Diamagnetic and Electrical Properties of SixMo2S3−x (x=0.1, 0.2, 0.33, 0.5) and A0.1Mo2S3−x (A=C, B, and Ru)
Mo 2 S 3 doped with Si, C, B, and Ru, is identified to bear the same crystalline structure P2 1 /m as that of Mo 2 S 3 through XRD analysis. Diamagnetic transitions with χ m ∼10 −4 emu/g Oe at temperature ranging from 2 K to 6 K were observed in the doped samples of Si x Mo 2 S 3− x ( x =0.1, 0.2,...
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Veröffentlicht in: | Journal of superconductivity and novel magnetism 2013, Vol.26 (3), p.503-510 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Mo
2
S
3
doped with Si, C, B, and Ru, is identified to bear the same crystalline structure P2
1
/m as that of Mo
2
S
3
through XRD analysis. Diamagnetic transitions with
χ
m
∼10
−4
emu/g Oe at temperature ranging from 2 K to 6 K were observed in the doped samples of Si
x
Mo
2
S
3−
x
(
x
=0.1, 0.2, 0.33, 0.5). And both of the
x
=0.2 and 0.5 samples were found to have double diamagnetic transitions with higher
T
c
at the same temperature of 6.01 K, while Si
x
Mo
2
S
3−
x
of
x
=0.33 displayed an extra ferromagnetic-like response at 63 K. The corresponding transition in resistivity of Si
x
Mo
2
S
3−
x
with
x
=0.1 was noticed to show a mild drop with less than 10 % of its original transition values as measured down to 2 K. But a superconducting-like magnetic field dependence on the phase transition of resistivity was also noted. Its diamagnetic signals were greatly reduced when the applied magnetic fields were raised to 10
3
Oes. In the doped samples of A
0.1
Mo
2
S
2.9
(A=C, B, and Ru), the phase transition in resistivity at 4.08 K, 4.62 K, and 4.35 K, respectively, exhibited similar fashion as that in the case of Si
0.1
Mo
2
S
2.9
. |
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ISSN: | 1557-1939 1557-1947 |
DOI: | 10.1007/s10948-013-2101-z |