Fiber laser-based frequency combs with high relative frequency stability

Author(s):  
N. R. Newbury ◽  
W. C. Swann ◽  
I. Coddington ◽  
L. Lorini ◽  
J. C. Bergquist ◽  
...  
2016 ◽  
Vol 37 (8) ◽  
pp. 1319-1325 ◽  
Author(s):  
Wioletta Krysa ◽  
Anna Sulek ◽  
Maria Rakowicz ◽  
Walentyna Szirkowiec ◽  
Jacek Zaremba

Author(s):  
Kutan Gürel ◽  
Valentin J. Wittwer ◽  
Sargis Hakobyan ◽  
Nayara Jornod ◽  
Stéphane Schilt ◽  
...  

2020 ◽  
Vol 28 (25) ◽  
pp. 38304
Author(s):  
Shuisen Jiang ◽  
Changlei Guo ◽  
Hongyan Fu ◽  
Kaijun Che ◽  
Huiying Xu ◽  
...  

Photonics ◽  
2021 ◽  
Vol 8 (12) ◽  
pp. 560
Author(s):  
Ji Wang ◽  
Wenwu Zhang ◽  
Tianrun Zhang

Greatly improving the energy of a single mode-locked pulse while ensuring the acquisition of the width of short pulses will contribute to the application of mode-locked pulse in basic research, such as precision machining. This report has investigated a Q-switched and mode-locked (QML) erbium doped ring fiber laser based on the nonlinear polarization rotation (NPR) technology and a mechanical Q-switched device. Without the working of the mechanical Q-switched device, the fiber laser exported the continuous-wave mode-locked (CWML) pulse, with a width of 212.5 ps, and a repetition frequency of 81.97 MHz. For the CWML operation, the maximum output average power is 25.7 mW, and the energy is only 0.31 nJ. For the QML operation, 18.03 mW average power is achieved at the Q-switching frequency of 100 Hz. The energy of the QML pulse is increased by over 1100 times to 360.6 nJ. The width of the QML pulse is 203.1 ps measured by an autocorrelation curve, with the time-band product (TBP) being 0.598. The power instability is 0.5% (RMS) and 0.7% (RMS), respectively, for CWML and QML operation within 120 min. Furthermore, the spectral signal-to-noise ratio is about 60 dB. For the QML operation, the power instability is 0.48% (RMS) within 60 s and 0.37% (RMS) within 10 s. After frequency stabilization, the frequency fluctuation is ±100 Hz in the long-term of 1200 s, with the frequency stability (FS) calculated to be 2.44 × 10−6. It indicates that the QML fiber laser has good power stability and frequency stability.


2017 ◽  
Vol 3 (1) ◽  
pp. 67-94 ◽  
Author(s):  
Kevin Heffernan ◽  
Yo Sato

Abstract This study presents apparent-time changes in the morphology of the expression mitai-na ‘similar to’. Based on apparent-time data, we argue that the morphological boundary between mitai and the attributive morpheme -na in the phrase mitai-na has disappeared, and that this complex phrase is now processed as a monomorphemic form. We suggest that relative frequency is the key to understanding the results. We further supplement our argument with data on the standardization of the adverbial adjective form in the Kansai dialect. Young speakers overwhelmingly use the standard form of adverbials for all adjectives except two: yō ‘a lot, well’ and hayō ‘quickly, early’ (instead of Standard Japanese yoku and hayaku). The three linguistic forms that display unusual behavior (mitai-na and the adverbial forms of yō and hayō) all have a high relative frequency. We conclude that when a complex form occurs more frequently than its components (high relative frequency), then it behaves as a monomorphemic unit. The irregular adverbial forms are leftover from an obsolete system, in the same way that many English irregular past forms are leftover from the Germanic strong verb system. In contrast, the irregular form mitai-na emerged from and competes with the regular inflection paradigm for mitai, illustrating a previously undocumented path for the diachronic emergence of irregular morphology.


Author(s):  
A. Ruehl ◽  
M. E. Fermann ◽  
I. Hartl ◽  
A. Cingöz ◽  
D. C. Yost ◽  
...  

2016 ◽  
Vol 2 (11) ◽  
pp. e1601227 ◽  
Author(s):  
David Burghoff ◽  
Yang Yang ◽  
Qing Hu

Dual-comb spectroscopy allows for high-resolution spectra to be measured over broad bandwidths, but an essential requirement for coherent integration is the availability of a phase reference. Usually, this means that the combs’ phase and timing errors must be measured and either minimized by stabilization or removed by correction, limiting the technique’s applicability. We demonstrate that it is possible to extract the phase and timing signals of a multiheterodyne spectrum completely computationally, without any extra measurements or optical elements. These techniques are viable even when the relative linewidth exceeds the repetition rate difference and can tremendously simplify any dual-comb system. By reconceptualizing frequency combs in terms of the temporal structure of their phase noise, not their frequency stability, we can greatly expand the scope of multiheterodyne techniques.


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