To celebrate the 60th anniversary of the first laser Joseph Braat co-author of Imaging Optics, 2019 describes his personal experiences in applied physics research dealing with lasers as special light sources and the enormous and unexpected impact of Maiman's discovery.
A rich literature is available on the discovery of Light Amplification by Stimulated Emission of Radiation and the construction of the first working (optical) ruby laser by Maiman. Personally, I very much appreciate the book The History of the Laser by Mario Bertolotti (IOP Publishing, Bristol, UK, 2005.), first edited in 1999. It presents a beautifully written time-line towards the final invention of the laser, comprising all physics developments, theoretical and experimental, that were essential for the first operation of this device on the 16th of May 1960. The book contains many illustrations to present the required material from various domains of physics, it uses just three small equations and presents a wealth of historical details. Another publication, Short history of laser development by Jeff Hecht (Opt. Eng., 49, 091002, 2010.), covers in a shorter framework the first 50 years of `laser action’. In Fig. 1 we show the impressive development, both in size and power, of the original optical laser device in 1960. In what follows I will discuss some personal experiences in applied physics research dealing with lasers as special light sources. I will also briefly sketch the vast field of laser-related research in physics (and chemistry) and give a short overview of the numerous laser applications in daily life.
(Left) Semiconductor laser in its housing. The proper laser device dimensions are typically 0.1 x 0.25 x 0.25 mm3 (Right) Part of the building that houses the Omega inertial fusion laser, ultimately meant to deliver nanosecond-duration pulses with an energy up to 2 MJ (power is 500 TW); courtesy OSA, Optics and Photonics News
As an undergraduate student, in 1966, I
was given an experimental assignment to measure the Raman effect of
nitrobenzene, using a classical mercury arc lamp as light source. To reveal the
anti- Stokes lines, exposure times of the order of eight hours were needed
overnight! In the master phase, a HeNe laser was my light source to
interferometrically measure very small angular displacements, down to 5.10-8 radians. As a graduate student at the
Institute of Optics in Paris, my research subject was the recording of
holograms with the aid of spatially incoherent light. Here I got back to my
cherished mercury arc lamp with forced cooling, making the interferometric
hologram recording rather delicate. The spatial incoherence at the hologram
recording was meant to study the influence of laser speckle. This subject was a
hot topic in the early years of laser experimenting, first to quantify the
statistics of speckle phenomena, secondly to eliminate its possibly negative influence
on hologram reconstruction noise. Reducing the speckle noise of a laser with
the aid of two diffusers in relative movement was a known principle. Another
method that proved to be successful was the time-sequential scanning of the
angle of incidence of a coherent laser beam on the object, within the total hologram
exposure time (J. Braat and S. Lowenthal. Short-exposure spatially incoherent
holography with a plane-wave illumination. J. Opt. Soc. Am. 63:388-390, 1973.).
Easy-to-fabricate consumer version of a HeNe-laser. (Left) Schematic layout of a HeNe laser cavity. (Right) Electrorestrictive cavity-length tuning element using the `sprung surfaces’ technique (J. Haisma. Gas laser. US patent 3,477,036, Sept. 10, 1969 (original Dutch application: NL6411121A, 1964)).
My next rendezvous with laser sources
was when I started working on optical disc systems at the Philips Electronics
company. Initially, this company which also owned a large lighting department,
had ambivalent feelings towards the laser source. As was often said in those
days, following Maiman’s assistant Irnee d’Haenens, the laser was `a solution in search of a problem‘. For
a consumer product company like Philips, it was clear that the typical street
price of a HeNe laser (500 to 1000 US dollar) was prohibitive for it becoming a
mass product. Optical, mechanical and electronic simplifications were needed to
bring the HeNe laser to the mass-production phase. See, for instance, Fig. 2
with some fabrication-friendly mechanical innovations enabling automatic
alignment of laser glass body, exit mirrors and cavity-length tuning unit. When
the ideas about optical data storage came about, first for frequency-modulated analogue
video signals, it was immediately clear that a classical source, even a high-pressure
mercury lamp would fall short of the required source radiance for such a system
with a typical signal bandwidth of 8 to 10 MHz. The read-out signal by means of
a diffraction-limited scanning spot focused on the information track of the
optical disc would severely suffer from the basic photon shot noise present in
the detector signal. As a comparison, a 50 W high-pressure arc lamp produces a
theoretical power of approximately 0.1 mW in a diffraction-limited focused spot,
a 1 mW HeNe-laser is capable to virtually focus its entire power in such a tiny
spot. Early optical data storage experiments quickly showed the inadequacy of
`classical’ light sources for optical data storage. It took several years to
bring the price of a classical HeNe laser down to a consumer-market level. In
the Video Long Play and LaserVision players at the end of the 1970s and the
beginning of the 1980s, some 50 to 100k HeNe lasers must have been incorporated
in the optical playing units until a new laser source was able to prove its
superior specifications for optical data storage: the AlGaAs semiconductor laser.
Its main advantages were the small volume of the light source, the high
wall-plug efficiency, its high peak power (up to a hundred mW) and, quite
importantly, its intensity modulation possibility, up to frequencies of several
hundred MHz. This latter property was essential for recording and/or
rewriteable storage systems and for optical telecommunication networks. Various
generations of this laser type have been produced, in output colour ranging
from infrared (780 nm) via red (635 to 650 nm, AlGaInP) to violet (405 nm,
GaN). The total number of produced semiconductor lasers (also present in the
majority of telecommunication networks, In-GaAsP) must exceed several billions.
Let me now briefly summarise, in
arbitrary order, the many other research fields and technical applications in
which laser sources play an essential role because of one or several specific
properties.
High power / high radiance; Melting, cutting, shaping, joining of materials, medical surgery (in particular eye surgery), nuclear fusion experiments. Nonlinear optics, optical photolithography, telecommunication.
Small size: Optical data storage, bar code scanners, laser printers, laser array sources.
Transfer of optical momentum: Optical tweezers in medical and biological research, laser cooling, single atom manipulation, creation of Bose-Einstein condensates.
Temporal coherence, specific temporal properties: Telecommunication, absorption spectroscopy, frequency-comb laser metrology, study of fundamental physical constants, nonlinear microscopic techniques.
Ultrashort pulses: Short-wavelength generation (Extreme UV and X-ray).
Spatial coherence: Holography.
The many new applications and research
fields created by the laser invention are further illustrated by the following
list of Nobel Prize laureates in physics and chemistry:
1964 (Physics) Charles Townes, Nikolay Basov & Aleksandr Prokhorov: maser/laser based oscillators
1966 (Physics) Alfred Kastler: optical spectroscopic methods
1971 (Physics) Dennis Gabor: holography
1981 (Physics) Nicolaas Bloembergen & Arthur Schawlow: laser spectroscopy
1989 (Physics) Norman Ramsey: atomic clocks based on maser or laser sources
1997 (Physics) Steven Chu, Claude Cohen-Tannoudji & William Philips: cooling and trapping of atoms with laser light
2005 (Physics) John Hall & Theodor Hänsch: optical frequency-comb laser
2014 (Physics) Shuji Nakamura: blue GaN semiconductor laser
2014 (Chemistry) Eric Betzig, Stefan Hell & William Moerner: nonlinear high-resolution fluorescence microscopy
2018 (Physics) Arthur Ashkin: optical tweezer
2018 (Physics) Gérard Mourou & Donna Strickland: ultrashort light pulses
To celebrate the 60th Anniversary of the Laser Cambridge are offering a 20% discount on selected books. Discover your discount, interesting journal articles and more laser information at our Content Hub on Cambridge Core.
Joseph Braat co-author of Imaging Optics, 2019 is Emeritus Professor of Optics at Technische Universiteit Delft, The Netherlands, and a Fellow of the Dutch Royal Academy of Arts and Sciences. Previously he was based at the Philips Research Laboratories in Eindhoven where...
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