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1.
Opt Express ; 14(16): 7329-41, 2006 Aug 07.
Article in English | MEDLINE | ID: mdl-19529102

ABSTRACT

A practical hollow-core photonic crystal fiber design suitable for attaining low-loss propagation is analyzed. The geometry involves a number of localized elliptical features positioned on the glass ring that surrounds the air core and separates the core and cladding regions. The size of each feature is tuned so that the composite core-surround geometry is antiresonant within the cladding band gap, thus minimizing the guided mode field intensity both within the fiber material and at material/air interfaces. A birefringent design, which involves a 2-fold symmetric arrangement of the features on the core-surround ring, gives rise to wavelength ranges where the effective index difference between the polarization modes is larger than 10(-4). At such high birefringence levels, one of the polarization modes retains favorable field exclusion characteristics, thus enabling low-loss propagation of this polarization channel.


Subject(s)
Fiber Optic Technology/instrumentation , Models, Theoretical , Anisotropy , Birefringence , Computer Simulation , Elasticity , Equipment Design , Photons , Scattering, Radiation , Stress, Mechanical
2.
Opt Lett ; 30(15): 1938-40, 2005 Aug 01.
Article in English | MEDLINE | ID: mdl-16092225

ABSTRACT

We report on the development of a 2.5 microm core photonic crystal fiber with a substantially reduced water-peak loss around 1.38 microm, which allows extended Raman-soliton supercontinuum generation up to 1.55 microm with a cw ytterbium fiber laser pump source. The resulting broadband, high-spectral-power-density, low-coherence light source can be employed for advanced, submicrometer resolution optical coherence tomography.

3.
Opt Lett ; 30(7): 717-9, 2005 Apr 01.
Article in English | MEDLINE | ID: mdl-15832916

ABSTRACT

Modes are selectively excited by launching light through the cladding from the side into a hollow-core photonic crystal fiber. Measuring the total output power at the end of the fiber as a function of the angle of incidence of the exciting laser beam provides a powerful diagnostic for characterizing the cladding bandgap. Furthermore, various types of modes on either side of the bandgap are excited individually, and their near-field images are obtained.

4.
Opt Express ; 13(1): 236-44, 2005 Jan 10.
Article in English | MEDLINE | ID: mdl-19488348

ABSTRACT

Hollow-core photonic crystal fibres have excited interest as potential ultra-low loss telecommunications fibres because light propagates mainly in air instead of solid glass. We propose that the ultimate limit to the attenuation of such fibres is determined by surface roughness due to frozenin capillary waves. This is confirmed by measurements of the surface roughness in a HC-PCF, the angular distribution of the power scattered out of the core, and the wavelength dependence of the minimum loss of fibres drawn to different scales.

5.
Opt Express ; 13(2): 558-63, 2005 Jan 24.
Article in English | MEDLINE | ID: mdl-19488385

ABSTRACT

The light radiated from the guided mode of a hollow core photonic crystal fiber into free space is measured as a function of angle and wavelength. This enables the direct experimental visualization of the photonic band gap and the identification of localized modes of the core region.

6.
Opt Express ; 13(20): 7779-93, 2005 Oct 03.
Article in English | MEDLINE | ID: mdl-19498806

ABSTRACT

The loss resulting from roughness scattering at hole interfaces within solid core photonic crystal fibers is theoretically analyzed and compared with measurements on fabricated fibers. It is found that a model roughness spectrum corresponding to frozen in capillary waves gives results in reasonably good agreement with experiments on small core fibers. In particular, the roughness scattering loss is shown to be only weakly dependent on wavelength. Agreement at a larger core size requires a long length-scale cut-off to be introduced to the roughness spectrum. Due to the long range nature of the roughness correlations, the scattering is non Rayleigh in character and cannot be interpreted in terms of a local photon density of states.

7.
Opt Express ; 13(20): 8277-85, 2005 Oct 03.
Article in English | MEDLINE | ID: mdl-19498857

ABSTRACT

The modal properties of an air core photonic crystal fiber which incorporates an anti-resonant feature within the region that marks the transition between the air core and the crystal cladding are numerically calculated. The field intensity at the glass/air interfaces is shown to be reduced by a factor of approximately three compared to a fiber with more conventional core surround geometry. The reduced interface field intensity comes at the expense of an increased number of unwanted core interface modes within the band gap. When the interface field intensity is associated with modal propagation loss, the findings are in accord with recent measurements on fabricated fibers which incorporate a similar antiresonant feature.

8.
Opt Express ; 11(14): 1613-20, 2003 Jul 14.
Article in English | MEDLINE | ID: mdl-19466039

ABSTRACT

We describe a hollow-core photonic bandgap fiber designed for use in the 850 nm wavelength region. The fiber has a minimum attenuation of 180dB/km at 847nm wavelength. The low-loss mode has a quasi- Gaussian intensity profile. The group-velocity dispersion of this mode passes through zero around 830nm, and is anomalous for longer wavelengths. The polarization beat length varies from 4 mm to 13 mm across the band gap. We expect this fiber to be useful for delivery of high-energy ultrashort optical pulses.

9.
Opt Lett ; 19(2): 111, 1994 Jan 15.
Article in English | MEDLINE | ID: mdl-19829561
10.
Opt Lett ; 18(11): 873, 1993 Jun 01.
Article in English | MEDLINE | ID: mdl-19802300
11.
Opt Lett ; 17(16): 1161-3, 1992 Aug 15.
Article in English | MEDLINE | ID: mdl-19794751

ABSTRACT

An active fiber-optic Fabry-Perot filter with an optical bandwidth adjustable in the 1-100-kHz range for lambda = 1088 nm radiation is described. Its bandwidth and peak transmission are stabilized by clamping the loss compensating gain of the filter to the gain of a nearby laser oscillation. The filter is electronically continuously tunable. Gain is provided by a Nd(3+)-doped fiber.

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