Abstract
The superconducting transition region in a Nb disk showing the paramagnetic Meissner effect (PME) has been investigated in detail. From the field-cooled magnetization behavior, two well-defined temperatures can be associated with the appearance of the PME: (Formula presented) indicates the characteristic temperature where the paramagnetic moment first appears and a lower temperature (Formula presented) defines the temperature where the positive moment no longer increases. During the subsequent warming, the paramagnetic moment begins to decrease at (Formula presented) and then vanishes at (Formula presented) with the magnitude of the magnetization change between these two temperatures being nearly the same as that during cooling. This indicates that the nature of the PME is reversible and not associated with flux motion. Furthermore, the appearance of this paramagnetic moment is even observable in fields as large as 0.2 T even though the magnetization does not remain positive to the lowest temperatures. Magnetic hysteresis loops in the temperature range between (Formula presented) and (Formula presented) also exhibit a distinct shape that is different from the archetypal shape of a bulk type-II superconductor. These behaviors are discussed in terms of the so-called “giant vortex state.”.
| Original language | English |
|---|---|
| Pages (from-to) | 14191-14194 |
| Number of pages | 4 |
| Journal | Physical Review B - Condensed Matter and Materials Physics |
| Volume | 58 |
| Issue number | 21 |
| DOIs | |
| Publication status | Published - 1998 Jan 1 |
| Externally published | Yes |
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ASJC Scopus subject areas
- Electronic, Optical and Magnetic Materials
- Condensed Matter Physics
Cite this
Detailed investigation of the superconducting transition of niobium disks exhibiting the paramagnetic Meissner effect. / Půst, L.; Wenger, L.; Koblischka, Michael Rudolf.
In: Physical Review B - Condensed Matter and Materials Physics, Vol. 58, No. 21, 01.01.1998, p. 14191-14194.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Detailed investigation of the superconducting transition of niobium disks exhibiting the paramagnetic Meissner effect
AU - Půst, L.
AU - Wenger, L.
AU - Koblischka, Michael Rudolf
PY - 1998/1/1
Y1 - 1998/1/1
N2 - The superconducting transition region in a Nb disk showing the paramagnetic Meissner effect (PME) has been investigated in detail. From the field-cooled magnetization behavior, two well-defined temperatures can be associated with the appearance of the PME: (Formula presented) indicates the characteristic temperature where the paramagnetic moment first appears and a lower temperature (Formula presented) defines the temperature where the positive moment no longer increases. During the subsequent warming, the paramagnetic moment begins to decrease at (Formula presented) and then vanishes at (Formula presented) with the magnitude of the magnetization change between these two temperatures being nearly the same as that during cooling. This indicates that the nature of the PME is reversible and not associated with flux motion. Furthermore, the appearance of this paramagnetic moment is even observable in fields as large as 0.2 T even though the magnetization does not remain positive to the lowest temperatures. Magnetic hysteresis loops in the temperature range between (Formula presented) and (Formula presented) also exhibit a distinct shape that is different from the archetypal shape of a bulk type-II superconductor. These behaviors are discussed in terms of the so-called “giant vortex state.”.
AB - The superconducting transition region in a Nb disk showing the paramagnetic Meissner effect (PME) has been investigated in detail. From the field-cooled magnetization behavior, two well-defined temperatures can be associated with the appearance of the PME: (Formula presented) indicates the characteristic temperature where the paramagnetic moment first appears and a lower temperature (Formula presented) defines the temperature where the positive moment no longer increases. During the subsequent warming, the paramagnetic moment begins to decrease at (Formula presented) and then vanishes at (Formula presented) with the magnitude of the magnetization change between these two temperatures being nearly the same as that during cooling. This indicates that the nature of the PME is reversible and not associated with flux motion. Furthermore, the appearance of this paramagnetic moment is even observable in fields as large as 0.2 T even though the magnetization does not remain positive to the lowest temperatures. Magnetic hysteresis loops in the temperature range between (Formula presented) and (Formula presented) also exhibit a distinct shape that is different from the archetypal shape of a bulk type-II superconductor. These behaviors are discussed in terms of the so-called “giant vortex state.”.
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U2 - 10.1103/PhysRevB.58.14191
DO - 10.1103/PhysRevB.58.14191
M3 - Article
VL - 58
SP - 14191
EP - 14194
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 0163-1829
IS - 21
ER -