1994
DOI: 10.1103/physrevb.49.5821
|View full text |Cite
|
Sign up to set email alerts
|

Sample-dependent optical dephasing in bulk crystalline samples ofY2O3

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

13
42
1

Year Published

2002
2002
2017
2017

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 52 publications
(56 citation statements)
references
References 19 publications
13
42
1
Order By: Relevance
“…[27][28][29] The extrapolated zero power homogeneous linewidths are Γ h = 7.5 ± 0.2 kHz (corresponding to a coherence lifetime T 2 = 1/(πΓ h ) of 42 µs) at 3.5 K. The same value was found for the 1.0% sample without additives, while the 0.5% sample with additives showed a slightly larger homogeneous linewidth of 9.2 ± 0.6 kHz (T 2 = 35 µs). Even though those homogeneous linewidths are still about one order of magnitude larger than that observed in the very best crystal known (Γ h = 760 Hz), 20 they are in the lower range of values observed for Eu 3+ :Y 2 O 3 crystals (Γ h = 2.4 − 42 kHz 19 ) and considerably narrower than that previously reported in transparent ceramics Γ h = 59 kHz. 12 The contribution to the homogeneous linewidth Γ h from the excited state population is given by Γ pop = 1/(2πT 1 ).…”
mentioning
confidence: 50%
See 1 more Smart Citation
“…[27][28][29] The extrapolated zero power homogeneous linewidths are Γ h = 7.5 ± 0.2 kHz (corresponding to a coherence lifetime T 2 = 1/(πΓ h ) of 42 µs) at 3.5 K. The same value was found for the 1.0% sample without additives, while the 0.5% sample with additives showed a slightly larger homogeneous linewidth of 9.2 ± 0.6 kHz (T 2 = 35 µs). Even though those homogeneous linewidths are still about one order of magnitude larger than that observed in the very best crystal known (Γ h = 760 Hz), 20 they are in the lower range of values observed for Eu 3+ :Y 2 O 3 crystals (Γ h = 2.4 − 42 kHz 19 ) and considerably narrower than that previously reported in transparent ceramics Γ h = 59 kHz. 12 The contribution to the homogeneous linewidth Γ h from the excited state population is given by Γ pop = 1/(2πT 1 ).…”
mentioning
confidence: 50%
“…The excited-state lifetimes measured in the ceramic samples (Table I) are similar to those reported for single crystals. 19 Thus, Γ pop is less than 200 Hz and therefore much smaller than the observed Γ h . Other possible contributions to Γ h are dynamic structural fluctuations due to tunneling between configurations with nearly equal energy referred to as two-level systems (TLSs).…”
mentioning
confidence: 99%
“…It has been proposed that low densities of TLS can be present in some crystalline materials with large inhomogeneous lattice strains [68]. Decoherence attributed to TLS has been previously observed in both bulk crystals [29,59] and powders [30], and it has also been suggested that TLS can cause rapid electron spin relaxation [69]. This interpretation is also consistent with past observations of increased electronic spin-lattice relaxation rates of Nd 3+ in YAG single crystals with a high density of structural defects in the lattice [70] as well as increased nuclear spin relaxation rates of 169 Tm 3+ in YAG powders fabricated by ball milling [49].…”
Section: Magnetic Field Dependence Of Coherence Lifetimesmentioning
confidence: 99%
“…Therefore, the usual characterization methods employed for REI-doped crystals such as 2PE, SHB, or FID are difficult to perform with powders. Previous measurements on powders have mostly employed detection of fluorescence emission to observe SHB [29,31,59], with direct transmission detection of SHB [49] and 2PE [36,37] only recently being successfully applied to powders. In particular, FID measurements on powders have not been previously reported to our knowledge.…”
Section: Optical Coherence Lifetime Measurementsmentioning
confidence: 99%
See 1 more Smart Citation