is enabled by the lower oxidation potential of Pt(II), if compared
with Pd(II).
Conclusions
Four cyclometallated Pd and Pt complexes coordinated simulta-
neously to a dipyrrin derivative and the 2-phenylpyridine ligand
have been synthesized and characterized. Within this series of
complexes, the Pt derivatives exhibit the highest luminescence.
As previously demonstrated, the limitation of rotational freedom,
imposed by the mesityl group, increases the emission intensity.
The development of novel functionalized dpm ligands with
hindered rotation and their combination with cyclometallated
complexes are currently under investigation. The elaboration of
heterometallic luminescent assemblies based on the use of the
secondary coordination sites on the dipyrrin moiety is also under
study.
The luminescence of complexes 5–8 is rather weak even at 77 K,
where all the complexes show two characteristic emission bands,
corresponding to progressive vibronic transitions from one single
electronic excited state. In fact, each pair of vibronic bands gives
rise to only one excitation spectrum, and displays the same excited
state lifetime (Fig. 3 and ESI†).
Experimental
Synthesis
Ligands 1 and 2 were prepared as described.14 The Pd and Pt
precursors, 3 and 4, were synthesised following the reported
procedures.11,15 All solvents were dried using standard procedures.
NMR chemical shifts are given in ppm and J values are given in
Hz.
Complex 5. To a solution of 3 (51 mg, 7.7 ¥ 10-5 mol) in MeCN
(4 mL), AgSbF6 (54 mg, 1.6 ¥ 10-4 mol) in MeCN (1 mL) was
added. This mixture was stirred overnight at room temperature.
The AgCl formed was filtered. The filtrate was then added to a
solution of 1 (22 mg, 8.4 ¥ 10-5 mol) in CHCl3 (3 mL). After
addition of an excess of NEt3, the solution was stirred at room
temperature for 5 h. Purification by column chromatography
(SiO2, CH2Cl2, Rf 0.94) afforded 5 (36 mg, 77%) as pure red powder
(Found: C, 56.87; H, 4.44; N, 6.58. C29H25N3Pt requires C, 57.04;
H, 4.13; N, 6.88%); dH (300 MHz, CD2Cl2) 2.11 (6H, s), 2.37 (3H,
s), 6.44 (1H, dd, J = 4.3, 1.6 Hz), 6.54 (1H, dd, J = 4.0, 1.6 Hz),
6.58 (1H, dd, J = 4.3, 1.3 Hz), 6.66 (1H, dd, J = 4.3, 1.1 Hz), 6.96
(2H, s), 7.14-7.24 (3H, m), 7.33 (1H, m), 7.62 (1H, m), 7.79-8.03
(4H, m) and 8.61-8.64 (1H, m); dC (75 MHz, CD2Cl2) 19.5, 20.8,
116.3, 116.9, 118.9, 121.2, 123.3, 123.4, 127.6, 128.5, 130.0, 130.3,
134.1, 134.7, 136.5, 137.1, 137.5, 138.1, 146.7, 147.0, 149.5, 149.9,
152.5 and 168.2; lmax (CH2Cl2)/nm 273 (log e 4.21), 284 (4.22),
334 (3.94), 434 (4.02) and 508 (4.27).
Fig. 3 Emission and excitation spectra of complex 5 in CH2Cl2 at 293
(solid line) and 77 K (dotted line).
The emission of the Pt complexes 5 and 6 is stronger than those
of their Pd analogues 7 and 8, implying that the Pd complexes
possess smaller radiative constants and higher non-radiative
deactivation rates. Indeed, the excited state lifetimes are two orders
of magnitude higher for Pt than for Pd (Table 1). This observation
can be explained by the out-of-plane distortion featured by the
Pd complexes (vide supra), leading to low-lying, metal-centered
d-d excited states that provide efficient non-radiative deactivation
pathways.
Complex 5 is the strongest emitter and its emission and
excitation spectra were investigated both at 77 K and room
temperature, as depicted in Fig. 3. The vibronic progression is
in this case better resolved, if compared with the other complexes
(compare Fig. 3 and ESI†). It is most likely related to the lack of
rotational freedom imposed by the methyl groups of the mesityl
moiety, which hinders its rotation with respect to the dpm chelate.
This feature has been also observed for Zn(1)2, Ga(1)3 and In(1)3
complexes.7,8
The rather low luminescence quantum yield, the emission
wavelength, the vibronic progression and the long excited state
lifetimes (even at room temperature in deareated solution) point
to a ligand centered excited triplet state localized on the dpm unit.
Moreover, the room temperature and 77 K emission spectra
present almost the same shape and energy range. Such an absence
of hypsochromic shifts confirms the lack of charge transfer
character in the excited state. Owing to the weakness of the
emission of 6–8, the quantum yield was not determined for these
compounds.
Complex 6. To a solution of 3 (54 mg, 8.1 ¥ 10-5 mol) in a
minimum of MeCN (4 mL), AgSbF6 (56 mg, 1.6 ¥ 10-4 mol)
in a minimum of MeCN (1 mL) was added. After stirring 3 h the
mixture at room temperature, AgCl was filtered and the filtrate was
added to a solution of 2 (20 mg, 8.1 ¥ 10-5 mol) in CHCl3 (4 mL).
Excess NEt3 was added and the solution turned immediately from
yellow to red. The solution was stirred at room temperature for
4 h. Solvents were removed under reduced pressure. Purification
by column chromatography (SiO2, CH2Cl2, Rf 0.71) afforded 6
(44 mg, 91%) as a red solid (Found: C, 54.44; H, 3.19; N, 9.11.
C27H18N4Pt requires C, 54.63; H, 3.05; N, 9.44%); dH (300 MHz,
CDCl3) 6.51 (1H, m), 6.59 (2H, m), 6.72 (1H, m), 7.13-7.35 (4H,
m), 7.58-7.67 (3H, m), 7.77 (3H, m), 7.89 (2H, m), 8.13 (1H, s)
and 8.58 (1H, d, J = 5.8 Hz); dC (75 MHz, CDCl3) 112.5, 117.4,
117.6, 118.5, 119.0, 121.2, 123.6, 123.7, 129.0, 131.0, 131.1, 131.2,
134.7, 135.9, 137.0, 138.1, 142.7, 144.7, 146.2, 148.2, 149.4, 150.8,
182 | Dalton Trans., 2010, 39, 180–184
This journal is
The Royal Society of Chemistry 2010
©