The time according to atoms
The first step consists of selecting the hydrogen atoms in their emitting state. Once this is achieved, a cloud of these atoms is sent to a cavity called a cavity resonator. There, they are subjected to an electromagnetic wave of the appropriate frequency. When the atoms are excited, they emit a signal (very low, approximately a tenth of a picowatt!) which is captured by a detector. But an atom can be easily disturbed by a magnetic field. Therefore, it is necessary to eliminate all the effects due to residual fields (for instance, the earth’s magnetic field), which requires surrounding the system with a magnetic shield. A vacuum must be created so that the hydrogen atoms are isolated in the cavity, hence the presence of vacuum pumps. Since the cavity can only accommodate one wave at a particular frequency, its size depends on the wavelength that excites the atoms, i.e., the one they have chosen. For hydrogen, a cavity of 20 cm in diameter is required (the cavities for rubidium clocks are smaller, but these clocks are less stable). A size that cannot vary in the least, especially under the effect of temperature, otherwise this will influence the frequency and disrupt the system. Therefore, it is necessary to stabilise everything to ten-thousandth of a degree! Not to mention a system that first splits the H2 molecules in the hydrogen gas into H atoms followed by all the signal detection electronics. In short, a hydrogen maser is a relatively voluminous and heavy system, which subsequently increases the size and weight (and therefore the launching cost!) of satellites when they have to be sent into space. |
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© 2007 ULi�ge
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