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  1. R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
    [CrossRef]
  2. J. F. Dillon, H. E. Earl, J. Appl. Phys. 32, 202 (1959).
    [CrossRef]
  3. F. B. Hagedorn, E. M. Gyorgy, J. Appl. Phys. 32, 282S (1961).
    [CrossRef]
  4. G. S. Krinchik, M. V. Chetkin, Sov. Phys.–JETP 13, 509 (1961).

1965 (1)

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

1961 (2)

F. B. Hagedorn, E. M. Gyorgy, J. Appl. Phys. 32, 282S (1961).
[CrossRef]

G. S. Krinchik, M. V. Chetkin, Sov. Phys.–JETP 13, 509 (1961).

1959 (1)

J. F. Dillon, H. E. Earl, J. Appl. Phys. 32, 202 (1959).
[CrossRef]

Chetkin, M. V.

G. S. Krinchik, M. V. Chetkin, Sov. Phys.–JETP 13, 509 (1961).

Dillon, J. F.

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

J. F. Dillon, H. E. Earl, J. Appl. Phys. 32, 202 (1959).
[CrossRef]

Earl, H. E.

J. F. Dillon, H. E. Earl, J. Appl. Phys. 32, 202 (1959).
[CrossRef]

Gyorgy, E. M.

F. B. Hagedorn, E. M. Gyorgy, J. Appl. Phys. 32, 282S (1961).
[CrossRef]

Hagedorn, F. B.

F. B. Hagedorn, E. M. Gyorgy, J. Appl. Phys. 32, 282S (1961).
[CrossRef]

Krinchik, G. S.

G. S. Krinchik, M. V. Chetkin, Sov. Phys.–JETP 13, 509 (1961).

LeCraw, R. C.

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

Remeika, J. P.

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

Wood, D. L.

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

Appl. Phys. Lett. (1)

R. C. LeCraw, D. L. Wood, J. F. Dillon, J. P. Remeika, Appl. Phys. Lett. 7, 27 (1965).
[CrossRef]

J. Appl. Phys. (2)

J. F. Dillon, H. E. Earl, J. Appl. Phys. 32, 202 (1959).
[CrossRef]

F. B. Hagedorn, E. M. Gyorgy, J. Appl. Phys. 32, 282S (1961).
[CrossRef]

Sov. Phys.–JETP (1)

G. S. Krinchik, M. V. Chetkin, Sov. Phys.–JETP 13, 509 (1961).

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Figures (1)

Fig. 1
Fig. 1

Latching magnetooptical polarization switch. A current pulse in the central drive wire reverses the circumferential magnetization, producing a net 90° rotation in the polarization of the transmitted light. The solid arrows correspond to one stable state, the dotted arrows to the other.

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