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Ph.D. thesis (pdf) - dirac

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126 Mean squared displacement<br />

1.4<br />

1.2<br />

0.4<br />

0.2<br />

int [arb. units]<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

−0.6<br />

10 K<br />

0.2 0.50 A −1<br />

−0.8 150 K<br />

1.68 A −1 210 K<br />

−1<br />

0<br />

0<br />

0 50 100 150 200 250 300<br />

1 2 3 4<br />

T [K]<br />

Q. 2 [A −2 ]<br />

ln(int) [arb uni]<br />

0<br />

−0.2<br />

−0.4<br />

Figure 7.3: Illustration of the temperature and Q dependence of the measured elastic<br />

intensity (DBP at atmospheric pressure). Left: the temperature dependence of the<br />

intensity at two different Q-values. Right: The logarithm of the measured intensity<br />

as a function of Q 2 at three different temperatures. The lines are fits to the Gaussian<br />

approximation.<br />

/ A 2<br />

1.5<br />

1<br />

0.5<br />

0.01 MPa<br />

500 MPa<br />

Tg<br />

Tg @ 500 MPa<br />

0<br />

0 50 100 150 200 250<br />

T / [K]<br />

Figure 7.4: The mean square displacement of DBP as a function of temperature at<br />

atmospheric pressure (dots) and at 500 MPa (full line). The vertical lines illustrate<br />

the positions of T g at these two pressures.<br />

[A 2 ]<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.01 MPa<br />

500 MPa<br />

Tg<br />

Tg @ 500 MPa<br />

0<br />

0 50 100 150 200<br />

T / [K]<br />

Figure 7.5: The mean square displacement of cumene at atmospheric pressure<br />

(squares) and 500 MPa (triangles). The vertical lines illustrate the positions of<br />

T g at these two pressures.

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