Of the seven SI base units, the second is by far the most precisely realized. Modern atomic clocks reach accuracies orders of magnitude beyond any direct length, mass, or temperature measurement. This is why the 2019 SI redefinition anchored four other base units on top of the second.

A short history

Before the 20th century. The second was defined as $\dfrac{1}{86400}$ of a mean solar day:

$$
1\ \text{s} \;=\; \dfrac{1\ \text{mean solar day}}{86400}
$$

Intuitive, but it rested on an assumption that turned out to be wrong: Earth’s rotation is not uniform. Tidal friction from the Moon slowly brakes Earth, and the solar day lengthens by about 2 ms per century. Irrelevant for daily life; a real problem for astronomy and navigation.

1956 (ephemeris second). CIPM redefined the second as a fraction of the 1900 tropical year:

$$
1\ \text{s} \;=\; \dfrac{1}{31{,}556{,}925.9747}\ \text{of the tropical year 1900}
$$

This dropped Earth’s rotation and anchored the second to Earth’s orbit around the Sun (more stable). Big drawback: could not be realized in a lab — required years of astronomical observations.

1967 (current). The CGPM redefined the second using a specific atomic transition in Cs-133:

$$
1\ \text{s} \;=\; 9{,}192{,}631{,}770 \times T
$$

where $T$ is the period of the electromagnetic radiation emitted by the transition between the two hyperfine sublevels of the ground state of Cs-133 (F=4 → F=3, $\Delta F = \pm 1$) at 0 K — i.e., a radiation frequency of exactly 9,192,631,770 Hz.

Why this odd number? Not arbitrary: chosen so the new definition would numerically agree with the older ephemeris second, keeping historical astronomical records valid. Nature did not dictate the number — international agreement did.

2019 (SI redefinition). The second’s definition did not change, but its role did: it became the anchor from which the meter (via constant $c$), the kilogram (via Planck’s constant $h$), and the ampere (via electron charge $e$) are all derived.

Why Cs-133?

Atomic clocks — real precision

Modern atomic clocks reach staggering precision:

Generation Example Relative uncertainty
First (1950s) NBS-1 $\sim 10^{-9}$
Microwave fountain NIST-F1 $\sim 10^{-16}$
Optical lattice (Sr, Yb) current best $\sim 10^{-18}$

$10^{-18}$ means a drift of about 1 second over 30 billion years — longer than the age of the universe.

Consequence: optical clocks are now so far ahead of Cs-based clocks that the SI second may itself be redefined via an optical transition sometime in the 2030s. The same move that happened for the meter in 1983 is now brewing for the second.

🔬 Want to know how these clocks actually work?
The six-stage cycle — from laser cooling to Ramsey interferometry and the feedback loop — is walked through in a supplementary article:
Appendix — How the cesium atomic clock works

The pattern

Era Anchor
Before 1956 Earth’s rotation
1956 Earth’s orbit around the Sun
1967 Hyperfine transition in Cs-133
Coming (probably 2030s) Optical transition in Sr or Yb

The pattern from the meter repeats: move from a variable phenomenon (Earth’s rotation), to a more stable one (an atom), to an even more stable one (optical clocks). Each step is a jump in precision, and other base units can inherit that precision.

What you should be able to do

After this section you should be able to:

📚 See also: Halliday Vol 1, Ch 1 §1-5 (time standard).
🎓 Watch: Veritasium — “The Insane Precision of Atomic Clocks” (youtube.com/@veritasium).
📖 Free reading: NIST Time and Frequency (nist.gov/pml/time-and-frequency-division).
📖 SI Brochure (9th ed.), BIPM — appendix on unit definitions (bipm.org).

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