Fig. 2 Photophysical characteristics.

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From: A High-Throughput Biophotonics Instrument to Screen for Novel Ocular Photosensitizing Therapeutic Agents Invest. Ophthalmol. Vis. Sci ;51(5):
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The fluorescent receptor chains exhibit their characteristic fluorescent signatures: images and spectra of human IFN-γR2/GFP and IFN-γR2/EBFP transfected.
Volume 2, Issue 4, Pages (April 2017)
Fig. 4 RISC mechanism of TADF-active molecules.
Fig. 5 In vivo MIP imaging of lipid and protein in C. elegans.
Fig. 1 Upward emission functions used to compute the maps.
Fig. 1 Sensing scheme with an atomic spin sensor.
Fig. 2 New bathymetry. New bathymetry. (A) Uninterpreted bathymetry. Black lines represent seismic profiles acquired. The white line shows the position.
Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.
Fig. 2 Rydberg-EIT spectra without control pulse.
Fig. 5 Metafluorophores with different photostability.
Fig. 2 SFG spectra for CTAB adsorption on PETS.
Fig. 4 States of the Antarctic Ice Sheet after 10,000 years.
Fig. 7 LSH database and similarity search example.
Fig. 4. Spectra of monochromatic light from the OLS
Fig. 2 EL performance of tBCzHxPO- and tBCzMxPO-based TADF diodes.
Fig. 1 Pump-probe signatures of vermilion (red HgS), black HgS, and metallic Hg. Pump-probe signatures of vermilion (red HgS), black HgS, and metallic.
Structural analysis of graphene-embedded FeN4 (FeN4/GN) catalysts
Fig. 1 Map of the trifurcation area of the SJFZ.
Fig. 3 Faculty placement distributions.
Fig. 2 Fluence-dependent emission characteristics of CH3NH3PbI3 recorded at 15 and 300 K. Fluence-dependent emission characteristics of CH3NH3PbI3 recorded.
Fig. 1 CFHT photometry converted into spectral reflectivity obtained on UT (Universal Time) 22 and 25 October 2014, is shown in comparison to the VLT reflectivity.
Fig. 2 Device characteristics.
Fig. 3 Raman spectroscopy of the phonon-polariton laser and the reference laser with GaAaSb barriers. Raman spectroscopy of the phonon-polariton laser.
Fig. 3 Controlled phase shift.
Fig. 2 Overview of writing, reading and erasing procedure.
Characterization of the MCs.
Fig. 2 Broadband IR s-SNOM of large crystallites.
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Fig. 4 Memristive characteristics in a 1T-TaS2 nano-thick crystal.
Fig. 3 ET dynamics on the control and treatment watersheds during the pretreatment and treatment periods. ET dynamics on the control and treatment watersheds.
Fig. 3 Transport characterization of dry-assembled devices.
Fig. 3 Evolutions of freshwater transport and salinity.
Fig. 1 Crystal structure and superconductivity in fcc fullerides.
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by Toan Trong Tran, Blake Regan, Evgeny A
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Fig. 2 Comparison of the observed DRs and the estimates by the VR model and FL. Comparison of the observed DRs and the estimates by the VR model and FL.
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Fig. 3 Depth-resolved structural characterization of perovskite nanocrystals in npSi films. Depth-resolved structural characterization of perovskite nanocrystals.
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Fig. 4 Polarizer tunable color multiplexing.
Fig. 4 Compressive stress-strain curves and specific strength of compressed GCs. Compressive stress-strain curves and specific strength of compressed GCs.
Fig. 10 Map of light pollution’s visual impact on the night sky.
SEM and TEM images and photoluminescence properties of composites
The combined signal spectra of PSD for protons and helium nuclei
Fig. 3 Voltage-driven phase switching in a 1T-TaS2 nano-thick crystal.
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Fig. 2 DFT calculations of stability and bandstructure of gallenene polymorphs. DFT calculations of stability and bandstructure of gallenene polymorphs.
Fig. 1 Uplift of the Isthmus of Panama and global sea levels over the last 20 My. Uplift of the Isthmus of Panama and global sea levels over the last 20.
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Fig. 2 Photophysical characteristics. Photophysical characteristics. (A) PL decay curves of 2CzBN, o-3CzBN, m-3CzBN, p-3CzBN, 4CzBN, and 5CzBN in toluene at 295 K. 2CzBN, o-3CzBN, and m-3CzBN showed only prompt fluorescence, whereas p-3CzBN, 4CzBN, and 5CzBN exhibited prompt and delayed fluorescence (TADF). Right: Disappearance of TADF due to deactivation of T states caused by O2. (B) ΔEST with an error of ±0.03 eV of CzBN derivatives, estimated from the threshold energy difference between the fluorescence and phosphorescence spectra (77 K) for each molecule (right). Note that only the energy of the phosphorescence spectrum of 2CzBN was chosen from a first peak top (0-0 peak). For 2CzBN, the phosphorescence spectrum of TCzB (black) is also shown to display the spectral similarities with 2CzBN. Inset: Chemical structure of TCzB. (C) ηEQE as a function of current density for OLEDs [ITO/TAPC (35 nm)/mCP (10 nm)/dopant (15 wt %):PPT (30 nm)/PPT (40 nm)/LiF (0.8 nm)/Al (100 nm)] containing o-3CzBN (green), m-3CzBN (light blue), p-3CzBN (light green), 4CzBN (light brown), and 5CzBN (red) as the emitter dopant. Takuya Hosokai et al. Sci Adv 2017;3:e1603282 Copyright © 2017, The Authors