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ZEEMAN EFFECTS OF THE PURELY CUBIC FIELD EMISSION LINE OF $MgO:C^{3+}_{r}$ CRYSTALS

Please use this identifier to cite or link to this item: http://hdl.handle.net/1811/7944

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dc.creator Sugano, S. en_US
dc.creator Varsanyi, F. en_US
dc.date.accessioned 2006-06-15T13:06:01Z
dc.date.available 2006-06-15T13:06:01Z
dc.date.issued 1960 en_US
dc.identifier 1960-E-5 en_US
dc.identifier.uri http://hdl.handle.net/1811/7944
dc.description $^{*}$Present address: Physics Department. The joins Hopkins University, Baltimore, Maryland. en_US
dc.description Author Institution: Bell Telephone Laboratories, Incorporated en_US
dc.description.abstract “The transverse Zeeman effect, has been studied of the most conspicuous red emission line ($14,319 cm^{-1}$) of a $MgO:C^{3+}_{r}$ single crystal. This line may be considered to be due to the chromium impurities with purely cubic environments. The six Zeeman patterns have been examined experimentally, with a magnetic field parallel to the. [001], [110], and [111] directions, and with polarizations $\sigma$ and $\pi$; for each direction of the magnetic field. Comparing these patterns with the theoretical ones, it has been found that the line is a magnetic dipole radiation due to the $t^{3}_{2} \ {^{2}E} \to t^{3}_{2} \ {^{4}A_{2}}$ transition. It has also been found that, at least seemingly, the degeneracy of the initial $^{2} E$ state is not removed, in other words, the effect of the Jahn-Teller distortion does not appear in this spectrum. The longitudinal Zeeman effect will be discussed in terms of circular polarization.” en_US
dc.format.extent 92099 bytes
dc.format.mimetype image/jpeg
dc.language.iso English en_US
dc.title ZEEMAN EFFECTS OF THE PURELY CUBIC FIELD EMISSION LINE OF $MgO:C^{3+}_{r}$ CRYSTALS en_US
dc.type article en_US