Magnetic-Field-Induced Spin Nematicity in FeSe_{1 – x}S_x and FeSe_{1 – y}Te_y Superconductor Systems

Connections between C(X) and C(Y), where Y is a subspace of X

In this paper, we introduce a method by which we can find a close connection between the set of prime $z$-ideals of $C(X)$ and the same of $C(Y)$, for some special subset $Y$ of $X$. For instance, if $Y=Coz(f)$ for some $fin C(X)$, then there exists a one-to-one correspondence between the set of prime $z$-ideals of $C(Y)$ and the set of prime $z$-ideals of $C(X)$ not containing $f$. Moreover, c...

Effect of Rb and Ta Doping on the Ionic Conductivity and Stability of the Garnet Li_{7+2<italic>x</italic><italic>y</italic>}(La_{3<italic>x</italic>}Rb_{<italic>x</italic>})(Zr_{2<italic>y</italic>}Ta_{<italic>y</italic>})O₁₂ (0 <italic>x</italic> 0.375, 0 <italic>y</italic> 1) Superionic Conductor: A First Principles Investigation

In this work, we investigated the effect of Rb and Ta doping on the ionic conductivity and stability of the garnet Li7+2x−y(La3−xRbx)(Zr2−yTay)O12 (0 ≤ x ≤ 0.375, 0 ≤ y ≤ 1) superionic conductor using first principles calculations. Our results indicate that doping does not greatly alter the topology of the migration pathway, but instead acts primarily to change the lithium concentration. The st...

Novel Magnetic and Optical Properties of Sn_1−xZn_xO₂ Nanoparticles

Structure Symmetry Determination and Magnetic Evolution in Sr₂Ir_{1−<em>x</em>}Rh_<em>x</em>O₄

Hole Spin Polarization in AlAs / Ga 1 � x � y Mn x Al y As Structures

During the last years spin-polarized transport became a matter of major interest [1, 2], giving rise to a eld usually called magnetoelectronics, or spintronics. Much e ort has been made in studying and producing the so-called spin-valve, where a spin-polarized current is generated. A promising system in that area is the recently grown structure of GaAs/AlAs with inclusions of Ga1 xMnxAs layers ...