2.1 ev Group Metastable second 1.67 ev 1.17 ev (1.06 µm) 0.50 eV First 0 ev Ground state Figure 30.64 Neodymium atoms in glass have these energy levels, one of which is metastable. The group of levels above the metastable state is convenient for achieving a population inversion, since photons of many different energies can be absorbed by atoms in the ground state.

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Chapter7: Quantum Theory Of The Atom
Section: Chapter Questions
Problem 7.113QP
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Some of the most powerful lasers are based on the energy levels of neodymium in solids, such as glass, as shown in Figure 30.64. Verify that the 1.17 eV transition produces 13.06 μm radiation.

2.1 ev
Group
Metastable
second
1.67 ev
1.17 ev (1.06 µm)
0.50 eV
First
0 ev
Ground state
Figure 30.64 Neodymium atoms in glass have these energy
levels, one of which is metastable. The group of levels above
the metastable state is convenient for achieving a population
inversion, since photons of many different energies can be
absorbed by atoms in the ground state.
Transcribed Image Text:2.1 ev Group Metastable second 1.67 ev 1.17 ev (1.06 µm) 0.50 eV First 0 ev Ground state Figure 30.64 Neodymium atoms in glass have these energy levels, one of which is metastable. The group of levels above the metastable state is convenient for achieving a population inversion, since photons of many different energies can be absorbed by atoms in the ground state.
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