The History of The
Principle of Self-Complementarity.
From the backgrounds of the origination and the discovery
to the extensions of the principle.
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(Minus number shows background). |
$B!]#4(B |
$B#1#9#4#1(B |
New expressions of the electromagnetic fields where both the electric and the magnetic quantities are treated on an equal basis. |
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J. A. Stratton (U.
S. A.) |
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$B!]#3(B |
$B#1#9#4#5(B |
A relationship between two radiation impedances for a narrow slot antenna and a complementary
wire antenna derived from a classical
antenna theory. |
Z1Z2$B"b(B(Z0/2)2 |
T.
Matsumoto (Hokkaido Univ.)
M. Ito (Hiroshima Tech. Coll.)
(1946)
H. G. Booker (U. K.) |
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$B!]#2(B |
$B#1#9#4#5(B |
Babinet's Principle in electromagnetic fields. |
M. Kotani (Univ. of Tokyo), G. Sunouchi (Tohoku Univ.) |
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$B!]#1(B |
$B#1#9#4#7(B |
A general relationship between two input impedances for an arbitrarily shaped slot
antenna and a complementary planar sheet antenna. |
Z1Z2 =(Z0/2)2 |
Y. Mushiake (Tohoku Univ.) |
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0 |
$B#1#9#4#8(B |
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$B#1(B |
$B#1#9#4#8(B |
Rotationally symmetric two-terminal self-complementary
planar antenna.
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Balanced type, 60$B&P(B$B"b(B188.4 [$B&8(B]. |
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Y. Mushiake (Tohoku Univ.) |
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$B#2(B |
$B#1#9#4#8(B |
Axially symmetric two-terminal self-complementary planar antenna.
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Unbalanced type, 60$B&P(B$B"b(B188.4 [$B&8(B]. |
Y. Mushiake (Tohoku Univ.) |
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$B#3(B |
$B#1#9#5#9(B |
Rotationally
symmetric four-terminal self-complementary planar antenna (turnstile type)
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Star-connection type, 30 $B&P(B$B"b(B 133.2 [$B&8(B] each. |
Y. Mushiake (Tohoku Univ.) |
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$B#4(B |
$B#1#9#5#9(B |
Rotationally
symmetric multi-terminal self-complementary planar antennas.
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Star-,
ring-, and other connections for various values of input impedances.
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G. A. Deschamps (U. S. A.) |
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$B#5(B |
$B#1#9#6#3(B |
Three-dimensional multi(N)-planar axially symmetric two-terminal self-complementary
antenna.
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Unbalanced type, 60$B&P(B/ N $B"b(B 94.2 [$B&8(B], for N=2. |
Y. Mushiake (Tohoku Univ.) |
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$B#6(B |
$B#1#9#7#2(B |
Checkerboard type multi-terminal
self-complementary planar antenna.*
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Balanced type, 60$B&P(B$B"b(B 188.4 [$B&8(B] each.. |
N. Inagaki (Nagoya Tech. Univ.) |
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$B#7(B |
$B#1#9#7#8(B |
Modified
three-dimensional self-complementary antenna.* *
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Unbalanced type, 30 $B&P(B$B"b(B 133.2 [$B&8(B]. |
T. Kasahara, T. Ishizone, Y. Mushiake (Tohoku Univ.) |
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$B#8(B |
$B#1#9#8#1(B |
Modified
three-dimensional self-complementary transmission line.
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Unbalanced type, 30 $B&P(B$B"b(B 133.2 [$B&8(B]. |
T. Ishizone (Tohoku Univ.) |
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$B#9(B |
$B#1#9#8#2(B |
Co-planar stacked self-complementary antenna. |
Unbalanced type, 60$B&P(B$B"b(B 188.4 [$B&8(B] each. |
Y. Mushiake (Tohoku Univ.) |
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$B#1#0(B |
$B#1#9#8#2(B |
Side-by-side stacked self-complementary antenna. |
Unbalanced type, 60$B&P(B$B"b(B 188.4 [$B&8(B] each. |
Y. Mushiake (Tohoku Univ.) |
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$B#1#1(B |
$B#1#9#8#2(B |
Compound-stacked self-complementary antenna. |
Unbalanced type, 60$B&P(B$B"b(B 188.4 [$B&8(B] each. |
Y. Mushiake (Tohoku Univ.) |
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$B#1#2(B |
$B#1#9#9#4(B |
Axially
symmetric self-complementary antenna with loaded multi-element.
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Unbalanced type, 60$B&P(B$B"b(B 188.4 [$B&8(B] each. |
Y. Mushiake (Tohoku Univ.) |
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* Freedom in the shape
is restricted to similitude-transformation.
* * Theoretical proof for general cases has not been
succeeded, except for the monopoly-slot type array antenna.
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