Neutron scattering studies on the vibrational excitations and the structure of ordered niobium hydrides: the   phases

2004 ◽  
Vol 16 (29) ◽  
pp. 5205-5228 ◽  
Author(s):  
B Hauer ◽  
R Hempelmann ◽  
T J Udovic ◽  
J J Rush ◽  
W Kockelmann ◽  
...  
1998 ◽  
Vol 57 (18) ◽  
pp. 11115-11124 ◽  
Author(s):  
B. Hauer ◽  
R. Hempelmann ◽  
T. J. Udovic ◽  
J. J. Rush ◽  
E. Jansen ◽  
...  

2010 ◽  
Vol 72 ◽  
pp. 158-163 ◽  
Author(s):  
Daniele Colognesi ◽  
Antonino Pietropaolo ◽  
Aníbal Javier Ramírez-Cuesta ◽  
Michele Catti ◽  
Angelo Claudio Nale ◽  
...  

Lithium imide (Li2NH) and amide (LiNH2) belong to the Li-H-N system, which has been recently considered for on-board hydrogen storage applications. However the imide low-temperature crystal structure is still highly controversial, with at least six options compatible with the diffraction experimental findings. A complementary study on low-temperature Li2NH and LiNH2 has been recently accomplished by the authors using neutron spectroscopy (with energy transfer in the 3-500 meV range). The rationale of these measurements was that crystal structures (especially their proton arrangements) affect in a strong way the neutron scattering spectra, so that a combined use of computer ab-initio simulations and inelastic neutron scattering could be a stringent validation method for the various models. Data analysis has pointed out broad and almost featureless proton-projected phonon densities of states for lithium imide, with large differences in the data sets derived from forward scattering and backscattering detector banks. On the contrary, a sharp phonon spectrum and much less discrepancy was found applying the same analytic procedure to lithium amide. This Li2NH peculiarity has been interpreted as an effect of the fast proton jump diffusion among the available lattice sites, which smears out the phonon vibrational excitations in a momentum transfer-dependent way.


1983 ◽  
Vol 27 (4) ◽  
pp. 1980-1990 ◽  
Author(s):  
J. Eckert ◽  
J. A. Goldstone ◽  
D. Tonks ◽  
D. Richter

Author(s):  
T. Egami ◽  
H. D. Rosenfeld ◽  
S. Teslic

Relaxor ferroelectrics, such as Pb(Mg1/3Nb2/3)O3 (PMN) or (Pb·88La ·12)(Zr·65Ti·35)O3 (PLZT), show diffuse ferroelectric transition which depends upon frequency of the a.c. field. In spite of their wide use in various applications details of their atomic structure and the mechanism of relaxor ferroelectric transition are not sufficiently understood. While their crystallographic structure is cubic perovskite, ABO3, their thermal factors (apparent amplitude of thermal vibration) is quite large, suggesting local displacive disorder due to heterovalent ion mixing. Electron microscopy suggests nano-scale structural as well as chemical inhomogeneity.We have studied the atomic structure of these solids by pulsed neutron scattering using the atomic pair-distribution analysis. The measurements were made at the Intense Pulsed Neutron Source (IPNS) of Argonne National Laboratory. Pulsed neutrons are produced by a pulsed proton beam accelerated to 750 MeV hitting a uranium target at a rate of 30 Hz. Even after moderation by a liquid methane moderator high flux of epithermal neutrons with energies ranging up to few eV’s remain.


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