TY - JOUR
T1 - Magnetic states at the surface of α-Fe2 O3 thin films doped with Ti, Zn, or Sn
AU - Ellis, David S.
AU - Weschke, Eugen
AU - Kay, Asaf
AU - Grave, Daniel A.
AU - Malviya, Kirtiman Deo
AU - Mor, Hadar
AU - De Groot, Frank M.F.
AU - Dotan, Hen
AU - Rothschild, Avner
N1 - Funding Information:
We gratefully acknowledge helpful discussions with Jaeyoung Kim, Maytal Caspary Toroker, and Amit Keren. We appreciate the use of Amit Keren's experimental facilities, and thank Itzik Kapon for preliminary magnetization tests on our samples. We thank Helmholtz-Zentrum Berlin (HZB) for the allocation of synchrotron radiation beamtime at Bessy II Berlin. D.S.E thankfully acknowledges financial support from HZB, and also acknowledges support from The Center for Absorption in Science at the Ministry of Aliyah and Immigrant absorption. This research has received funding from the European Research Council under the European Union's Seventh Framework programme (FP/200702013)/ERC Grant Agreement No. 617516. D.A.G. acknowledges support from Marie-Sklodowska-Curie Individual Fellowship No. 659491.
Publisher Copyright:
© 2017 American Physical Society.
PY - 2017/9/20
Y1 - 2017/9/20
N2 - The spin states at the surface of epitaxial thin films of hematite, both undoped and doped with 1% Ti, Sn, or Zn, respectively, were probed with x-ray magnetic linear dichroism (XMLD) spectroscopy. Morin transitions were observed for the undoped (TM≈200 K) and Sn-doped (TM≈300 K) cases, while Zn- and Ti-doped samples were always in the high- and low-temperature phases, respectively. In contrast to what has been reported for bulk hematite doped with the tetravalent ions Sn4+ and Ti4+, for which TM dramatically decreases, these dopants substantially increase TM in thin films, far exceeding the bulk values. The normalized Fe LII-edge dichroism for T<TM does not strongly depend on doping or temperature, except for an apparent increase of the peak amplitudes for T<100 K. We observed magnetic field-induced inversions of the dichroism peaks. By applying a magnetic field of 6.5 T on the Ti-doped sample, a transition into the T>TM state was achieved. The temperature dependence of the critical field for the Sn-doped sample was characterized in detail. It was demonstrated the sample-to-sample variations of the Fe LIII-edge spectra were, for the most part, determined solely by the spin orientation state. Calculations of the polarization-dependent spectra based on a spin-multiplet model were in reasonable agreement with the experiment and showed a mixed excitation character of the peak structures.
AB - The spin states at the surface of epitaxial thin films of hematite, both undoped and doped with 1% Ti, Sn, or Zn, respectively, were probed with x-ray magnetic linear dichroism (XMLD) spectroscopy. Morin transitions were observed for the undoped (TM≈200 K) and Sn-doped (TM≈300 K) cases, while Zn- and Ti-doped samples were always in the high- and low-temperature phases, respectively. In contrast to what has been reported for bulk hematite doped with the tetravalent ions Sn4+ and Ti4+, for which TM dramatically decreases, these dopants substantially increase TM in thin films, far exceeding the bulk values. The normalized Fe LII-edge dichroism for T<TM does not strongly depend on doping or temperature, except for an apparent increase of the peak amplitudes for T<100 K. We observed magnetic field-induced inversions of the dichroism peaks. By applying a magnetic field of 6.5 T on the Ti-doped sample, a transition into the T>TM state was achieved. The temperature dependence of the critical field for the Sn-doped sample was characterized in detail. It was demonstrated the sample-to-sample variations of the Fe LIII-edge spectra were, for the most part, determined solely by the spin orientation state. Calculations of the polarization-dependent spectra based on a spin-multiplet model were in reasonable agreement with the experiment and showed a mixed excitation character of the peak structures.
UR - http://www.scopus.com/inward/record.url?scp=85029950930&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.96.094426
DO - 10.1103/PhysRevB.96.094426
M3 - Article
AN - SCOPUS:85029950930
VL - 96
JO - Physical Review B
JF - Physical Review B
SN - 2469-9950
IS - 9
M1 - 094426
ER -