| Literature DB >> 36183021 |
Rashid Javaid1, Aziz Ul Rehman2,3, Manan Ahmed4, Mohammad Hashemi Karouei5, Nima Sayyadi5,2.
Abstract
This study presents the design and synthetic pathway of unsymmetric ligands based on pyridine-pyrazolate scaffold with Donor-Acceptor (D-A) molecular arrays and their boron complexes to achieve a large Stokes shift. Intermolecular charge transfer (ICT) triggered by the uneven molecular charge distribution from electronically dense pyrazolate (donor) part of the ligands to electron-deficient boron centre (acceptor) resulted in a mega Stokes shift up to 263 nm for selected compounds while retaining the characteristic quantum efficiency and chemical stability. The photophysical properties of derivatization of pyrazolate group in the pyridine-pyrazolate scaffold of diaryl boron complexes were explored based on UV-Visible, steady-state and time-resolved fluorescence spectroscopy. An interesting dual emission along with quenching behaviour was also observed for 2-(6-methoxynaphthelene) 5-(2-pyridyl) pyrazolate boron complex (P5) due to the formation of a twisted intermolecular charge transfer (TICT) state from a locally excited (LE) state rendering it a potential candidate for sensing applications based on H-Bond quenching. In addition, the extended excited state lifetime of the reported compounds compared to classical boron-dipyrromethene (BODIPY) makes them suitable as potential probes for analytical applications requiring a longer excited state lifetime.Entities:
Year: 2022 PMID: 36183021 PMCID: PMC9526719 DOI: 10.1038/s41598-022-20796-2
Source DB: PubMed Journal: Sci Rep ISSN: 2045-2322 Impact factor: 4.996
Figure 1Synthetic route for the pyridine-pyrazolate boron complexes.
Figure 2UV–Vis absorption spectra of P1–P6 in CH2Cl2 (25 µM) at 298 K.
Photophysical properties of synthesized boron complexes.
| Absorption (CH2Cl2) | Emission | ||||||
|---|---|---|---|---|---|---|---|
| Compound | λabs[nm](ε[M−1 cm−1])a | λem[nm] a | Stokes Shift [nm] a | ΦF a | Knr[ns] c | Kr[ns] c | |
| P1 | 244 (20,300) | 12.94 | 463 | 219 | 0.50 | 0.039 | 0.039 |
| P2 | 278 (10,200) | 6.96 | 461 | 183 | 0.64 | 0.052 | 0.091 |
| P3 | 277 (19,900) | 10.43 | 508 | 231 | 0.71 | 0.028 | 0.068 |
| P4 | 288 (13,700) | 8.83 | 433 | 145 | 0.62 | 0.044 | 0.07 |
| P5 | 250 (29,400) | 10.62 | 370,513 | 120, 263 | 0.43 | 0.054 | 0.04 |
| P6 | 280 (18,400) | 10.05 | 486 | 206 | 0.71 | 0.029 | 0.071 |
aλabs (absorption), λem (emission) measured in CH2Cl2 at 25 µM and room temperature. Uncertainty for λabs and λem: ± 1 nm. Uncertainty for o ± 0.3 ns.
bLifetimes measured using CH2Cl2 under an inert atmosphere. Uncertainty for o: ± 0.1 ns.
cRates constants of radiative (kr) and non-radiative (knr) decay calculated using the formula and (ΦF stands for emission efficiency) o refers to lifetime. .
Figure 3Normalized emission spectra of P1–P6 in CH2Cl2 (25 µM) at 298 K. Scattering is marked as *.
Figure 4UV–Vis absorption spectra of P5 (25 µM) as a function of solvent s at 298 K. Spectra zeroed at 450 nm, even for compounds with significant scattering apparent.
Figure 5Normalized emission spectra of P5 (25 µM) as a function of solvent at 298 K.
Solvatochromic properties of P5.
| Absorption (CH2Cl2) | Emission | |||||
|---|---|---|---|---|---|---|
| Solvent | λabs[nm](ε[M−1 cm−1])a | λem[nm] a | ΦF a | Knr[ns] c | Kr[ns]c | |
| Benzene | 278(6200) | 6.83 | 371,488 | 0.73 | 0.04 | 0.106 |
| Ethyl Acetate | 278(16,700) | 5.64 | 371,508 | 0.68 | 0.056 | 0.121 |
| THF | 308(19,600) | 6.19 | 508 | 0.90 | 0.017 | 0.145 |
| DCM | 250(29,400) | 10.62 | 370,513 | 0.43 | 0.054 | 0.04 |
| Pyridine | 317(19,600) | 2.90 | 524 | 0.95 | 0.019 | 0.326 |
| Methanol | 252(15,700) | 3.83 | 371 | 0.37 | 0.164 | 0.097 |
aMeasured in CH2Cl2 at 25 µM and room temperature. Uncertainty for λabs and λem: ± 1 nm. Uncertainty for o ± 0.3 ns.
bLifetimes measured using CH2Cl2 under an inert atmosphere. Uncertainty for o: ± 0.1 ns.
cRates constants of radiative (kr) and non-radiative (knr) decay calculated using the formula and .