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fxdung
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If we do not consider diffraction,why lasers rays are parallel?Do atoms stimulatedly emission photons in same direction?It seems to me stimulated emission photons have same frequancy but random in direction?
fxdung said:I do not understand why stimulatedly emitted photon has the same phase and direction as the incident photon?
What source did you read that didn’t mention the direction? Perhaps you should use a better source like Wikipediafxdung said:I have learned about stimulated emission in lasers. I know that laser is nearly monochromatic.But I do not know whether there is a random in direction in stimulated emission or there is only one direction in stimulated emission.
Dale said:Perhaps you should use a better source like Wikipedia
fxdung said:I do not understand why stimulatedly emitted photon has the same phase and direction as the incident photon?
DaveE said:A good foundation in quantum mechanics is required at a minimum.
fxdung said:It seems to me stimulated emission photons have same frequancy but random in direction?
My intuitive thought is that photons go and back between two parallel mirrors many times with increasing their numbers. From this two-way route some of them escape beyond one mirror to form a straight beam.fxdung said:If we do not consider diffraction,why lasers rays are parallel?
The effect of the laser resonator is really a different thing than stimulated emission. By providing a structure that selects a particular direction of radiation to send back to through the gain medium, the resonator just makes almost all of the photons that cause stimulated emission to be coherent.anuttarasammyak said:My intuitive thought is that photons go and back between two parallel mirrors many times with increasing numbers. From their route axis some of them escape to form a beam.
fxdung said:Why the stimulated emission polarization of photon is the same as incident photon?
PeterDonis said:Same answer as I gave in post #11: the polarization is part of the photon's state, and the stimulated emission photon is emitted in the same state as the photons that are already present.
Drakkith said:Within the medium, is there a particular axis along which most of the photons generated by spontaneous emission move?
PeterDonis said:AFAIK spontaneous emission photons would be emitted with random momentum and polarization.
Yes. The photons that start in the correct direction get fed back through the gain medium and are amplified by SE. Then there are a bunch more photons going in the correct direction and phase that also get amplified, etc. The gain is big for the desired photons and below 1 for the others (way below 1). So the ones that grow in numbers take over the distribution. For the transitions of interest the excited state doesn't have much spontaneous emission (long upper state lifetime) compared to the huge number of circulating photons. A typical output coupler is maybe 1-10%, which means a 1W laser output has 10-100W bouncing back and forth in the resonator constantly causing depopulation of the excited state by stimulated emission.Drakkith said:that the photons that don't get generated along this axis are quickly absorbed by the medium/cavity walls, leading to an avalanche effect where the on-axis photons end up stimulating the emission of the vast majority of photons by virtue of surviving longer than the off-axis ones.
They have the same state. But to see it in terms of electric field amplitude, one needs to take the state from Eq 1.40 and do something like Eq. 1.19 and Eq 1.20 in the notes by Genes. For the phase, I think there was a reference to a phase operator in one of your other threads, maybe see if you can do a similar calculation for the phase as for the electric field amplitude.fxdung said:And why stimulated emission photon is in phase with incident photon(Genes only explains the two photon have same direction)?
The spontaneous emission is one important source of the linewidth of the laser light. This minimal linewidth is inversely proportional to the lawer power, because the more intense the lase is the more the stimulated emission dominates over the spontaneous.PeterDonis said:AFAIK spontaneous emission photons would be emitted with random momentum and polarization. However, I don't think spontaneous emission is significant in a laser compared to stimulated emission.
DaveE said:Yes. The photons that start in the correct direction get fed back through the gain medium and are amplified by SE. Then there are a bunch more photons going in the correct direction and phase that also get amplified, etc. The gain is big for the desired photons and below 1 for the others (way below 1). So the ones that grow in numbers take over the distribution. For the transitions of interest the excited state doesn't have much spontaneous emission (long upper state lifetime) compared to the huge number of circulating photons. A typical output coupler is maybe 1-10%, which means a 1W laser output has 10-100W bouncing back and forth in the resonator constantly causing depopulation of the excited state by stimulated emission.
Saw said:This correct explanation that you give is the one that once gave me comfort as to why, if you shine two lasers upwards from the centers of two wagons in relative motion wrt each other that are momentarily side by side, they both hit the mid-points of the respective ceilings, whereas if the lasers point in the same direction, the beams will be traveling together. In the second case, the motion of the source does not affect the outcome, which is the same behavior in both cases (even if, due to te interplay of time and length, one can still hold that relativity holds in each wagon), but in the first case, the outcomes are actually different, as if the motion of the source did affect light's behavior.
A laser's beam is parallel because of the unique properties of laser light. Unlike regular light, which is made up of many different wavelengths and travels in all directions, laser light is made up of a single wavelength and travels in a very narrow beam. This is due to the process of stimulated emission, where photons are emitted in a specific direction and at the same wavelength as the incoming photons, causing the beam to stay focused and parallel.
A laser produces parallel light through a process called optical amplification. This involves exciting atoms in a laser medium (such as a gas or crystal) with energy, causing them to emit photons in a specific direction and at a specific wavelength. These photons then stimulate other excited atoms to emit more photons in the same direction and wavelength, creating a coherent and parallel beam of light.
While a laser beam can be very close to being perfectly parallel, it can never be completely parallel due to factors such as diffraction and imperfections in the laser medium. These factors can cause the beam to slightly diverge or spread out over long distances, but the beam will still remain much more parallel than regular light.
The parallel beam of a laser has many practical applications in various fields such as medicine, communication, and manufacturing. It is used in laser cutting and welding, laser printing, laser eye surgery, and fiber optics for high-speed data transmission. The parallel nature of the beam allows for precise and controlled delivery of energy, making it useful in a wide range of applications.
While the parallel beam of a laser has many advantages, there are also some disadvantages. One of the main drawbacks is that the beam can be harmful to the eyes and skin if not used properly, as it is highly concentrated and can cause burns. Additionally, the equipment and technology required to produce and control a laser beam can be expensive and complex, making it less accessible for some applications.