000057127 001__ 57127
000057127 005__ 20211109141620.0
000057127 0247_ $$2DOI$$a10.1088/1367-2630/8/10/254
000057127 0247_ $$2WOS$$aWOS:000241655500001
000057127 0247_ $$2Handle$$a2128/28965
000057127 037__ $$aPreJuSER-57127
000057127 041__ $$aeng
000057127 082__ $$a530
000057127 084__ $$2WoS$$aPhysics, Multidisciplinary
000057127 1001_ $$0P:(DE-HGF)0$$aValencia, S.$$b0
000057127 245__ $$aFaraday rotation spectra at shallow core levels: 3p edges of Fe, Co, and Ni
000057127 260__ $$a[Bad Honnef]$$bDt. Physikalische Ges.$$c2006
000057127 300__ $$a254
000057127 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000057127 3367_ $$2DataCite$$aOutput Types/Journal article
000057127 3367_ $$00$$2EndNote$$aJournal Article
000057127 3367_ $$2BibTeX$$aARTICLE
000057127 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000057127 3367_ $$2DRIVER$$aarticle
000057127 440_0 $$08201$$aNew Journal of Physics$$v8$$x1367-2630
000057127 500__ $$aRecord converted from VDB: 12.11.2012
000057127 520__ $$aWe present magneto-optical ( MO) Faraday spectra measured at the 3(p) edges of Fe, Co, and Ni. A polarization analysis of the final state of the transmitted radiation is employed to determine the Faraday rotation at these edges. The MO effect becomes resonantly enhanced at the 3p edges and accordingly large values for the intrinsic rotation constant k of 2.2 x 10(5), 1.5 x 10(5) and 0.8 x 10(5) deg/mm for the three ferromagnetic elements Fe, Co, and Ni, respectively, have been measured. These values are large and comparable to those observed at the 2p edges. This remarkable feature emphasizes the importance of the exchange ( EX) splitting over the spin-orbit ( SO) interaction of the core levels in determining MO effects in the extreme ultra-violet ( EUV) region. From these measurements the complete set of MO constants at the 3p edges has been derived.
000057127 536__ $$0G:(DE-Juel1)FUEK414$$2G:(DE-HGF)$$aKondensierte Materie$$cP54$$x0
000057127 588__ $$aDataset connected to Web of Science
000057127 650_7 $$2WoSType$$aJ
000057127 7001_ $$0P:(DE-HGF)0$$aGaupp, A.$$b1
000057127 7001_ $$0P:(DE-HGF)0$$aGudat, W.$$b2
000057127 7001_ $$0P:(DE-HGF)0$$aMertins, H.-Ch.$$b3
000057127 7001_ $$0P:(DE-HGF)0$$aOppeneer, P. M.$$b4
000057127 7001_ $$0P:(DE-HGF)0$$aAbramsohn, D.$$b5
000057127 7001_ $$0P:(DE-Juel1)130948$$aSchneider, C. M.$$b6$$uFZJ
000057127 773__ $$0PERI:(DE-600)1464444-7$$a10.1088/1367-2630/8/10/254$$gVol. 8, p. 254$$p254$$q8<254$$tNew journal of physics$$v8$$x1367-2630$$y2006
000057127 8567_ $$uhttp://dx.doi.org/10.1088/1367-2630/8/10/254
000057127 8564_ $$uhttps://juser.fz-juelich.de/record/57127/files/Valencia_2006_New_J._Phys._8_254.pdf$$yOpenAccess
000057127 909CO $$ooai:juser.fz-juelich.de:57127$$popenaire$$popen_access$$pVDB$$pdriver$$pdnbdelivery
000057127 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt bis 2009
000057127 9141_ $$aNachtrag$$y2006
000057127 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000057127 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000057127 9201_ $$0I:(DE-Juel1)VDB38$$d31.12.2006$$gIFF$$kIFF-IEE$$lElektronische Eigenschaften$$x1
000057127 9201_ $$0I:(DE-82)080009_20140620$$gJARA$$kJARA-FIT$$lJülich-Aachen Research Alliance - Fundamentals of Future Information Technology$$x2
000057127 970__ $$aVDB:(DE-Juel1)89872
000057127 980__ $$aVDB
000057127 980__ $$aConvertedRecord
000057127 980__ $$ajournal
000057127 980__ $$aI:(DE-Juel1)PGI-6-20110106
000057127 980__ $$aI:(DE-82)080009_20140620
000057127 980__ $$aUNRESTRICTED
000057127 9801_ $$aFullTexts
000057127 981__ $$aI:(DE-Juel1)PGI-6-20110106
000057127 981__ $$aI:(DE-Juel1)VDB881