First-order field-induced transition, magnetoresistance, and giant magnetostriction in single crystals of(La0.4Pr0.6)1.2Sr1.8Mn2O7

2001 ◽  
Vol 64 (1) ◽  
Author(s):  
M. Apostu ◽  
R. Suryanarayanan ◽  
A. Revcolevschi ◽  
H. Ogasawara ◽  
M. Matsukawa ◽  
...  
1982 ◽  
Vol 12 (8) ◽  
pp. 1603-1612 ◽  
Author(s):  
B M Geerken ◽  
R Griessen ◽  
G Benediktsson ◽  
H U Astrom ◽  
C van Dijk

1999 ◽  
Vol 11 (2) ◽  
pp. 543-554 ◽  
Author(s):  
D T Adroja ◽  
Y Echizen ◽  
T Takabatake ◽  
Y Matsumoto ◽  
T Suzuki ◽  
...  

Author(s):  
C. De Blasi ◽  
D. Manno

The study of dislocations and stacking faults in melt grown GaSe single crystals has been carried out by the Convergent Beam Electron Diffraction (CBED) technique.The presence of stacking faults induces distortions in the Kikuchi lines observed in the CBED transmitted disk. According to the kinematical condition of the stacking fault visibility, such lines show modifications when g·R is not integer, The displacement vector R has been determined by the analysis of the visibility and invisibility conditions in the transmitted disk, recorded according to the Tanaka method, The Burgers vector b of dislocations has been determined by the analysis of the modifications induced both in Kikuchi lines and in the First Order Laue Zone (FOLZ) reflections, observed in low camera length CBED patterns. Splitting and unsplitting of the reflections correspond to the visibility and invisibility of the dislocations in the kinematical approximation of diffraction contrast, The condition g·b = 0 is not strictly a sufficient condition for the vanishing of the modifications induced by the dislocation, neverthless it is generally very useful as a criterion for determining the direction of b, Moreover, some reflections g give g·b = ⅓ in the case of partial dislocations. This condition does not produce enough contrast to be detected, so that it is one more for the defect invisibility. The Thompson construction has been used in order to calculate the amplitude of b and to discriminate perfect or partial dislocations.


1995 ◽  
Vol 09 (03n04) ◽  
pp. 229-235
Author(s):  
MOON-SEOG JIN ◽  
HO-JUN SONG ◽  
YONG-GEUN KIM ◽  
HYUNG-GON KIM ◽  
JEONG-DAE KOH ◽  
...  

SbSBr, BiSBr, SbSBr:Ni, and BiSBr:Ni single crystals were grown by the Bridgman technique. The grown single crystals crystallized in an orthorhombic structure and have an indirect band structure. The temperature dependence of their optical energy gap shows an anomalous property at the first order phase transition temperature and at the second order one. Nickel doped as an impurity site at the T d symmetry point in the host single crystals as Ni 2+ ion. The impurity optical absorption peaks appeared by the electron transitions between the energy levels of these ions.


SPIN ◽  
2015 ◽  
Vol 05 (02) ◽  
pp. 1540002 ◽  
Author(s):  
Yukio Yasui ◽  
Noriaki Hamachi ◽  
Yohei Kono ◽  
Shunichiro Kittaka ◽  
Toshiro Sakakibara

The neutron diffraction and measurements of specific heat and magnetization were carried out on single crystals of a quantum spin ice system Yb 2 Ti 2 O 7. The thermal hysteresis loops of temperature dependence of the magnetization and neutron diffraction intensity indicate a first-order ferromagnetic transition, where the used single crystals are confirmed to have a sharp peak structure in the specific heat (C)–temperature (T) curve at T C ∼ 0.2 K. The magnetic structure analysis of neutron diffraction results revealed that the Yb 3+ moments have a ferromagnetic collinear structure along [001] directions with ordered moment value 1.1 ± 0.1 μB at 0.03 K. The mechanism of ferromagnetic transition of Yb 2 Ti 2 O 7 will be discussed.


2009 ◽  
Vol 1 (2) ◽  
pp. 192-199 ◽  
Author(s):  
A. Ouedraogo ◽  
K. Palm ◽  
G. Chanussot

The paper examines the ferroelectric-paraelectric phase transition in Cu:BaTiO3 single crystals. Using thermo-currents and dielectric measurements, we found for pure samples the phase transition temperature to be close to Curie temperature (Tc=120°C) with an anisotropy of the dielectric constantε.The lowering of temperature Tm, corresponding to the maximum of pyroelectric signal, with the increase of concentration of impurities is confirmed by measurements of ε. Moreover, the e(T) curves show progressive broadening as well as higher peak with the increase of  impurity concentration, and the transition becomes more and more diffuse. The same effect occurs when the samples are subjected to a laser irradiation (λ=5145Ǻ). During annealing, crystals lose copper and Tm is thereafter observed to increase again. BaTiO3 is a displacive ferroelectric (having high permittivity k-values) which undergoes a first order phase transition. Ions substitutions have an effect on the lattice dynamics attributed to charge transfer to Ti and a lowering of elastic forces in BaTiO3. Kewwords: Ferroelectric transition; BaTiO3 single crystals; Thermo-currents; Dielectric constant.  © 2009 JSR Publications. ISSN: 2070-0237 (Print); 2070-0245 (Online). All rights reserved. DOI: 10.3329/jsr.v1i2.1876  


1978 ◽  
Vol 56 (20) ◽  
pp. 2616-2619 ◽  
Author(s):  
Ritchie MacLaren Murray ◽  
Etalo A. Secco

Phase transformation studies on pure Na2SO4 revealed four phases only; phase IV was not observed.Electrical conductivity measurements have been made on polycrystalline undoped and K-doped Na2SO4 and on single crystals of undoped Na2SO4. Kinetic measurements on II → III transformation in undoped Na2SO4 show rate of conversion to be time independent and inversely related to temperature.The presence of K in Na2SO4 effects a lowering of both the transition temperature and the enthalpy of transition along with an alteration from the "athermal" kinetic behavior to first-order kinetics.


1992 ◽  
Vol 7 (10) ◽  
pp. 2833-2839 ◽  
Author(s):  
Hung-Ye Lin ◽  
Yu-Zen Tsai ◽  
Sanboh Lee

The evolution of hardness and transmittance of irradiated LiF single crystals at elevated temperatures has been investigated. The Vickers hardness is proportional to φ1/3 where φ is the dosage of γ-rays. The thermal annealing of hardness which is analyzed according to a first-order kinetic process has one stage for φ = 100 KGy and two stages for φ ≥ 250 KGy. For a given dosage, the activation energy of stage I is larger than that of stage II. The transmittance of irradiated LiF crystals is attributed to F, M, R1, and R2 centers. The transmittance decreases with increasing time at the brief durations, then oscillates, and finally increases monotonically. The region in which the transmittance increases monotonically with time is simulated by a second-order kinetic process of the color center. The activation energy of optical absorption was determined. Comparing both activation energies of hardness and optical absorption, we find that the mechanism of the kinetic process for hardness differs from that for optical absorption.


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