scholarly journals Phase boundary of several multicube superconducting circuits in a magnetic field of arbitrary magnitude and direction

1992 ◽  
Vol 46 (9) ◽  
pp. 5448-5453 ◽  
Author(s):  
You-Min Yi ◽  
Chia-Ren Hu
2020 ◽  
Vol 5 (6) ◽  
Author(s):  
Mihails Birjukovs ◽  
Valters Dzelme ◽  
Andris Jakovics ◽  
Knud Thomsen ◽  
Pavel Trtik

2011 ◽  
Vol 172-174 ◽  
pp. 362-371 ◽  
Author(s):  
Masato Enomoto ◽  
Guo Hong Zhang ◽  
Kai Ming Wu

The characteristics and the mechanism of ferrite transformation in alloy steels which contain a carbide-forming element have attracted considerable attention for past decades. Since it is reported that the nucleation and growth of ferrite in Fe-C base alloys is accelerated by high magnetic field, the influence of a magnetic field of 12 Tesla on ferrite transformation was studied in a Fe-C- Mo alloy. Whereas a significant amount of expedition was observed at lower temperatures, the principal features of ferrite transformation, namely, a marked retardation of transformation at intermediate temperatures and premature cessation of transformation before it reaches the final equilibrium amount below the bay temperature were essentially retained. In contrast, the influence of magnetic field was much less at higher temperatures. These results are discussed in terms of the influence of magnetic field on the phase equilibrium and coupled-solute drag effects on the migration a/g phase boundary.


1992 ◽  
Vol 06 (17) ◽  
pp. 2913-2924 ◽  
Author(s):  
JAE DONG NOH ◽  
DOOCHUL KIM

Transfer matrix methods are used to locate accurate phase boundary of the triangular lattice antiferromagnetic Ising model in magnetic field. Universal quantities such as the central charge and the first few scaling dimensions are obtained along the phase boundary except near the zero field point where the crossover effect degrades convergence. Numerical results are fully consistent with the operator content of the 3-state Potts model indicating that whole phase boundary belongs to the 3-state Potts universality class.


1986 ◽  
Vol 56 (21) ◽  
pp. 2280-2283 ◽  
Author(s):  
James M. Gordon ◽  
A. M. Goldman ◽  
J. Maps ◽  
D. Costello ◽  
R. Tiberio ◽  
...  

1987 ◽  
Vol 35 (16) ◽  
pp. 8396-8404 ◽  
Author(s):  
A. Behrooz ◽  
M. J. Burns ◽  
D. Levine ◽  
B. Whitehead ◽  
P. M. Chaikin

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Zhe Wang ◽  
Ignacio Gutiérrez-Lezama ◽  
Dumitru Dumcenco ◽  
Nicolas Ubrig ◽  
Takashi Taniguchi ◽  
...  

AbstractRecent experiments on van der Waals antiferromagnets have shown that measuring the temperature (T) and magnetic field (H) dependence of the conductance allows their magnetic phase diagram to be mapped. Similarly, experiments on ferromagnetic CrBr3 barriers enabled the Curie temperature to be determined at H = 0, but a precise interpretation of the magnetoconductance data at H ≠ 0 is conceptually more complex, because at finite H there is no well-defined phase boundary. Here we perform systematic transport measurements on CrBr3 barriers and show that the tunneling magnetoconductance depends on H and T exclusively through the magnetization M(H, T) over the entire temperature range investigated. The phenomenon is reproduced by the spin-dependent Fowler–Nordheim model for tunneling, and is a direct manifestation of the spin splitting of the CrBr3 conduction band. Our analysis unveils a new approach to probe quantitatively different properties of atomically thin ferromagnetic insulators related to their magnetization by performing simple conductance measurements.


2000 ◽  
Vol 53 (4) ◽  
pp. 537
Author(s):  
J. S. Thakur ◽  
D. Neilson

We discuss the destabilisation of the electron 2D metallic state by an in-plane magnetic field. We demonstrate that such a field can destabilise the metallic state through spin polarisation which significantly enhances the exchange correlations between electrons. We find that the conducting phase of the fully spin polarised system is almost completely suppressed. We discuss this phenomenon within a memory function formalism which treats both disorder and exchange-correlation effects. We determine the shift in the position of the metal–insulator phase boundary as the system is polarised by an increasing parallel magnetic field.


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