TY - GEN
T1 - SwiftHohenberg equation with third order dispersion for optical resonators
AU - Tlidi, M.
AU - Kostet, B.
AU - Hariz, A.
AU - Bahloul, L.
AU - Cherbi, L.
AU - Clerc, M.
AU - Ferré, M.
AU - Panajotov, K.
N1 - Publisher Copyright:
© 2019 IEEE
PY - 2019/1/1
Y1 - 2019/1/1
N2 - The control of linear and nonlinear properties of Photonic Crystal Fibers (PCF) has led to several applications in optoelectronics, sensing, and laser science [1]. In particular, driven optical microcavities are widely used for the generation of optical frequency combs. They can be modeled by the Lugiato- Lefever equation that possesses solutions in the form of localized structures (LSs) [2]. Optical frequency- combs generated in high-Q Kerr resonators [3] are in fact the spectral content of the stable temporal pattern occurring in the cavity.
AB - The control of linear and nonlinear properties of Photonic Crystal Fibers (PCF) has led to several applications in optoelectronics, sensing, and laser science [1]. In particular, driven optical microcavities are widely used for the generation of optical frequency combs. They can be modeled by the Lugiato- Lefever equation that possesses solutions in the form of localized structures (LSs) [2]. Optical frequency- combs generated in high-Q Kerr resonators [3] are in fact the spectral content of the stable temporal pattern occurring in the cavity.
UR - http://www.scopus.com/inward/record.url?scp=85084522135&partnerID=8YFLogxK
M3 - Conference contribution
AN - SCOPUS:85084522135
SN - 9781728104690
T3 - Optics InfoBase Conference Papers
BT - European Quantum Electronics Conference, EQEC_2019
PB - Optica Publishing Group (formerly OSA)
T2 - European Quantum Electronics Conference, EQEC_2019
Y2 - 23 June 2019 through 27 June 2019
ER -