Photoluminescence properties of pyrazoline and pyrazole
Figure 5. Frontier orbitals of P1 and P2 in excited state.
correlated well with the small variations in their absorption and
fluorescence spectra in solutions. The main transition orbitals from
the energetically lowest-lying excited state (S1 state) to ground
state (S0 state) were HOMO-LUMO transitions in P1 and P2
(Table 2). As observed from Fig. 5, the HOMO orbital of P1 was
distributed on the whole molecular while the LUMO orbital was
located on the anthryl moiety and the two orbitals only
overlapped on the anthryl moiety. As a result, the S1 state of P1
corresponding to an emissive locally excited singlet state and
electron-transfer state simultaneously (17) can be termed an
incomplete electron-transfer state leading to relative low oscillator
strength for the S1-S0 transition. To the best of our knowledge,
there have been no studies on this type of S1 state that exhibits
both characters of locally excited and electron-transfer states. In
addition, these observations explain the phenomenon that P1
had an extremely and theoretically low fluorescent quantum yield.
In P2, the HOMO and LUMO orbitals were both located on the
anthryl moiety, resulting in a larger overlap degree relative to P1.
The HOMO-LUMO transition was an optically allowed p-p*
transition and led to the locally excited state S1. Hence, the S1-S0
transition of P2 had high oscillator strength and was responsible
for the strong fluorescence of P2. Combined with the higher molar
absorption coefficient, it can be concluded that P2 had stronger
fluorescence than anthracene.
Acknowledgements
This project was supported by the National Basic Research
Program of China (2011CB302004) and Open Project of Southeast
University Key Laboratory of Environmental Medicine Engineering
of Ministry of Education (2010EME009).
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Conclusions
We prepared 1,3-diphenyl-5-(9-anthryl)-2-pyrazoline and 1,3-
diphenyl-5-(9-anthryl)-1H-pyrazole. The optical properties of
the two compounds changed from nearly no fluorescence to
bright emission in solutions. Density-functional theory calcula-
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the fluorescence properties of P1 and P2. In P1, the S1 state
possessed the characteristics of locally excited and electron-
transfer states, which resulted in fluorescence quenching of
anthryl chromophore, whereas in P2, the S1 state corresponded
to an optically allowed state that led to the high fluorescence
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Luminescence 2012
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