X-ray diffraction experiments under strong pulsed magnetic fields
Inquiry number
SOL-0000001024
Beamline
BL22XU (JAEA Actinide Science I)
Scientific keywords
A. Sample category | inorganic material, research on method, instrumentation |
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B. Sample category (detail) | magnetic material, solid-state crystal |
C. Technique | X-ray diffraction, absorption and its secondary process |
D. Technique (detail) | single crystal, magnetic scattering, XANES |
E. Particular condition | polarization (linear), low-T (~ liquid He), magnetic field (> 2 T), time-resolved (ms) |
F. Photon energy | X-ray (4-40 keV) |
G. Target information | chemical state, crystal structure, structural change, spin/magnetism, phase transition |
Industrial keywords
level 1---Application area | storage device |
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level 2---Target | HD,MO |
level 3---Target (detail) | magnetic layer |
level 4---Obtainable information | crystal structure, electronic state, magnetic moment, valence |
level 5---Technique | diffraction, NEXAFS |
Classification
A80.14 magnetic materials, A80.30 inorganic material, M10.10 single crystal diffraction, M25.10 magnetic scattering, M40.10 XAFS
Body text
A pulsed magnet enables x-ray diffraction experiments under strong magnetic fields above 15 Tesla, which cannot be achieved by using a super-conducting magnet. One can observe the order parameters in phase transitions under very high magnetic fields from a structural point of view using this method.
The pulse duration of magnetic fields is about 1 msec. X-ray diffraction experiments up to 33 Tesla are available now.
In the figure, the field-induced valence-transition of YbInCu4 is shown. The 200 Bragg diffraction peak moves toward high angle above 26T, and this indicates that reduction of the lattice volume, which accompanies the valence transition.
Utilizing this pulsed magnet, we also performed x-ray absorption experiments up to 41T.
Figure -2 profiles of the 200 Bragg peak of YbInCu4 as a function of magnetic field
[ T. Inami, K. Ohawada, Y. Matsuda, Y. Ueda, H. Nojiri, Y. Murakami, T. Arima, H. Ohta, W. Zhang and K. Yoshimura, Nuclear Instruments and Methods in Physics Research B 238, 233-236 (2005), Fig. 2,
©2005 Elsevier Science Publisher ]
Source of the figure
Private communication/others
Description
Technique
We use very small pulsed magnets. The typical dimensions are 2cm in diameter, 2cm in length, and 3mm in bore diameter. It is possible to cool the magnet by a conventional closed-cycle He refrigerator, since the magnet is small and produces little heat. Hence we can perform x-ray diffraction experiments without introducing any modification to the diffractometer.
Figure A pulsed magnet mounted on the cold head of a closed-cycle He refrigerator
[ Journal of the Crystallographic Society of Japan 47, 244 (2005), Fig. 5,
©2005 The Crystallographic Society of Japan ]
Source of the figure
Private communication/others
Description
Required time for experimental setup
24 hour(s)
Instruments
Instrument | Purpose | Performance |
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Experimental hutch 3 | X-ray diffraction under strong magnetic fields | 30T |
References
Document name |
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Y. H. Matsuda et al., Physica B, 346-347, 519-523 (2004) |
T. Inami et al., NIMB in press (2005). |
Related experimental techniques
Questionnaire
This solution is an application of a main instrument of the beamline.
With user's own instruments.
Ease of measurement
Middle
Ease of analysis
Easy
How many shifts were needed for taking whole data in the figure?
Two-three shifts