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Atomic Motion in Low-Coverage Helium Films Adsorbed in FSM Nanochannels

机译:FSM纳米通道中吸附的低覆盖氦膜中的原子运动。

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~4He and ~3He films adsorbed in nanoporous silicates have shown similar heat capacities until the quantum-fluid layer appears at coverages over the first-layer completion n_1. To obtain information on dynamics of adatoms at low coverages below the quantum fluid region, we have done pulsed-NMR experiment at 3.3 MHz for ~3He films adsorbed in straight 2.4 nm nanochannels of FSM silicates. The spin-lattice and spin-spin relaxation times T_1 and T_2 observed at 0.54-7 K were well described by the two-dimensional version of the Bloembergen-Purcell-Pound model. At coverages 0.4-1.7n_1, minima of T_1, indicating the spin correlation time τ_c of 4.8 × 10~(-8) sec, were observed at temperatures between 6 and 3 K. With decreasing temperature, changes in T_1 and T_2 become small below about 1.5 K, suggesting crossover from thermally-activated motion to quantum tunneling. In contrast to large variations below n_1, both relaxation times above n_1 are almost independent of coverage, which is likely to indicate that τ_c is determined by interlayer exchange of adatoms. Below n_1, onsets for localization of adatoms were suggested by a decrease in T_2.
机译:吸附在纳米多孔硅酸盐中的〜4He和〜3He膜显示出相似的热容,直到量子流体层出现在第一层完成n_1的覆盖范围内。为了获得有关在量子流体区域以下低覆盖率的低原子吸附原子动力学的信息,我们在3.3 MHz上对FSM硅酸盐的直接2.4 nm纳米通道中吸附的〜3He薄膜进行了NMR脉冲实验。 Bloembergen-Purcell-Pound模型的二维形式很好地描述了在0.54-7 K处观察到的自旋晶格和自旋自旋弛豫时间T_1和T_2。在覆盖度0.4-1.7n_1处,在6至3 K之间观察到T_1的最小值,表明自旋相关时间τ_c为4.8×10〜(-8)sec。随着温度的降低,T_1和T_2的变化在以下温度下变小大约1.5 K,表明从热激活运动到量子隧穿的交叉。与n_1以下的较大变化相反,n_1以上的两个弛豫时间几乎都与覆盖率无关,这很可能表明τ_c是由吸附原子的层间交换确定的。在n_1以下,通过T_2的减少暗示了原子的局部化。

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