Masers serve as high precision
frequency references. These "atomic frequency standards" are one of the many forms of
atomic clocks. Masers were also used as
low-noise microwave amplifiers in
radio telescopes, though these have largely been replaced by amplifiers based on
FETs. During the early 1960s, the
Jet Propulsion Laboratory developed a maser to provide ultra-low-noise amplification of
S-band microwave signals received from deep space probes. This maser used deeply refrigerated helium to chill the amplifier down to a temperature of 4
kelvin. Amplification was achieved by exciting a ruby comb with a 12.0 gigahertz
klystron. In the early years, it took days to chill and remove the impurities from the hydrogen lines. Refrigeration was a two-stage process, with a large Linde unit on the ground, and a crosshead compressor within the antenna. The final injection was at through a micrometer-adjustable entry to the chamber. The whole system
noise temperature looking at cold sky (2.7
kelvin in the microwave band) was 17 kelvin. This gave such a low noise figure that the
Mariner IV space probe could send still pictures from
Mars back to the
Earth, even though the output power of its
radio transmitter was only 15
watts, and hence the total signal power received was only −169
decibels with respect to a
milliwatt (dBm).
Hydrogen maser The hydrogen maser is used as an
atomic frequency standard. Together with other kinds of atomic clocks, these help make up the
International Atomic Time standard ("Temps Atomique International" or "TAI" in French). This is the international time scale coordinated by the
International Bureau of Weights and Measures.
Norman Ramsey and his colleagues first conceived of the maser as a timing standard. More recent masers are practically identical to their original design. Maser oscillations rely on the stimulated emission between two
hyperfine energy levels of atomic
hydrogen. Here is a brief description of how they work: • First, a beam of atomic hydrogen is produced. This is done by submitting the gas at low pressure to a high-frequency
radio wave discharge (see the picture on this page). • The next step is "state selection"—in order to get some stimulated emission, it is necessary to create a
population inversion of the atoms. This is done in a way that is very similar to the
Stern–Gerlach experiment. After passing through an aperture and a magnetic field, many of the atoms in the beam are left in the upper energy level of the lasing transition. From this state, the atoms can decay to the lower state and emit some microwave radiation. • A high
Q factor (quality factor)
microwave cavity confines the microwaves and reinjects them repeatedly into the atom beam. The stimulated emission amplifies the microwaves on each pass through the beam. This combination of
amplification and
feedback is what defines all
oscillators. The
resonant frequency of the microwave cavity is tuned to the frequency of the hyperfine
energy transition of hydrogen: 1,420,405,752
hertz. • A small fraction of the signal in the microwave cavity is coupled into a coaxial cable and then sent to a coherent
radio receiver. • The microwave signal coming out of the maser is very weak, a few
picowatts. The frequency of the signal is fixed and
extremely stable. The coherent receiver is used to amplify the signal and change the frequency. This is done using a series of
phase-locked loops and a high performance
quartz oscillator. ==Astrophysical masers==