scholarly journals Metal-insulator and magnetic transition of NiO at high pressures

2004 ◽  
Vol 69 (3) ◽  
Author(s):  
Xiao-Bing Feng ◽  
N. M. Harrison
JETP Letters ◽  
2018 ◽  
Vol 107 (5) ◽  
pp. 311-314 ◽  
Author(s):  
V. A. Sidorov ◽  
Jing Guo ◽  
Liling Sun ◽  
V. V. Brazhkin

2020 ◽  
Vol 117 (16) ◽  
pp. 8783-8787
Author(s):  
Liangzi Deng ◽  
Hung-Cheng Wu ◽  
Alexander P. Litvinchuk ◽  
Noah F. Q. Yuan ◽  
Jey-Jau Lee ◽  
...  

A skyrmion state in a noncentrosymmetric helimagnet displays topologically protected spin textures with profound technological implications for high-density information storage, ultrafast spintronics, and effective microwave devices. Usually, its equilibrium state in a bulk helimagnet occurs only over a very restricted magnetic field–temperature phase space and often in the low-temperature region near the magnetic transition temperature Tc. We have expanded and enhanced the skyrmion phase region from the small range of 55 to 58.5 K to 5 to 300 K in single-crystalline Cu2OSeO3 by pressures up to 42.1 GPa through a series of phase transitions from the cubic P213, through orthorhombic P212121 and monoclinic P21, and finally to the triclinic P1 phase, using our newly developed ultrasensitive high-pressure magnetization technique. The results are in agreement with our Ginzburg–Landau free energy analyses, showing that pressures tend to stabilize the skyrmion states and at higher temperatures. The observations also indicate that the skyrmion state can be achieved at higher temperatures in various crystal symmetries, suggesting the insensitivity of skyrmions to the underlying crystal lattices and thus the possible more ubiquitous presence of skyrmions in helimagnets.


2017 ◽  
Vol 110 (17) ◽  
pp. 172404 ◽  
Author(s):  
Chongyang Yin ◽  
Run Zhang ◽  
Guoyu Qian ◽  
Qingshan Fu ◽  
Canglong Li ◽  
...  

Author(s):  
Kota Kataoka ◽  
Daigorou Hirai ◽  
Akihiro Koda ◽  
Ryosuke Kadono ◽  
Takashi Honda ◽  
...  

Abstract Semimetallic osmium pyrochlore oxide Cd2Os2O7 undergoes a magnetic transition to an all-in-all-out (AIAO)-type order at 227 K, followed by a crossover to an AIAO insulator at around 210 K. Here, we studied the isostructural and isoelectronic compound Hg2Os2O7 through thermodynamic measurements, µSR spectroscopy and neutron diffraction experiments. A similar magnetic transition, probably to an AIAO-type order, was observed at 88 K, while the resistivity showed a decrease at the transition and remained metallic down to 2 K. Thus, the ground state of Hg2Os2O7 is most likely an AIAO semimetal, which is analogous to the intermediate-temperature state of Cd2Os2O7. Hg2Os2O7 exists on the verge of the metal–insulator boundary on the metal side and provides an excellent platform for studying the electronic instability of 5d electrons with moderate electron correlations and strong spin–orbit interactions.


1996 ◽  
Vol 449 ◽  
Author(s):  
P. Perlin ◽  
T. Suski ◽  
A. Polian ◽  
J. C. Chervin ◽  
W. Knap ◽  
...  

ABSTRACTCharacter of the metal-insulator transition which occurs at about 23 GPa in bulk GaN crystals has been studied by means of high pressure Raman spectroscopy. The related freeze-out of electrons is caused by the localized donor state formed by most likely oxygen and emerging at high pressures to the band gap of GaN. As a result, the electron concentration drops from its initial value of 5.1019 cm-3 to about 3. 1018 cm-3. These remaining electrons originate likely from another donor center with effective mass character, probably carbon. The obtained results raise a question whether the nitrogen vacancy is abundant enough to be observed in bulk GaN crystals.


2000 ◽  
Vol 14 (29n31) ◽  
pp. 3596-3601 ◽  
Author(s):  
J. MESOT ◽  
A. KAMINSKI ◽  
H. M. FRETWELL ◽  
S. ROSENKRANZ ◽  
J. C. CAMPUZANO ◽  
...  

The doping dependence of the low-temperature spectral function is precisely determined from angle resolved photoemision (ARPES) measurements. It is found that, as the doping decreases, the maximum of the superconducting gap increases, but the slope of the gap near the nodes decreases. Though consistent with d-wave symmetry, the gap with underdoping cannot be fit by the simple cos(kx)-cos(ky) form. We suggest that this arises due to the increasing importance of long range interactions as one approaches the insulator. It is also shown that the shape of the spectral function at the (π, 0) point below T c can be explained by the interaction of the electrons with a collective mode whose energy matches that of the magnetic resonance as obtained by inelastic neutron scattering data, and points to the intimate relation of magnetic correlatins to high Tc superconductivity.


2003 ◽  
Vol 88 (2-3) ◽  
pp. 257-261 ◽  
Author(s):  
Stephen A. Gramsch ◽  
Ronald E. Cohen ◽  
Sergej Yu Savrasov

1999 ◽  
Vol 85 (8) ◽  
pp. 5396-5398 ◽  
Author(s):  
M. Pattabiraman ◽  
Narayani Senthilkumaran ◽  
P. Murugaraj ◽  
G. Rangarajan

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