Proton NMR Study of Random Mixture Fe1-xMnxCl2·2H2O with Competing Anisotropies and Exchange Interactions
Kazuko Zenmyo, Hidenori Kubo, Hiroyuki Deguchi, Kazuyoshi Takeda
Abstract
Kazuko Zenmyo, Hidenori Kubo, Hiroyuki Deguchi, Kazuyoshi Takeda
Abstract
Proton NMR measurements of Fe 1- x Mn x Cl 2 ·2H 2 O are carried out. In the Mn-type antiferromagnetic phase all spins are parallel to the b -axis which is the easy axis of MnCl 2 ·2H 2 O. In the Fe-type antiferromagnetic phase, for Fe-rich region, all spins are parallel to the α-axis which is the easy axis of FeCl 2 ·2H 2 O, and with increasing Mn concentration some Mn spins tilt from the α-axis. In the “intermediate” phase Fe- or Mn-type (oblique) antiferromagnetic spins coexist with the spin glass spins. All spins lie in the α b -plane with the angle depending on the Mn concentration.
OpenAlex reports 4 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Proton NMR measurements of Fe 1- x Mn x Cl 2 ·2H 2 O are carried out. In the Mn-type antiferromagnetic phase all spins are parallel to the b -axis which is the easy axis of MnCl 2 ·2H 2 O. In the Fe-type antiferromagnetic phase, for Fe-rich region, all spins are parallel to the α-axis which is the easy axis of FeCl 2 ·2H 2 O, and with increasing Mn concentration some Mn spins tilt from the α-axis. In the “intermediate” phase Fe- or Mn-type (oblique) antiferromagnetic spins coexist with the spin glass spins. All spins lie in the α b -plane with the angle depending on the Mn concentration.
Key concepts: Spins, Antiferromagnetism, Anisotropy, Crystallography, Materials science, Phase (matter), Proton, Spin (aerodynamics)