Fe-excess Ions as Electronic Charge Suppliers for Zero Thermal Expansion in the Normal State of Fe1.16Te0.6Se0.4

2015 ◽  
Vol 84 (9) ◽  
pp. 094713
Author(s):  
Sunil K. Karna ◽  
Chi-Hung Lee ◽  
Wen-Hsien Li ◽  
Raman Sankar ◽  
Fang-Cheng Chou ◽  
...  
2004 ◽  
Vol 402 (1-2) ◽  
pp. 88-93 ◽  
Author(s):  
X.S. Wu ◽  
H.L. Cai ◽  
Y.M. Xu ◽  
W.S. Tan ◽  
A. Hu ◽  
...  

2013 ◽  
Vol 27 (22) ◽  
pp. 1350119
Author(s):  
M. BASSAN ◽  
B. BUONOMO ◽  
G. CAVALLARI ◽  
E. COCCIA ◽  
S. D'ANTONIO ◽  
...  

We describe a result coming from an experiment based on an Al - Mg alloy (~5% Mg ) suspended bar hit by an electron beam and operated above and below the temperature of transition from superconducting to normal state of the material. The amplitude of the bar first longitudinal mode of oscillation, excited by the beam interacting with the bulk, and the energy deposited by the beam in the bar are the quantities measured by the experiment. These quantities, inserted in the equations describing the mechanism of the mode excitation and complemented by an independent measurement of the specific heat, allow us to determine the linear expansion coefficient α of the material. We obtain α = [(10.9±0.4)T+(1.3±0.1)T3]×10-10 K -1 for the normal state of conduction in the temperature interval 0.9 < T < 2 K and α = [(-2.45±0.60)+(-10.68±1.24)T +(0.13±0.01)T3]×10-9 K -1 for the superconducting state in the interval 0.3 < T< 0.8 K .


2007 ◽  
Vol 21 (01) ◽  
pp. 133-143 ◽  
Author(s):  
J. MEENA DEVI ◽  
K. RAMACHANDRAN

Thermal expansion of MgB 2 at normal state is measured experimentally in the temperature range 300–400 K. Lattice and electronic contribution to the thermal expansion is determined from the Gruneisen relation using electronic and lattice specific heat. This is compared with the low temperature measurements for predicting superconducting transition.


Author(s):  
J. Cooper ◽  
O. Popoola ◽  
W. M. Kriven

Nickel sulfide inclusions have been implicated in the spontaneous fracture of large windows of tempered plate glass. Two alternative explanations for the fracture-initiating behaviour of these inclusions have been proposed: (1) the volume increase which accompanies the α to β phase transformation in stoichiometric NiS, and (2) the thermal expansion mismatch between the nickel sulfide phases and the glass matrix. The microstructure and microchemistry of the small inclusions (80 to 250 μm spheres), needed to determine the cause of fracture, have not been well characterized hitherto. The aim of this communication is to report a detailed TEM and EDS study of the inclusions.


1995 ◽  
Vol 05 (C8) ◽  
pp. C8-1109-C8-1113
Author(s):  
T.R. Finlayson, ◽  
M. Liu ◽  
T.F. Smith
Keyword(s):  

1978 ◽  
Vol 39 (C6) ◽  
pp. C6-406-C6-407 ◽  
Author(s):  
T. Fukase ◽  
T. Kobayashi ◽  
M. Isino ◽  
N. Toyota ◽  
Y. Muto

1980 ◽  
Vol 41 (C8) ◽  
pp. C8-875-C8-877
Author(s):  
E. Girt ◽  
P. Tomić ◽  
A. Kuršumović ◽  
T. Mihać-Kosanović

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-1903-C8-1904
Author(s):  
S. U. Jen ◽  
Y. D. Yao ◽  
H. Y. Pai

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-159-C8-160
Author(s):  
T. Suzuki ◽  
T. Kanomata ◽  
T. Kaneko

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