NIST-F1 is a cesium fountain clock, a type of atomic clock, in the National Institute of Standards and Technology (NIST) in Boulder, Colorado, and serves as the United States' primary time and frequency standard. The clock took less than four years to test and build, and was developed by Steve Jefferts and Dawn Meekhof of the Time and Frequency Division of NIST's Physical Measurement Laboratory.
The clock replaced NIST-7, a cesium beam atomic clock used from 1993 to 1999. NIST-F1 is ten times more accurate than NIST-7. It has been succeeded by a new standard, NIST-F2, announced in April 2014. The NIST-F2 standard aims to be about three times more accurate than the NIST-F1 standard, and there are plans to operate it simultaneously with the NIST-F1 clock.
The apparatus consists of an optical molasses made of counter-propagating lasers which cool and trap a gas of cesium atoms. Once trapped, the atoms are propelled upward by two vertical lasers inside a microwave chamber. Depending on the exact frequency of the microwaves, the cesium atoms will reach an excited state. Upon passing through a laser beam, the atoms will fluoresce (emit photons). The microwave frequency which produces maximum fluorescence is used to define the second.
Similar atomic fountain clocks, with comparable accuracy, are operated by other time and frequency laboratories, such as the Paris Observatory, the National Physical Laboratory (NPL) in the United Kingdom and the Physikalisch-Technische Bundesanstalt in Germany.
As of 2013, the clock's uncertainty was about 3.1 × 10−16. It is expected to neither gain nor lose a second in more than 100 million years.
The evaluated accuracy uB reports of various primary frequency and time standards are published online by the International Bureau of Weights and Measures (BIPM).
In May 2013 the NIST-F1 cesium fountain clock reported a uB of 3.1 × 10−16. However, that BIPM report and the other recent reports are based on an evaluation that dates to 2005. It used a model developed by NIST  to evaluate Doppler frequency shifts, known as distributed cavity phase, which was shown to be incorrect. The recent evaluation of NIST-F2 did not use the NIST model of distributed cavity phase used for NIST-F1 and, while NIST-F2 instead used an approach more inline with other standards, that evaluation of distributed cavity phase was shown to have other shortcomings.
- "NIST-F1 Cesium Fountain Atomic Clock: The Primary Time and Frequency Standard for the United States". NIST. August 26, 2009. Retrieved 2 May 2011.
- Ost, Laura (April 3, 2014). "NIST Launches a New U.S. Time Standard: NIST-F2 Atomic Clock". Retrieved 2 January 2015.
- T.P. Heavner, S.R. Jefferts, E.A. Donley, J.H. Shirley, and T.E. Parker, “NIST-F1: Recent Improvements and Accuracy Evaluations,” Metologia, vol. 42, pp 411-422, 2005
- S.R. Jefferts, J.H. Shirley, N. Ashby, E.A. Burt, and G.J. Dick, “Power Dependence of Distributed Cavity Phase-Induced Frequency Biases in Atomic Fountain Frequency Standards,” IEEE Trans. on Ultrasonics, Ferroelectrics, and Frequency Control, vol. 52, pp 2314-2321, 2004.
- "Comment on ‘Accurate rubidium atomic fountain frequency standard’," Ruoxin Li and Kurt Gibble, Metrologia 48, 446-447 (2011).
- Comment on 'First accuracy evaluation of NIST-F2,' Kurt Gibble, Metrologia 52, 163, January 2015
- U.S. Atomic Time
- NIST-F1 Cesium Fountain Clock
- S R Jefferts; J Shirley; T E Parker; T P Heavner; D M Meekhof; C Nelson; F Levi; G Costanzo; A De Marchi; R Drullinger; L Hollberg; W D Lee; F L Walls (2002). "Accuracy evaluation of NIST F-1" (PDF). Metrologia. 39 (4): 321–336. Bibcode:2002Metro..39..321J. doi:10.1088/0026-1394/39/4/1.