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Encyclopedia > Hyperfine transition

Hyperfine structure is a small perturbation in the energy levels (or spectral) of atoms due to the proton-electron dipole moment interaction. The amount of correction to the Bohr energy levels due to "hyperfine splitting" is on the order of:

where m is the mass of an electron, mp is the mass of a proton, α is the fine structure constant (1/137.036), and c is the speed of light. This is a much smaller perturbation than the fine structure or Lamb shift.


Also hyperfine structure gives the 21 cm line observed in HI region in interstellar medium.


Use in defining the SI second

The hyperfine structure transition can be used to make a microwave notch filter with very high stability, repeatability and Q factor, which can thus be used as a basis for very precise atomic clocks. Typically, the hyperfine structure transition frequency of a particular isotope of caesium or rubidium atoms is used as a basis for these clocks.


Due to the accuracy of hyperfine structure transition-based atomic clocks, they are now used as the basis for the definition of the second. One second is now defined to be exactly 9,192,631,770 cycles of the hyperfine structure transition frequency of caesium-133 atoms.


  Results from FactBites:
 
Hyperfine structure - Wikipedia, the free encyclopedia (735 words)
In atomic physics, hyperfine structure is a small perturbation in the energy levels (or spectra) of atoms or molecules due to the magnetic dipole-dipole interaction, arising from the interaction of the nuclear magnetic dipole with the magnetic field of the electron.
Carl Sagan and Frank Drake considered the hyperfine transition of hydrogen to be a sufficiently universal phenomenon so as to be used as a base unit of time and length on the Pioneer plaque and later Voyager Golden Record.
Typically, the hyperfine structure transition frequency of a particular isotope of caesium or rubidium atoms is used as a basis for these clocks.
Fine tuning of atomic frequency standards - Patent 4740761 (2812 words)
The number of atomic state transitions in the atomic frequency resonator 14 is maximum when the frequency of the phase modulated transition inducing signal 16 is equal to the hyperfine transition resonance center frequency of the resonator 14.
According to the present invention, the hyperfine transition resonance center frequency of the atomic resonator 14 remains fixed, and a DC bias offset signal 38 is applied to the input of the summing integrator 34 in the frequency-lock loop.
Since the hyperfine transition resonance center frequency f.sub.r and the new synthesized center frequency f.sub.c no longer coincide, an error signal 32 is produced which is proportionately related to the difference between f.sub.r and f.sub.c.
  More results at FactBites »


 

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