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American Mineralogist; April 2008; v. 93; no. 4; p. 548-557; DOI: 10.2138/am.2008.2680
© 2008 Mineralogical Society of America
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Low-temperature calorimetric and magnetic data for natural end-members of the axinite group

Jan Filip1,2,*, Edgar Dachs3, Jirí Tucek1,4, Milan Novák2 and Petr Bezdicka5

1 Centre for Nanomaterial Research, Palacky University in Olomouc, Svobody 26, 771 46 Olomouc, Czech Republic
2 Department of Geological Sciences, Masaryk University, Kotlárská 2, 611 37 Brno, Czech Republic
3 Department of Material Engineering and Physics, University of Salzburg, Hellbrunnerstrasse 34, 5020 Salzburg, Austria
4 Department of Experimental Physics, Palacky University in Olomouc, Svobody 26, 771 46 Olomouc, Czech Republic
5 Institute of Inorganic Chemistry, Academy of Science of the Czech Republic, 250 68 Rez, Czech Republic


Figure 1
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FIGURE 1. Chemical compositions of axinite-group minerals. Symbols represent electron microprobe analyses on crystals selected for this study.

 

Figure 2
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FIGURE 2. Room-temperature 57Fe Mössbauer spectra of axinite-group minerals (except Fe-free magnesioaxinite). Note, both Fe2+ and Fe3+ are in a high-spin state.

 

Figure 3
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FIGURE 3. Temperature dependence of the heat capacity of axinite-group minerals. Low-temperature regions in the range 0–12 K are inserted. (a) Data for end-member ferroaxinite and magnesioaxinite. (b) Data for manganaxinite and tinzenite.

 

Figure 4
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FIGURE 4. Heat capacity of ferroaxinite, manganaxinite, and tinzenite in the low-temperature region 0–15 K and functions used to extrapolate CP to 0 K. For manganaxinite and tinzenite, this extrapolation is done in the temperature range 0–5 K on the basis of a Schottky anomaly (solid curves, representing CP lattice + CP Schottky); for ferroaxinite, a lambda-type CP anomaly between 0 and 2 K with a peak at around 1 K was assumed as indicated by the stippled curve.

 

Figure 5
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FIGURE 5. The results of magnetic measurements of ferroaxinite. (a) Inverse temperature dependence of magnetic mass susceptibility ({chi}) with an inset of low-temperature region 0–20 K. (b) Plot of {chi}T vs. T with an inset of low-temperature region 0–50 K (AF = arrow points to the temperature where antiferromagnetic interactions contribute to ferroaxinite magnetic ordering). (c) Field dependence of the magnetization at selected temperatures with an inset of the hysteresis loop near the origin.

 

Figure 6
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FIGURE 6. The results of magnetic measurements of manganaxinite (left) and tinzenite (right). (a) Inverse temperature dependence of magnetic mass susceptibility ({chi}) with an inset of low-temperature region 0 20 K. (b) Plot of {chi}T vs. T with an inset of low-temperature region 0–50 K. (c) Field dependence of the magnetization at selected temperatures with an inset of the hysteresis loop near the origin.

 





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