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1.
Opt Lett ; 21(19): 1535-7, 1996 Oct 01.
Artigo em Inglês | MEDLINE | ID: mdl-19881716

RESUMO

A detalled investigation of the coupled dynamlcs of the copropagatlng and counterpropagatlng polarlzation states in the optical loop fiber of a nonlinear amplifying loop mirror is performed Analysis of the dynamlcs yields evidence for the existence of a polarization-insensitive cofiguration of the device.

2.
Opt Lett ; 20(11): 1250-2, 1995 Jun 01.
Artigo em Inglês | MEDLINE | ID: mdl-19859489

RESUMO

Transparency of a 91-km distributed erbium-doped fiber is achieved with 0.46 mW/km of pump power at a signal power of -12 d Bm. The accumulation of amplif ier noise is measured to be smaller than the minimum noise accumulation that can be achieved in a 91-km link with two lumped amplifiers separated by 45 km.

3.
Opt Lett ; 18(11): 867, 1993 Jun 01.
Artigo em Inglês | MEDLINE | ID: mdl-19802298
4.
Opt Lett ; 18(20): 1709-11, 1993 Oct 15.
Artigo em Inglês | MEDLINE | ID: mdl-19823492

RESUMO

A theoretical analysis of the noise properties of an Er-doped superfluorescent fiber source is presented. The optimum fiber design with respect to the signal-to-noise ratio and output power is found.

5.
Opt Lett ; 18(22): 1908-10, 1993 Nov 15.
Artigo em Inglês | MEDLINE | ID: mdl-19829443

RESUMO

Initial overlap between solitons propagating at different carrier frequencies gives rise to a change in the frequencies of the solitons. The frequency change can have a severe effect on the transmission system because it will result in a time displacement of the solitons that is due to the fiber dispersion. The frequency change caused by initial overlap between two solitons at different carrier frequencies is calculated for a transmission system with periodic gain and loss.

6.
Opt Lett ; 16(17): 1355-7, 1991 Sep 01.
Artigo em Inglês | MEDLINE | ID: mdl-19776969

RESUMO

A simple fiber-optic temperature sensor is constructed that uses the temperature dependence of microbending loss. The sensor is tested and shows high sensitivity and a strict linear scale over a wide range from 20 to 180 K. It is shown that a proper choice of signal wavelength can be used either to make the sensor more sensitive or to make it independent of changes in laser wavelength.

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