Shortdood13th asks:
"Could something like this technology be used to amplify LASER emissions. Lets say I've got a 5 kilo watt LASER (traveling north at 50 miles per hour, no no) and I bounce these waves (cause I like waves, I realize we are talking about more than just waves of light) back and forth in this or some similar type of recycling system. Could we hypothetically get amplification through wave harmonics?
"One of the largest draw backs to LASER systems right now is power, for example it takes about the same volume as a bus or two worth of chemical energy to power a weapons grade zapper for missile defense. Could this tech be a first step towards finding a means to buff this technology without necessarily creating a new portable power system?"
It's quite common to pump lasers with harmonics from another laser. That's how green laser pointers work. Harmonic pumping isn't particularly good for power applications, because you generally lose too much power in the conversion.
http://en.wikipedia.org/wiki/Laser_pointer...n_laser_pointerThere's also amplifying fiberoptic. Instead of putting booster relays along the fiberoptic, the fiberoptic glass itself is doped with a material that can lase to boost the signal, when pumped by another frequency injected into the fiberoptic as a power source.
Harmonic wizardry isn't very useful for military lasers, because the frequency of a chemical laser is poorly controlled -- a hydrogen-fluorine laser, for instance, is basically rocket fuel that can lase -- but there's frequency broadening due to the high temperature and collisions between atoms / molecules as they lase. With a high-powered chemical laser, you don't want to do anything to the beam except get it out the business end and on target before it fries the reaction chamber and adaptive optics.
For signaling applications, power isn't usually a problem. What limits your bandwidth is mainly dispersion in air. High-end fiberoptic cable is now transparent enough to wrap it around the planet without needing boosters. Transmission through air is a different story. The refractive index of air varies with frequency. Shaping a data pulse creates a range of frequency components ( sidebands ). These components travel at slightly different speeds in air, eventually degrading the pulse shape.
For long-distance space communications, e.g. from a probe orbiting Neptune, the signal beam suffers no distortion. The laser's power-handling capability is less important to bandwidth than the probe's power-GENERATING capability, which iu generally only a few hundred watts because solar is impractical that far from the Sun. The main bottleneck still isn't power, it's signal-to-noise ratio. The trick to getting over the noise is to transmit in ultra-short, high-powered data bursts which can get over the noise. Ultrashort-pulse lasers can in some cases reach peak power in the hundreds of billions of watts for a few femtoseconds. The catch is that to receive such a signal from a deep space probe, the receiver has to be outside the atmosphere, again because atmosphere degrades ultrashort data bursts.
You don't need to put a laser on rails to upshift laser frequency or power. A laser in motion doesn't generate harmonics -- all you get is a small-fractional doppler shift. You'd need a train traveling at very nearly lightspeed toward the laser, with a reflector on the front. There IS a way to do that, used to convert a regular laser beam into a high-powered X-ray laser pulse. What you do is put a fairly powerful laser pulse on a collision course with a pulsed beam from a charged-particle accelerator. The end-result is called Compton scattering -- some of the laser photons recoil from the charged particles, and get kicked into the X-ray range. The resultant X-ray beam isn't powerful enough to melt nissiles, but it is powerful enough to take holographic pictures of DNA reactions. To resolve features as small as a molecule, you need short-wavelength X-rays.
You might think that if a laser beam bounced off a reflector going the other way at nearly lightspeed, the laser frequency / energy per photon would merely double. Turns out you get a big boost from relativity -- because in the reference frame of a heavier charged particle going the other way at nearly lightspeed, the incoming laser photon is ALREADY compressed to an energetic X-ray ( by Lorentz contraction
http://en.wikipedia.org/wiki/Lorentz_Contraction ) and THAT energy doubles when the photon rebounds.
There are more powerful sources of coherent X-rays, such as the Z Machine at Sandia labs, which discharges a huge bank of capacitors through a cage of thin tungsten wires. As the wires are disintegrating into plasma, they lase furiously in the X-ray band.
http://en.wikipedia.org/wiki/Z_Machine X-ray lasers have been contemplated for destroying missiles, by detonating a small nuclear weapon surrounded by metal tubes aimed at the target. Again, the tubes act as X-ray lasers in the instant they turn to hot plasma. The catch is that the laser has to be in orbit because atmosphere attenuates X-rays -- but if you set off a nuke in high enough orbit to get the drop on a sub-orbital missile, the electromagnetic pulse fries most of the electronics on the continent below
http://en.wikipedia.org/wiki/Electromagnetic_pulseUntil recently, producing "bright" coherent X-rays by less extreme methods required at minimum a particle accelerator the size of a football field. However it's now possible to fit a particle accelerator on a tabletop, which shows great promise -- again using tricks of phase velocity. For a long time it was assumed [wrongly] that you could only accelerate charged particles in a high vacuum -- otherwise they'd smack into any atoms or whatever. But it turns out that particle beams can travel table-top distances through a tenuous plasma, losing only a small percentage of particles to collisions. Therein lies the secret to tabletop accelerators -- a rippling plasma can generate very high electric fields traveling at a phase velocity very close to light in a vacuum. Inject a low-energy particle beam at one end, and the particles 'surf' their way to high energy on the rippling plasma -- which oddly enough, helps focus the particle beam. A narrow beam is what you want to Compton-scatter a laser beam.
Your main question seemed to be whether tricks with refractive index can increase laser power. The short answer is, it can and it does. Researchers developing femtosecond lasers (q.v.) routinely use every trick in the book to keep the power high and the pulse short. In order to 'freeze frame' molecules 'in the act' of a chemical reaction, researchers need BOTH an ultra-short pulse, and enough total power to take the picture. Some femtosecond pulses are so powerful that their high electric fields destroy any matter they come in contact with, literally ripping off the electron shells and accelerating them to near lightspeed within under a centimeter of distance. The total energy release is fairly small -- it's the ultra-short pulse duration that concentrates such high electric fields into such a small moment in time. Femtosecond lasers have been used to delicately remove grime from centuries-old paintings, and shave microscopically thin samples of brain tissue.
Pulses of such high intensity were once thought impossible, because they'd ionize any matter they come in contact with INCLUDING THE LASER MEDIUM. The trick is to produce a longer pulse, then 'squeeze' it outside the laser, in a vacuum. Here's how they do it: a very tiny, very low-powered laser produces an ultra-short pulse of moderate field intensity, A set of mirrors and diffraction gratings then separates the pulse into frequency components, which are then reassembled by another grating into a longer pulse train that can be amplified without burning out the amplifying laser. The frequency-spreading process is then reversed, by putting the power pulse through an identical set of mirrors and gratings in reverse order. The power-pulse exits that process into a vacuum, and reassembles itself into an ultra-short power pulse on the way to the target.
The part where researchers have to use every trick in the book is to make the ultra-short pulses in the first place, so they can then be taken apart, amplified, and reassembled. See
http://www.aip.org/pnu/ search term
Normally, a pulse laser is set off by a trigger laser pulse, which passes through the laser medium setting off a cascade reaction. That's not fast enough for a femtosecond laser, because it takes too longer than femtoseconds for a trigger pulse to cross the laser. Light travels less than three tenths of a micron per femtosecond. You need to set up the pulse in advance ( "one, two, three, GO" ), so that all the atoms kick in their energy at exactly the right time. In a normal laser, the lasing atoms have plenty of time to get in synch, because the laser pulse builds up in the cavity over thousands or millions of oscillations. In a femtosecond laser, the pulse may be over and gone in as little as one wavelength, and the leading edge of the pulse is so strong it would trigger atoms to lase prematurely. So tricks of phase velocity are used to create the "One, two, three GO" effect", though of course it's more complicated than that. Harmonic effects can be useful in the pumping sequence, but you generally don't want harmonics in the output beam, because the higher the frequency, the greater the energy losses within the laser cavity, which show up as heat that has to be gotten rid of / limiis power.
Tricks with phase velocity and refractive index are just ONE tool of many. For example, the easiest way ( in principle ) to turn electrical power into laser power is to send electrons through periodic structures, so that the electron automatically interacts with periodic fields, and so that the structural automatically selects for a precise wavelength. The structural periodicity required is in the nanometer range, achievable by either nano-fabrication or by some sort of self-organizing system.
Tricks with refractive index and phase velocity get a lot easier if you can 'draw' 3-D interference patterns inside an optronic crystal -- and erase / rewrite then at will. Optically programmable crystals are a challenge in materials science / solid state physics, The behavior of interfering light waves has been thoroughly studied for over a century -- the first really good interferometer able to verify the constancy of the speed of light was built in 1886 for the Michelson-Morley Experiment. The hard part is developing optically programmable materials that do what engineers tell them.
Another promising direction in laser technology is quantum confinement. Light amplification by stimulated emission of radiation is fundamentally a quantum-mechanical process. Buckytubes ( q.v.) are turning out to have remarkable electronic and optical properties, because electrons are constrained to move in essentially oine dimension along the axis of the tube. Quantum dots don't allow an electron to move at all, and have remarkable ability to resonate with light / participate in quantum entanglement. Quantum holes in ultrathin metal sheets can trap and control light to an amazing degree. These small structures act in essence like quantum antenna arrays for light. The quantum physics involved isn't new, but it takes experimental proof-of-concept to direct research funding toward fabrication techniques for such devices. Near-total control of light is the Next Big Thing in computing, because photons light can do what electrons cannot. Light can travel through through a deeply layered chip whild generating almost no heat. Photons of light are inherently cooperative -- they don't repel each other as electrons do. Coherent light can perform complex computations ( Fourier transforms ) while traveling through a vacuum, and so on.
Researchers are even starting to have success with matter lasers -- coherent streams of atoms which can create interference patterns over distances the size of single atoms. In principle, layered geometric patterns could be 'sprayed onto' a chip by matter lasers, creating antenna structures and waveguides covering the entire range from coherent infrared light to coherent X-ray.
The problem is not lack of a 'new physics'. The physics is already on the horizon -- it just needs enough talent and enough enterprise to turn the physics into engineering, and THEN we'll see some _2001_ stuff that'll have people slack-jawed with wonder. Ya just gotta approach it the right way. Einstein's way ( the most successful to date ) was to view nature as a tapestry, and realize that we're only seeing a few threads in the near distance. By following a single thread ( the invariance of the speed of light ), Einstein arrived at some mind-boggling insights -- and because he'd really STUDIED physics, saw that they 'clicked' with other natural phenomena. An amazing thing about nature is how it all fits together -- that's the Big Clue. Seeing how physics fits together is half the fun, but ya gotta look at the tapestry, not just one knot in one thread.
--
"The trick is to find the right angle." -- Pythagoras.