Magnetic Compton scattering study of Laves phase ZrFe2 and Sc doped ZrFe2: Experiment and Green function based relativistic calculations
Creators
- 1. Department of Physics, M.L. Sukhadia University, Udaipur 313001 (India)
- 2. Department of Physics, Kamla Rai College (J P University), Gopalganj, Bihar 841428 (India)
- 3. UM-DAE Centre for Excellence in Basic Sciences, Vidyanagari, Santacruz (E), Mumbai 400098 (India)
- 4. Japan Synchrotron Radiation Research Institute, SPring8, 1-1-1 Kouto, Sayo, Hyogo 976-5198 (Japan)
Description
Highlights: • Reported spin momentum densities of ZrFe2 and Zr0.8Sc0.2Fe2 using magnetic Compton spectrometer. • Discussed site-specific spin moments deduced from magnetic Compton profiles (MCPs). • Derived MCPs, density of states and site-specific spin moments using SPR-KKR method. • Discussed role of orbital moment and covalent magnetism in both the compounds. Spin momentum densities of ferromagnetic ZrFe2 and Zr0.8Sc0.2Fe2 have been measured using magnetic Compton scattering with 182.65 keV circularly polarized synchrotron radiations. Site specific spin moments, which are responsible for the formation of total spin moment, have been deduced from Compton line shapes. At room temperature, the computed spin moment of ZrFe2 is found to be slightly higher than that of Sc doped ZrFe2 which is in consensus with the magnetization data. To compare the experimental data, we have also computed magnetic Compton profiles (MCPs), total and partial spin projected density of states (DOS) and the site specific spin moments using spin-polarized relativistic Korringa-Kohn-Rostoker method. It is observed that the spin moment at Fe site is aligned antiparallel to that of Zr site in both ZrFe2 and Zr0.8Sc0.2Fe2. The MCP results when compared with vibrating sample magnetometer based magnetization data, show a very small contribution of orbital moment in the formation of total magnetic moments in both the compounds. The DOS of ferromagnetic ground state of ZrFe2 and Zr0.8Sc0.2Fe2 are interpreted on the basis of a covalent magnetic model beyond the Stoner rigid band model. It appears that on alloying between a magnetic and a non-magnetic partner (with low valence), a polarization develops on the non-magnetic atom which is anti-parallel to that of the magnetic atom.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jmmm.2018.01.069Additional details
Identifiers
- DOI
- 10.1016/j.jmmm.2018.01.069;
- PII
- S0304885317338817;
Publishing Information
- Journal Title
- Journal of Magnetism and Magnetic Materials
- Journal Volume
- 454
- Journal Page Range
- p. 125-130
- ISSN
- 0304-8853
- CODEN
- JMMMDC
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 53034707
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- COMPTON EFFECT; COMPTON SPECTROMETERS; DENSITY OF STATES; INTERMETALLIC COMPOUNDS; MAGNETIC MOMENTS; MAGNETISM; MAGNETIZATION; POLARIZATION; RELATIVISTIC RANGE; SPIN; SPIN ORIENTATION; SYNCHROTRON RADIATION; TEMPERATURE RANGE 0273-0400 K; VIBRATING SAMPLE MAGNETOMETERS; X-RAY DIFFRACTION
- Descriptors DEC
- ALLOYS; ANGULAR MOMENTUM; BREMSSTRAHLUNG; COHERENT SCATTERING; DIFFRACTION; ELASTIC SCATTERING; ELECTROMAGNETIC INTERACTIONS; ELECTROMAGNETIC RADIATION; ENERGY RANGE; FUNDAMENTAL INTERACTIONS; GAMMA SPECTROMETERS; INTERACTIONS; MAGNETOMETERS; MEASURING INSTRUMENTS; ORIENTATION; PARTICLE PROPERTIES; RADIATIONS; SCATTERING; SPECTROMETERS; TEMPERATURE RANGE
Optional Information
- Copyright
- Copyright (c) 2018 Elsevier B.V. All rights reserved.