The caesium standard is a primary frequency standard in which the photon absorption by transitions between the two hyperfine ground states of caesium-133 atoms are used to control the output frequency. The first caesium clock was built by Louis Essen in 1955 at the National Physical Laboratory in the UK. and promoted worldwide by Gernot M. R. Winkler of the USNO. Caesium atomic clocks are the most accurate time and frequency standards, and serve as the primary standard for the definition of the second in the International System of Units . By definition, radiation produced by the transition between the two hyperfine ground states of caesium has a frequency,, of exactly. That value was chosen so that the caesium second equalled, to the limit of human measuring ability in 1960 when it was adopted, the existing standard ephemeris second based on the Earth's orbitaround the Sun. Because no other measurement involving time had been as precise, the effect of the change was less than the experimental uncertainty of all existing measurements.
Technical details
The official definition of the second was first given by the BIPM at the 13thGeneral Conference on Weights and Measures in 1967 as: "The second is the duration of periods of the radiation corresponding to the transition between the two hyperfine levels of the ground state of the caesium 133 atom." At its 1997 meeting the BIPM added to the previous definition the following specification: "This definition refers to a caesium atom at rest at a temperature of 0 K." The BIPM restated this definition in its 26th conference, "The second is defined by taking the fixed numerical value of the caesium frequency ∆Cs, the unperturbed ground-state hyperfine transition frequency of the caesium 133 atom, to be 9 192 631 770 when expressed in the unit Hz, which is equal to s–1." The meaning of the preceding definition is as follows. The caesium atom has a ground state electron state with configuration 6s1 and, consequently, atomic term symbol2S1/2. This means that there is one unpaired electron and the total electron spin of the atom is 1/2. Moreover, the nucleus of caesium-133 has a nuclear spin equal to 7/2. The simultaneous presence of electron spin and nuclear spin leads, by a mechanism called hyperfine interaction, to a splitting of all energy levels into two sub-levels. One of the sub-levels corresponds to the electron and nuclear spin being parallel, leading to a total spin F equal to ; the other sub-level corresponds to anti-parallel electron and nuclear spin, leading to a total spin. In the caesium atom it so happens that the sub-level lowest in energy is the one with, while the sub-level lies energetically slightly above. When the atom is irradiated with electromagnetic radiation having an energy corresponding to the energetic difference between the two sub-levels the radiation is absorbed and the atom is excited, going from the sub-level to the one. After a small fraction of a second the atom will re-emit the radiation and return to its ground state. From the definition of the second it follows that the radiation in question has a frequency of exactly, corresponding to a wavelength of about 3.26 cm and therefore belonging to the microwave range.
