2011
DOI: 10.1103/physrevlett.107.105504
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Identification of Strong and Weak Interacting Two-Level Systems in KBr:CN

Abstract: Tunneling two-level systems (TLSs) are believed to be the source of phenomena such as the universal low temperature properties in disordered and amorphous solids, and 1/f noise. The existence of these phenomena in a large variety of dissimilar physical systems testifies for the universal nature of the TLSs, which however, is not yet known. Following a recent suggestion that attributes the low temperature TLSs to inversion pairs [M. Schechter and P. C. E. Stamp, arXiv:0910.1283.] we calculate explicitly the TLS… Show more

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Cited by 21 publications
(51 citation statements)
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“…Thus, the TLS-DOS in disordered lattices is not small, but the relevant TLSs are τ -TLSs, between which the interaction is small and can therefore be neglected, and the experimentally observed smallness of the TLSs DOS is related to the fact that only TLSs with appreciable tunneling amplitude can be detected. Note that in KBr:CN the TLS is formed by each CN low energy state and the state related to it by a CN flip [12,14,23,29], and is thus a τ -TLS, where all other single particle states of a given CN impurity are much higher in energy [27], as they constitute an S excitation with respect to the CN low energy state [23].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Thus, the TLS-DOS in disordered lattices is not small, but the relevant TLSs are τ -TLSs, between which the interaction is small and can therefore be neglected, and the experimentally observed smallness of the TLSs DOS is related to the fact that only TLSs with appreciable tunneling amplitude can be detected. Note that in KBr:CN the TLS is formed by each CN low energy state and the state related to it by a CN flip [12,14,23,29], and is thus a τ -TLS, where all other single particle states of a given CN impurity are much higher in energy [27], as they constitute an S excitation with respect to the CN low energy state [23].…”
Section: Introductionmentioning
confidence: 99%
“…These results support both the two-TLS model and the notion that it is indeed CN flips that constitute the TLSs for KBr:CN. However, the ab-initio and DFT calculations [29] required the use of very small samples, not allowing the study of the effective TLS-TLS interactions and their distance dependence.…”
Section: Introductionmentioning
confidence: 99%
“…Experimentally, TLSs can be directly probed by phonon echo experiments [47][48][49]. However, because of the scarcity of S-TLSs [34] at energies probed by these experiments so far (of order 10GHz and below), experiments find only one type of TLSs, with a coupling constant shown to agree with that of τ-TLSs [36]. However, under certain conditions the S-TLSs can dominate spectral diffusion and the acoustic response.…”
Section: Spectral Diffusion and Nonlinear Acoustic Absorptionmentioning
confidence: 99%
“…example C in figure 1 of [48]) states. Since defect-phonon coupling in amorphous solids is expected to be an order of magnitude larger than in disordered crystals [26,[50][51][52], our results suggest that the tunneling amplitude of inversion asymmetric TLSs, such as in example C in figure 1 of [48] for KCl (from [56]) and the geometry factor [23] is = f 1 5 t . With these parameters the Debye-Waller exponent equation (A.1) can be determined keeping in mind that the longitudinal speed of sound is larger and the transversal one and thus contributions from longitudinal phonon branches are negligible in equation (A.1).…”
Section: Experimental Relevancementioning
confidence: 99%
“…Most experimental data, however, is acquired in samples with defect concentrations  n 100 ppm, where many body effects complicate the situation. From a first-principle argumentation one actually expects for tunneling defects with no special symmetry, rather strong defect-phonon couplings [24,26].…”
Section: Introductionmentioning
confidence: 99%