Element specific magnetic hysteresis loops of AlMnFeGe spin-glass alloy
Inquiry number
SOL-0000001172
Beamline
BL25SU (Soft X-ray Spectroscopy of Solid)
Scientific keywords
A. Sample category | inorganic material |
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B. Sample category (detail) | metal, alloy, magnetic material |
C. Technique | absorption and its secondary process |
D. Technique (detail) | MCD, LD |
E. Particular condition | polarization (circular), ultra-high vacuum, surface, low-T (~ liquid He), magnetic field (< 2 T) |
F. Photon energy | soft X-ray |
G. Target information | spin/magnetism |
Industrial keywords
level 1---Application area | storage device, industrial material |
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level 2---Target | HD,MO |
level 3---Target (detail) | magnetic layer |
level 4---Obtainable information | magnetic moment |
level 5---Technique | XMCD |
Classification
A30.20 surface・interface, A80.14 magnetic materials, M40.40 soft x-ray spectroscopy
Body text
X-ray magnetic circular dichroism (XMCD) is a powerful tool to study magnetic properties of materials. XMCD gives information of electronic state and magnetic moments. Element specificity is inherent at the absorption edges, which is a great advantage of XMCD. Figure shows ESMH of Al40Mn25Fe15Ge20 quasicrystal at the Mn and Fe L2,3-edges at 25K.At 25K,the magnetic property of Al40Mn25Fe15Ge20 quasicrystal has been characterized as the spin glass system of Tg=41K. A significant difference has been found in the ESMH loops between Mn and Fe in the quasicrystal, where only the Mn loop has an obvious remanent-like magnetization. This result of ESMH has suggested that Mn and Fe magnetic moments have different magnetic viscosity in the spin-glass quasicrystal.
[ T. Nakamura, Y. Yokoyama, N. Kamakura, T. Matsushita, T. Hirono, T. Muro and K. Kobayashi, Nuclear Instruments and Methods in Physics Research B 238, 251-254 (2005), Fig. 2,
©2005 Elsevier Science Publisher ]
Source of the figure
Original paper/Journal article
Journal title
T. Nakamura et al., Nucl. Instr. and Meth. B, 238 (2005) 251-254
Figure No.
2
Technique
XMCD is defined as the difference of absorption coefficients between the left- and right handed circularly polarized soft x-rays .XMCD signal is recorded synchronizing with the helicity switching by 1 Hz using the twin helical undulators. XMCD spectrum and ESMH are obtained by rotating the grating angle and the magnetic field, respectively. The present example was measured using the electromagnet type XMCD spectrometer installed at BL25SU.
[ T. Nakamura, T. Muro, F.-Z. Guo, T. Matsushita, T. Wakita, T. Hirono, Y. Takeuchi and K. Kobayashi, Journal of Electron Spectroscopy and Related Phenomena 144-147, 1035-1038 (2005), Fig. 2,
©2005 Elsevier Science Publisher ]
Source of the figure
Original paper/Journal article
Journal title
T. Nakamura et. al, J. Elecron. Spectrosc. and Relat Phenom. 144-147, 1035-1038 (2005).
Figure No.
1
Required time for experimental setup
4 hour(s)
Instruments
Instrument | Purpose | Performance |
---|---|---|
Magnetic Circular Dichroism Measurement System (MCD) | Measurements of ESMH | 1.9 T, 16K - 300K |
References
Document name |
---|
T. Nakamura et. al, J. Elecron. Spectrosc. and Relat Phenom. 144-147, 1035-1038 (2005). |
T. Muro et al., AIP conference proceedings 705, 1051 (2004). |
Related experimental techniques
ESMH using hard x-ray at the BL39XU, VSM, SQUID, PEEM, Kerr effect, Mossbauer spectroscopy
Questionnaire
This solution is an application of a main instrument of the beamline.
Similar experiments account for more than 30% of the beamline's subject.
This solution is application of a new instrument installed in the past two years.
Ease of measurement
Easy
Ease of analysis
Easy
How many shifts were needed for taking whole data in the figure?
Two-three shifts