2016
DOI: 10.1021/acs.jpcc.6b02446
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Linear Photophysics and Femtosecond Nonlinear Spectroscopy of a Star-Shaped Squaraine Derivative with Efficient Two-Photon Absorption

Abstract: The synthesis, comprehensive linear photophysical and photochemical study, two-photon absorption (2PA) spectrum, ultrafast relaxation kinetics in the excited states, and efficient superluminescence properties of a new symmetrical three-armed star-shaped squaraine derivative (1) are presented. The steady-state spectral parameters of 1 in a number of organic solvents, including fluorescence excitation anisotropy spectra, revealed a weak interaction between the squaraine branches and the effect of symmetry breaki… Show more

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Cited by 34 publications
(45 citation statements)
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“…Moreover, AM‐1 was synthesized under similar reaction conditions by condensation of C and squaric acid. [2a] 1 H NMR, 13 C NMR, and MALDI‐TOF mass spectroscopy confirmed the molecular structures and purities of the related compounds. Synthesis and molecular characterization details are presented in the Supporting Information.…”
Section: Resultsmentioning
confidence: 82%
See 2 more Smart Citations
“…Moreover, AM‐1 was synthesized under similar reaction conditions by condensation of C and squaric acid. [2a] 1 H NMR, 13 C NMR, and MALDI‐TOF mass spectroscopy confirmed the molecular structures and purities of the related compounds. Synthesis and molecular characterization details are presented in the Supporting Information.…”
Section: Resultsmentioning
confidence: 82%
“…[8b] Because of the twisted molecular structure and lower conjugation efficiency related to the intermolecular charge transfer interactions, it was reasonable to expect a modest 2PA cross section for AM‐1′ . [2a], , …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The main ESA bands were observed in the short wavelength region at ∼450–530 nm (for 1 ) and ∼500–570 nm (for 2 ) that are typical for symmetrical squaraines with λ ab max at ∼600–700 nm. 33,34,37 It should be mentioned that gain (i.e., optical amplification via stimulated emission) is not possible in the spectral range λ < 600 nm, and saturable absorption (SA) is negligible because of a weak linear absorption at λ < 570 nm for both molecules. Observed negative changes in the optical densities (i.e., Δ D < 0) in the spectral range of 580–680 nm for 1 and 600–700 nm for 2 are related to SA processes and some possible inputs of gain in the corresponding fluorescence contours (Figure 6c,d, curves (3)).…”
Section: Resultsmentioning
confidence: 99%
“…The degenerate 2PA spectra of 1 and 2 were obtained in THF ( 1 ) and ACN ( 2 ) at room temperature in 1 mm path length quartz cuvettes with molecular concentrations C ≈ 10 –3 M, using an open aperture Z -scan method. 59 Transient absorption pump–probe measurements 34,60 were performed in DCM ( 1 ) and ACN ( 2 ) at room temperature in a 1 mm quartz flow cell to minimize thermo-optical distortion and photodecomposition processes. Experimental details of the femtosecond laser system and process employed were comprehensively described previously.…”
Section: Methodsmentioning
confidence: 99%