2017
DOI: 10.1007/s00340-017-6808-6
|View full text |Cite
|
Sign up to set email alerts
|

Optical frequency locked loop for long-term stabilization of broad-line DFB laser frequency difference

Abstract: In multiple applications, phase coherence of the two laser fields locked at a frequency offset is not required [2][3][4][5][6][7][8][9][10][11] and a mere frequency lock is a sufficient solution. Nevertheless, one of the most commonly used solutions is the optical phase locked loop (OPLL) [12][13][14][15]. In a generic OPLL the master laser (ML) and the slave laser (SL) are combined and the beat note is measured on a fast photodiode (PD), compared with a reference value and then the difference is fed through t… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
16
0

Year Published

2017
2017
2024
2024

Publication Types

Select...
9

Relationship

5
4

Authors

Journals

citations
Cited by 26 publications
(16 citation statements)
references
References 26 publications
0
16
0
Order By: Relevance
“…In this paper, we focus on the experimental realization of the phase locking and the performance optimization in the DW good-bad-cavity laser systems, to suppress the residual cavity-pulling effect, which is a necessary step moving towards the cavity-stabilized AOCs. We built two independent DW systems and locked the two cavities together by phase locking technique [32][33][34][35][36][37] of 1064 nm good-cavity lasers, which can synchronize the cavity-lengths change between two DW-AOCs. It is aimed at eliminating the impact of the common-mode noise, which is caused by the asynchronous lengths variation of two independent maincavities of DW-AOCs, on the beating linewidth of the 1470 nm bad-cavity lasers.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we focus on the experimental realization of the phase locking and the performance optimization in the DW good-bad-cavity laser systems, to suppress the residual cavity-pulling effect, which is a necessary step moving towards the cavity-stabilized AOCs. We built two independent DW systems and locked the two cavities together by phase locking technique [32][33][34][35][36][37] of 1064 nm good-cavity lasers, which can synchronize the cavity-lengths change between two DW-AOCs. It is aimed at eliminating the impact of the common-mode noise, which is caused by the asynchronous lengths variation of two independent maincavities of DW-AOCs, on the beating linewidth of the 1470 nm bad-cavity lasers.…”
Section: Introductionmentioning
confidence: 99%
“…The first term arises from the frequency difference ∆ν of the users' lasers and can be easily compensated using phase-locking techniques 27 routinely employed in optical communications. 28 With a feasible value ∆ν < 1 Hz, 29 the phase uncertainty would be ∼ 0.01 rad over 300 km of fibre, negligibly contributing to the QBER. The second term represents a more serious impairment.…”
mentioning
confidence: 99%
“…For accurate shaping of the beam we use a spatial light modulator (SLM, Holoeye Pluto) coupled with a charge-coupled device (CCD) camera (Basler Scout scA1400-17fm). The SLM is illuminated with an elliptically shaped beam from a semiconductor taper amplifier (Toptica, BoosTA) seeded with a light from an ECDL (Toptica DL 100) locked using an offset-lock setup [73]. Temporal ac Stark pulse profile is controlled with an acousto-optic modulator.…”
Section: Sii Experimental Setupmentioning
confidence: 99%
“…S4 for experimental geometry. All lasers are locked to either cooler or repumper laser through a beat-note offset lock [73]. In the I-sCMOS experiment the image intensifier gate is open during writing and reading.…”
Section: Sii Experimental Setupmentioning
confidence: 99%