2019
DOI: 10.1016/j.saa.2019.03.054
|View full text |Cite
|
Sign up to set email alerts
|

Hydrogen bond configuration and protonation of ground and lowest excited triplet states of 4‑amino‑4′‑nitrobiphenyl based on nanosecond transient absorption spectroscopy

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
5
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 52 publications
0
5
0
Order By: Relevance
“…To confirm the presence of the ICT state, strong acid (TFA) was used to protonate the aTTz derivative, limiting the shift of electron density and increasing polarity in the excited state (Figure S19, Supporting Information). [ 18,39 ] Due to the dual solvatofluorochromic effect in Bu 2 N‐TTz‐NO 2 and Ph 2 N‐TTz‐NO 2, the excited‐state dipole moments ( Table 1 ) were calculated separately for the SWB and LWB bands using the Lippert‐Mataga (LM) equation (Equation ): νaνf=2()μμ24πε0hca3Δf+const.;Δf=ε12ε+1η212η2+1$$\begin{eqnarray} {\nu }_a - {\nu }_f = \frac{{2{{\left( {{\mu }^{\rm{*}} - \mu } \right)}}^2}}{{4{{\pi}}{\epsilon }_0hc{a}^3}}\Delta f + const. ;\Delta f = \left( {\frac{{\varepsilon - 1}}{{2\varepsilon + 1}} - \frac{{{\eta }^2 - 1}}{{2{\eta }^2 + 1}}} \right)\nonumber\\ \end{eqnarray}$$where ν a and ν f are the absorption and emission peaks in cm −1 , µ * and µ are the excited state and ground state dipoles, ε 0 is the vacuum permittivity, h is Planck's constant, c is the speed of light, a is the Onsager cavity radius, Δ f is the orientation polarizability, ε is the relative permittivity, and η is the refractive index.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…To confirm the presence of the ICT state, strong acid (TFA) was used to protonate the aTTz derivative, limiting the shift of electron density and increasing polarity in the excited state (Figure S19, Supporting Information). [ 18,39 ] Due to the dual solvatofluorochromic effect in Bu 2 N‐TTz‐NO 2 and Ph 2 N‐TTz‐NO 2, the excited‐state dipole moments ( Table 1 ) were calculated separately for the SWB and LWB bands using the Lippert‐Mataga (LM) equation (Equation ): νaνf=2()μμ24πε0hca3Δf+const.;Δf=ε12ε+1η212η2+1$$\begin{eqnarray} {\nu }_a - {\nu }_f = \frac{{2{{\left( {{\mu }^{\rm{*}} - \mu } \right)}}^2}}{{4{{\pi}}{\epsilon }_0hc{a}^3}}\Delta f + const. ;\Delta f = \left( {\frac{{\varepsilon - 1}}{{2\varepsilon + 1}} - \frac{{{\eta }^2 - 1}}{{2{\eta }^2 + 1}}} \right)\nonumber\\ \end{eqnarray}$$where ν a and ν f are the absorption and emission peaks in cm −1 , µ * and µ are the excited state and ground state dipoles, ε 0 is the vacuum permittivity, h is Planck's constant, c is the speed of light, a is the Onsager cavity radius, Δ f is the orientation polarizability, ε is the relative permittivity, and η is the refractive index.…”
Section: Resultsmentioning
confidence: 99%
“…To confirm the presence of the ICT state, strong acid (TFA) was used to protonate the aTTz derivative, limiting the shift of electron density and increasing polarity in the excited state (Figure S19, Supporting Information). [18,39] Due to the dual solvatofluorochromic effect in Bu 2 N-TTz-NO 2 and Ph 2 N-TTz-NO 2, the excited-state dipole moments (Table 1) were calculated separately for the SWB and LWB bands using the Lippert-Mataga (LM) equation (Equation 1):…”
Section: Photophysical Characteristicsmentioning
confidence: 99%
“…As a result, nπ* is involved in the lowest excited singlet state, which facilitates both ISC and nonradiative decay rate. On the other hand, the non-fluorescence behavior of 3 e in ethanol can be explained by the non-radiative decay routes aroused form the hydrogen bond interactions between the protic solvent molecules and nitro groups as illustrated by Jin et al [40] The results manifest the importance of relative energy alignment between nπ* and ππ* state and its interplay with the strong À NO 2 electron withdrawing property. These unique properties make À NO 2 substituents versatile in applications, among which the fluorescence probe and fluorescence sensing have received particular attention and will be reviewed in the following section.…”
Section: Introductionmentioning
confidence: 98%
“…2B. Unlike most NPAHs, which have a microsecond lifetime in their T 1 states in solution, 8,49–51 the T 1 state NO 2 -QN-OH decays within ∼10 ns (Fig. 2B), resulting in transient absorption with an additional band in the 450 to 500 nm range compared to the T 1 state NO 2 -QN-OH.…”
Section: Resultsmentioning
confidence: 98%
“…The nanosecond TA measurements were performed using a laser flash photolysis system (LP-920, Edinburgh Instruments) as previously described. [49][50][51] The excitation laser pulse was generated using the third harmonic output of an Nd:YAG Q-switched laser. The laser pulse has a 355 nm wavelength, a 10 ns pulse width, and an 80 mJ pulse energy.…”
Section: Experimental and Calculation Methodsmentioning
confidence: 99%