An Yb optical lattice clock: Current status at KRISS
The current status of an Yb optical lattice clock at the Korea Research Institute of Standards and Science (KRISS) is reported. The systematic uncertainty of the Yb clock in the first accuracy evaluation was 1.5 × 10 −14 [Park et al. , Metrologia 50, 119 (2013)]. The uncertainty was dominated by the...
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Published in | Journal of the Korean Physical Society Vol. 63; no. 4; pp. 883 - 889 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Dordrecht
Springer Netherlands
01.08.2013
한국물리학회 |
Subjects | |
Online Access | Get full text |
ISSN | 0374-4884 1976-8524 |
DOI | 10.3938/jkps.63.883 |
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Abstract | The current status of an Yb optical lattice clock at the Korea Research Institute of Standards and Science (KRISS) is reported. The systematic uncertainty of the Yb clock in the first accuracy evaluation was 1.5 × 10
−14
[Park
et al.
, Metrologia 50, 119 (2013)]. The uncertainty was dominated by the large uncertainties in the lattice ac Stark shift and the collisional shift, which were mainly limited by the large linewidth and jitter of the clock laser. Recently, a highly stable clock laser at 578 nm was developed with a short-term linewidth of 3.5 Hz and a frequency jitter of about 25 Hz at 1 s and 10 s measurement times, respectively. The long-term frequency drift showed only a linear dependence on time, confirming that the temperature of the super-cavity was maintained a zero coefficient of thermal expansion. The frequency of the lattice laser at 759 nm was phase locked to the optical frequency comb and could be stabilized at the “absolute” frequency of the “magic wavelength”, to within a 1-MHz uncertainty. This improvement greatly reduced the fractional uncertainty due to the lattice ac Stark shift down to 2 × 10
−16
. The systematic uncertainty of the clock is currently 5.3 × 10
−15
and is dominated by the collisional frequency shift. |
---|---|
AbstractList | The current status of an Yb optical lattice clock at the Korea Research Institute of Standards and Science (KRISS) is reported. The systematic uncertainty of the Yb clock in the first accuracy evaluation was 1.5 × 10−14 [Park et al., Metrologia 50, 119 (2013)]. The uncertainty was dominated by the large uncertainties in the lattice ac Stark shift and the collisional shift, which were mainly limited by the large linewidth and jitter of the clock laser. Recently, a highly stable clock laser at 578 nm was developed with a short-term linewidth of 3.5 Hz and a frequency jitter of about 25Hz at 1 s and 10 s measurement times, respectively. The long-term frequency drift showed only a linear dependence on time, confirming that the temperature of the super-cavity was maintained a zero coefficient of thermal expansion. The frequency of the lattice laser at 759 nm was phase locked to the optical frequency comb and could be stabilized at the “absolute” frequency of the “magic wavelength”, to within a 1-MHz uncertainty. This improvement greatly reduced the fractional uncertainty due to the lattice ac Stark shift down to 2 × 10−16. The systematic uncertainty of the clock is currently 5.3 × 10−15 and is dominated by the collisional frequency shift. KCI Citation Count: 7 The current status of an Yb optical lattice clock at the Korea Research Institute of Standards and Science (KRISS) is reported. The systematic uncertainty of the Yb clock in the first accuracy evaluation was 1.5 × 10 −14 [Park et al. , Metrologia 50, 119 (2013)]. The uncertainty was dominated by the large uncertainties in the lattice ac Stark shift and the collisional shift, which were mainly limited by the large linewidth and jitter of the clock laser. Recently, a highly stable clock laser at 578 nm was developed with a short-term linewidth of 3.5 Hz and a frequency jitter of about 25 Hz at 1 s and 10 s measurement times, respectively. The long-term frequency drift showed only a linear dependence on time, confirming that the temperature of the super-cavity was maintained a zero coefficient of thermal expansion. The frequency of the lattice laser at 759 nm was phase locked to the optical frequency comb and could be stabilized at the “absolute” frequency of the “magic wavelength”, to within a 1-MHz uncertainty. This improvement greatly reduced the fractional uncertainty due to the lattice ac Stark shift down to 2 × 10 −16 . The systematic uncertainty of the clock is currently 5.3 × 10 −15 and is dominated by the collisional frequency shift. |
Author | Mun, Jongchul Lee, Sangkyung Yu, Dai-Hyuk Lee, Won-Kyu Park, Sang Eon Park, Chang Yong Lee, Sang-Bum Kwon, Taeg Yong |
Author_xml | – sequence: 1 givenname: Dai-Hyuk surname: Yu fullname: Yu, Dai-Hyuk organization: Korea Research Institute of Standards and Science – sequence: 2 givenname: Chang Yong surname: Park fullname: Park, Chang Yong organization: Korea Research Institute of Standards and Science – sequence: 3 givenname: Won-Kyu surname: Lee fullname: Lee, Won-Kyu email: oneqlee@kriss.re.kr organization: Korea Research Institute of Standards and Science – sequence: 4 givenname: Sangkyung surname: Lee fullname: Lee, Sangkyung organization: Korea Research Institute of Standards and Science – sequence: 5 givenname: Sang Eon surname: Park fullname: Park, Sang Eon organization: Korea Research Institute of Standards and Science – sequence: 6 givenname: Jongchul surname: Mun fullname: Mun, Jongchul organization: Korea Research Institute of Standards and Science – sequence: 7 givenname: Sang-Bum surname: Lee fullname: Lee, Sang-Bum organization: Korea Research Institute of Standards and Science – sequence: 8 givenname: Taeg Yong surname: Kwon fullname: Kwon, Taeg Yong organization: Korea Research Institute of Standards and Science |
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CitedBy_id | crossref_primary_10_1063_1_4974756 crossref_primary_10_1088_1681_7575_ac1950 crossref_primary_10_1109_TIM_2016_2620187 crossref_primary_10_1109_TIM_2016_2637559 crossref_primary_10_1088_1681_7575_ad1ca9 crossref_primary_10_1088_1367_2630_18_3_033030 crossref_primary_10_1103_PhysRevLett_113_187002 crossref_primary_10_7567_JJAP_56_050302 crossref_primary_10_1364_AO_404817 |
Cites_doi | 10.1088/0026-1394/50/2/119 10.1364/JOSAB.29.000178 10.1103/PhysRevLett.104.070802 10.1103/PhysRevA.81.051603 10.1007/BF02520327 10.1139/p08-053 10.1103/PhysRevLett.99.123001 10.1103/PhysRevLett.101.170504 10.1126/science.1154622 10.1103/PhysRevLett.98.070501 10.1103/PhysRevLett.103.063001 10.1088/0026-1394/48/5/007 10.1103/PhysRevA.73.031804 10.1038/nphoton.2010.313 10.1103/PhysRevA.84.052724 10.1364/OL.19.001777 10.1103/PhysRevLett.103.135301 10.1103/PhysRevLett.100.140801 10.1038/nphoton.2012.217 10.1038/nphys1535 10.1103/PhysRevLett.93.250602 10.1126/science.1196442 10.1103/PhysRevLett.109.230801 10.1103/PhysRevLett.102.110503 10.1088/1367-2630/11/10/103033 10.1103/PhysRevLett.93.170801 10.1126/science.1153341 10.1103/PhysRevA.82.053624 |
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Keywords | Sub-Hz laser Optical frequency comb Lattice clock |
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Snippet | The current status of an Yb optical lattice clock at the Korea Research Institute of Standards and Science (KRISS) is reported. The systematic uncertainty of... |
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Title | An Yb optical lattice clock: Current status at KRISS |
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