Modifying phase transitions and spin structure of Ni$_{3}$V$_{2}$O$_{8}$ through transition metal doping

POSTER

Abstract

Ni$_{3}$V$_{2}$O$_{8}$ is a Kagome staircase material which has attracted considerable interest in recent years as it provides an excellent platform for studying the spin structure in geometrically frustrated materials. We have studied the effects of transition metal doping on the magnetic phase transitions of powder Ni$_{3}$V$_{2}$O$_{8}$ through dielectric, heat capacity and AC susceptibility measurements. (Ni$_{1-x}$M$_{x})_{3}$V$_{2}$O$_{8}$ (M = Zn, Cu and Co) powder samples were prepared using a standard metal-organic solution synthesis. We have mainly focused on the two phase transitions at T$_{H}$ = 9.2 K and T$_{L}$ = 6.3 K in undoped Ni$_{3}$V$_{2}$O$_{8}$. On doping with non magnetic Zn, the system acts similar to spin dilution where the transition temperature is suppressed linearly with the Zn fraction. However, spin 1/2 Cu and spin 3/2 Co doping shows significant deviation from simple site dilution. The Co:Ni$_{3}$V$_{2}$O$_{8}$ system has a crossover at moderate Co fraction where the system changes into a Co$_{3}$V$_{2}$O$_{8}$ type spin structure. Cu doping completely suppresses at least one phase transition at a relatively low Cu fraction. We also find that the Ni$_{3}$V$_{2}$O$_{8}$ spin structure is fairly robust and remains largely unaffected by introducing a few percent of a dopant, unlike the Co$_{3}$V$_{2}$O$_{8}$ spin structure, which is very sensitive to doping.

Authors

  • Akila Kumarasiri

    Wayne State University

  • J.A. Summers

    Duke University Medical Physics Graduate Program, Southwest Research Institute, Kettering University, Department of Physics and Astronomy, Wayne State University, Wayne State University, University of Nebraska, University of Stockholm, University of Michigan-Dearborn, Wayne State University, Detroit, MI, Cornell Univ., Air Force Research Labs, Univ. Akron, National Center for Manufacturing Sciences (NCMS), Youngstown State U, Dept. Physics, Department of Natural Sciences, University of Michigan-Dearborn, Department of Physics and Astronomy, Wayne State University, Detroit, Bhabha Atomic Research Centre, Hyderabad, India, NIST Center for Neutron Research, NIST, Gaithersburg, Maryland, Max Planck Institute for Solid State Research, Michigan State University

  • J.A. Summers

    Duke University Medical Physics Graduate Program, Southwest Research Institute, Kettering University, Department of Physics and Astronomy, Wayne State University, Wayne State University, University of Nebraska, University of Stockholm, University of Michigan-Dearborn, Wayne State University, Detroit, MI, Cornell Univ., Air Force Research Labs, Univ. Akron, National Center for Manufacturing Sciences (NCMS), Youngstown State U, Dept. Physics, Department of Natural Sciences, University of Michigan-Dearborn, Department of Physics and Astronomy, Wayne State University, Detroit, Bhabha Atomic Research Centre, Hyderabad, India, NIST Center for Neutron Research, NIST, Gaithersburg, Maryland, Max Planck Institute for Solid State Research, Michigan State University

  • J.A. Summers

    Duke University Medical Physics Graduate Program, Southwest Research Institute, Kettering University, Department of Physics and Astronomy, Wayne State University, Wayne State University, University of Nebraska, University of Stockholm, University of Michigan-Dearborn, Wayne State University, Detroit, MI, Cornell Univ., Air Force Research Labs, Univ. Akron, National Center for Manufacturing Sciences (NCMS), Youngstown State U, Dept. Physics, Department of Natural Sciences, University of Michigan-Dearborn, Department of Physics and Astronomy, Wayne State University, Detroit, Bhabha Atomic Research Centre, Hyderabad, India, NIST Center for Neutron Research, NIST, Gaithersburg, Maryland, Max Planck Institute for Solid State Research, Michigan State University