Extended Data Fig. 4: Measurements and simulations of the 800 nm/700 nm -emission as a function of Tm3+ concentration. | Nature

Extended Data Fig. 4: Measurements and simulations of the 800 nm/700 nm -emission as a function of Tm3+ concentration.

From: Infrared nanosensors of piconewton to micronewton forces

Extended Data Fig. 4

a. Single particle spectra, measured for different Tm3+ concentration pre-ANPs/ANPs, at their respective saturation regimes (excitation wavelength: 1064 nm; excitation intensity: 376 kW cm−2 (4% Tm3+), 1,849 kW cm−2 (5% Tm3+), 517 kW cm−2 (15% Tm3+)). b. 800 nm / 700 nm -emission ratio as a function of Tm3+ concentration for different Tm3+ concentration pre-ANPs/ANPs, measured at their respective saturation regimes (excitation wavelength: 1064 nm; excitation intensity: 376 kW cm−2 (4% Tm3+), 1,849 kW cm−2 (5% Tm3+), 517 kW cm−2 (15% Tm3+)). Error bars are the standard deviations of three single-NP measurements. c. Photon avalanche differential rate equation (DRE) model simulations of the 800 nm / 700 nm -emission ratio as a function of Tm3+ concentration. The DRE simulations for the different Tm3+ concentrations were performed with the respective parameters (per Tm3+ concentration) extracted from fitting the emission versus excitation graphs measured at zero applied force (Supplementary Note 6, Table S3, and Fig. S5). Note that the DRE model predicts Tm3+ emissions from these levels up to a certain excitation threshold, above which other, higher-level, excited states are populated and thus must be taken into account. Any discrepancies between the simulated values here and the measured ones in a-b may be accounted for by adding DREs for higher levels (above 3F2). Other factors – such as determination of exact concentrations and hence energy transfer rates, or discernment of the precise 700 nm emission at lower concentrations and hence experimental 800 nm / 700 nm -emission ratios – may also reduce discrepancies between simulated and measured values. The DRE simulations show that higher cross-relaxation rates, attained at higher Tm3+ concentrations, decrease the 800 nm / 700 nm -emission ratio by: 1. Populating 3F4 at a faster rate, which, in turn, populates 3F3 at a faster rate by direct excited state absorption. 2. Depopulating 3H4 at a faster rate.

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