1992
DOI: 10.1364/josab.9.000794
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Persistent infrared spectral hole burning of Tb^3+ in the glasslike mixed crystal Ba_1−x_−yLaxTbyF_2+x_+y

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Cited by 27 publications
(37 citation statements)
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“…39 It is clear that g(V) obtained from experimental data and sketched in Figure 8B is not Gaussian and resembles the results of refs 10−12, where the g(V) ∼ 1/√V barrier distribution was deduced. A small plateau in the experimental data (diamonds) at the lowest temperatures can be explained by the smallest-barrier systems recovering due to tunneling during the first hour at burn temperature, before thermocycling started.…”
Section: Protein Energysupporting
confidence: 80%
“…39 It is clear that g(V) obtained from experimental data and sketched in Figure 8B is not Gaussian and resembles the results of refs 10−12, where the g(V) ∼ 1/√V barrier distribution was deduced. A small plateau in the experimental data (diamonds) at the lowest temperatures can be explained by the smallest-barrier systems recovering due to tunneling during the first hour at burn temperature, before thermocycling started.…”
Section: Protein Energysupporting
confidence: 80%
“…It is known that hole depth is closely related to the quantum efficiency of hole formation. 17,18 Thus, the efficiency of hole formation appears to be saturated beyond a certain condition ͑BNEC05͒. On the other hand, hole width increased further in the BNEC10 glass while maintaining the depth.…”
Section: Resultsmentioning
confidence: 97%
“…When we consider a two-level system which consists of burnt and unburnt states separated by a barrier with height V, hole relaxation can be described as a reaction between two states by either tunneling through or overcoming the barrier. 18,[35][36][37] The rate at which a burnt hole relaxes to an unburnt state is given by 18…”
Section: B Relaxation and Stability Of The Burnt Holementioning
confidence: 99%
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