Abstract

A novel AsSe2-As2S5 hybrid MOF (HMOF) is designed and fabricated by the rod-in-tube drawing technique. The core is made from AsSe2 glass and the cladding is made from As2S5 glass. The loss is ~1.2 dB/m at ~3000 nm. Zero dispersion wavelength (ZDW) of the HMOF is ~3380 nm. Supercontinuum (SC) generation in a 2 cm-long HMOF is investigated with the pump wavelengths of ~3062, 3241 and 3389 nm from a tunable optical parametric oscillator (OPO) system. Broadband mid-infrared (MIR) SC generation with the spectrum from ~1256 to 5400 nm is obtained with the peak power of ~1337 kW at the wavelength of ~3389 nm.

© 2014 Optical Society of America

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    [Crossref] [PubMed]

2014 (9)

T. L. Cheng, Y. Kanou, K. Asano, D. H. Deng, M. S. Liao, Y. Kanou, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Soliton self-frequency shift and dispersive wave in a hybrid four-hole AsSe2-As2S5 microstructured optical fiber,” Appl. Phys. Lett. 104(12), 121911 (2014).
[Crossref]

J. Swiderski and M. Michalska, “High-power supercontinuum generation in a ZBLAN fiber with very efficient power distribution toward the mid-infrared,” Opt. Lett. 39(4), 910–913 (2014).
[Crossref] [PubMed]

W. Q. Gao, Z. C. Duan, K. Asano, T. L. Cheng, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Mid-infrared supercontinuum generation in a four-hole As2S5 chalcogenide microstructured optical fiber,” Appl. Phys. B 116(4), 847–853 (2014).
[Crossref]

O. Mouawad, J. Picot-Clémente, F. Amrani, C. Strutynski, J. Fatome, B. Kibler, F. Désévédavy, G. Gadret, J.-C. Jules, D. Deng, Y. Ohishi, and F. Smektala, “Multioctave midinfrared supercontinuum generation in suspended-core chalcogenide fibers,” Opt. Lett. 39(9), 2684–2687 (2014).
[Crossref] [PubMed]

Y. Yu, X. Gai, P. Ma, D. Y. Choi, Z. Yang, R. Wang, S. Debbarma, S. J. Madden, and B. Luther-Davies, “A broadband, quasi-continuous, mid-infrared supercontinuum generated in a chalcogenide glass waveguide,” Laser Photonics Rev. 8, 792–798 (2014).

I. Kubat, C. S. Agger, U. Møller, A. B. Seddon, Z. Tang, S. Sujecki, T. M. Benson, D. Furniss, S. Lamrini, K. Scholle, P. Fuhrberg, B. Napier, M. Farries, J. Ward, P. M. Moselund, and O. Bang, “Mid-infrared supercontinuum generation to 12.5μm in large NA chalcogenide step-index fibres pumped at 4.5μm,” Opt. Express 22(16), 19169–19182 (2014).
[Crossref]

I. Kubat, C. R. Petersen, U. V. Møller, A. Seddon, T. Benson, L. Brilland, D. Méchin, P. M. Moselund, and O. Bang, “Thulium pumped mid-infrared 0.9-9μm supercontinuum generation in concatenated fluoride and chalcogenide glass fibers,” Opt. Express 22(4), 3959–3967 (2014).
[Crossref] [PubMed]

T. L. Cheng, W. Q. Gao, M. S. Liao, Z. C. Duan, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Tunable third-harmonic generation in a chalcogenide-tellurite hybrid optical fiber with high refractive index difference,” Opt. Lett. 39(4), 1005–1007 (2014).
[Crossref] [PubMed]

T. L. Cheng, Y. Kanou, D. H. Deng, X. J. Xue, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Fabrication and characterization of a hybrid four-hole AsSe₂-As₂S₅ microstructured optical fiber with a large refractive index difference,” Opt. Express 22(11), 13322–13329 (2014).
[Crossref] [PubMed]

2013 (7)

C. W. Rudy, A. Marandi, K. L. Vodopyanov, and R. L. Byer, “Octave-spanning supercontinuum generation in in situ tapered As2S3 fiber pumped by a thulium-doped fiber laser,” Opt. Lett. 38(15), 2865–2868 (2013).
[Crossref] [PubMed]

C. Wei, X. Zhu, R. A. Norwood, F. Song, and N. Peyghambarian, “Numerical investigation on high power midinfrared supercontinuum fiber lasers pumped at 3 μm,” Opt. Express 21(24), 29488–29504 (2013).
[Crossref]

W. Yuan, “2–10 μm mid-infrared supercontinuum generation in As2Se3 photonic crystal fiber,” Laser Phys. Lett. 10(9), 095107 (2013).
[Crossref]

F. Théberge, J. F. Daigle, D. Vincent, P. Mathieu, J. Fortin, B. E. Schmidt, N. Thiré, and F. Légaré, “Mid-infrared supercontinuum generation in fluoroindate fiber,” Opt. Lett. 38(22), 4683–4685 (2013).
[Crossref] [PubMed]

M. Klimczak, G. Stepniewski, H. Bookey, A. Szolno, R. Stepien, D. Pysz, A. Kar, A. Waddie, M. R. Taghizadeh, and R. Buczynski, “Broadband infrared supercontinuum generation in hexagonal-lattice tellurite photonic crystal fiber with dispersion optimized for pumping near 1560 nm,” Opt. Lett. 38(22), 4679–4682 (2013).
[Crossref] [PubMed]

M. S. Liao, W. Q. Gao, T. L. Cheng, Z. C. Duan, H. Kawashima, T. Suzuki, and Y. Ohishi, “Ultrabroad Supercontinuum Generation Through Filamentation in Tellurite Glass,” Laser Phys. Lett. 10(3), 036002 (2013).
[Crossref]

A. Demircan, S. Amiranashvili, C. Brée, and G. Steinmeyer, “Compressible Octave Spanning Supercontinuum Generation by Two-Pulse Collisions,” Phys. Rev. Lett. 110(23), 233901 (2013).
[Crossref]

2012 (2)

S. P. Stark, J. C. Travers, and P. St. J. Russell, “Extreme supercontinuum generation to the deep UV,” Opt. Lett. 37(5), 770–772 (2012).
[Crossref] [PubMed]

J. H. V. Price, X. Feng, A. M. Heidt, G. Brambilla, P. Horak, F. Poletti, G. Ponzo, P. Petropoulos, M. Petrovich, J. Shi, M. Ibsen, W. H. Loh, H. N. Rutt, and D. J. Richardson, “Supercontinuum generation in non-silica fibers,” Opt. Fiber Technol. 18(5), 327–344 (2012).
[Crossref]

2011 (6)

A. M. Heidt, A. Hartung, G. W. Bosman, P. Krok, E. G. Rohwer, H. Schwoerer, and H. Bartelt, “Coherent octave spanning near-infrared and visible supercontinuum generation in all-normal dispersion photonic crystal fibers,” Opt. Express 19(4), 3775–3787 (2011).
[Crossref] [PubMed]

L. E. Hooper, P. J. Mosley, A. C. Muir, W. J. Wadsworth, and J. C. Knight, “Coherent supercontinuum generation in photonic crystal fiber with all-normal group velocity dispersion,” Opt. Express 19(6), 4902–4907 (2011).
[Crossref] [PubMed]

L. Liu, G. Qin, Q. Tian, D. Zhao, and W. Qin, “Numerical investigation of mid-infrared supercontinuum generation up to 5 μm in single mode fluoride fiber,” Opt. Express 19(11), 10041–10048 (2011).
[Crossref] [PubMed]

D. D. Hudson, S. A. Dekker, E. C. Mägi, A. C. Judge, S. D. Jackson, E. Li, J. S. Sanghera, L. B. Shaw, I. D. Aggarwal, and B. J. Eggleton, “Octave spanning supercontinuum in an As2S3 taper using ultralow pump pulse energy,” Opt. Lett. 36, 1122–1124 (2011).

F. Poletti, X. Feng, G. M. Ponzo, M. N. Petrovich, W. H. Loh, and D. J. Richardson, “All-solid highly nonlinear singlemode fibers with a tailored dispersion profile,” Opt. Express 19(1), 66–80 (2011).
[Crossref] [PubMed]

C. Conseil, Q. Coulombier, C. Boussard-Plédel, J. Troles, L. Brilland, G. Renversez, D. Mechin, B. Bureau, J. L. Adam, and J. Lucas, “Chalcogenide step index and microstructured single mode fibers,” J. Non-Cryst. Solids 357(11-13), 2480–2483 (2011).
[Crossref]

2010 (3)

2009 (1)

G. Qin, X. Yan, C. Kito, M. Liao, C. Chaudhari, T. Suzuki, and Y. Ohishi, “Ultrabroadband supercontinuum generation from ultraviolet to 6.28 μm in a fluoride fiber,” Appl. Phys. Lett. 95(16), 161103 (2009).
[Crossref]

2008 (1)

2006 (2)

J. M. Dudley, G. Genty, and S. Coen, “Supercontinuum generation in photonic crystal fiber,” Rev. Mod. Phys. 78(4), 1135–1184 (2006).
[Crossref]

D. R. Austin, C. M. de Sterke, B. J. Eggleton, and T. G. Brown, “Dispersive wave blue-shift in supercontinuum generation,” Opt. Express 14(25), 11997–12007 (2006).
[Crossref] [PubMed]

2003 (1)

D. Lezal, “Chalcogenide glasses - survey and progress,” J. Optoelectron. Adv. Mater. 5, 23–34 (2003).

2000 (1)

Adam, J. L.

C. Conseil, Q. Coulombier, C. Boussard-Plédel, J. Troles, L. Brilland, G. Renversez, D. Mechin, B. Bureau, J. L. Adam, and J. Lucas, “Chalcogenide step index and microstructured single mode fibers,” J. Non-Cryst. Solids 357(11-13), 2480–2483 (2011).
[Crossref]

J. Troles, Q. Coulombier, G. Canat, M. Duhant, W. Renard, P. Toupin, L. Calvez, G. Renversez, F. Smektala, M. El Amraoui, J. L. Adam, T. Chartier, D. Mechin, and L. Brilland, “Low loss microstructured chalcogenide fibers for large non linear effects at 1995 nm,” Opt. Express 18(25), 26647–26654 (2010).
[Crossref] [PubMed]

Aggarwal, I. D.

Agger, C. S.

Amiranashvili, S.

A. Demircan, S. Amiranashvili, C. Brée, and G. Steinmeyer, “Compressible Octave Spanning Supercontinuum Generation by Two-Pulse Collisions,” Phys. Rev. Lett. 110(23), 233901 (2013).
[Crossref]

Amrani, F.

Asano, K.

W. Q. Gao, Z. C. Duan, K. Asano, T. L. Cheng, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Mid-infrared supercontinuum generation in a four-hole As2S5 chalcogenide microstructured optical fiber,” Appl. Phys. B 116(4), 847–853 (2014).
[Crossref]

T. L. Cheng, Y. Kanou, K. Asano, D. H. Deng, M. S. Liao, Y. Kanou, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Soliton self-frequency shift and dispersive wave in a hybrid four-hole AsSe2-As2S5 microstructured optical fiber,” Appl. Phys. Lett. 104(12), 121911 (2014).
[Crossref]

Austin, D. R.

Bang, O.

Bartelt, H.

Benson, T.

Benson, T. M.

Bookey, H.

Bosman, G. W.

Boussard-Plédel, C.

C. Conseil, Q. Coulombier, C. Boussard-Plédel, J. Troles, L. Brilland, G. Renversez, D. Mechin, B. Bureau, J. L. Adam, and J. Lucas, “Chalcogenide step index and microstructured single mode fibers,” J. Non-Cryst. Solids 357(11-13), 2480–2483 (2011).
[Crossref]

Brambilla, G.

J. H. V. Price, X. Feng, A. M. Heidt, G. Brambilla, P. Horak, F. Poletti, G. Ponzo, P. Petropoulos, M. Petrovich, J. Shi, M. Ibsen, W. H. Loh, H. N. Rutt, and D. J. Richardson, “Supercontinuum generation in non-silica fibers,” Opt. Fiber Technol. 18(5), 327–344 (2012).
[Crossref]

Brée, C.

A. Demircan, S. Amiranashvili, C. Brée, and G. Steinmeyer, “Compressible Octave Spanning Supercontinuum Generation by Two-Pulse Collisions,” Phys. Rev. Lett. 110(23), 233901 (2013).
[Crossref]

Brilland, L.

Brown, T. G.

Buczynski, R.

Bureau, B.

C. Conseil, Q. Coulombier, C. Boussard-Plédel, J. Troles, L. Brilland, G. Renversez, D. Mechin, B. Bureau, J. L. Adam, and J. Lucas, “Chalcogenide step index and microstructured single mode fibers,” J. Non-Cryst. Solids 357(11-13), 2480–2483 (2011).
[Crossref]

Byer, R. L.

Calvez, L.

Canat, G.

Chartier, T.

Chaudhari, C.

G. Qin, X. Yan, C. Kito, M. Liao, C. Chaudhari, T. Suzuki, and Y. Ohishi, “Ultrabroadband supercontinuum generation from ultraviolet to 6.28 μm in a fluoride fiber,” Appl. Phys. Lett. 95(16), 161103 (2009).
[Crossref]

Cheng, T. L.

T. L. Cheng, Y. Kanou, K. Asano, D. H. Deng, M. S. Liao, Y. Kanou, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Soliton self-frequency shift and dispersive wave in a hybrid four-hole AsSe2-As2S5 microstructured optical fiber,” Appl. Phys. Lett. 104(12), 121911 (2014).
[Crossref]

W. Q. Gao, Z. C. Duan, K. Asano, T. L. Cheng, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Mid-infrared supercontinuum generation in a four-hole As2S5 chalcogenide microstructured optical fiber,” Appl. Phys. B 116(4), 847–853 (2014).
[Crossref]

T. L. Cheng, W. Q. Gao, M. S. Liao, Z. C. Duan, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Tunable third-harmonic generation in a chalcogenide-tellurite hybrid optical fiber with high refractive index difference,” Opt. Lett. 39(4), 1005–1007 (2014).
[Crossref] [PubMed]

T. L. Cheng, Y. Kanou, D. H. Deng, X. J. Xue, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Fabrication and characterization of a hybrid four-hole AsSe₂-As₂S₅ microstructured optical fiber with a large refractive index difference,” Opt. Express 22(11), 13322–13329 (2014).
[Crossref] [PubMed]

M. S. Liao, W. Q. Gao, T. L. Cheng, Z. C. Duan, H. Kawashima, T. Suzuki, and Y. Ohishi, “Ultrabroad Supercontinuum Generation Through Filamentation in Tellurite Glass,” Laser Phys. Lett. 10(3), 036002 (2013).
[Crossref]

Cheong, S. W.

Choi, D. Y.

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W. Q. Gao, Z. C. Duan, K. Asano, T. L. Cheng, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Mid-infrared supercontinuum generation in a four-hole As2S5 chalcogenide microstructured optical fiber,” Appl. Phys. B 116(4), 847–853 (2014).
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Y. Yu, X. Gai, P. Ma, D. Y. Choi, Z. Yang, R. Wang, S. Debbarma, S. J. Madden, and B. Luther-Davies, “A broadband, quasi-continuous, mid-infrared supercontinuum generated in a chalcogenide glass waveguide,” Laser Photonics Rev. 8, 792–798 (2014).

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T. L. Cheng, W. Q. Gao, M. S. Liao, Z. C. Duan, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Tunable third-harmonic generation in a chalcogenide-tellurite hybrid optical fiber with high refractive index difference,” Opt. Lett. 39(4), 1005–1007 (2014).
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T. L. Cheng, Y. Kanou, K. Asano, D. H. Deng, M. S. Liao, Y. Kanou, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Soliton self-frequency shift and dispersive wave in a hybrid four-hole AsSe2-As2S5 microstructured optical fiber,” Appl. Phys. Lett. 104(12), 121911 (2014).
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T. L. Cheng, W. Q. Gao, M. S. Liao, Z. C. Duan, D. H. Deng, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Tunable third-harmonic generation in a chalcogenide-tellurite hybrid optical fiber with high refractive index difference,” Opt. Lett. 39(4), 1005–1007 (2014).
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T. L. Cheng, Y. Kanou, K. Asano, D. H. Deng, M. S. Liao, Y. Kanou, M. Matsumoto, T. Misumi, T. Suzuki, and Y. Ohishi, “Soliton self-frequency shift and dispersive wave in a hybrid four-hole AsSe2-As2S5 microstructured optical fiber,” Appl. Phys. Lett. 104(12), 121911 (2014).
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Figures (5)

Fig. 1
Fig. 1 (a) Cross section of the AsSe2-As2S5 HMOF taken by the SEM. (b) Refractive index of the fundamental mode. (c) Calculated chromatic dispersion of the AsSe2-As2S5 HMOF. (d) confinement loss of the AsSe2-As2S5 HMOF
Fig. 2
Fig. 2 (a) Experimental setup for SC generation in the AsSe2-As2S5 HMOF. (b) Mode field profile intensity of the propagation from OPO at ~3000 nm.
Fig. 3
Fig. 3 Measured SC in the AsSe2-As2S5 HMOF at the pump wavelengths of ~3062 nm with the peak power of ~1031 (a), and 1356 W (b).
Fig. 4
Fig. 4 Measured SC in the AsSe2-As2S5 HMOF at the pump wavelengths of ~3241 nm with the peak power of ~1025 (a), and 1350 W (b).
Fig. 5
Fig. 5 Measured SC in the AsSe2-As2S5 HMOF at the pump wavelengths of ~3389 nm with the peak power of ~1338 W.

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