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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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The scattering function of a polycrystal is obtained by averaging over all crystal orientations<br />

S(Q, w) - 1 P<br />

~rüw 2 +112<br />

For small momentum transfers Qs k « 1 one eau expand f (Q) and obtains<br />

The second relation allows an interpretation<br />

dependence of the linewidth P - T .<br />

.S2<br />

P = 2Q2 6-F = 2Q 2 D (17 .22)<br />

of the macroscopic diffusion coefficient D of<br />

(17 .5) by the microscopie jump rate . While for small Q the macroscopic behaviour with the<br />

Q2 dependence of the linewidth is observed the data at large Q show the elementary step of a<br />

diffusion process . The fig . 17 .4 shows results for H in Pd .<br />

Transport jumps are thermally activated and follow an Arrhenius law<br />

E<br />

7 = 7oexp(-,) (17 .23)<br />

kBT<br />

From this relation the barrier height between neighbour sites is obtained from the temperature<br />

17 .2.4 More complex cases<br />

More than one sublattice<br />

For bec metals (fig . 17 .3), intermetallic compounds or metallic glasses one finds non equivalent<br />

hydrogen sites with different coordination numbers and jump rates . In case of bec lattices<br />

protons may occupy octahedral or different types of tetrahedral sites . The scattering function<br />

requires the Integration over the many possible different starting configurations . S(Q, w) consists<br />

now of a number ofLorentzians with different widths and partly rate dependent intensities<br />

[3] . The formalisme is more complex but basically identical .<br />

Blocking<br />

With increasing hydrogen concentration the diffusion changes since somejump directions may<br />

be blocked by a hydrogen neighbour . "Blocking" leads also to an increased probability ofback<br />

jumps, since the starting site is with certainty empty after thejump .<br />

Phonon-assisted Ibnnelling<br />

In some cases like NbHo .o2 the temperature dependence of the diffusion coefficient deviates<br />

from classical behaviour. The observation of an increasedjump rate at low temperature lead to<br />

the idea of "phonon-assisted tunnelling" : phonons of suited symmetry can increase temporarily<br />

the distance between the atours of the kost lattice which determine the jump barrier . The<br />

17- 8

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