Prefer a chat interface with context about you and your work?
Dispersion of Magnetic Excitations in Optimally Doped Superconducting<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">Y</mml:mi><mml:mi mathvariant="normal">B</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">u</mml:mi></mml:mrow><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O…
Detailed neutron scattering measurements of ${\mathrm{Y}\mathrm{B}\mathrm{a}}_{2}{\mathrm{C}\mathrm{u}}_{3}{\mathrm{O}}_{6.95}$ found that the resonance peak and incommensurate magnetic scattering induced by superconductivity represent the same physical phenomenon: two dispersive branches that converge near 41 meV and the in-plane wave vector ${\mathbf{q}}_{\mathrm{A}\mathrm{F}}=(\ensuremath{\pi}/a,\ensuremath{\pi}/a)$ to form the resonance peak. One branch has a circular symmetry around ${\mathbf{q}}_{\mathrm{A}\mathrm{F}}$ …