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| 001 | 102766351 | ||
| 003 | MiAaHDL | ||
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| 006 | m d | ||
| 007 | cr bn ---auaua | ||
| 008 | 090331e196610 maua bt f000 0 eng d | ||
| 035 | ⊔ | ⊔ | ‡a(MiU)990180507440106381 |
| 035 | ⊔ | ⊔ | ‡asdr-miu.990180507440106381 |
| 035 | ⊔ | ⊔ | ‡z(MiU)MIU01000000000000018050744-goog |
| 035 | ⊔ | ⊔ | ‡a(OCoLC)317483502 |
| 035 | ⊔ | ⊔ | ‡z(MiU)Aleph018050744 |
| 040 | ⊔ | ⊔ | ‡aLHL ‡beng ‡cLHL ‡dOCLCF ‡dOCLCO ‡dOCLCQ ‡dCOD ‡dRIU ‡dTRAAL |
| 049 | ⊔ | ⊔ | ‡aMAIN |
| 086 | 0 | ⊔ | ‡aD 301.45/40:274 |
| 088 | ⊔ | ⊔ | ‡aAD 648480 |
| 088 | ⊔ | ⊔ | ‡aAFCRL 66-692 |
| 100 | 1 | ⊔ | ‡aLessin, Irving. ‡eauthor. |
| 245 | 1 | 0 | ‡aEnergy levels in iron-doped sapphire / ‡cIrving Lessin. |
| 264 | ⊔ | 1 | ‡aL. G. Hansom Field, Bedford, Massachusetts : ‡bAir Force Cambridge Research Laboratories, Office of Aerospace Research, United States Air Force, ‡c1966. |
| 300 | ⊔ | ⊔ | ‡avi, 32, [3] pages : ‡billustrations ; ‡c28 cm. |
| 336 | ⊔ | ⊔ | ‡atext ‡btxt ‡2rdacontent |
| 337 | ⊔ | ⊔ | ‡aunmediated ‡bn ‡2rdamedia |
| 338 | ⊔ | ⊔ | ‡avolume ‡bnc ‡2rdacarrier |
| 490 | 0 | ⊔ | ‡aAFCRL ; ‡v66-692 |
| 490 | 0 | ⊔ | ‡aPhysical Sciences Research Papers ; ‡vNo. 274 |
| 500 | ⊔ | ⊔ | ‡a"Solid State Sciences Laboratory Project 4608." |
| 500 | ⊔ | ⊔ | ‡a"AD0648480 (from http://www.dtic.mil)." |
| 500 | ⊔ | ⊔ | ‡a"October 1966." |
| 504 | ⊔ | ⊔ | ‡aIncludes bibliographical references (page 32). |
| 520 | ⊔ | ⊔ | ‡aEnergy levels of the ferric ion in a sapphire lattice are machine-calculated as a function of applied magnetic field and polar and azimuthal angles. The levels are derived for a spin 5/2 system, wherein the Spin Hamiltonian contains one coordinate system pertaining to the cubic system and another for a trigonal system. Use is made of the rotation matrix and a set of functions belonging to an irreducible tensor operator of rank L = 4 to transform the cubic part of the Spin Hamiltonian operator into the trigonal frame of reference, and matrix elements are then calculated. As a check, the matrix elements of the cubic operator are first calculated in the cubic system, and then transformed into the trigonal system. In this connection, a table of the matrix elements of the rotation operator d(5/2) (Beta) is presented, as well as some of the matrix elements of d(4) (Beta) used in the first approach. (Author). |
| 538 | ⊔ | ⊔ | ‡aMode of access: Internet. |
| 650 | ⊔ | 0 | ‡aLasers. |
| 650 | ⊔ | 0 | ‡aCalculus of tensors. |
| 650 | ⊔ | 0 | ‡aMagnetic fields. |
| 650 | ⊔ | 0 | ‡aEnergy levels (Quantum mechanics) |
| 650 | ⊔ | 0 | ‡aCrystal lattices. |
| 650 | ⊔ | 0 | ‡aSapphires. |
| 710 | 2 | ⊔ | ‡aAir Force Cambridge Research Laboratories (U.S.) |
| 730 | 0 | ⊔ | ‡aTechnical Report Archive & Image Library (TRAIL) |
| 899 | ⊔ | ⊔ | ‡a39015095294586 |
| CID | ⊔ | ⊔ | ‡a102766351 |
| DAT | 0 | ⊔ | ‡b20230928000000.0 |
| DAT | 1 | ⊔ | ‡a20230928062550.0 ‡b2024-03-05T18:37:06Z |
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| FMT | ⊔ | ⊔ | ‡aBK |
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| 974 | ⊔ | ⊔ | ‡bMIU ‡cGWLA ‡d20240305 ‡sgoogle ‡umdp.39015095294586 ‡y1966 ‡rpd ‡qbib ‡tUS fed doc |