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◆ Quantum Science and Technology2025-10-09· Black-body radiation

Transportable strontium lattice clock with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>4</mml:mn> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>19</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> blackbody radiation shift uncertainty

Ingo Nosske, Chetan Vishwakarma, Tim Lücke, Johannes Rahm, Navraj Poudel, S. Weyers, Erik Benkler, Sören Dörscher, Christian Lisdat

原始摘要(英文原文)· Original abstract
Abstract We describe a transportable optical lattice clock based on the 1 S 0 → 3 P 0 transition of lattice-trapped 87 Sr atoms with a total systematic uncertainty of 2.1 × 10 − 18 . The blackbody radiation shift, which is the leading systematic effect in many strontium lattice clocks, is controlled at the level of 4.0 × 10 − 19 , as the atoms are interrogated inside a well-characterised, cold thermal shield. Using a transportable clock laser, the clock reaches a frequency instability of about 5 × 10 − 16 / τ / s , which enables fast reevaluations of systematic effects. By comparing this clock to the primary caesium fountain clocks CSF1 and CSF2 at Physikalisch-Technische Bundesanstalt, we measure the clock transition frequency with a fractional uncertainty of 1.9 × 10 − 16 , in agreement with previous results. The clock was successfully transported and operated at different locations. It holds the potential to be used for geodetic measurements with centimetre-level or better height resolution and for accurate inter-institute frequency comparisons.
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Transportable strontium lattice clock with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>4</mml:mn> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>19</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> blackbody radiation shift uncertainty — 科研速览 Science Skim