Table 1. Quantum yields of photocleavage reaction upon UV
irradiationa
decreased by introducing an electron-withdrawing group into the
axial group. It is noted that there is a rough correlation between the
LUMO energy and the photoreactivity; the quantum yield of the
photocleavage reaction is small when the acceptor ability of the
axial group is high (Table 1).
In conclusion, TATA leuco derivatives bearing different axial
groups at the central carbon atom were synthesized and their
photoreactivity was investigated. Owing to the good donor
property of the TATA framework, a typical CT character was
observed upon photoexcitation. It was found that the photo-
cleavage reaction becomes clean and effective in the following
conditions: (i) in polar media, (ii) in the presence of a protic
solvent, and (iii) with a high LUMO energy of the axial group.
These observations are of importance for the design of smart
photoresponsive materials that can release small molecular
components upon photoirradiation, especially on a 2-dimensional
surface, via a photochemical reaction.
Orbital energyc/eV
Quantum yieldb
(Φr)
HOMO-LUMO
gap/eV
Compd
HOMO
LUMO
1
2
3
4
5
6
0.013
0.56
0.45
0.35
<0.01
<0.01
¹5.25
¹5.29
¹5.22
¹5.28
¹5.33
¹5.30
¹0.75
¹1.22
¹0.88
¹2.26
¹2.84
¹2.76
4.50
4.07
4.34
3.02
2.49
2.54
aBy irradiation with 313 nm light. bMeasured in ethanol. cCalculated at
B3LYP/6-311g(2d,p)-SCRF(PCM)// 6-31g(d) level.
control experiments under dark condition, the process of thermal
cleavage reaction from the TATA leuco derivative to the TATA
cation was found to compete with the photoreaction for 5 and 6
(Figures S6-S8). Analysis by the Eyring plot gave the activation
free energy of the thermal reaction for 5 as ¦G‡ = 101 kJ mol¹1 at
25 °C (¦H‡ = 95 kJ mol¹1, ¦S‡ = ¹20 J K¹1 mol¹1) (Figure S9).
On the basis of these parameters, the halflife (t1/2) of 5 in ethanol is
14 h at 25 °C, which is significantly shorter than that of 2 (t1/2 = 10
days, Figure S10). In the case of compounds 1-4, the photo-
chemical process was dominant, so that the thermal process was
not easily discerned. For compound 6, a small change in the
absorption spectrum was also detected around 350 nm, which is
due to the cis-trans photoisomerization of the azobenzene moiety.
The photoisomerization of 6 became more distinct in toluene20
(Figure S11).
The quantum yield of the photocleavage reaction was inves-
tigated in ethanol by monitoring the increase of absorbance at
525 nm upon UV irradiation (Table 1). Compared to the quantum
yield of the phenyl derivative 1 (Φr = 0.013), those of the
arylethynyl derivatives 2-4 were significantly large (Φr = 0.35-
0.56). On the other hand, the quantum yields of the 10-cyano-9-
anthrylethynyl derivative 5 and the 4-(phenyldiazenyl)phenyl-
ethynyl derivative 6 were notably small (Φr < 0.01). The differ-
ence in Φr between 1 and 2 can be explained by the presence or
absence of the ethenyl group. The difference in Φr among 2-6
should be caused by the substituent effect and difference in the
aromatic framework, i.e., benzene or anthracene.
In order to investigate the difference in the photoreactivity,
time-dependent density functional theory (TD-DFT) calculations
were performed on 1-6 at the B3LYP/6-311g(2d,p)// 6-31g(d)
level. The solvent effect was taken into account by using the self-
consistent reaction field (SCRF) with the polarizable continuum
model (PCM). HOMOs of the leuco derivatives mainly localize at
the TATA moiety while LUMOs localize at the axial groups
(Figure S12). According to the contributions of molecular orbitals
(MOs) calculated by TD-DFT, the lowest energy excited state has
an intramolecular charge-transfer (CT) property from the TATA
moiety to the axial groups. The LUMO energies were significantly
lowered as the acceptor ability of axial groups increased; the
LUMO energies of the 10-cyano-9-anthrylethynyl derivative 5
(¹2.84 eV) and 4-(phenyldiazenyl)phenylethynyl derivative 6
(¹2.76 eV) are lower than that of the 9-anthrylethynyl derivative
4 (¹2.26 eV) and the phenylethynyl derivative 2 (¹1.22 eV).
In contrast, the HOMO energies of 1-6 were almost constant
(ca. ¹5.3 eV), which is attributed to the localization of HOMOs
at the TATA moiety. Therefore, the HOMO-LUMO gap efficiently
This work was supported by NEXT program (No. GR062)
from JSPS and Grant-in-Aid for Scientific Research on Innovative
Areas “Photosynergetics” (No. 26107008) from MEXT, Japan.
Supporting Information is available electronically on J-STAGE.
References and Notes
1
2
V. Nair, S. Thomas, S. C. Mathew, K. G. Abhilash, Tetrahedron
3
4
5
J. Lux, E. J. Peña, F. Bolze, M. Heinlein, J.-F. Nicoud,
G. Lukinavičius, K. Umezawa, N. Olivier, A. Honigmann, G. Yang,
T. Plass, V. Mueller, L. Reymond, I. R. Corrêa, Jr., Z.-G. Luo, C.
Schultz, E. A. Lemke, P. Heppenstall, C. Eggeling, S. Manley, K.
6
7
8
9
J. H. Malpert, O. Grinevich, B. Strehmel, V. Jarikov, A. Mejiritski,
references therein.
14 B. Baisch, D. Raffa, U. Jung, O. M. Magnussen, C. Nicolas, J.
15 S. Kuhn, B. Baisch, U. Jung, T. Johannsen, J. Kubitschke, R. Herges,
16 U. Jung, S. Kuhn, U. Cornelissen, F. Tuczek, T. Strunskus, V.
Zaporojtshenko, J. Kubitschke, R. Herges, O. Magnussen, Langmuir
17 U. Jung, C. Schütt, O. Filinova, J. Kubitschke, R. Herges, O.
19 Y. Haketa, S. Sasaki, N. Ohta, H. Masunaga, H. Ogawa, N. Mizuno,
© 2015 The Chemical Society of Japan