Research output: Chapter in Book/Report/Conference proceeding › Conference contribution › Research › peer-review
Experimental evidences of non-hermitian mode-locking in fibre laser. / Kuznetsov, A. G.; Vatnik, I. D.; Perego, A. M. et al.
European Quantum Electronics Conference, EQEC_2019. OSA - The Optical Society, 2019. 2019-ef_p_30 (Optics InfoBase Conference Papers; Vol. Part F143-EQEC 2019).Research output: Chapter in Book/Report/Conference proceeding › Conference contribution › Research › peer-review
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TY - GEN
T1 - Experimental evidences of non-hermitian mode-locking in fibre laser
AU - Kuznetsov, A. G.
AU - Vatnik, I. D.
AU - Perego, A. M.
AU - Churkin, D. V.
AU - Staliunas, K.
PY - 2019/1/1
Y1 - 2019/1/1
N2 - Mode-locking (ML) is an established technique used to generate high power, ultrashort (ranging from ps to few fs duration) coherent light pulses in lasers. Mode-locking techniques could be classified into two broad categories. First one is passive mode-locking techniques in which modes are locked through dynamical intracavity self-organization processes not requiring extra energy sources. Another one is active mode-locking where locking between cavity modes is induced by external energy source. Active mode-locking could be either amplitude mode-locking (AML), for example achieved by a periodic (in time) modulation of the loss coefficient, or phase mode-locking (PML), for example via periodical modulation of the length/detuning of the cavity. In amplitude mode-locking periodic forcing induces synchronization of the cavity modes symmetrically coupled to the closest neighbors due to the action of the modulator: the spectrum broadens symmetrically, resulting in coherent frequency comb centered at the middle of the gain line, see Fig.1a.
AB - Mode-locking (ML) is an established technique used to generate high power, ultrashort (ranging from ps to few fs duration) coherent light pulses in lasers. Mode-locking techniques could be classified into two broad categories. First one is passive mode-locking techniques in which modes are locked through dynamical intracavity self-organization processes not requiring extra energy sources. Another one is active mode-locking where locking between cavity modes is induced by external energy source. Active mode-locking could be either amplitude mode-locking (AML), for example achieved by a periodic (in time) modulation of the loss coefficient, or phase mode-locking (PML), for example via periodical modulation of the length/detuning of the cavity. In amplitude mode-locking periodic forcing induces synchronization of the cavity modes symmetrically coupled to the closest neighbors due to the action of the modulator: the spectrum broadens symmetrically, resulting in coherent frequency comb centered at the middle of the gain line, see Fig.1a.
UR - http://www.scopus.com/inward/record.url?scp=85084615090&partnerID=8YFLogxK
M3 - Conference contribution
AN - SCOPUS:85084615090
T3 - Optics InfoBase Conference Papers
BT - European Quantum Electronics Conference, EQEC_2019
PB - OSA - The Optical Society
T2 - European Quantum Electronics Conference, EQEC_2019
Y2 - 23 June 2019 through 27 June 2019
ER -
ID: 24278348