Carrier-envelope phase drift measurement of picosecond pulses by an all-linear-optical means
Carrier-envelope phase (CEP) drift of a pulse train of 2 ps pulses has been measured by a multiple beam interferometer. The round trip time of the interferometer is slightly mistuned from the pulse sequence, leading to spectral interference fringes. We extract the pulse-to- pulse CEP drift fr...
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| Dokumentumtípus: | Cikk |
| Megjelent: |
2014
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| Sorozat: | OPTICS LETTERS
39 No. 20 |
| Tárgyszavak: | |
| doi: | 10.1364/OL.39.005913 |
| mtmt: | 2760854 |
| Online Access: | http://publicatio.bibl.u-szeged.hu/34063 |
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| 024 | 7 | |a 2760854 |2 mtmt | |
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| 100 | 1 | |a Jójárt Péter | |
| 245 | 1 | 0 | |a Carrier-envelope phase drift measurement of picosecond pulses by an all-linear-optical means |h [elektronikus dokumentum] / |c Jójárt Péter |
| 260 | |c 2014 | ||
| 300 | |a 5913-5916 | ||
| 490 | 0 | |a OPTICS LETTERS |v 39 No. 20 | |
| 520 | 3 | |a Carrier-envelope phase (CEP) drift of a pulse train of 2 ps pulses has been measured by a multiple beam interferometer. The round trip time of the interferometer is slightly mistuned from the pulse sequence, leading to spectral interference fringes. We extract the pulse-to- pulse CEP drift from the position of the spectral interference pattern. The length of the interferometer has been actively stabilized to ±10 nm, which sets the ultimate limit on the accuracy of the measurement to 78 mrad, while the CEP-drift (rms) noise of the measurement was 127 mrad (at 800 nm). | |
| 650 | 4 | |a Fizikai tudományok | |
| 700 | 0 | 1 | |a Börzsönyi Ádám |e aut |
| 700 | 0 | 1 | |a Soskov V. |e aut |
| 700 | 0 | 1 | |a Zomer F. |e aut |
| 700 | 0 | 1 | |a Chiche R. |e aut |
| 700 | 0 | 1 | |a Cormier Eric |e aut |
| 700 | 0 | 1 | |a Osvay Károly |e aut |
| 856 | 4 | 0 | |u http://publicatio.bibl.u-szeged.hu/34063/1/2760854.pdf |z Dokumentum-elérés |