2009
DOI: 10.1016/j.optlastec.2008.09.001
|View full text |Cite
|
Sign up to set email alerts
|

Large amplitude noise reduction in ultrashort pulse trains using a power-symmetric nonlinear optical loop mirror

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
5
0

Year Published

2013
2013
2023
2023

Publication Types

Select...
6
1

Relationship

2
5

Authors

Journals

citations
Cited by 7 publications
(5 citation statements)
references
References 39 publications
0
5
0
Order By: Relevance
“…In order to compensate for the residual fibre birefringence and obtain an isotropic behaviour [24], a moderate twist of 2 turns/m is considered. Assuming that the fibre is wound on a spool with a radius of curvature of at least 30 cm, calculations suggest that this twist is sufficient to nearly suppress the effects of linear birefringence, whereas it remains small enough to avoid pulse distortion [29]. It has to be noted that the isotropc behaviour of a twisted fibre has been confirmed experimentally.…”
Section: Numerical Studymentioning
confidence: 96%
See 1 more Smart Citation
“…In order to compensate for the residual fibre birefringence and obtain an isotropic behaviour [24], a moderate twist of 2 turns/m is considered. Assuming that the fibre is wound on a spool with a radius of curvature of at least 30 cm, calculations suggest that this twist is sufficient to nearly suppress the effects of linear birefringence, whereas it remains small enough to avoid pulse distortion [29]. It has to be noted that the isotropc behaviour of a twisted fibre has been confirmed experimentally.…”
Section: Numerical Studymentioning
confidence: 96%
“…In this section we study numerically the operation of the proposed scheme in the frame of amplitude regeneration of a WDM signal consisting of two data trains at different wavelengths and presenting different power levels. When both chromatic dispersion and Kerr nonlinearity are at play, one option consists in operating the NOLM in the soliton regime, which was shown to enhance its regeneration capabilities [29]. However, as the device will process two signals with different power levels and variable power ratio, the pulses at both wavelengths propagating in the loop can hardly be close to fundamental solitons simultaneously, so that the soliton regime cannot be exploited in this case.…”
Section: Numerical Studymentioning
confidence: 99%
“…In the HNLF, the SPM and cross-phase modulation (XPM) effects occur contributing to the nonlinear phase shift of the counter-propagating fields [14,15], and the former effect is involved in the following discussion, performing the SPM-NOLM. The expressions of the above-mentioned optical fields can be derived as follows [16][17][18]: The expressions of the above-mentioned optical fields can be derived as follows [16][17][18]:…”
Section: Normalized Power Transfer Function Of Single Nolmmentioning
confidence: 99%
“…[12][13][14]. The flexibility and robustness of such NOLM-based devices with strict polarization control allowed envisioning their use in optical transmission and data processing systems to perform a wide range of essential operations including pedestal removal, all-optical signal regeneration [15][16][17][18][19], even at various wavelengths simultaneously for WDM systems [20] or in the case of complex, multilevel modulation formats (constellations) [21], wavelength conversion for OTDM systems [22], as well as all-optical logic gates [14]. Other noticeable uses of the PI-NOLM include the determination of the temporal profile of ultrashort optical pulses [23], as well as estimating the amplitude statistics of a bunch of optical pulses [24,25], which provided in particular one of the first experimental pieces of evidence of the emergence of ultrashort extreme events (optical rogue waves, ORWs) in noise-like pulses (NLPs) [25].…”
Section: Introductionmentioning
confidence: 99%