2015
DOI: 10.1209/0295-5075/109/56001
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Inversion symmetric vs. asymmetric excitations and the low-temperature universal properties of Ar:N 2 and Ar:N 2 :CO glasses

Abstract: The bias energies of various two-level systems (TLSs) and their strengths of interactions with the strain are calculated for Ar:N2 glass. Unlike the case in KBr:CN, a distinct class of TLSs having weak interaction with the strain and untypically small bias energies is not found. The addition of CO molecules introduces CO flips which form such a class of weakly interacting TLSs, albeit at much lower coupling than that at which they are typically observed in solids. We conclude that because of the absence of a d… Show more

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Cited by 4 publications
(12 citation statements)
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“…We applied the developed technique for an analysis of the coupling on an Ar:N 2 mixture, as it is a physically intriguing case of disordered lattice where ample experimental information is available. A discussion about the physical properties of this system, which employs the method presented here, is performed in .…”
Section: Discussionmentioning
confidence: 99%
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“…We applied the developed technique for an analysis of the coupling on an Ar:N 2 mixture, as it is a physically intriguing case of disordered lattice where ample experimental information is available. A discussion about the physical properties of this system, which employs the method presented here, is performed in .…”
Section: Discussionmentioning
confidence: 99%
“…We can see that we have over 700 possible TLSs for each case on this range and is enough to be considered as a statistically representative sample even for a low density study. The results for higher densities and their physical meaning, which are outside the scope of this paper, are further discussed in .…”
Section: Disordered Infinite Medium Excitations For Tunneling Effectmentioning
confidence: 99%
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“…First considering only elastic interactions, the Two-TLS model divides TLSs into two groups, with bimodal distribution of their interaction strengths with the strain, denoted by γ w for the weakly interacting τ -TLSs, which correspond to the abundant TLSs at low energies, and by γ s for the other defects, where g ≡ γ w /γ s ≈ 0.02 [13,[44][45][46][47][48]. The Hamiltonian 2 is then derived as the low-energy effective Hamiltonian of the system (see Ref.…”
Section: Interaction Between Nn General Defects Tls Disorder Energy I...mentioning
confidence: 99%
“…The Two-TLS model was microscopically derived [13] and thoroughly validated [44][45][46][47][48] for disordered lattices which share the same universal low temperature phenomena with amorphous solids [2]. Here we assume the generalized validity of the Two-TLS model in describing TLSs in amorphous solids.…”
mentioning
confidence: 95%