Abstract
We show that the four-level model for the CO{sub 2} laser with modulated losses predicts a critical exponent close to 1/2 for the characteristic times in two homoclinic crises. In the five-dimensional Poincare map corresponding to this model, a sequential horseshoe formation due to the period three unstable orbit takes place after a region of multistability. (author). 14 refs, 4 figs.
Citation Formats
Pando L, C L, and Cerdeira, H A.
Homoclinic crises in a model for the CO{sub 2} laser.
IAEA: N. p.,
1993.
Web.
Pando L, C L, & Cerdeira, H A.
Homoclinic crises in a model for the CO{sub 2} laser.
IAEA.
Pando L, C L, and Cerdeira, H A.
1993.
"Homoclinic crises in a model for the CO{sub 2} laser."
IAEA.
@misc{etde_10152145,
title = {Homoclinic crises in a model for the CO{sub 2} laser}
author = {Pando L, C L, and Cerdeira, H A}
abstractNote = {We show that the four-level model for the CO{sub 2} laser with modulated losses predicts a critical exponent close to 1/2 for the characteristic times in two homoclinic crises. In the five-dimensional Poincare map corresponding to this model, a sequential horseshoe formation due to the period three unstable orbit takes place after a region of multistability. (author). 14 refs, 4 figs.}
place = {IAEA}
year = {1993}
month = {Apr}
}
title = {Homoclinic crises in a model for the CO{sub 2} laser}
author = {Pando L, C L, and Cerdeira, H A}
abstractNote = {We show that the four-level model for the CO{sub 2} laser with modulated losses predicts a critical exponent close to 1/2 for the characteristic times in two homoclinic crises. In the five-dimensional Poincare map corresponding to this model, a sequential horseshoe formation due to the period three unstable orbit takes place after a region of multistability. (author). 14 refs, 4 figs.}
place = {IAEA}
year = {1993}
month = {Apr}
}