2009
DOI: 10.1007/s10686-008-9132-7
|View full text |Cite
|
Sign up to set email alerts
|

Air-clad fibres for astronomical instrumentation: focal-ratio degradation

Abstract: Focal-ratio degradation (FRD) of light launched into high-numerical aperture (NA) single-annulus all-silica undoped air-clad fibres at an NA of 0.54 is reported. The measured annular light distribution remained Gaussian after 30 m of propagation, but the angular FWHM of the output annulus doubled from 4 • after 1 m propagation to 8.5 • after 30 m, which is significantly larger than that reported of standard doped-silica fibres (NA < 0.22). No significant diffractive effects were observed. The design of air-cla… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
5
0

Year Published

2009
2009
2022
2022

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 11 publications
(5 citation statements)
references
References 13 publications
0
5
0
Order By: Relevance
“…The self-assembled wires are of sufficient dimension and high index contrast with the surrounding air-cladding to act as highly multimode slab (rectangular) waveguides. When light is launched into several angular rays [ 22 , 23 ], after propagating a few centimeters there is sufficient cross-coupling between all modes, aided by interface scattering, to ensure even coupling into all modes of the waveguide at the point at which optical interrogation is undertaken. A schematic of the experimental setup is shown in Figure 4 .…”
Section: Results and Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…The self-assembled wires are of sufficient dimension and high index contrast with the surrounding air-cladding to act as highly multimode slab (rectangular) waveguides. When light is launched into several angular rays [ 22 , 23 ], after propagating a few centimeters there is sufficient cross-coupling between all modes, aided by interface scattering, to ensure even coupling into all modes of the waveguide at the point at which optical interrogation is undertaken. A schematic of the experimental setup is shown in Figure 4 .…”
Section: Results and Analysismentioning
confidence: 99%
“…From the slope of this expression, an estimated mass spectrometer intensity based diffusion coefficient is D ~ 4.8 x 10 -4 nm 2 s -1 . Since I C = c.N A where N A is Avogadro's number, the diffusion coefficient for the hydrated Zn 2+ can also be extracted from the slope of lnC vs x 2 by converting to C noting I 0 obtained from extrapolating to x 2 = 0 in Figure 6(b) is assumed to equal 0.1 M x 6.022 x10 23 . From this, the effective molecular diffusion coefficient is estimated to be a little lower: D ~ 3 x 10 -4 nm 2 s -1 .…”
Section: Measuring Diffusion Through Laser Ablation Of Self-assembled...mentioning
confidence: 99%
“…(19) and Eq. (20) can also describe the FRD properties because FRD can broaden the output ring in both inner and outer directions, which makes the ring diffused and widens the FWHM (Murphy et al 2008(Murphy et al , 2013Aslund & Canning 2009). Here we consider it as FWHM model.…”
Section: Frd Dependence On Optical Fibre Lengthmentioning
confidence: 99%
“…These particular fibres are especially important for astrophotonics and imaging applications because they can have extraordinarily high numerical apertures as a result of approaching the idealised air ring fibre. Recently, careful consideration to the effect on focal ratio degradation (FRD) was reported [88]-whilst no significant impact from diffractive scattering was noted, scattering generally off the corrugated surface was observed to give rise to degradation in FRD.…”
Section: Refractive Index Measurements Using Photonic Crystal Fibresmentioning
confidence: 99%