Abstract
By use of the Babinet principle it is proved that the electric singularity exponent for a conducting plane sector is identical to the magnetic singularity exponent for the complementary sector.
| Original language | English |
|---|---|
| Pages (from-to) | 1484-1485 |
| Number of pages | 2 |
| Journal | Electronics Letters |
| Volume | 27 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - 1991 |