ch1. lasers and fibres

0.0(0)
studied byStudied by 0 people
full-widthCall with Kai
GameKnowt Play
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
Card Sorting

1/16

encourage image

There's no tags or description

Looks like no tags are added yet.

Study Analytics
Name
Mastery
Learn
Test
Matching
Spaced

No study sessions yet.

17 Terms

1
New cards

characteristics of laser (4)

- highly monochromatic

- highly coherent

- highly directional

- sharply focused

(not found in ordinary night)

2
New cards

types of emmision

spontaneous emmision, stimulated emmision

3
New cards

absorption

when radiation (photon) of a frequency hits a atom and basically it goes to a higher energy level from e1 to e2

ok so the wiggly line is the photon and the ball is an atom

"Absorption of a photon of frequency f takes place when the energy difference E2 – E1 of the allowed energy states of the atomic system equals the energy hf of the photon. Then the photon disappears and the atomic system moves to upper energy state E2.”

<p>when radiation (photon) of a frequency hits a atom and basically it goes to a higher energy level from e1 to e2</p><p>ok so the wiggly line is the photon and the ball is an atom</p><p></p><p>"Absorption of a photon of frequency f takes place when the energy difference E<sub>2</sub> – E<sub>1</sub> of the allowed energy states of the atomic system equals the energy hf of the photon. Then the photon disappears and the atomic system moves to upper energy state E<sub>2</sub>.”</p>
4
New cards

spontaneous emmision

okok so basically like the photon is already at e2 right. and so the lifetime here is 10-8 sec so it cant stay there longer than that. so when it comes back down, it releases this ray thingy of radiation, but its like super scattered and random which cant be used as a laser,

  • “Spontaneous emission is the emission of a photon when a system transits from a higher energy state to a lower energy state without the aid of any external agency.

  • The average life time of the atomic system in the excited state is of the order of 10-8 s.

  • After the life time of the atomic system in the excited state, it comes back to the state of lower energy on its own accord by emitting a photon of energy hf = E2– E1 .”

<p>okok so basically like the photon is already at e2 right. and so the lifetime here is 10<sup>-8</sup> sec so it cant stay there longer than that. so when it comes back down, it releases this ray thingy of radiation, but its like super scattered and random which cant be used as a laser, </p><p></p><ul><li><p>“Spontaneous emission is the emission of a photon when a system transits from a higher energy state to a lower energy state without the aid of any external agency.</p></li><li><p>The average life time of the atomic system in the excited state is of the order of 10<sup>-8</sup> s.</p></li><li><p>After the life time of the atomic system in the excited state, it comes back to the state of lower energy on its own accord by emitting a photon of energy hf = E<sub>2</sub>– E<sub>1</sub> .”</p></li></ul><p></p>
5
New cards

time of atomic system in excited state

The average life time of the atomic system in the excited state is of the order of 10-8 s.

6
New cards

stimulated emmision

so like the atom is already at e2 right, but the thing is if it comes down by itself the radiation will be random and scattered and not laser. if theres an additional photon/ radiaiton sent then it will come back down at 10-3 seconds (metastable state), so it will come down faster

and like the radiaiton coming out is same frequency, state of polarisation, so it causes laser.

  • “When a photon (called stimulating photon) of suitable frequency interacts with an excited atomic system, the latter comes down to ground state before its life time.

  • In stimulated emission, both the stimulating photon and the stimulated photon are of same frequency, same phase and are in same state of polarization.

  • These photons are emitted in the same direction.”

Stimulated emission occurs when an excited atomic system emits a photon after being triggered by another photon of the same frequency, resulting in two coherent photons moving in the same direction.

<p>so like the atom is already at e2 right, but the thing is if it comes down by itself the radiation will be random and scattered and not laser. if theres an additional photon/ radiaiton sent then it will come back down at 10<sup>-3 </sup>seconds (metastable state), so it will come down faster</p><p>and like the radiaiton coming out is same frequency, state of polarisation, so it causes laser.</p><p></p><ul><li><p>“When a photon (called stimulating photon) of suitable frequency interacts with an excited atomic system, the latter comes down to ground state before its life time.</p></li></ul><ul><li><p>In stimulated emission, both the stimulating photon and the stimulated photon are of same frequency, same phase and are in same state of <mark data-color="yellow" style="background-color: yellow; color: inherit">polarization</mark>.</p></li><li><p>These photons are emitted in the same direction.”</p></li></ul><p></p><p>Stimulated emission occurs when an excited atomic system emits a photon after being triggered by another photon of the same frequency, resulting in two coherent photons moving in the same direction.</p>
7
New cards

polarization

light is like a bunch of tiny jump ropes and polarization means theyre moving in the same direction

  • They wiggle at the same speed (same frequency),

  • They wiggle together (same phase),

  • And they wiggle in the same direction (same polarization).

Polarization in stimulated emission means that the electric fields of both the stimulating and the emitted photons oscillate in the same direction. This makes them more coherent and is one of the reasons laser light is so uniform and powerful.

8
New cards
<p>population inversion</p>

population inversion

usually there are like more atoms in e1 than e2 but for laser basically like we need stimulated emmision right but we cant do that when theres soo less atoms in e2, so population inversion bascially just brings the ones at the bottom to the top through metastable state

k= boltzman constant

N1= density of atoms with energy E1

N2= density of atoms with energy E2

Population inversion is the condition where a greater number of atoms or molecules are in an excited state than in a lower energy state, allowing for stimulated emission to dominate over spontaneous emission.

<p>usually there are like more atoms in e1 than e2 but for laser basically like we need stimulated emmision right but we cant do that when theres soo less atoms in e2, so population inversion bascially just brings the ones at the bottom to the top through metastable state</p><p></p><p>k= boltzman constant</p><p>N<sub>1</sub>= density of atoms with energy E1</p><p>N<sub>2</sub>= density of atoms with energy E2</p><p></p><p>Population inversion is the condition where a greater number of atoms or molecules are in an excited state than in a lower energy state, allowing for stimulated emission to dominate over spontaneous emission.</p>
9
New cards

metastable state

a place higher than e2 (10-3 sec) so that atoms can undergo stimulated emmision

10
New cards

einstein’s coefficients (3 cases)

how likely it is for atom to fall or rise to different energy levels.

(i) absorption

(ii)

(iii)

(i)

  • Einstein's coefficients are parameters that describe the probability of stimulated emission, spontaneous emission, and absorption processes in atomic systems, relating the transition rates between energy levels

11
New cards

[stuff]

12
New cards

semiconductor laser

so basically like the holes and electrons right so like when an electron enters a hole it releases the light and theres like a window in the semiconductor so like there is a way for the light to come out

Semiconductor laser explanation using analogy:

  • Applying voltage (toll) lets electrons (cars) cross and recombine with holes (parking spots).

  • Recombination releases photons (honks).

  • Photons bounce between mirrors, stimulating more honking — this is stimulated emission.

  • A small window in one mirror lets out a coherent, directional beam of light — the laser.

<p>so basically like the holes and electrons right so like when an electron enters a hole it releases the light and theres like a window in the semiconductor so like there is a way for the light to come out</p><p></p><p><strong>Semiconductor laser explanation using analogy:</strong> </p><ul><li><p>Applying voltage (toll) lets electrons (cars) cross and recombine with holes (parking spots).</p></li><li><p>Recombination releases <strong>photons</strong> (honks).</p></li><li><p>Photons bounce between mirrors, stimulating more honking — this is <strong>stimulated emission</strong>.</p></li><li><p>A small window in one mirror lets out a <strong>coherent, directional beam of light</strong> — the <strong>laser</strong>.</p></li></ul><p></p>
13
New cards

applications of laser

  • barcode scanner

  • laser printer

  • laser cooling

14
New cards

optical fibers

15
New cards

total internal reflection

  • most superior type of reflection (slay)

  • almost the entire energy is returned to the first medium through relection without

<ul><li><p>most superior type of reflection (slay) </p></li><li><p>almost the entire energy is returned to the first medium through relection without </p></li></ul><p></p>
16
New cards

optical fiber

used to guide ir and visible light waved through a curved path

basically like its special bc the outer cladding thing has a higher refractive index compared to the inside thing so the light can go through total internal reflection inside it

17
New cards

numerical aperture