Therefore, as shown in Equation 4, the quantum yield for FITC molecules experimentally measured 0.12, which was excited at 405 nm and emitted at 510 nm.
Figure 7b demonstrates the PL spectra of the CdS-decorated TiO2 NRAs, which are excited at a wavelength of 350 nm.
Numerical results are presented for the power flow between two coupled beams one of which is excited at a point by a random force.
The emission spectra of DTH-Fe3O4@SiO2, which is excited at 397 nm, exhibit the emission maximum at 452 nm with a low quantum yield (Φ = 0.0042) at room temperature in ethanol.
The intracellular DCF fluorescence intensity, which is excited at 485 nm and emitted at 530 nm, was detected using a microplate reader (Synergy-2; BioTek Instruments) to investigate the extent of oxidative stress.
After washing with PBS, the intracellular DCF fluorescence intensity which was excited at 485 nm and emitted at 530 nm was detected using a microplate reader (Synery-2, Biotek, USA) to investigate the extent of oxidative stress.
For a clamped joint the dominant source of the diffraction radiation is the interaction with the joint of flexural waves in the coated plate which are excited at resonance by low wavenumber components of the turbulence wall pressure.
Here, the remarkable decrease of fluorescence intensity can be explained as follow: The fluorescence intensity of BHN-Fe3O4@SiO2 BHN-Fe3O4@SiO2ted at a 415 nm lamp, exhibits the high fluorescence at 518 nm due to the 1,8-naphthalimide which has a bis conjugatexcitedem.
Free Dox and Dox-loaded TPP-NPs at the same amount of Dox were treated with both cells, and the intensity of fluorescence from Dox which was excited at 479 nm and emitted at 587 nm was quantified using a microplate reader.
The slices were stained with the fluorescent intravital Na+ indicator SFBI (Harootunian et al, 1989), which was excited at a wavelength of 820 nm.
