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148 Chapter Four


Figure 4.26The principle of the laser.

hv′

hv′

hv′

hv′

E 2

Excited state

E 0
Ground state

E 1
Metastable
state

E 2

E 1

hv

′′
hv

′′
hv

′′
E 2

E 1

E 0 E 0

E 2

E 1

E 0

hv

hv
hv
hv
hv
hv

Atoms in ground state
are pumped to state E 2
by photons of
hv′ = E 2 – E 0 (or
by collisions).

Rapid transition to
metastable state E 1
by spontaneous
emission of photons
of hv′′ = E 2 – E 1 (or
in some other way).

Metastable states
occupied in many
atoms.

Stimulated emission occurs when
photons of hv = E 1 – E 0 are
incident, with the secondary
photons themselves inducing
further transitions to produce
an avalanche of coherent
photons.

Figure 4.27The ruby laser. In order for stimulated emission to exceed stimulated absorption, more than half the Cr3+ions in the ruby
rod must be in the metastable state. This laser produces a pulse of red light after each flash of the lamp.

Radiationless transition

Laser transition
694.3 nm

Optical pumping
550 nm

Ground state

1.79 eV

2.25 eV

Metastable state

Cr3+ ion

Xenon flash lamp

Ruby rod

Partly transparent
mirror

Mirror

of atoms, the more upward transitions there will be from the ground state to the
metastable state. However, at the same time the pumping will stimulate downward
transitions from the metastable state to the ground state. When half the atoms are in
each state, the rate of stimulated emissions will equal the rate of stimulated absorp-
tions, so the assembly cannot ever have more than half its atoms in the metastable
state. In this situation laser amplification cannot occur. A population inversion is only
possible when the stimulated absorptions are to a higher energy level than the
metastable one from which the stimulated emission takes place, which prevents the
pumping from depopulating the metastable state.
In a three-level laser, more than half the atoms must be in the metastable state for
stimulated induced emission to predominate. This is not the case for a four-level laser.

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