2017
DOI: 10.1080/15421406.2017.1358018
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Significant emission red-shift of BODIPY derivatives with strong electron-acceptor attached

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Cited by 6 publications
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“…When the room temperature emission spectra were normalized at their maxima, a redshift was also observed from ∼538 nm of the free BODIPY to ∼552 nm of the complex with a 500 nm excitation. The redshift is due to the coordination of the BODIPY to the metal center further lowering the energy of the π → π* BODIPY transition due to the rhodium center pulling electron density away from the ligand. For the intermediate compound, [Rh­(bpy-2BODIPY)­(DMF)­Cl 3 ], the fluorescence was completely quenched when excited at 500 nm where a large decrease in fluorescence intensity was observed (Figure ). At the emission maximum of the [Rh­(bpy-2BODIPY)­(DMF)­Cl 3 ] complex (λ em = 535 nm), the emission intensity was at ∼2700 a.u., while the emission intensity of the [Rh­(bpy-2BODIPY)­(phen)­Cl 2 ]­[PF 6 ] (λ em = 552 nm) was ∼40,000 a.u.…”
Section: Resultsmentioning
confidence: 99%
“…When the room temperature emission spectra were normalized at their maxima, a redshift was also observed from ∼538 nm of the free BODIPY to ∼552 nm of the complex with a 500 nm excitation. The redshift is due to the coordination of the BODIPY to the metal center further lowering the energy of the π → π* BODIPY transition due to the rhodium center pulling electron density away from the ligand. For the intermediate compound, [Rh­(bpy-2BODIPY)­(DMF)­Cl 3 ], the fluorescence was completely quenched when excited at 500 nm where a large decrease in fluorescence intensity was observed (Figure ). At the emission maximum of the [Rh­(bpy-2BODIPY)­(DMF)­Cl 3 ] complex (λ em = 535 nm), the emission intensity was at ∼2700 a.u., while the emission intensity of the [Rh­(bpy-2BODIPY)­(phen)­Cl 2 ]­[PF 6 ] (λ em = 552 nm) was ∼40,000 a.u.…”
Section: Resultsmentioning
confidence: 99%