Abstract
A phenomenological model of electron mobility in liquid hydrocarbons is presented, which incorporates ballistic motion in the quasi-free state, showing that this effect predominates in the low-mobility case. Even for infinite quasi-free mobility finite overall mobility results due to random cycles of trapping and detrapping. Experimental comparison for n-hexane, a typical low-mobility liquid, reveals quasi-free mobility, trap density and binding energy in the trap at room temperature respectively as ≈ 100 cm 2/V s, 10 19 cm −3 and 0.15 eV.
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