4.7 Article

Free volume in imidazolium triflimide ([C3MIM][NTf2] ionic liquid from positron lifetime: Amorphous, crystalline, and liquid states

Journal

JOURNAL OF CHEMICAL PHYSICS
Volume 133, Issue 12, Pages -

Publisher

AMER INST PHYSICS
DOI: 10.1063/1.3487522

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Positron annihilation lifetime spectroscopy (PALS) is used to study the ionic liquid 1-methyl-3-propylimidazolium bis(trifluoromethylsulfonyl)imide [C3MIM][NTf2] in the temperature range between 150 and 320 K. The positron decay spectra are analyzed using the routine LifeTime-9.0 and the size distribution of local free volumes (subnanometer-size holes) is calculated. This distribution is in good agreement with Furth's classical hole theory of liquids when taking into account Furth's hole coalescence hypothesis. During cooling, the liquid sample remains in a supercooled, amorphous state and shows the glass transition in the ortho-positronium (o-Ps) lifetime at 187 K. The mean hole volume varies between 70 angstrom(3) at 150 K and 250 angstrom(3) at 265-300 K. From a comparison with the macroscopic volume, the hole density is estimated to be constant at 0.20 x 10(21) g(-1) corresponding to 0.30 nm(-3) at 265 K. The hole free volume fraction varies from 0.023 at 185 K to 0.073 at T-m + 12 K=265 K and can be estimated to be 0.17 at 430 K. It is shown that the viscosity follows perfectly the Cohen-Turnbull free volume theory when using the free volume determined here. The heating run clearly shows crystallization at 200 K by an abrupt decrease in the mean and standard deviation sigma(3) of the o-Ps lifetime distribution and an increase in the o-Ps intensity I-3. The parameters of the second lifetime component and sigma(2) behave parallel to the o-Ps parameters, which also shows the positron's (e(+)) response to structural changes. During melting at 253 K, all lifetime parameters recover to the initial values of the liquid. An abrupt decrease in I-3 is attributed to the solvation of e(-)and e(+) particles. Different possible interpretations of the o-Ps lifetime in the crystalline state are briefly discussed. (C) 2010 American Institute of Physics. [doi: 10.1063/1.3487522]

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