Druck-Materie 20b.qxd - JUWEL - Forschungszentrum Jülich
Druck-Materie 20b.qxd - JUWEL - Forschungszentrum Jülich
Druck-Materie 20b.qxd - JUWEL - Forschungszentrum Jülich
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the formula also to the libration modes of around 170 (2) and 370 meV (3), and get the effective<br />
masses of 2.71 m and 3.13 m, respectively. They are also close to the free rotation effective<br />
mass. So, the recoil may be due to rotation.<br />
To get the information about the lattice mode in detail we obtained data with an incident<br />
energy of 100 meV. Scattering intensity against the neutron energy is shown in Fig. 2, where<br />
we compared the intensities between methane hydrate and ice. We can see several peaks in<br />
both intensity spectra and there is almost no difference between them. The levels observed are<br />
assigned to TA mode of 8.8 meV, LA mode of 18 meV, TO mode of 27 meV and TO mode<br />
of 35 meV. Librational modes appeared above about 65 meV. This suggests that around this<br />
energy region the neutron cross section of methane hydrate is expressed by linear combination<br />
of each material, methane and ice.<br />
To investigate the low energy level we performed experiments using an incident energy<br />
of 15 meV. Scattering intensity maps are indicated in Fig. 3 for CH4-D2O and D2O. It is<br />
clearly recognized the energy levels originated from methane hydrate by comparing the spectra.<br />
The level below 5 meV would be attributed to the methane mode. Level assignment is<br />
shown in Fig.4.<br />
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TA<br />
Translations<br />
LA<br />
LO<br />
TO<br />
Figure 2. Lattice modes of H2O in methane hydrate and ice<br />
Figure 3. Scattering intensities from CH4-D2O and D2O<br />
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£<br />
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99<br />
CH4-H2O<br />
(13K)<br />
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Librations<br />
H2O