optical clock
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2022 ◽  
Author(s):  
Christoph Hotter ◽  
David Plankensteiner ◽  
G.A. Kazakov ◽  
Helmut Ritsch

2021 ◽  
Vol 18 ◽  
pp. 100326
Author(s):  
L. Pelzer ◽  
K. Dietze ◽  
J. Kramer ◽  
F. Dawel ◽  
L. Krinner ◽  
...  

2021 ◽  
Vol 104 (5) ◽  
Author(s):  
Saleh O. Allehabi ◽  
V. A. Dzuba ◽  
V. V. Flambaum
Keyword(s):  

2021 ◽  
Vol 1 ◽  
pp. 73
Author(s):  
Anna Bychek ◽  
Christoph Hotter ◽  
David Plankensteiner ◽  
Helmut Ritsch

Background: Theoretical studies of superradiant lasing on optical clock transitions predict a superb frequency accuracy and precision closely tied to the bare atomic linewidth. Such a superradiant laser is also robust against cavity fluctuations when the spectral width of the lasing mode is much larger than that of the atomic medium. Recent predictions suggest that this unique feature persists even for a hot and thus strongly broadened ensemble, provided the effective atom number is large enough. Methods: Here we use a second-order cumulant expansion approach to study the power, linewidth and lineshifts of such a superradiant laser as a function of the inhomogeneous width of the ensemble including variations of the spatial atom-field coupling within the resonator. Results: We present conditions on the atom numbers, the pump and coupling strengths required to reach the buildup of collective atomic coherence as well as scaling and limitations for the achievable laser linewidth. Conclusions: We show how sufficiently large numbers of atoms subject to strong optical pumping can induce synchronization of the atomic dipoles over a large bandwidth. This generates collective stimulated emission of light into the cavity mode leading to narrow-band laser emission at the average of the atomic frequency distribution. The linewidth is orders of magnitudes smaller than that of the cavity as well as the inhomogeneous gain broadening and exhibits reduced sensitivity to cavity frequency noise.


2021 ◽  
Author(s):  
Nikita Zhadnov ◽  
Konstantin Kudeyarov ◽  
Denis Kryuchkov ◽  
Gulnara Vishnyakova ◽  
Ksenia Khabarova ◽  
...  

2021 ◽  
Author(s):  
Yani Zuo ◽  
Shaoyang Dai ◽  
Shiying Cao ◽  
Weiliang Chen ◽  
Kun Liu ◽  
...  

2021 ◽  
Author(s):  
Artem Golovizin ◽  
DMITRY TREGUBOV ◽  
Denis Mishin ◽  
Daniil Provorchenko ◽  
Nikolai Kolachevsky

2021 ◽  
Vol 23 (9) ◽  
pp. 093024
Author(s):  
Sebastian Koke ◽  
Erik Benkler ◽  
Alexander Kuhl ◽  
Gesine Grosche

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Artem A. Golovizin ◽  
Dmitry O. Tregubov ◽  
Elena S. Fedorova ◽  
Denis A. Mishin ◽  
Daniil I. Provorchenko ◽  
...  

AbstractOptical atomic clocks have already overcome the eighteenth decimal digit of instability and uncertainty, demonstrating incredible control over external perturbations of the clock transition frequency. At the same time, there is an increasing demand for atomic (ionic) transitions and new interrogation and readout protocols providing minimal sensitivity to external fields and possessing practical operational wavelengths. One of the goals is to simplify the clock operation while maintaining the relative uncertainty at a low 10−18 level achieved at the shortest averaging time. This is especially important for transportable and envisioned space-based optical clocks. Here, we demonstrate implementation of a synthetic frequency approach for a thulium optical clock with simultaneous optical interrogation of two clock transitions. Our experiment shows suppression of the quadratic Zeeman shift by at least three orders of magnitude. The effect of the tensor lattice Stark shift in thulium can also be reduced to below 10−18 in fractional frequency units. This makes the thulium optical clock almost free from hard-to-control systematic shifts. The “simultaneous” protocol demonstrates very low sensitivity to the cross-talks between individual clock transitions during interrogation and readout.


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