876 (1999).
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J. Chem. Phys. (1)

L. Martinsson, P. E. Bengtsson, M. Aldén, S. Kröll, and J. Bonamy, “A test of different rotational Raman linewidth models: Accuracy of rotational coherent anti‐Stokes Raman scattering thermometry in nitrogen from 295 to 1850 K,” J. Chem. Phys. 99(4), 2466–2477 (1993).
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F. Poletti, N. Petrovich Marco, and J. Richardson David, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 315 (2013).
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F. Poletti, M. N. Petrovich, and D. J. Richardson, “Hollow-core photonic bandgap fibers: technology and applications,” Nanophotonics 2(5-6), 4 (2013).
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Nat. Photonics (1)

P. S. J. Russell, P. Hölzer, W. Chang, A. Abdolvand, and J. C. Travers, “Hollow-core photonic crystal fibres for gas-based nonlinear optics,” Nat. Photonics 8(4), 278–286 (2014).
[Crossref]

Opt. Commun. (1)

X. Liu, “Adaptive higher-order split-step Fourier algorithm for simulating lightwave propagation in optical fiber,” Opt. Commun. 282(7), 1435–1439 (2009).
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Opt. Express (15)

S. A. Mousavi, S. R. Sandoghchi, D. J. Richardson, and F. Poletti, “Broadband high birefringence and polarizing hollow core antiresonant fibers,” Opt. Express 24(20), 22943–22958 (2016).
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A. V. Gorbach and D. V. Skryabin, “Soliton self-frequency shift, non-solitonic radiation and self-induced transparency in air-core fibers,” Opt. Express 16(7), 4858–4865 (2008).
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L. Vincetti and V. Setti, “Waveguiding mechanism in tube lattice fibers,” Opt. Express 18(22), 23133–23146 (2010).
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F. Poletti, “Nested antiresonant nodeless hollow core fiber,” Opt. Express 22(20), 23807–23828 (2014).
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F. Guichard, A. Giree, Y. Zaouter, M. Hanna, G. Machinet, B. Debord, F. Gérôme, P. Dupriez, F. Druon, C. Hönninger, E. Mottay, F. Benabid, and P. Georges, “Nonlinear compression of high energy fiber amplifier pulses in air-filled hypocycloid-core Kagome fiber,” Opt. Express 23(6), 7416–7423 (2015).
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A. R. Bhagwat and A. L. Gaeta, “Nonlinear optics in hollow-core photonic bandgap fibers,” Opt. Express 16(7), 5035–5047 (2008).
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W. Ding and Y. Wang, “Analytic model for light guidance in single-wall hollow-core anti-resonant fibers,” Opt. Express 22(22), 27242–27256 (2014).
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A. Hartung, J. Kobelke, A. Schwuchow, K. Wondraczek, J. Bierlich, J. Popp, T. Frosch, and M. A. Schmidt, “Double antiresonant hollow core fiber--guidance in the deep ultraviolet by modified tunneling leaky modes,” Opt. Express 22(16), 19131–19140 (2014).
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L. Chen, G. J. Pearce, T. A. Birks, and D. M. Bird, “Guidance in Kagome-like photonic crystal fibres I: analysis of an ideal fibre structure,” Opt. Express 19(7), 6945–6956 (2011).
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P. Jaworski, F. Yu, R. R. Maier, W. J. Wadsworth, J. C. Knight, J. D. Shephard, and D. P. Hand, “Picosecond and nanosecond pulse delivery through a hollow-core Negative Curvature Fiber for micro-machining applications,” Opt. Express 21(19), 22742–22753 (2013).
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C. Li, K. P. Rishad, P. Horak, Y. Matsuura, and D. Faccio, “Spectral broadening and temporal compression of ∼ 100 fs pulses in air-filled hollow core capillary fibers,” Opt. Express 22(1), 1143–1151 (2014).
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F. Emaury, C. F. Dutin, C. J. Saraceno, M. Trant, O. H. Heckl, Y. Y. Wang, C. Schriber, F. Gerome, T. Südmeyer, F. Benabid, and U. Keller, “Beam delivery and pulse compression to sub-50 fs of a modelocked thin-disk laser in a gas-filled Kagome-type HC-PCF fiber,” Opt. Express 21(4), 4986–4994 (2013).
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B. Debord, M. Alharbi, L. Vincetti, A. Husakou, C. Fourcade-Dutin, C. Hoenninger, E. Mottay, F. Gérôme, and F. Benabid, “Multi-meter fiber-delivery and pulse self-compression of milli-Joule femtosecond laser and fiber-aided laser-micromachining,” Opt. Express 22(9), 10735–10746 (2014).
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G. P. Agrawal, Nonlinear Fiber Optics (Academic Press, 2007).

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Figures (9)

Fig. 1
Fig. 1 Scanning electron micrographs (SEMs) of the cross-section of fabricated (a) HC-PBGF, (c) HC-KF, (e) the optical microscopic image of the cross-section of fabricated HC-TF. The loss and dispersion profile of (b) HC-PBGF, (d) HC-KF, (f) HC-TF.

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Fig. 2
Fig. 2 Experimental setup including free space launching mechanism and measurement systems.

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Fig. 3
Fig. 3 The measured output spectrum of the pulsed laser with ~6 ps pulse length at 1030 nm launched in (a) 5 m of HC-PBGF with average laser power (Pavg) range of 1 - 6W and (b) 9.6 m of HC-TF with Pavg of 1 - 7W. The phase matching condition (PMC) detuning wavelengths are superposed over the experimental results for (c) HC-PBGF and (d) HC-TF with 10 dBm shift for each plot (10 dBm/div). The PMC is out of the plot range for HC-PBGF (d) due to the higher nonlinear coefficient of this fiber.

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Fig. 4
Fig. 4 The output spectrum of the pulsed laser with ~6ps length at 1030 nm launched in to (a) HC-TF with average laser power (Pavg) of 10, 15, 20 W and (b) HC-KF with Pavg of 2, 5, 10, 15, 20 W. The higher power output spectrums from overlapping sidebands to broad supercontinuum are presented for Pavg = 25, 30, 35, 40, 45 and 50W in (a) HC-TF and (b) HC-KF.

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Fig. 5
Fig. 5 Comparison between experimental results of air-filled HC-KF (Fig. 4(b)) and GNLSE simulation results using SDO model for air (a) Pavg = 10 W, (b) Pavg = 15 W, (c) Pavg = 25 W. The SDO model cannot properly predict A. the position of the RRS at low power. B. VRS is not reproduced at all. C. The broadening effect is not correctly reproduced due to lack of VRS.

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Fig. 6
Fig. 6 (a) Comparison between the time domain rotational Raman response for Nitrogen by the SDO model and SQM, (c) real and imaginary parts of the frequency response of the SDO model for Nitrogen, (c) real and imaginary parts of the frequency response of SQM for Nitrogen.

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Fig. 7
Fig. 7 (a) Experimental output spectra for HC-KF at different Pavg (Fig. 4(b.d)), (b) simulation results using SQM in the GNLSE for the HC-KF (averaged over 20 shots). The comparison of simulation and experimental results for (c) 5 W, (d) 15 W, (e) 25 W, (f) 35 W, (g) 50 W.

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Fig. 8
Fig. 8 Comparison of experimental output spectrum and simulation results using the SQM in the GNLSE for HC-KF for Pavg of (a) 15 W, (b) 25 W, (c) 35 W.

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Fig. 9
Fig. 9 Power spectrum evolution of a 800 fs pulse (a) propagating along HC-KF at 1030 nm with 200 µJ energy, (b) at the output of the fiber; (c) Power spectrum evolution of a 50 ps pulse propagating along HC-KF at 1030 nm with 200 µJ energy, (d) the power spectrum of the 50 ps pulse at the output of the fiber.

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Equations (7)

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β(ω)= ω c n gas 2 (ω,P,T)− ( 2.4048c ω⋅a(ω) ) 2
∂ E ¯ (z,ω) ∂z −iD(ω) E ¯ (z,ω)=⋯ i ∑ j=1 2 K j γ j (ω)F{ E(z,t) ∫ −∞ +∞ R (T) j | E(z,t−T) | 2 dT } , j=1,2.
R j (t)=(1− f r j )δ(t)+ f r j H j (t),  j=1,2. ∫ −∞ +∞ R j (t)dt=1.
H ro t k (t)=u(t) C ro t k ∑ J e (−t/ τ ro t k J ) A k J sin(4π B k c(2J+3)) , A k J =( N k (J+2) − N k J ) q k J (J+2)(J+1) (2J+3) , N k J =exp[ −hc B k J(J+1)/ KT ]. k=1,2.
H vi b k (t)=u(t) C vi b k ∑ J e (−t/ τ vib k J ) M k J sin( ω k J t) , ω k J ≈2πc( Ω ¯ k − η k J(J+1) ), M k J = q k J (2J+1)exp[ −hc B k J(J+1)/ KT ], k=1,2.
H 1 (t)= ∑ k=1 2 σ k n ¯ 1 [ μ ro t k H ro t k (t)+(1− μ ro t k ) H vi b k (t) ] ,
∂ E ¯ (z,ω) ∂z −iD(ω) E ¯ (z,ω)=i γ total (ω)F{ E(z,t) ∫ −∞ +∞ R (T) total | E(z,t−T) | 2 dT }.

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