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Neutron and x-ray spectroscopy. self-contained introduction neutron scattering and spectroscopy x-ray scattering and spectroscopy application to correlated-electron materials bulk interfaces. outline. B. Keimer Max-Planck-Institute for Solid State Research.
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Neutron and x-ray spectroscopy • self-contained introduction • neutron scattering and spectroscopy • x-ray scattering and spectroscopy • application to correlated-electron materials • bulk • interfaces outline B. Keimer Max-Planck-Institute for Solid State Research
Neutron scattering neutron E1 q1 excitation: E= E2-E1 q=q2-q1 E2 q2 interaction strong (nuclear) interaction elastic lattice structure inelastic lattice dynamics magnetic (dipole-dipole) interaction elastic magnetic structure inelastic magnetic excitations
Neutron sources neutron flux Maxwellian profile energy ~ 30 meV spectrum example research reactor FRM-II Garching, Germany
Elastic nuclear neutron scattering Bragg peaks at reciprocal lattice vectors K scattering length b ~ size of nucleus ~ 10-15 m
Neutron radiography mass attenuation coefficient
Elastic magnetic neutron scattering one electron “classical electron radius” non-spin-flip average for unpolarized beam σzσx , σy spin-flip (not possible for nuclear scattering)
Elastic magnetic neutron scattering one atom approximated as magnetized sphere, magnetization density M(r)
Elastic magnetic neutron scattering magnetic reciprocal lattice vectors generalization for collinear magnets Bragg peaks magnetic structure factor polarization factor
Neutron diffractometer single crystal powder
Example one-dimensional ferromagnet use interference between nuclear and magnetic scattering to create spin-polarized neutrons (up to prefactors)
Example vortex lattice in type-II superconductor small-angle neutron scattering
Example vortex lattice in type-II superconductor structural phase transition in vortex lattice H ~ Hc1: electrodynamic interaction between flux lines H ~ Hc2: vortex cores overlap structure depends onsuperconductingcoherence length
Inelastic neutron scattering elastic cross section inelastic cross section inelastic nuclear neutron scattering initial, final state of sample energy of excitation created by neutron in sample partition function
Inelastic nuclear neutron scattering thermal average characterized by population ns of phonons of energy in branch s Debye-Waller factor due to thermal lattice vibrations K) K)} phonon creation neutron energy loss phonon annihilaion neutron energy gain
Triple-axis spectrometer analyzer detector sample monochromator
Triple-axis spectrometer TRISP at FRM-II
Example C60 typical inelastic nuclear scattering scans with a triple-axis spectrometer lattice structure
Example C60 fcc lattice at room temperature molecules rotate freely molecules “lock in“ at low temperatures unit cell becomes larger new optical phonon modes appear
Inelastic magnetic neutron scattering Heisenberg antiferromagnet, magnon creation Km) Km, a = 0, 1 q, Km itinerant electrons next lecture polarization factor spin-spin correlation function
Example molecular magnetism Mn12 acetate molecule energy levels inelastic magnetic neutron scattering intensity Mn atoms
X-ray sources: tube setup spectrum
X-ray sources: synchrotron synchrotron primary spectrum insertion devices: wiggler, undulator
X-ray sources: synchrotron ESRF Grenoble, France
Thompson scattering – one electron differential cross section: one electron
Thompson scattering – one atom approximated as charged sphere, charge density ρ(r) atomic form factor × (polarization factor)
Thompson scattering – crystal lattice equilibrium positions thermal vibrations + … expansion of Debye-Waller factor Bragg reflections at reciprocal lattice vectors K thermal diffuse scattering
Inelastic x-ray scattering triple-axis spectrometer photon energy ~ 10 keV phonon energy ~ 10 meV resolution ΔE/E < 10-7 required
Inelastic x-ray scattering ID-16 ESRF Grenoble, France
Example MgB2 B vibration • - modulates Fermi surface • drives superconductivity (Tc = 39 K) IXS data
X-ray absorption interaction Hamiltonian absorption photon annihilated scattering photon number conserved absorption cross section
X-ray absorption mass absorption coefficient
Example K-edge transitions into continuum absorption cross section
Example Fe L-edge valence state chemical analysis example Fe thin film example TbFeCo alloy
X-ray radiography dual-energy x-ray radiography discriminate between carbohydrates and metals
Example K-edge selection rules transition into unoccupied excited state electric dipole matrix element
Magnetic circular dichroism example single atom electric dipole selection rules
Magnetic circular dichroism classical calculation for bound electron analogous to Thompson scattering
Magnetic circular dichroism circular birefringence index of refraction circular dichroism absorption coefficient