Two-dimensional zone-center spin-wave excitations in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
C. J. Peters(Massachusetts Institute of Technology), R. J. Birgeneau(Massachusetts Institute of Technology), M. A. Kastner(Massachusetts Institute of Technology), H. Yoshizawa(Massachusetts Institute of Technology), Y. Endoh(Brookhaven National Laboratory), J. M. Tranquada(Massachusetts Institute of Technology), G. Shirane(Brookhaven National Laboratory), Y. Hidaka(Massachusetts Institute of Technology), Masahiro Oda(Massachusetts Institute of Technology), M. Suzuki(Massachusetts Institute of Technology), T. Murakami(NTT (Japan))
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Abstract
We have studied the spin-wave excitations near the two-dimensional zone center at 80 K in a single crystal of ${\mathrm{La}}_{2}$Cu${\mathrm{O}}_{4}$ which orders at ${T}_{N}=195$ K. In-plane and out-of-plane modes are observed at energies of 1.0\ifmmode\pm\else\textpm\fi{}0.25 meV and 2.5\ifmmode\pm\else\textpm\fi{}0.5 meV, respectively, The in-plane mode energy is determined primarily by the antisymmetric exchange and it measures this term directly. The out-of-plane mode energy corresponds to a planar anisotropy energy of \ensuremath{\sim}0.016 meV. We observe, in addition, the appearance of significant $E\ensuremath{\simeq}0$ scattering below 30 K.
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