The measurement of tunnel triodes by a small ac signal r parameter technique is shown to give a new way of directly measuring the oxide barrier height and barrier asymmetry. This type of measurement permits distinguishing between true hot‐electron collection and leakage currents. A saturation of the hot electron transport coefficient has been found vs the emitter‐base bias. The most direct explanation for this saturation is that those hot electrons which are collected are mainly ballistic, i.e., that they have come from the emitter with little or no momentum change due to collisions. The Al base attenuation length has been measured to be 150 Å at 77°K for electrons 2.0 eV above the Fermi level. Collector‐voltage dependence of the triode has been explained on the basis of electron‐phonon losses in the collector oxide. The major part of the large hot electron attenuation factor in these triodes cannot be explained by either metal base losses or electron‐phonon losses in the oxides, which together give rise to an attenuation factor of ≈ (¼) in a typical triode. An interfacial loss mechanism appears to be the most likely explanation for the large attenuation factor of ≈ (1/100) remaining after taking the above volume losses into account.

1.
There have been many investigations of tunnel cathodes. Two of the more recent papers which refer to earlier literature are the following:
E. D.
Savoye
and
D. E.
Anderson
,
J. Appl. Phys.
38
,
3245
(
1967
),
and
Robert M.
Handy
,
J. Appl. Phys.
37
,
4620
(
1966
).
See also Refs. 28 and 29.
2.
C. A.
Mead
,
Proc. IRE
48
,
359
(
1960
).
3.
C. A.
Mead
,
J. Appl. Phys.
32
,
646
(
1961
).
4.
G. T.
Advani
,
J. M.
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, and
M. S.
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,
Proc. IRE
50
,
1530
(
1962
).
5.
O. L.
Nelson
and
D. E.
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,
J. Appl. Phys.
37
,
66
(
1966
).
6.
Although early investigations (Refs. 2, 3) have reported α to be 0.1–0.3, these values would appear to be anomalously large due perhaps to an emitter collector diode and not to hot‐electron collection. See Sec. III.A.
7.
J. J.
Quinn
,
Phys. Rev.
126
,
1453
(
1962
).
8.
J. F.
Delord
,
K. H.
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R. E.
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,
B.
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,
C.
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, and
M.
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,
Appl. Phys. Letters
11
,
287
(
1967
).
9.
Varian Associates, Palo Alto, California.
10.
Designed by A. G. Baker and manufactured by Varian Associates.
11.
S. R.
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and
C. E.
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,
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35
,
1503
(
1964
).
12.
J. L.
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110
,
1240
(
1963
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13.
S. R.
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C. E.
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,
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233
,
497
(
1965
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14.
See, e.g., A. W. Lo et al., Transistor Electronics (Prentice‐Hall, Inc., Englewood Cliffs, N.J., 1955).
15.
Keithley Instruments Inc., Cleveland, Ohio.
16.
The phase detector which was used for null detection averaged the magnitude of that component of the 1 Hz signal which was in phase with ie over about 10 sec.
17.
G. W.
Lewicki
and
C. A.
Mead
,
Appl. Phys. Letters
8
,
98
(
1966
).
18.
J. G.
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34
,
2581
(
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19.
E. E.
Huber
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,
Appl. Phys. Letters
8
,
169
(
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A.
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M.
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G. S.
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14
,
219
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21.
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37
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77
(
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22.
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34
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23.
J. G.
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24.
D. V.
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33
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25.
E.
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6
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26.
R. W. Davies (private communication).
27.
R. N.
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F.
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156
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364
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28.
C. A.
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,
56
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29.
R. E.
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and
L. W.
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7
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R. W.
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C. R.
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32.
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J. G.
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34.
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35.
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28
,
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(
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).
36.
R. H.
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,
Phys. Rev.
106
,
874
(
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).
37.
E. A.
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R. A.
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120
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(
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).
38.
H.
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,
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8
,
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(
1967
).
39.
H. Mayer in Structure and Properties of Thin Films, C. A. Neugebauer et al., Eds. (John Wiley & Sons, Inc., New York, 1959).
40.
J. G.
Simmons
and
R. R.
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,
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A301
,
77
(
1967
).
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