1995
DOI: 10.1103/physreva.52.4229
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Polarization instability in lasers. I. Model and steady states of neodymium-doped fiber lasers

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Cited by 30 publications
(23 citation statements)
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“…32,33 Note that in the scalar model the lasing field E5E x e x 1E y e y burns a hole in the field distribution with depth h~E x j j 2 z E y 2 and so there is no coherent coupling of the polarisation modes caused by polarisation hole burning. 1-11, 27 As a result, the polarisation mode coupling is incoherent in this case, and the scalar model, which works well for the soliton description, cannot govern the observed complex dynamics.…”
Section: Vector Model Of An Edf Laser Model Locked With Carbon Nanotubesmentioning
confidence: 99%
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“…32,33 Note that in the scalar model the lasing field E5E x e x 1E y e y burns a hole in the field distribution with depth h~E x j j 2 z E y 2 and so there is no coherent coupling of the polarisation modes caused by polarisation hole burning. 1-11, 27 As a result, the polarisation mode coupling is incoherent in this case, and the scalar model, which works well for the soliton description, cannot govern the observed complex dynamics.…”
Section: Vector Model Of An Edf Laser Model Locked With Carbon Nanotubesmentioning
confidence: 99%
“…The absorption cross-section of an elliptically polarized pump is s a,p~s p ð Þ a m a e p À Á 2 and as a result, the pump light creates an orientational distribution of the population inversion n(h) 27,32,33 ( Figure 3). The lasing field E5E x e x 1E y e y burns a hole in this distribution with depth 27,32,33…”
Section: Vector Model Of An Edf Laser Model Locked With Carbon Nanotubesmentioning
confidence: 99%
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“…To simplify equations (2.8) further, we use an approximation introduced in [8,24] the validity of which has been justified in [25], i.e. we suggest that dipole moments of the transition with absorption and emission for erbium-doped silica (m a , m e ) and the dipole moment of the transition with absorption for CNT μ a are located in the plane defined by the orthogonal components of the lasing field E = E x e x + E y e y transverse to the direction of propagation [8] ( figure 1c).…”
Section: Vector Model Of Erbium-doped Fibre Laser Mode Locked By Carbmentioning
confidence: 99%