Abstract
We have studied the thickness and quench-rate dependent internal friction of amorphous selenium (a-Se) thin films deposited at room temperature. The internal friction of a-Se films exhibit a temperature independent plateau below 1 K followed by a broad maximum at 10 K. The plateau, which is seen in almost all amorphous solids, is caused by dissipation by two-level tunneling systems (TLS), whose origin is still unknown. The maximum is caused by thermal relaxation over the same energy barrier that induces TLS. The internal friction and shear modulus are almost thickness independent from 100 nm to 10 µm. Unlike other elemental amorphous materials, the sufficiently low glass transition temperature (Tg) of a-Se (only about 10 K above room temperature) allows in-situ quench-rate dependent study of TLS. The amorphous structure resets itself by a thermal equilibration cycle above Tg. We show that a faster quench rate freezes a-Se to a lower density structure with a higher TLS density and vice versa. The changes are reversible supporting a relationship between different quenched states and the density of TLS. Our study shows that a-Se can be a simple monatomic amorphous system to constrain models for the origin of TLS in amorphous solids.
Highlights
One of the unsolved mysteries in condensed matter physics is the origin of the low-energy excitations in amorphous solids 1,2
As we show that tunneling systems (TLS) are linked to the frozen-in states in amorphous selenium (a-Se), a study of substrate temperature dependence of TLS density would help us to answer the following questions: if vapor deposited a-Se can become ultrastable, and if TLS can be removed from this twofold covalently bonded amorphous system
In this work we show that the internal friction and the relative change of speed of sound of a-Se films exhibit the typical behavior of amorphous solids
Summary
One of the unsolved mysteries in condensed matter physics is the origin of the low-energy excitations in amorphous solids 1,2. The existence of such ubiquitous lowenergy excitations enables amorphous solids to exhibit many universal properties that are absent in crystalline solids. While defect states in crystals usually have characteristic energies, the low-energy excitations of amorphous solids have a broad and almost energy independent distribution They are the source of anomalous thermal, elastic and dielectric properties of amorphous solids 2, such as: a linear temperature (T) dependent specific heat, T2 thermal conductivity below 1 K, and an almost T independent plateau in internal friction at a few K. The challenge of identifying the microscopic origin of TLS stems from the universality of the excitations
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