Heisenberg Model Analysis on Inelastic Powder Neutron Scattering Data Using Pure and K doped BaMn2As2 samples
ORAL
Abstract
Low temperature powder inelastic neutron scattering measurements (INS) were performed on powders of Ba(1-x)KxMn2As2 with x=0(BMA),0.125 and 0.25. BMA is a G type antiferromagnet (AFM) which has local magnetic modulations bridging between the pnictide and cuprate superconductors. Hole doping (K) introduces more metallic behavior. The magnetic contribution to the intensities were retrieved by subtracting the estimated phonon background obtained at high momentum transfers from the raw. The resultant estimated magnetic intensities were analyzed by using damped harmonic oscillator model. The K doping effects create a broadening in the magnetic peak profiles consistent with expected weak FM fluctuations. We also analyzed the INS data using a powder integration routine which is based on J1-J2-Jz Heisenberg Model. The Monte Carlo integration technique is used to obtain the powder-averaged S(Q,E) for a series of Js. The representative values (with lowest chi-squared) obtained for BMA are in agreement with previous results. The values obtained for K doped samples were found in the close proximity to the parent ones. Overall we conclude that the original AFM structure seen in BMA retained its character even in the K doped samples with minimal differences.
*Work at Ames Laboratory is supported by USDOE under Contract No. DE-AC02-07CH11358 and Work at ITU is supported by TUBITAK 2232
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Authors
Mehmet Ramazanoglu
Istanbul Techinal Univiversity
A. Sapkota
Ames Lab., Dept. of Physics and Astronomy, Iowa State Univ.
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University
Ames Lab. & Iowa State Univ., Ames, IA, 50011
A. Pandey
Ames Lab., Dept. of Physics and Astronomy, Iowa State Univ.
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University
Ames Laboratory, Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
Ames Lab. & Iowa State Univ., Ames, IA, 50011
David C. Johnston
Ames Lab., Dept. of Physics and Astronomy, Iowa State Univ.
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University
Ames Laboratory, Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
Ames Lab. & Iowa State Univ., Ames, IA, 50011
Iowa State Univ
Ames Laboratory, Dept. of Phys. and Astro, Iowa State Univ.
Alan Goldman
Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
Ames Lab., Dept. of Physics and Astronomy, Iowa State Univ.
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University
Ames Lab. & Iowa State Univ., Ames, IA, 50011
Iowa State University
A. Kreyssig$^{*}$
Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
Ames Lab., Dept. of Physics and Astronomy, Iowa State Univ.
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University
Ames Lab. & Iowa State Univ., Ames, IA, 50011
$^*$Ames Laboratory, Dept. of Phys. and Astro., Iowa State University, IA, USA; $^+$University of Missouri Research Reactor, MO, USA
Douglas Abernathy
Oak Ridge National Laboratory
Oak Ridge NAtional Lab., TN, 37831
Jennifer L. Niedziela
Oak Ridge National Laboratory
Oak Ridge NAtional Lab., TN, 37831
Oak Ridge National Laboratory, Materials Science Division
Matthew Stone
Oak Ridge NAtional Lab., TN, 37831
Quantum Condensed Matter Division, Oak Ridge National Laboratories
Quantum Condensed Matter Division, Oak Ridge National Laboratory
Oak Ridge National Laboratory
Spallation Neutron Source, Oak Ridge National Laboratory
R.J. McQueeney
Ames Laboratory, Dept. of Physics and Astronomy, Iowa State University