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  1. P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
    [CrossRef]
  2. J. Warner, IEEE Trans. Microwave Theory Tech. MTT-21, 769 (1973).
    [CrossRef]
  3. A. YarivIEEE J. Quantum Electron. QE-9, 919 (1973).
    [CrossRef]
  4. The birefringent coupling prisms ensure that laser polarization errors give rise to TM driving fields at β values well removed from those of interest.
  5. J. Warner, 1974OSA Conf. on Integrated Optics, New Orleans.

1973 (2)

J. Warner, IEEE Trans. Microwave Theory Tech. MTT-21, 769 (1973).
[CrossRef]

A. YarivIEEE J. Quantum Electron. QE-9, 919 (1973).
[CrossRef]

1972 (1)

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

Blank, S. L.

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

LeCraw, R. C.

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

Martin, R. J.

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

Tien, P. K.

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

Warner, J.

J. Warner, IEEE Trans. Microwave Theory Tech. MTT-21, 769 (1973).
[CrossRef]

J. Warner, 1974OSA Conf. on Integrated Optics, New Orleans.

Wolfe, R.

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

Yariv, A.

A. YarivIEEE J. Quantum Electron. QE-9, 919 (1973).
[CrossRef]

Appl. Phys, Lett. (1)

P. K. Tien, R. J. Martin, R. Wolfe, R. C. LeCraw, S. L. Blank, Appl. Phys, Lett. 21, 394 (1972).
[CrossRef]

IEEE J. Quantum Electron. (1)

A. YarivIEEE J. Quantum Electron. QE-9, 919 (1973).
[CrossRef]

IEEE Trans. Microwave Theory Tech. (1)

J. Warner, IEEE Trans. Microwave Theory Tech. MTT-21, 769 (1973).
[CrossRef]

Other (2)

The birefringent coupling prisms ensure that laser polarization errors give rise to TM driving fields at β values well removed from those of interest.

J. Warner, 1974OSA Conf. on Integrated Optics, New Orleans.

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Figures (2)

Fig. 1
Fig. 1

Sketch of apparatus. For clarity the prism clamps and goniometer assembly are not shown, neither is the solenoid that biases the film magnetization parallel to the propagation direction. The goniometer has a rotation axis normal to the triangular faces of the coupling prisms.

Fig. 2
Fig. 2

Image converter display when viewing TM polarized output for various angles of TE polarized input radiation. Output beam angle increases from left to right.

Tables (2)

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Table I Summary of Experimental Data

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Table II Summary of Observations on Eigenmodes

Equations (3)

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β a , b = 1 / 2 ( β e + β m ) ± [ / 4 1 ( β e - β m ) 2 + K 2 ] 1 / 2 ,
R a , b = β e - β m ± [ ( β e - β m ) 2 + 4 K 2 ] 1 / 2 / 4 K 2 .
β = n k 0 sin [ α + sin - 1 ( sin θ / n ) ] ,

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