irradiation time (2.0ꢀ8.0 min) and a new one appeared at
264 nm. Narrow spectral alterations with two consecutive
isosbestic points clearly suggested the presence of more
than one species.12 Closer examination of the absorption
spectra of L and L0 (Figure 2) indicated some structural
changes (i.e., orientation, geometry, etc.) retaining con-
jugation length. This can be rationalized by assuming the
movement of pyridyl ring (E,Z) to form an eight mem-
bered cyclic ring (Z,Z) involving CꢀH N hydrogen
3 3 3
bonding between methyl protons and nitrogen lone
pair.13 The effect of metal ions were investigated under
analogous conditions. Notably, interactions between L0 and
various metal ions led to insignificant changes (Figure S8,
Supporting Information) suggesting Lbecomesinert toward
the tested metal ions after UV exposure.
Figure 3. (a) Fluorescence spectra of L and L0 (c, 10 μM; λexc
350 nm). Inset shows structural and color changes upon irradia-
tion. (b) Fluorescence titrations of L to L0 (c, 10 μM). Inset shows
fluorescence enhancement of Lwith respect to fraction of UV-light/min.
,
The Schiff base L fluoresces weakly at 430 nm (λex,
350 nm; Φfl, 0.032)14 with a Stokes shift of 5316 cmꢀ1 (Figure3
and Table S2, Supporting Information), which may be attrib-
uted to photoinduced electron transfer process.14 To
examine the photostability of L fluorescence spectra of
the same solution was acquired repeatedly with 1 min
time interval which showed gradual increase in the rela-
tive emission intensity (∼91%). The light-induced fluo-
rescence enhancement motivated us to scrutinize the
cause of photoswitching ability. Therefore, fluorescence
titrations were performed using L as a ‘host’ and light as a
‘guest’. After each excitation and proper mixing (Δt,
1.0 min) L showed gradual increase in the fluorescence
intensity (Figure 3b) with insignificant change in the Stokes
shift (53 cmꢀ1). The trend continued and attained satura-
tion after 8.0 min (Figure 5, inset) with an increase in
quantum yield by a factor of ∼11 (Φfl, 0.377). Time versus
intensity plot gave a sigmoid curve indicating two step
structural changes (Figure 3b, inset). Fluorescence “turn-on”
without any significant change in Stokes shift suggested
the possibility of structural changes rather than photo-
cleavage. The interaction of solvent with L under influ-
ence of UV light cannot be ruled out; therefore, fluo-
rescence behavior of L was investigated in MeOH, THF,
DMF, DMSO, 1,4-dioxane, CH2Cl2, and C6H6. Notably,
it exhibited an analogous pattern in the aforesaid solvents
except a small decrease in relative intensity in C6H6
(Figure S7b, Supporting Information).
gain deep insight into wavelength triggered structural
changes, L was irradiated at 254 nm. It showed behavior
similar to that observed at 365 nm (Figure S9b, Support-
ing Information). Additionally, L0 remains unchanged in
dark (298 K, CH2Cl2, 24 h).
Based on our earlier findings,10 the report by Ray et al.,11
and NMR, HRMS, UVꢀvis, and fluorescence spec-
tral data, we propose that light-induced structural chan-
ges in L retain the extent of conjugation and controlled
by intramolecular CꢀH N interactions.13 The resulting
3 3 3
eight-membered ring creates rigidity in the molecule
which controls vibrational motion and in turn, fluores-
cence “turn-on”.15 One can speculate that L0 would be less
reactive or inert toward metal ions. To affirm our postu-
lation, nitrate salts of various metal ions were added to a
solution of L0 (Figure S9a, Supporting Information). It
was observed that the fluorescence spectrum of L0 re-
mains unchanged indicating inertness of L0 toward the
metal ions. In contrast, such type of ligands show good
coordination ability toward transition metals.10
Therefore, L and L0 were treated with various metal
ions in the absence of UV light in methanol at room
temperature. Notably, L reacted readily with most of the
metal nitrates and afforded binuclear metallacycles
[{M(C21H20N4)}2}2] (Xꢀ)n, (1ꢀ6), [Co (C12H8N3O2)2]-
PF6 H2O (2b), and [{Ni(C21H20N4)(H2O)2}2] (NO3)4
3
To understand the reversibility of structural changes in
the presence and absence of UV light, L (MeCN, 3 mL,
100 μM) was irradiated for different durations (10 min to
24 h, 365 nm) and monitored by emission spectral studies.
The spectral features were similar for a sample irradiated
for short (10 min) or long (24 h) time period suggesting
that ∼10 min is sufficient for the conversion of L to L0. To
(3a) (Scheme S2, Supporting Information), characterized
by elemental analyses and spectral (FT-IR, NMR, ab-
sorption, and emission) and electrochemical studies
(Figures S10ꢀS12, Supporting Information). Structures
of 1, 2b, 3a, and 5 have been determined crystallographi-
cally (Figure 4 and Figure S13 and Table S1, Supporting
Information). The crystal structure of 3a exhibited a
looped arrangement with double-stranded 12-membered
metallamacrocycle cation [{Ni(C21H24N4O2)}2]4þ along
with coordinated water molecules. In the cations of 3a
immediate coordination geometry about each Ni(II) is
distorted octahedral with NiN4O2 environment16 and N4O2
€
(12) Wohri, A. B.; Katona, G.; Johansson, L. C.; Fritz, E.;
Malmerberg, E.; Andersson, M.; Vincent, J.; Eklund, M.; Cammarata,
M.; Wulff, M.; Davidsson, J.; Groenhof, G.; Neutze, R. Science 2010,
328, 630.
(13) (a) Lin, C.-W.; Chou, P.-T.; Liao, Y.-H.; Lin, Y.-C.; Chen
C.-T.; Chen, Y.-C.; Lai, C.-H.; Chen, B.-S.; Liu, Y.-H.; Wang, C.-C.;
Ho., M.-L. Chem.;Eur. J. 2010, 16, 3770. (b) Harlow, R. L.; Li, C.;
Sammes, M. P. J. Chem. Soc., Chem. Commun. 1984, 818.
(14) (a) Deda, M. L.; Ghedini, M.; Aiello, I.; Grisolia, A. Chem. Lett.
2004, 33, 1060. (b) Williams, N. J.; Gan, W.; Reibenspies, J. H.;
Hancock, R. D. Inorg. Chem. 2009, 48, 1407.
(15) Grobner, G.; Burnett, I. J.; Glaubitz, C.; Choi, G.; James, A.;
Watts, M. A. Nature 2000, 405, 810.
ꢁ
(16) Palacios, M. A.; Rodrıguez-Dieguez, A.; Sironi, A.; Herrera,
´
J. M.; Mota, A. J.; Cano, J.; Colacio, E. Dalton Trans. 2009, 8538.
Org. Lett., Vol. 14, No. 2, 2012
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