Dousmanis etal. [Phys. Rev. 133, A316 (1964)] demonstrated that GaAs light‐emitting diodes could produce a cooling effect if the quantum efficiency (ratio of photon flux to junction current) is very close to unity (e.g., >0.97). Here, it is pointed out that for narrow‐bandgap semiconductors, the quantum efficiency need not be so high to produce cooling. Also, for narrow‐bandgap semiconductors there is an additional cooling mode in which the reverse‐biased diode cools its radiant environment by absorbing infrared radiation. Maximum cooling rates per unit of junction area are on the order of n2σT4, where n is the index of refraction, σ is the Stefan–Boltzmann constant, and T is the temperature. For small cooling rates the efficiency for cooling can approach the limit imposed by the second law of thermodynamics.

1.
K.
Lehovec
,
C. A.
Accardo
, and
E.
Jamgochian
,
Phys. Rev.
89
,
20
25
(
1953
).
2.
J.
Tauc
,
Czechosl. J. Phys.
7
,
275
276
(
1957
).
3.
W. E. Bradley, U.S. Patent No. 2 898 743 (1959).
4.
R. J.
Keyes
and
T. M.
Quist
,
Proc. IRE
,
50
,
1822
1823
(
1962
).
5.
G. C.
Dousmanis
,
C. W.
Mueller
, and
H.
Nelson
,
Appl. Phys. Lett.
3
,
133
135
(
1963
).
6.
G. C.
Dousmanis
,
C. W.
Mueller
,
H.
Nelson
, and
K. G.
Petzinger
,
Phys. Rev.
133
,
A316
A318
(
1964
).
7.
L.
Landau
,
J. Phys. (Moscow)
10
,
503
506
(
1946
).
8.
M. A.
Weinstein
,
J. Opt. Soc. Am.
50
,
597
602
(
1960
).
9.
P.
Gerthsen
and
E.
Kauer
,
Phys. Lett.
17
,
255
256
(
1965
).
10.
P. T.
Landsberg
and
D. A.
Evans
,
Phys. Rev.
166
,
242
246
(
1968
).
11.
O.
Kafri
and
R. D.
Levine
,
Opt. Commun.
12
,
118
122
(
1974
).
12.
Yu. P.
Chukova
,
Sov. Phys. JETP
41
,
613
616
(
1976
).
13.
P. T.
Landsberg
and
G.
Tonge
,
J. Appl. Phys.
51
,
R1
R20
(
1980
).
14.
Other physical configurations can lead to thermodynamically similar devices. One example of interest is a thin semiconducting layer in a parallel magnetic field, whose two surfaces are treated to have very different recombination rates. If electrical current is passed through such a layer, transverse to the magnetic field, the resistance is low in one direction and high for the other polarity. Positive luminescence due to carrier recombination is seen for forward bias and negative luminescence for reverse bias. See, for example,
S. S.
Bolgov
,
V. K.
Malyutenko
, and
V. I.
Pipa
,
Sov. Phys. Semicond.
17
,
134
137
(
1983
);
T.
Morimoto
and
M.
Chiba
,
Phys. Lett.
85A
,
395
398
(
1981
);
F. R.
Kessler
and
J. W.
Mangelsdorf
,
Phys. Status Solidi B
105
,
525
535
(
1981
).
15.
P.
Würfel
,
J. Phys. C
15
,
3967
3985
(
1982
).
16.
A.
De Vos
and
H.
Pauwels
,
Appl. Phys.
25
,
119
125
(
1981
).
This content is only available via PDF.
You do not currently have access to this content.