Abstract
After a basic description of a laser in the first parts of the book, we now are dealing with the question how we can operate a laser. For this purpose, we will first discuss laser resonators. In this chapter, we treat the cavity resonator, which is a closed resonator. In the next chapter, we will study the open resonator.
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Problems
Problems
10.1
Modes of a cubic cavity. Determine the frequencies of the four modes of lowest frequencies of a cubic cavity resonator (side length \(a= 1\) cm).
10.2
Degeneracy of modes of a rectangular cavity resonator.
-
(a)
Determine the degree of degeneracy of the 011, 110, and 101 modes if \(a_1= a_2= L\).
-
(b)
Determine the degree of degeneracy of the 011, 110, and 101 modes if \(a_1= a_2 \ne L\).
-
(c)
Determine the degree of degeneracy of the 011, 110, and 101 modes if \(a_1 \ne a_2 \ne L\).
-
(d)
Determine the degree of degeneracy of the 111 mode.
10.3
Density of modes of a cavity resonator. Determine the density of modes of a cubic cavity resonator of 1 cm side length at a frequency corresponding to a vacuum wavelength \(\lambda =700\) nm for the following cases.
-
(a)
If the cube (with metallic walls) is empty,
-
(b)
If the cube contains an Al\(_2\)O\(_3\) crystal (refractive index \(\mathrm{n}= 1.8\)) and fills the cavity completely,
-
(c)
If the cube contains a GaAs crystal (\(\mathrm{n}= 3.65\)) that completely fills out the cube.
10.4
Number of modes. Determine the number of modes of a cubic cavity (side length 1 cm) in the frequency interval 1 \(\times \) 10\(^{14}\) Hz, 1.1 \(\times \) 10\(^{14}\) Hz.
10.5
Mode density on different scales. Determine the relations between the mode density on the frequency scale and on different other scales:
-
(a)
scale of photon energy \(h \nu \); (b) \(\omega \) scale; (c) scale of vacuum wavelength \(\lambda \).
10.6
Variation of the resonance frequency of a mode . By changing the length L of a resonator, the resonance frequencies change. Determine the dependence of the frequency \(\nu \) of the 101 mode on the change \(\delta L\) of the length L of a long resonator (\(L \gg a_1\)).
10.7
Density of modes in free space. Determine the density of modes of electromagnetic waves in free space. [Hint: make use of periodic boundary conditions.]
10.8
Energy of a field in a cavity resonator.
-
(a)
Determine the energy of a field in the 101 mode of a rectangular cavity resonator (width \(a_1\), height \(a_2\), length L; field of amplitude A).
-
(b)
Determine the energy content in the case that \(a_1=1\) cm, \(a_2=0.5\) cm, \(L= 2\) cm, \(A=1\) V cm\(^{-1}\).
10.9
Magnetic field in a rectangular cavity resonator.
-
(a)
Derive the wave equations describing the H field.
-
(b)
Solve the wave equations. [Hint: the normal component \(H_\mathrm{n}\) of the magnetic field is zero everywhere on the walls, \(H_\mathrm{n}\) \((\mathrm{wall})= 0\).]
10.10
TE \(_\mathrm{mnl}\) modes of a rectangular cavity resonator.
-
(a)
Determine the fields of a TE\(_\mathrm{mnl}\) mode.
-
(b)
Express the amplitudes of the field components by the amplitude of the z component of the H field. [Hint: take into account that \(\varvec{k} \times \varvec{E}= 0\) and \(\varvec{k} \times \varvec{H}= 0\).]
10.11
TM mode of a rectangular cavity resonator.
-
(a)
Determine the fields of a TM\(_\mathrm{mnl}\) mode.
-
(b)
Express the amplitudes of the field components by the amplitude of the z component of the E field.
10.12
Field components of different modes of a rectangular cavity resonator.
-
(a)
Determine the magnetic field components of the 101 mode. [Solutions are given in (10.54) and (10.55).]
-
(b)
Determine the electric and magnetic field components of the 011 mode.
-
(c)
Determine the electric and magnetic field components of the TE\(_{111}\) mode and the TM\(_{111}\) mode.
-
(d)
Show that the 101, 011 and 110 modes exist only as TE modes.
-
(e)
Show that the TE\(_\mathrm{mnl}\) and TM\(_\mathrm{mnl}\) modes are degenerate if none of the three numbers is zero.
10.13
Rectangular waveguide. If we omit in a rectangular resonator the two walls perpendicular to the z axis, we obtain a rectangular waveguide.
-
(a)
Characterize the TE mode of lowest order.
-
(b)
Characterize the TM mode of lowest order.
10.14
Show that the number of (short-wavelength) cavity modes in a frequency interval \(\hbox {d}\nu \) for a rectangular cavity is given by \((8\pi /\lambda ^{3})\hbox { }V_c \hbox { d}\nu \hbox {/}\nu ,\) where \(V\) \(_{c }\) is the cavity volume and \(\lambda \) the free-space wavelength. Show that the number of modes in a spherical cavity is given by the same expression.
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Renk, K.F. (2017). Cavity Resonator. In: Basics of Laser Physics. Graduate Texts in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-50651-7_10
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DOI: https://doi.org/10.1007/978-3-319-50651-7_10
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