LOW TEMPERATURE SPECIFIC HEAT OF YBa2Cu3O7

1993 ◽  
Vol 07 (01n03) ◽  
pp. 166-169 ◽  
Author(s):  
R. CASPARY ◽  
P. HELLMANN ◽  
T. WOLF ◽  
F. STEGLICH
Keyword(s):  
Low Temperature ◽  
Magnetic Fields ◽  
Specific Heat ◽  
Spin Glass ◽  
Oxygen Content ◽  
Theoretical Models ◽  
Specific Heat Data ◽  
Field Dependent ◽  
Low Temperature Specific Heat ◽  
Heat Data

We show specific heat data in magnetic fields to B = 8T on new polycrystals with different oxygen content and compare them with earlier results. The analysis reveals a field dependent residual linear term which is discussed within theoretical models of Bulaevskii and for a spin-glass.

Fast Dynamics in Glass-Formers: Relation to Fragility and the Kohlrausch Exponent

1996 ◽  
Vol 455 ◽  
Author(s):  
K. L. Ngai ◽  
C. M. Roland
Keyword(s):  
Relaxation Time ◽  
Low Temperature ◽  
Specific Heat ◽  
Raman Spectra ◽  
Low Temperatures ◽  
Coupling Model ◽  
Boson Peak ◽  
Specific Heat Data ◽  
Low Temperature Specific Heat ◽  
Heat Data

ABSTRACTFrom the Raman spectra and related inferences from low temperature specific heat data, Sokolov and coworkers have established that the ratio of the quasielastic and vibrational contributions at low temperatures (5∼10K) up to Tg correlates well with the degree of fragility and β of the glass-former. As pointed out by Sokolov (see his contribution in this Volume) such a correlation between the fast dynamics and structural a-relaxation at Tg(i.e., m and β) is intriguing, since at and below Tg, the α-relaxation time τα is more than twelve orders of magnitude longer than the quasielastic contribution and the boson peak. We show in this paper how the Coupling Model (CM) may provide an explanation for this correlation.

Chemical Ways to YBa2Cu3O7−x Superconducting Materials

1988 ◽  
Vol 121 ◽  
Author(s):  
J. C. Bernier ◽  
S. Vilminot ◽  
S. El Hadigui ◽  
C. His ◽  
J. Guille ◽  
...  
Keyword(s):  
Low Temperature ◽  
Specific Heat ◽  
Magnetic Measurements ◽  
The Other ◽  
Superconducting Materials ◽  
Superconducting Properties ◽  
Specific Heat Data ◽  
Oxalate Coprecipitation ◽  
Low Temperature Specific Heat ◽  
Heat Data

ABSTRACTYBa2Cu3O7−x has been synthesized by two chemical ways, one from oxalate coprecipitation, the other one from metalloorganic decomposition. Superconducting properties of the resulting samples have been checked by means of resistivity and magnetic measurements. Low temperature specific heat data allow to propose an explanation to the residual linear term.

Nodal gap behavior of Bi2Sr2−xLnxCuO6+δ (Ln = La, Eu) investigated by specific heat measurements

2015 ◽  
Vol 29 (25n26) ◽  
pp. 1542014 ◽  
Author(s):  
M. Shimizu ◽  
Y. Moriya ◽  
S. Baar ◽  
N. Momono ◽  
Y. Amakai ◽  
...  
Keyword(s):  
Low Temperature ◽  
Magnetic Fields ◽  
Fermi Surface ◽  
Specific Heat ◽  
Excitation Spectrum ◽  
Cuprate Superconductors ◽  
Electronic Excitation ◽  
Linear Term ◽  
Electronic Specific Heat ◽  
Low Temperature Specific Heat

We performed low-temperature specific heat measurements on slightly underdoped samples of monolayer cuprate superconductors [Formula: see text] (Ln = La, Eu, Ln-Bi2201) under magnetic fields [Formula: see text]. In La-Bi2201, the coefficient [Formula: see text] of [Formula: see text]-linear term in the electronic specific heat [Formula: see text] at [Formula: see text] shows [Formula: see text] dependence, as expected in [Formula: see text] -wave superconductors. In Eu-Bi2201, [Formula: see text] shows almost the same [Formula: see text] dependence as that of La-Bi2201 below [Formula: see text] T, while [Formula: see text] is suppressed above [Formula: see text] T and deviates downward from the [Formula: see text] curve of La-Bi2201. This result suggests the the gap and the electronic excitation spectrum near nodes are modified in Eu-Bi2201 except the region of the Fermi surface in the immediate vicinity of nodes.

Low-temperature specific heat ofBaCuO2andBaCuO2.14in magnetic fields to 7 T

2000 ◽  
Vol 61 (1) ◽  
pp. 538-548 ◽  
Author(s):  
R. A. Fisher ◽  
D. A. Wright ◽  
J. P. Emerson ◽  
B. F. Woodfield ◽  
N. E. Phillips ◽  
...  
Keyword(s):  
Low Temperature ◽  
Magnetic Fields ◽  
Specific Heat ◽  
Low Temperature Specific Heat

Low-temperature specific heat of antiferromagneticEuNi5P3and mixed-valentEuNi2P2in magnetic fields to 7 T

1995 ◽  
Vol 52 (18) ◽  
pp. 13519-13525 ◽  
Author(s):  
R. A. Fisher ◽  
P. Radhakrishna ◽  
N. E. Phillips ◽  
J. V. Badding ◽  
A. M. Stacy
Keyword(s):  
Low Temperature ◽  
Magnetic Fields ◽  
Specific Heat ◽  
Low Temperature Specific Heat

scholarly journals Magnetic studies of monoclinic Cu4O(SeO3)3, a copper-oxo-selenite derivative

2020 ◽  
Vol 233 ◽  
pp. 01002
Author(s):  
José F. Malta ◽  
Marta S.C. Henriques ◽  
José A. Paixão ◽  
António P. Gonçalves
Keyword(s):  
Low Temperature ◽  
Specific Heat ◽  
Intermediate Phase ◽  
Magnetic Transition ◽  
Chemical Vapour ◽  
Specific Heat Data ◽  
Magnetic Studies ◽  
Chemical Vapour Transport ◽  
Maximum Value ◽  
Heat Data

Cu4O(SeO3)3 is a copper-oxo-selenite belonging to the CuxO(SeO3)(x–1) family of the topological chiral magnet Cu2OSeO3. We report magnetometry and specific heat data measured in a monoclinic Cu4O(SeO3)3 single crystal grown through a Chemical Vapour Transport (CVT) reaction. Our study shows a typical antiferromagnetic behaviour, with a Néel temperature TN = 58 K, similar to that of the Cu2OSeO3 and an additional transition at 13 K. The effective magnetic moment per Cu atom is 1.84 μB, close to the expected theoretical value for Cu2+. The low-temperature M(H) curves, show a transition starting at Hc1 ~ 400 Oe at 1.8 K shifting to a lower value of ~ 280 Oe at 30 K, likely from a helical into a conical intermediate phase, and a second transition at Hc2 ~ 1 kOe, above which the net moment increases linearly with applied field. The magnetisation moment value in a 90 kOe field is 0.053 μB/Cu at 1.8 K and attains a maximum value of 0.061 μB at 13 K. Low-temperature specific heat measurements confirm the presence of the magnetic transition at 13 K, slightly shifting to lower temperatures under an applied magnetic field.

Low-temperature specific heat of the 123, 124 and 247 phases of Y-Ba-Cu-O in magnetic fields up to 14 Tesla

1992 ◽  
Vol 200 (1-2) ◽  
pp. 1-11 ◽  
Author(s):  
D. Sanchez ◽  
A. Junod ◽  
J.-Y. Genoud ◽  
T. Graf ◽  
J. Muller
Keyword(s):  
Low Temperature ◽  
Magnetic Fields ◽  
Specific Heat ◽  
Low Temperature Specific Heat
Sign in / Sign up

Export Citation Format

Share Document