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Ph.D. thesis (pdf) - dirac

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116 High Q collective modes<br />

[Alba-Simionesco et al., 2004; Casalini and Roland, 2004], and the density dependence<br />

of the relaxation time, which is contained in<br />

d log e(ρ)<br />

d log ρ .<br />

m P<br />

/m ρ<br />

2<br />

1.9<br />

1.8<br />

1.7<br />

1.6<br />

1.5<br />

1.4<br />

1.3<br />

1.2<br />

1.1<br />

1<br />

0 0.2 0.4 0.6 0.8<br />

α<br />

m P<br />

/m ρ<br />

2.2<br />

2<br />

1.8<br />

1.6<br />

1.4<br />

1.2<br />

1<br />

0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9<br />

f(T g<br />

)<br />

Figure 6.24: The ratio between isochoric and isobaric fragility as a function of f Q (T g )<br />

and α. The legend is found in figure 6.21.<br />

dlog e(ρ)<br />

In figure 6.25 we show the f Q (T g ) value versus<br />

d log ρ<br />

. The amount of data is<br />

limited and the uncertainty on this type of data is large, but it is striking that we<br />

d log e(ρ)<br />

d log ρ<br />

. It is striking<br />

can be determined from the dynamics of the non-viscous<br />

obtain a new correlation. The smaller f Q (T g ) is the larger is<br />

most of all because<br />

d log e(ρ)<br />

d log ρ<br />

liquid at high temperatures [Alba-Simionesco et al., 2002]. We contemplate that<br />

the correlation proposed between f Q (T g ) and m P is a reminiscent signature of a<br />

dlog e(ρ)<br />

correlation between f Q (T g ) and<br />

d log ρ<br />

. An excellent test case for this hypo<strong>thesis</strong><br />

would be to measure f Q (T g ) on sorbitol which has a very high m P -value combined<br />

d log e(ρ)<br />

with an exceptionally low value of<br />

d log ρ<br />

[Roland et al., 2005].<br />

It appears that the anti-correlation between<br />

correlation between<br />

d log e(ρ)<br />

dlog ρ<br />

dlog e(ρ)<br />

d log ρ<br />

and f Q (T g ) is better than the<br />

and α. This is particularly true when considering the<br />

pressure dependence of the quantities in the case of cumene;<br />

d log e(ρ)<br />

dlog ρ<br />

does not depend<br />

on pressure and the pressure dependence of f Q (T g ) is weak whereas α has a<br />

significant pressure dependence. It is difficult to know if the pressure independence<br />

dlog e(ρ)<br />

of f Q (T g ) of cumene is a coincidence or if this could be general for systems with constant<br />

dlog ρ . f Q(T g ) decreases with pressure both in the case of PIB and DBP, the<br />

correlation suggested from figure 6.25 therefore implies that should increase<br />

dlog e(ρ)<br />

d log ρ<br />

with pressure. In section 5.2.1 we show that DBP is in fact a system where<br />

increases with pressure, and PIB could be a similar system (see appendix A).<br />

d log e(ρ)<br />

dlog ρ<br />

A physical significance of the correlation is that the larger the vibrational compressibility<br />

is relative to the total compressibility the more sensitive to density is the

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