Standard

Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate. / Arkhipov, R. M.; Arkhipov, M. V.; Babushkin, I.; Rosanov, N. N.

European Quantum Electronics Conference, EQEC_2019. OSA - The Optical Society, 2019. 2019-ee_p_12 (Optics InfoBase Conference Papers; Том Part F143-EQEC 2019).

Результаты исследований: Публикации в книгах, отчётах, сборниках, трудах конференцийстатья в сборнике материалов конференциинаучнаяРецензирование

Harvard

Arkhipov, RM, Arkhipov, MV, Babushkin, I & Rosanov, NN 2019, Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate. в European Quantum Electronics Conference, EQEC_2019., 2019-ee_p_12, Optics InfoBase Conference Papers, Том. Part F143-EQEC 2019, OSA - The Optical Society, European Quantum Electronics Conference, EQEC_2019, Munich, Великобритания, 23/06/19.

APA

Arkhipov, R. M., Arkhipov, M. V., Babushkin, I., & Rosanov, N. N. (2019). Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate. в European Quantum Electronics Conference, EQEC_2019 [2019-ee_p_12] (Optics InfoBase Conference Papers; Том Part F143-EQEC 2019). OSA - The Optical Society.

Vancouver

Arkhipov RM, Arkhipov MV, Babushkin I, Rosanov NN. Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate. в European Quantum Electronics Conference, EQEC_2019. OSA - The Optical Society. 2019. 2019-ee_p_12. (Optics InfoBase Conference Papers).

Author

Arkhipov, R. M. ; Arkhipov, M. V. ; Babushkin, I. ; Rosanov, N. N. / Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate. European Quantum Electronics Conference, EQEC_2019. OSA - The Optical Society, 2019. (Optics InfoBase Conference Papers).

BibTeX

@inproceedings{bcb96afd629b47a4a657be5ec03b1d59,
title = "Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate",
abstract = "Passive mode-locking is one of the main methods for generation of ultra-short pulses in lasers [1]. The critical part of a passively mode-locked lasers is a nonlinear absorber placed in a cavity. It was shown to be possible [2, 3], in the coherent regime of light-matter interaction (in particular using self-induced-transparency (SIT) effects), to achieve a mode-locking (so called coherent or SIT mode-locking) with a pulse duration smaller than the polarization relaxation time T2 of the medium - the limit which can be not be conquered by other mode-locking approaches.",
author = "Arkhipov, {R. M.} and Arkhipov, {M. V.} and I. Babushkin and Rosanov, {N. N.}",
note = "Publisher Copyright: {\textcopyright} 2019 IEEE; European Quantum Electronics Conference, EQEC_2019 ; Conference date: 23-06-2019 Through 27-06-2019",
year = "2019",
language = "English",
series = "Optics InfoBase Conference Papers",
publisher = "OSA - The Optical Society",
booktitle = "European Quantum Electronics Conference, EQEC_2019",
address = "United States",

}

RIS

TY - GEN

T1 - Generation of single-cycle pulses in mode-locked laser with sub-terahertz repetition rate

AU - Arkhipov, R. M.

AU - Arkhipov, M. V.

AU - Babushkin, I.

AU - Rosanov, N. N.

N1 - Publisher Copyright: © 2019 IEEE

PY - 2019

Y1 - 2019

N2 - Passive mode-locking is one of the main methods for generation of ultra-short pulses in lasers [1]. The critical part of a passively mode-locked lasers is a nonlinear absorber placed in a cavity. It was shown to be possible [2, 3], in the coherent regime of light-matter interaction (in particular using self-induced-transparency (SIT) effects), to achieve a mode-locking (so called coherent or SIT mode-locking) with a pulse duration smaller than the polarization relaxation time T2 of the medium - the limit which can be not be conquered by other mode-locking approaches.

AB - Passive mode-locking is one of the main methods for generation of ultra-short pulses in lasers [1]. The critical part of a passively mode-locked lasers is a nonlinear absorber placed in a cavity. It was shown to be possible [2, 3], in the coherent regime of light-matter interaction (in particular using self-induced-transparency (SIT) effects), to achieve a mode-locking (so called coherent or SIT mode-locking) with a pulse duration smaller than the polarization relaxation time T2 of the medium - the limit which can be not be conquered by other mode-locking approaches.

UR - http://www.scopus.com/inward/record.url?scp=85084574678&partnerID=8YFLogxK

M3 - Conference contribution

AN - SCOPUS:85084574678

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: 88560653