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KF5JRV > TECH     15.09.16 13:33l 69 Lines 3607 Bytes #999 (0) @ WW
BID : 2007_KF5JRV
Read: GUEST
Subj: Speed of Light Standard
Path: IW8PGT<CX2SA<N0KFQ<KF5JRV
Sent: 160915/1121Z 2007@KF5JRV.#NWAR.AR.USA.NA BPQ1.4.65

Speed of light standard

The krypton-86 discharge lamp operating at the triple point of nitrogen 
(63.14 K, ) was the state-of-the-art light source for 
interferometry in 1960, but it was soon to be superseded by a new 
invention: the laser, of which the first working version was 
constructed in the same year as the redefinition of the metre.
Laser light is usually highly monochromatic, and is also coherent 
(all the light has the same phase, unlike the light from a discharge 
lamp), both of which are advantageous for interferometry.

The shortcomings of the krypton standard were demonstrated by the 
measurement of the wavelength of the light from a methane-stabilized 
helium\endash neon laser ( 3.39 nm. The krypton line was found to be 
asymmetrical, so different wavelengths could be found for the laser 
light depending on which point on the krypton line was taken for 
reference. The asymmetry also affected the precision to which the 
wavelengths could be measured.

Developments in electronics also made it possible for the first 
time to measure the frequency of light in or near the visible 
region of the spectrum, instead of inferring the frequency from 
the wavelength and the speed of light. Although visible and 
infrared frequencies were still too high to be directly measured, 
it was possible to construct a "chain" of laser frequencies that, 
by suitable multiplication, differ from each other by only a 
directly measurable frequency in the microwave region. The 
frequency of the light from the methane-stabilized laser was 
found to be 88.376\u8201?181\u8201?627(50) THz.

Independent measurements of frequency and wavelength are, in 
effect, a measurement of the speed of light (c = f\f1\'eb), and the 
results from the methane-stabilized laser gave the value for 
the speed of light with an uncertainty almost 100 times lower 
than previous measurements in the microwave region. Or, somewhat 
inconveniently, the results gave two values for the speed of 
light, depending on which point on the krypton line was chosen 
to define the metre. This ambiguity was resolved in 1975, when 
the 15th CGPM approved a conventional value of the speed of 
light as exactly 299792 m/s.

Nevertheless, the infrared light from a methane-stabilized laser 
was inconvenient for use in practical interferometry. It was 
not until 1983 that the chain of frequency measurements reached 
the 633 nm line of the helium\endash neon laser, stabilized using 
molecular iodine. That same year, the 17th CGPM adopted 
the current definition of the metre, in terms of the 1975 
conventional value for the speed of light:

    The metre is the length of the path travelled by light in 
vacuum during a time interval of 1/299,792,458 of a second.

The concept of defining a unit of length in terms of a time 
received some comment, although it was similar to Wilkins' 
original proposal in 1668 to define the universal unit of length 
in terms of the seconds pendulum. In both cases, the practical 
issue is that time can be measured more accurately than length 
(one part in 1013 for a second using a caesium clock as opposed 
to four parts in 109 for the metre in 1983). The definition in 
terms of the speed of light also means that the metre can be 
realized using any light source of known frequency, rather than 
defining a "preferred" source in advance. Given that there are 
more than 22,000 lines in the visible spectrum of iodine, any 
of which could be potentially used to stabilize a laser source, 
the advantages of flexibility are obvious.

73, Scott kf5jrv
KF5JRV @ KF5JRV.#NWAR.AR.USA.NA


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