Laser Stabilization
Victor Zhao
Stony Brook Laser Teaching Center
September 2008
Advisors: Dr. Sam Goldwasser and Dr. John Noe
Motivation
The purpose of this project was to construct a negative feedback system
for a stabilized laser and investiate its properties.
Background
Lasers are useful for their properties of coherent, monochromatic
light. Because of their monochromaticity, the operating frequencies of
many lasers are restricted to frequency ranges around the operating
atomic transition of a particular laser type. Yet it is useful to
stabilize a laser's operating frequency to a even smaller variation
through a variety of techniques.
In particular, a gas laser consists of a resonant cavity--an enclosed
tube with highly reflective mirrors at both ends--in which a gas gain
medium is enclosed and light emitted by excited atoms travels and builds
in between the two mirrors. For the light traveling in between the two
mirrors inside the resonant optical cavity to amplify properly, the
wavelength of the resonating light needs to be a divisible
half-wavelength of total length of the laser tube. The possible resonating
wavelengths, which are called resonant modes, in the tube are thus
affected by the actual lenght of the laser tube. How much light is
produced from a resonant mode is dependent on how much gain the medium
inside the tube can provide, which is centered around an atomic
transition, but is wider due to effects such as doppler-broadening, the
shifting in wavelength produced by transitioning atoms because of their
gaseous motion. The formula describing the wavelength of a resonant
mode thus follows:
[lambda] = (2*L) / n
Lambda is the wavelength of the resonant mode, L is the length of the
resonant optical cavity, and n is the mode number and is very large to
produce a wavelength within the gain curve, which indicates how much
a frequency of light is amplified by a particular atomic transition.
The individual resonant modes that travel within the laser tube and are
output have wavelengths much smaller than the width of the gain curve,
about [..]. Since the length of a laser tube is the determining factor
for the frequency of a resonant mode and therefore the frequency of
light output by the laser, many laser stabilization techniques seek to
control the length of the laser tube and therefore the wavelength of the
resonant modes.
One utilized method of controlling laser tube length is through
feedback-controlled heating of the tube, which prevents minute changes
in laser tube length due to temperature changes which nonetheless cause
significant variations in laser output frequency.
There are many applications of the laser which depend on a precise
operating frequency much narrower that of a normal laser. Such lasers
have uses in metrology, the science of measurement, where they are used
to measure precise lengths, define units of measurement, and measure
minute gravitational effects.
A stabilized laser system consisting of a short laser tube, a heater,
and negative feedback circuitry has been built and intensity measurements
have been taken.
Setup
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Measurements
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