 |
| The hyperfine structure of the ground state
of the 133Cs atom serves as the definition of one metric second. |
The previous decades have seen impressive progress in the development
of very precise atomic frequency standards (eg. atomic clocks).
The fractional change in frequency of certain narrow microwave and
optical transitions can be measured to 10-15, with the prospect
of measurements to a precision of 10-18 on the horizon. This presents
great opportunities for applied and fundamental science, in particular
in searching for any variation of fundamental constants.
Many modern theories that unify gravity with other interactions
or describe a non-stationary universe allow fundamental constants
to vary. Analysis of quasar absorption spectra performed at our
school suggests that the fine structure constant, a, might have
been smaller in the past: 10 billion years ago it was smaller by
a tiny (10-5) fraction of its current value. If we assume that a
is changing at a constant rate over the cosmological time scale
we would expect it to still be changing at the relative rate of
10-15 per year. A variation such as this could be observed with
atomic clocks. Different atomic clocks depend differently on a so
by comparing their frequencies over a long time interval (a year
or more) any change in a can be studied.
Note that these measurements can only reveal the change in the
ratio of the atomic frequencies. Atomic calculations are needed
to link this change to any variation of a. These calculations are
performed by our group. The table shows recent constraints on possible
present day a variation obtained from using our results in conjunction
with the comparison of some extremely stable atomic frequencies
to the cesium primary frequency standard. The cesium primary frequency
standard is the frequency of the microwave transition between the
components of the 133Cs hyperfine structure. The sensitivity of
atomic clocks to the variation of a is now approaching that of quasar
absorption spectra. It is worth mentioning that the possible measurement
of the variation of a using atomic clocks was mentioned in the description
of the work awarded this year’s Noble prize.
Another way to improve the sensitivity of atomic measurements is
by finding atomic frequencies that change much faster that a if
a varies. A unique example of this can be found in the dysprosium
atom. The dysprosium atom possesses two very close levels of opposite
parity and different electron configurations. The small transition
frequency between these levels changes 108 times faster than a,
if a varies. An experiment utilizing this sensitivity is currently
underway at Berkley. The first very promising results have already
been obtained and the prospects for further improvement in accuracy
are very good.
| Clock1/Clock2 |
Da/a |
| Rb(hfs) /Cs(hfs) |
0.05(1.3) |
| Hg+(opt)/Cs(hfs) |
-0.03(1.2) |
| H(opt)/Cs(hfs) |
-1.1(2.3) |
| Yb+(opt)/Cs(hfs) |
-0.2(2.0) |
| Rb(hfs)/Cs(hfs) |
0.07(0.75) |
| The relative variation of the
fine structure constant, ?a/a in units 10-15 per year. |
Elizabeth Angstmann, Vladimir Dzuba
and Victor Flambaum
|