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Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due Wednesday Oct. 28
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Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms

Jan 18, 2021

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Page 1: Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms

Laser Physics I (PHYS/ECE 464), Fall 2020

Homework #8, Due Wednesday Oct. 28

Page 2: Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms
Page 3: Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms
Page 4: Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms
Page 5: Laser Physics I (PHYS/ECE 464), Fall 2020 Homework #8, Due … Laser Physics I/hw20... · 2020. 11. 20. · 8.7. Consider the ideal laser medium shown below. pump excites the atoms

(a) For this problem, the key is to recall that when the laser is oscillating, the upper state population

N2 , and thus the gain saturates to loss levels. When the cavity is blocked, N2 increases back to

its unsaturated (small signal) value.

Thus

𝑁2 ≈𝑁20

1 + 𝐼𝜈/𝐼𝑠

where 𝐼𝜈 is the total intracavity intensity.

The side fluorescence (spont. Emission) power (from a gain volume V) is

𝑃 = 𝐴21𝑁2ℎ𝜈𝑉

The ratio of fluorescence power in two cases of lasing on and off is therefore:

𝑃

𝑃0=𝑁2

𝑁20 =

1

1 + 𝐼𝜈/𝐼𝑠

(b) 𝑃

𝑃0=

1

2 leading to

𝐼𝜈

𝐼𝑠= 1

(Also remember in a high-Q cavity, output intensity would have been 𝐼𝑜𝑢𝑡 ≈𝑇2𝐼𝜈

2 , in case one was

interested!).