Stimulated Emission: Understanding Its Changing Rate

In summary: Therefore, if we consider the system at equilibrium at temperature T, the rate of change of N2 is: dN2/dt = -N2 A21 (1 + ρ(\nu)/N2 B21) = -N2 A21 (1 + 8πh\nu3/c3B21 * 1/{exp(h\nu/kT)-1})In summary, the article only considers the rate of stimulated emission, which is calculated by neglecting the other two processes (spontaneous emission and absorption) in the mathematical model. This is because we are specifically looking at stimulated emission in this case. However, in a real system, all three processes occur and the rate of change of N2
  • #1
BareFootKing
30
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I am having trouble understand why
96a7c20a95aa3406b6f4840982c7d586.png
is true I would think that the rate in which N2 is changing is the rate of stimulated emission and spontanous emission together. Why is it just the rate of stimulated emission


It is in the mathematical model section
http://en.wikipedia.org/wiki/Stimulated_emission
 
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  • #2
That's because the article is about stimulated emission only. The spontaneous emission is neglected.
 
  • #3
Why can we neglect spontaneous emission?
 
  • #4
There are some systems where spontaneous emission can be neglected, and some where this is not possible. The article considers the first type only.
 
  • #5
BareFootKing said:
I am having trouble understand why
96a7c20a95aa3406b6f4840982c7d586.png
is true I would think that the rate in which N2 is changing is the rate of stimulated emission and spontanous emission together. Why is it just the rate of stimulated emission
Actually, it's not that we neglect spontaneous emission in this case, it's that *we don't consider it* by definition, because we are computing the rate of decay by stimulated emission only.

If we consider *all 3 processes happening*, as it happens in every real system, then dN2/dt is:

dN2/dt = -N2 A21 - N2B21 ρ([itex]\nu[/itex]) + N1B12 ρ([itex]\nu[/itex]).

The 3 coefficients A21, B21 and B12 are defined by the relations:

1. Spontaneous emission dN2/dt = -A21N2
2. Stimulated emission dN2/dt = -B21N2 ρ([itex]\nu[/itex])
3. Absorption: dN1/dt = -B12N1 ρ([itex]\nu[/itex])

To find the relationship between the 3 coefficients we can consider a system at thermodynamic aequilibrium, in which ρ([itex]\nu[/itex]) is that of the blackbody:

ρ([itex]\nu[/itex]) = 8πh[itex]\nu[/itex]3/c3 * 1/{exp(h[itex]\nu[/itex]/kT)-1}

and in which N2/N1 is given by Boltzmann' statistic:

N2/N1 = exp{-(E2-E1)/kT} = exp{-h[itex]\nu[/itex]/kT}.

At the aequilibrium, dN2/dt = 0 (as well as dN1/dt) so:

0 = -N2 A21 - N2B21 ρ([itex]\nu[/itex]) + N1B12 ρ([itex]\nu[/itex])

Substituting the relations for ρ([itex]\nu[/itex]) and N2/N1 and understanding that the coefficients don't have to depend on T, it's easy to find:

i) A21 = 8πh[itex]\nu[/itex]3/c3
ii) B12 = B21
 
Last edited:

1. What is stimulated emission?

Stimulated emission is a process in which an atom or molecule in an excited state emits a photon of light after being stimulated by an external electromagnetic field.

2. How does stimulated emission differ from spontaneous emission?

Stimulated emission is a result of an external stimulus, while spontaneous emission occurs randomly without an external stimulus.

3. What is the significance of stimulated emission in lasers?

Stimulated emission is the principle behind the operation of lasers, as it allows for the production of a coherent, intense beam of light.

4. How does the rate of stimulated emission change in different mediums?

The rate of stimulated emission is dependent on the properties of the medium, such as its refractive index and population inversion. In different mediums, the rate of stimulated emission may vary and can be manipulated to control the output of a laser.

5. What are some real-world applications of stimulated emission?

Stimulated emission has a wide range of applications, including in telecommunications, medical equipment, and scientific research. It is also used in everyday devices such as DVD players and barcode scanners.

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