# # arev:/usr/local/unicat/unireq/beamreq/req00075.txt # UNICAT Member Beam Time Request #75 # created Fri Jul 02 16:09:20 CDT 1999 # days: 5 description: Momentum Conservation and Resonant Inelastic X-ray Scattering in Al3Ni Z. Hasan and A. Panchula, Stanford University; C. Burns, Western Michigan University; P. Canfield, Ames Laboratory and Iowa State University; E.E. Alp, Advanced Photon Source; D. Muller and E.D. Isaacs, Bell Laboratories, Lucent Technologies. Resonant inelastic x-ray scattering (RIXS) is rapidly developing as a technique for probing elementary excitations in condensed matter and liquid systems. Large resonance enhancements of the inelastic scattering cross-section make it possible to study electronic excitations in systems where absorption would otherwise make such measurements impossible. However, the fate of resonant inelastic scattering ultimately depends on whether it can be used to measure the true electronic excitation spectra. In particular, there is currently heated debate as to whether resonance techniques can be used to measure dispersion or rather a joint density-of-states. Recent studies of charge transfer excitations in insulating La2CuO4 have shown strong evidence that the resonant inelastic cross-section has the relatively simple form; . (1) In other words, the resonant cross-section is in fact the dynamic structure factor times resonant denominators which depend on the incident, wi, and scattered, wf photon energies, respectively. This form results from the fact that the excited states of the system (S(q,w)) are accessed through Coulomb interactions with the intermediate state (1S hole/4P electron pair). The Coulomb interaction will of course conserve energy and momentum. The essence of this study was that energy is conserved through the resonance process, i.e., that excitation spectra depends only on the energy difference, w = wf - wi. However, in this study no variations with q were observed for the charge transfer excitation at 6 eV. Nor were they expected since the charge transfer excitation was localized on the CuO6 complex. Therefore, there is not yet conclusive evidence the resonance processes conserve momentum, q = qf - qi. Therefore, we propose to study resonant inelastic scattering in Al3Ni at and below the Ni K-edge. Al3Ni is known to have a sharp plasmon near 16 eV only slightly shifted from Al. In other words, Al3Ni is a free-electron like system with the added attraction of having the Ni atom with an accessible K-edge at 8.333 keV. Furthermore, the penetration depth in Al3Ni just below the K-edge is large, ~ 50 mm. Therefore, we should be able to measure the plasmon dispersion both on-and off-resonance. If Eq. (1) is correct these two measurements will be identical, once the resonance denominators are factored out. Al3Ni does not melt congruently and is thus difficult to grow in large single crystals. However, we are lucky enough to be able to collaborate with Prof. Paul C. Canfield, Department of Physics and Astronomy at Iowa State and Ames Laboratory who has just recently grown single crystals of 1 - 2 mm in size. Since a detailed understanding of S(q,w) is essential for the success of this experiment we are also collaborating with Dr. David Muller of Bell Laboratories who is an expert in electron-energy-loss spectroscopy (EELS). He has already extensively studied AlNi3 and AlNi and will participate in this study by measuring S(q,w) in our Al3Ni samples prior to the measurement at the APS. While we have yet to measure the plasmon in Al3Ni, from Dr. Muller's previous measurements we believe that the plasmon width should be about 1 eV. This means that our measurement is reasonably well matched to the ~2 eV energy resolution produced by the 33ID Si(111) monochromator. We propose to work at 33ID and will provide the Si(551), spherically-bent analyzer whose resolution is approximately 100 meV. This collaboration will also include Prof. Clement Burns of Western Michigan University, an expert in inelastic x-ray scattering, and Zahid Hasan and Alex anchula both students at Stanford University preparing theses based at synchrotron facilities. equipment+required: High resolution analyzer experiment: Resonant Plasmon Dispersion hazards: None name: E.D.Isaacs new+request: on nonmembers: Several (see above) station: 33ID-D unacceptable+dates: #QUERY_STRING: #REMOTE_HOST: pwk.uni.aps.anl.gov #REMOTE_ADDR: 164.54.216.37 #CONTENT_LENGTH: 4803 #HTTP_REFERER: http://www.uni.aps.anl.gov/unireq.htm #HTTP_USER_AGENT: Mozilla/4.5 [en] (Win98; I)