No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
INTERACTION BETWEEN AXIAL MODES OF A ZEEMAN LASER
1.W. L. Faust, R. A. McFarlane, C. K. N. Patel, and C. G. B. Garrett, Appl. Phys. Letters 1, 85 (1962).
2.R. L. Fork, W. J. Tomlinson, and L. J. Heilos, Appl. Phys. Letters 8, 162 (1966).
3.W. E. Lamb, Jr., Phys. Rev. 134, A1429 (1964).
4.W. Culshaw and J. Kannelaud, Phys. Rev. 141, A228 (1966).
4.Also J. Kannelaud and W. Culshaw, Phys. Rev. 141, A237 (1966).
5.R. L. Fork and C. K. N. Patel, Appl. Phys. Letters 2, 180 (1963). In this work, which used a long laser operating on the 2.026‐μ Xe transition and magnetic fields up to 6.8 kG, a dependence of the intensity ratios of the Zeeman components on the magnetic field was observed.
6.R. L. Fork and M. Sargent III, Phys. Rev. 139, A617 (1965).
7.W. Culshaw and J. Kannelaud, Phys. Rev. 145, A257 (1966). The condition is also necessary for stable two‐mode operation in regions where one mode does not quench the other.
8.A. Szöke and A. Javan, Phys. Rev. Letters 10, 521 (1963);
8.A. Szöke and A. Javan, Phys. Rev. 145, 137 (1966).
9.R. L. Fork and M. A. Pollack, Phys. Rev. 139, A1408 (1964).
10.W. Hopper and E. B. Soloman, Phys. Rev. Letters 15, 441 (1965).
Article metrics loading...
Full text loading...
Most read this month
Most cited this month