3. TOPICS: GAS LASERS & ATOMIC LASERS
INTRODUCTION
The first gas laser, the Helium–neon laser (HeNe), was co-invented by Iranian-
American engineer and scientist Ali Javan and American physicist William R. Bennett,
Jr., in 1960.
It produced a coherent light beam in the infrared region of the spectrum at 1.15
micrometres.
DEFINATION
A gas laser is a laser in which an electric current is discharged through a gas to produce
coherent light. The gas laser was the first continuous-light laser and the first laser to
operate on the principle of converting electrical energy to a laser light output.
4. GAS LASERS
Most widely used lasers and most varied:
• Low power ( He-Ne) to High power (CO2 ) lasers
• Operates with rarified gases as active medium excited by electric discharge
• Carbon dioxide lasers, or CO2 lasers can emit hundreds of kilowatts at 9.6 µm
and 10.6 µm, and are often used in industry for cutting and welding. The
efficiency of a CO2 laser is over 10%.
• Carbon monoxide or "CO" lasers have the potential for very large outputs, but
the use of this type of laser is limited by the toxicity of carbon monoxide gas.
Human operators must be protected from this deadly gas.
Gas lasers using many gases have been built and used for many purposes:
5. TYPES OF GAS LASER
Chemical lasers (HF Laser) Excimer Lasers
Ion Lasers
Argon Laser
Helium-Cadmium Laser Copper-Vapour Laser
6. Schematic of Gas Lasers
• In gases, energy levels of atoms involved in lasing action are well defined and
narrow; broad pump bands do not exist.
• To excite gaseous atoms; pump sources with sharp wavelengths are required =
Optical pumping not suitable for gas lasers.
• Most common method; Passing electric discharge through the gas medium.
• Gas contained in a tube with cavity mirrors.
• A high DC voltage ionizes the gas for conduction.
• Electrons in the discharge transfer energy to atoms in the gas by collisions.
7. WORKING PRINCIPLE
• It is a four energy level laser system.
• The electrons produced from electric discharge collide with He and Ne atom and
excite them to the higher energy levels He2 and Ne4 at 20.61 eV and 20.66 eV
respectively.
• These two states are metastable so the atoms may stay there for a longer time.
8. Advantages
• High volume of active material
• Active material is relatively inexpensive
• Almost impossible to damage the active material
• Heat can be removed quickly from the cavity
Applications
• He-Ne laser is mainly used in making holograms.
• In laser printing He-Ne laser is used as a source for writing on the photosensitive
material.
• He-Ne lasers were used in reading Bar Codes, which are imprinted on products in
stores. They have been largely replaced by laser diodes.
• Nitrogen lasers and excimer laser are used in pulsed dye laser pumping.
• Ion lasers, mostly argon, are used in CW dye laser pumping.
9. ATOMIC LASERS
HISTORY
• The first pulsed atom laser was demonstrated at MIT by Professor Wolfgang Ketterle
et al. in November 1996.
• Ketterle used an isotope of sodium and used an oscillating magnetic field as their
output coupling technique, letting gravity pull off partial pieces looking much like a
dripping tap.
• From the creation of the first atom laser there has been a surge in the recreation of
atom lasers along with different techniques for output coupling and in general
research.
• The current developmental stage of the atom laser is analogous to that of the optical
laser during its discovery in the 1960s.
• To that effect the equipment and techniques are in their earliest developmental
phases and still strictly in the domain of research laboratories.
• The brightest atom laser so far has been demonstrated at IESL-FORTH,
Crete, Greece.
10. DEFINATION
An atom laser is analogous to an optical laser, but it emits matter waves instead of
electromagnetic waves. Its output is a coherent matter wave, a beam of atoms which can
be focused to a pinpoint or can be collimated to travel large distances without spreading.
• It is a source capable of producing an intense, highly directional, coherent beam in
which all the atoms have the same wavelength just like the photons in a laser beam.
11. CONTINUE…
The exotic quantum phenomenon of Bose–Einstein condensation is the key ingredient in
a new type of laser that emits atoms rather than photons, and that promises to
revolutionize atom optics.
Bose-Einstein basics
• The idea for an atom laser predates the demonstration of the exotic quantum
phenomenon of Bose-Einstein condensation in dilute atomic gases. But it was only
after the first such condensate was produced in 1995 that the pursuit to create a
laser-like source of atomic de Broglie waves became intense.
• In a Bose condensate all the atoms occupy the same quantum state and can be
described by the same wavefunction.
• In a Bose-Einstein condensate all the atoms have the same energy and hence the
same de Broglie wavelength. If this property can be maintained when the atoms are
released from the condensate, we will have a highly monochromatic source of
matter waves.
12.
13. Applications
• Atom lasers are critical for atom holography. Similar to conventional holography,
atom holography uses the diffraction of atoms.
• As the de Broglie wavelength of the atoms is much smaller than the wavelength of
light, an atom laser could create much higher resolution holographic images. Atom
holography might be used to project complex integrated-circuit patterns, just a few
nanometres in scale, onto semiconductors.
• In fundamental research and industry where atomic beams are used, e.g., atomic
clocks, atom optics, precision measurements of fundamental constants, tests of
fundamental symmetries, atomic beam deposition for chip production (atom
lithography), and, more generally, nanotechnology.
The semiclassical theory of gas lasers has been reformulated by adding rate terms to the density-matrix component differential equations. The solution to these equations, in the form of a Fourier series, is applicable at high laser intensities. A calculation of the effect of phase-changing collisions is also included so that the results can be compared to experimental data taken with a He-Ne laser operating at a wavelength of 1.15 μm.
For optimum operation, in practice, laser medium contains a mixture of two gases (A&B) at low pressure.
Atoms of kind A are initially excited by electron impact.
Transfer their energy to atoms of kind B, which are actual active centres.
Cavity mirrors can be either inside the gas container or outside:
If inside, the output light is generally unpolarized.
For outside case, mirrors placed at Brewster angle = Polarized light
Atomic physicists are hoping that the invention of the “atom laser” will spark a similar revolution in the field of atom optics, or matter-wave optics as it is also known. Researchers in this field have relied heavily on the analogy between light and the wave-like nature of atoms. Lenses, mirrors and beam splitters have all been developed to control atomic beams just as their optical counterparts manipulate light. But what has been lacking in atom optics, until recently, is a source capable of producing an intense, highly directional, coherent beam in which all the atoms have the same wavelength just like the photons in a laser beam. This would be an atom laser.
In a laser all the photons share the same wavefunction. This is possible because photons have an intrinsic angular momentum, or “spin”, of the Planck constant h divided by 2p. Particles that have a spin that is an integer multiple of h/2p obey Bose-Einstein statistics. This means that more than one so-called boson can occupy the same quantum state. Particles with half-integer spin – such as electrons, neutrons and protons, which all have spin h/4p – obey Fermi-Dirac statistics. Only one fermion can occupy a given quantum state.
A composite particle, such as an atom, is a boson if the sum of its protons, neutrons and electrons is an even number; the composite particle is a fermion if this sum is an odd number.
Atom lasers and optical lasers There is a close analogy between an optical laser and an atom laser. An optical laser emits coherent electromagnetic waves, while an atom laser emits coherent matter waves, (a) In an optical laser most of the photons occupy just one or a few of the modes in the laser cavity. This cavity is typically formed by two mirrors (blue), and the modes of the laser are essentially wavelengths defined by the round-trip time of light inside the cavity. Only one mode is shown in the figure. The “gain” medium is pumped by an external source of energy to ensure that large numbers of photons are emitted into that mode. One of the mirrors is usually partially transmitting to allow photons to “leak” out of the cavity, forming a beam of coherent light (green), (b) In an atom laser, a Bose–Einstein condensate in a magnetic trap (blue) contains many atoms in a single state, the lowest-energy state of the trap. The gain medium is a thermal cloud of atoms. The atoms can be extracted from the trap by allowing them to tunnel through the confining potential. The extracted atoms form a beam of coherent matter waves (green).
Atom interferometers, which can be more sensitive than optical interferometers, could be used to test quantum theory, and have such high precision that they may even be able to detect changes in space-time. This is because the de Broglie wavelength of the atoms is much smaller than the wavelength of light, the atoms have mass, and because the internal structure of the atom can also be exploited.