Alessia Provino

Self-magnetic compensation and shifted hysteresis loops in ferromagnetic samarium systems

For

R3Au9Pn (R = Y, Gd–Tm; Pn = Sb, Bi): A Link between Cu10Sn3 and Gd14Ag51

{text{Sm}}^{3+}

Synthesis, Crystal and Electronic Structure of the Quaternary Magnetic EuTAl4Si2 (T = Rh and Ir) Compounds

ions in a vast majority of metallic systems, the following interesting scenario has been conjured up for long, namely, a magnetic lattice of tiny self- (spin-orbital) compensated

The R10Pd21 compounds (R = Y, Pr, Nd, Sm, Gd–Lu). Crystal structure and magnetism of the ‘RPd2’ phases

4f

On the RMgSn rare earth compounds

-moments exchange coupled (and phase reversed) to the polarization in the conduction band. We report here the identification of a self-compensation behavior in a variety of ferromagnetic Sm intermetallics via the fingerprint of a shift in the magnetic hysteresis

New tetragonal derivatives of cubic NaZn13-type structure: RNi6Si6 compounds, crystal structure and magnetic ordering (R=Y, La, Ce, Sm, Gd–Yb)

(Mtext{ensuremath{-}}H)

The Ho-Ni-Ge system: Isothermal section and new rare-earth nickel germanides

loop from the origin. Such an attribute, designated as exchange bias in the context of ferromagnetic/antiferromagnetic multilayers, accords these compounds a potential for niche applications in spintronics. We also present results on magnetic compensation behavior on small Gd doping

New structures formed by R3Au4Sn3, R5Au8Sn5 and R3Au6Sn5 compounds (R= rare earths)

(2.5text{ }text{at}text{.}text{ }mathrm{%})

Structure and thermal stability of the RMgPb rare earth compounds, and the anomalous melting behaviour of SmMgPb

in one of the Sm ferromagnets (viz.,

Gold in the Layered Structures of R3Au7Sn3: From Relativity to Versatility

{text{SmCu}}_{4}text{Pd}