Surface tension and boundary conditions for superfluid Fermi liquid. Size effect and the effect of a magnetic field on the phase diagram

1975 ◽  
Vol 12 (11) ◽  
pp. 4825-4829 ◽  
Author(s):  
I. A. Privorotskii
Keyword(s):  
Magnetic Field ◽  
Phase Diagram ◽  
Surface Tension ◽  
Size Effect ◽  
Boundary Conditions ◽  
Fermi Liquid ◽  
Superfluid Fermi

Phase diagram for the superfluid fermi-gas in a strong magnetic field

1996 ◽  
Vol 46 (S1) ◽  
pp. 209-210
Author(s):  
M. Yu Kagan ◽  
M. A. Baranov ◽  
D. V. Efremov ◽  
M. S. Mar’enko
Keyword(s):  
Magnetic Field ◽  
Phase Diagram ◽  
Strong Magnetic Field ◽  
Fermi Gas ◽  
Superfluid Fermi Gas ◽  
Superfluid Fermi

scholarly journals Comparison of two superconducting phases induced by a magnetic field in UTe2

2021 ◽  
Vol 4 (1) ◽  
Author(s):  
W. Knafo ◽  
M. Nardone ◽  
M. Vališka ◽  
A. Zitouni ◽  
G. Lapertot ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Phase Diagram ◽  
Fermi Liquid ◽  
Theoretical Models ◽  
Residual Resistivity ◽  
Resistivity Measurements ◽  
Magnetization Axis ◽  
Normal States ◽  
Superconducting Pairing ◽  
Itinerant Ferromagnets

AbstractSuperconductivity induced by a magnetic field near metamagnetism is a striking manifestation of magnetically-mediated superconducting pairing. After being observed in itinerant ferromagnets, this phenomenon was recently reported in the orthorhombic paramagnet UTe2. Here we explore the phase diagram of UTe2 under two magnetic-field directions: the hard magnetization axis b, and a direction titled by ≃25-30° from b in the (b,c) plane. Zero-resistivity measurements confirm that superconductivity is established beyond the metamagnetic field Hm in the tilted-field direction. While superconductivity is locked exactly at fields either smaller (for H | | b), or larger (for H tilted by ≃27° from b to c), than Hm, the variations of the Fermi-liquid coefficient in the electrical resistivity and of the residual resistivity are similar for the two field directions. The resemblance of the normal states for the two field directions puts constraints for theoretical models of superconductivity and implies that some subtle ingredients must be in play.

Phase diagrams and hysteresis behaviors of a ferrimagnetic mixed spins S = 1/2 and S = 1 Ising nanowire

2018 ◽  
Vol 32 (26) ◽  
pp. 1850289 ◽  
Author(s):  
A. Alrajhi ◽  
M. Madani ◽  
N. Hachem ◽  
M. El Bouziani
Keyword(s):  
Magnetic Field ◽  
Phase Diagram ◽  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Phase Transitions ◽  
External Magnetic Field ◽  
Size Effect ◽  
Hysteresis Loops ◽  
Mixed Spins ◽  
Mixed Spin

The ferrimagnetic mixed spin-1/2 and spin-1 cubic Ising nanowire is studied in the framework of the Monte Carlo simulation. The competition between the bilinear interaction and crystal field of spin-1 atoms as well as the nanowire size effect is highlighted. The corresponding phase diagram is discussed showing compensation points and critical second-order phase transitions. The effect of an external magnetic field and the hysteresis loops behavior are also carried out. Finally, we compare our results with other works in the literature.

Strong Magnetic Field Effect on Surface Tension Associated with an Interfacial Magnetic Pressure

2012 ◽  
Vol 116 (33) ◽  
pp. 17676-17681 ◽  
Author(s):  
Z.H.I. Sun ◽  
X. Guo ◽  
M. Guo ◽  
C. Li ◽  
J. Vleugels ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Surface Tension ◽  
Strong Magnetic Field ◽  
Field Effect ◽  
Magnetic Field Effect ◽  
Magnetic Pressure

scholarly journals Ground state and stability of the fractional plateau phase in metallic Shastry–Sutherland system TmB4

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Matúš Orendáč ◽  
Slavomír Gabáni ◽  
Pavol Farkašovský ◽  
Emil Gažo ◽  
Jozef Kačmarčík ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Phase Diagram ◽  
Ground State ◽  
Constant Magnetic Field ◽  
Paramagnetic Phase ◽  
The Other ◽  
Zero Field ◽  
Plateau Phase ◽  
Low Field ◽  
Zero Field Cooling

AbstractWe present a study of the ground state and stability of the fractional plateau phase (FPP) with M/Msat = 1/8 in the metallic Shastry–Sutherland system TmB4. Magnetization (M) measurements show that the FPP states are thermodynamically stable when the sample is cooled in constant magnetic field from the paramagnetic phase to the ordered one at 2 K. On the other hand, after zero-field cooling and subsequent magnetization these states appear to be of dynamic origin. In this case the FPP states are closely associated with the half plateau phase (HPP, M/Msat = ½), mediate the HPP to the low-field antiferromagnetic (AF) phase and depend on the thermodynamic history. Thus, in the same place of the phase diagram both, the stable and the metastable (dynamic) fractional plateau (FP) states, can be observed, depending on the way they are reached. In case of metastable FP states thermodynamic paths are identified that lead to very flat fractional plateaus in the FPP. Moreover, with a further decrease of magnetic field also the low-field AF phase becomes influenced and exhibits a plateau of the order of 1/1000 Msat.

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