Ángela Vivancos1, Delia Bautista2, Pablo González-Herrero1. 1. Departamento de Química Inorgánica, Facultad de Química, Universidad de Murcia, Campus de Espinardo, 19, 30100 Murcia, Spain. 2. Área Científica y Técnica de Investigación, Universidad de Murcia, Campus de Espinardo, 21, 30100 Murcia, Spain.
Abstract
The synthesis, structure, photophysical properties, and electrochemistry of the first series of Pt(IV) tris-chelates bearing cyclometalated aryl-NHC ligands are reported. The complexes have the general formula [Pt(trz)2(C∧N)]+, combining two units of the cyclometalated, mesoionic aryl-NHC ligand 4-butyl-3-methyl-1-phenyl-1H-1,2,3-triazol-5-ylidene (trz) with a cyclometalated 2-arylpyridine [C∧N = 2-(2,4-difluorophenyl)pyridine (dfppy), 2-phenylpyridine (ppy), 2-(p-tolyl)pyridine (tpy), 2-(2-thienyl)pyridine (thpy), 2-(9,9-dimethylfluoren-2-yl)pyridine (flpy)], and presenting a mer arrangement or metalated aryls. They exhibit a significant photostability under UV irradiation and long-lived phosphorescence in the blue to yellow color range, arising from 3LC excited states involving the C∧N ligands, with quantum yields of up to 0.34 in fluid solution and 0.77 in the rigid matrix at 298 K. The time-dependent density functional theory (TD-DFT) calculations reveal that nonemissive, deactivating excited states of ligand-to-metal charge-transfer (LMCT) character are pushed to high energies as a consequence of the strong σ-donating ability of the carbenic moieties, making the Pt(trz)2 subunit an essential structural component that enables efficient emissions from the chromophoric C∧N ligands, with potential application for the development of different Pt(IV) emitters with tunable properties.
The synthesis, structure, photophysical properties, and electrochemistry of the first series of Pt(IV) tris-chelates bearing cyclometalated aryl-NHC ligands are reported. The complexes have the general formula [Pt(trz)2(C∧N)]+, combining two units of the cyclometalated, mesoionic aryl-NHC ligand 4-butyl-3-methyl-1-phenyl-1H-1,2,3-triazol-5-ylidene (trz) with a cyclometalated 2-arylpyridine [C∧N = 2-(2,4-difluorophenyl)pyridine (dfppy), 2-phenylpyridine (ppy), 2-(p-tolyl)pyridine (tpy), 2-(2-thienyl)pyridine (thpy), 2-(9,9-dimethylfluoren-2-yl)pyridine (flpy)], and presenting a mer arrangement or metalated aryls. They exhibit a significant photostability under UV irradiation and long-lived phosphorescence in the blue to yellow color range, arising from 3LC excited states involving the C∧N ligands, with quantum yields of up to 0.34 in fluid solution and 0.77 in the rigid matrix at 298 K. The time-dependent density functional theory (TD-DFT) calculations reveal that nonemissive, deactivating excited states of ligand-to-metal charge-transfer (LMCT) character are pushed to high energies as a consequence of the strong σ-donating ability of the carbenic moieties, making the Pt(trz)2 subunit an essential structural component that enables efficient emissions from the chromophoric C∧N ligands, with potential application for the development of different Pt(IV) emitters with tunable properties.
The use of N-heterocyclic carbene ligands
(NHCs) for the design
of strongly luminescent transition-metal complexes has become widespread,
mostly associated with the development of phosphors for organic light-emitting
devices (OLEDs).[1−4] Mesoionic NHCs have received special attention within this field
because their exceptionally strong σ-donating ability makes
them particularly well suited to induce large ligand-field splittings,
raising the energies of dissociative, metal-centered (MC) excited
states and reducing the nonradiative deactivation that takes place
through the thermal population of such states.[5−7] This effect
has even been applied with remarkable success to extend the excited-state
lifetimes of strongly deactivated first-row transition-metal complexes.[8−11]Bidentate cyclometalated aryl-substituted NHC ligands (aryl-NHCs,
C∧C*) have been extraordinarily successful with the Ir(III)[12−21] and Pt(II)[22−31] ions as a replacement of cyclometalated 2-arylpyridines (C∧N),
enabling better photostabilities, wider color tunability, and higher
emission efficiencies. These enhancements are brought about by the
larger ligand-field splitting induced by the NHC moiety with respect
to the pyridine and, consequently, the reduced thermal accessibility
of MC states from the triplet, mixed ligand-centered/metal-to-ligand
charge-transfer (3LC/MLCT) emissive state of Ir(III) and
Pt(II) complexes. The most relevant tris-chelates bearing C∧C*
ligands are homoleptic Ir(III) complexes mer/fac-[Ir(C∧C*)3][12,16,17,21] and mixed-carbene
variations,[19] which can achieve blue phosphorescent
emissions, thanks to the large π–π* gap of the
ligands. Heteroleptic tris-chelates of the type [Ir(C∧C*)(C∧N)2] have also been reported, in which the arylcarbene acts as
a supporting, nonchromophoric ligand, whereas the emission is mostly
determined by the C∧N ligands,[13,18,32−34] except for a few cases that incorporate
C∧C* ligands featuring low π–π* gaps.[35−37] However, very few heteroleptic tris-chelates bearing two C∧C*
ligands are known, which include complexes [Ir(C*∧C∧C∧C*)(C∧N)]
bearing a bis-aryl-NHC[38] and [Ir(C∧C*)2(N∧N)] or [Ir(C∧C*)2(N∧N)]+, where N∧N is a pyridylpyrazolate, pyridyltriazolate,
pyridylbenzimidazolate,[39−41] or bipyridyl.[42] Such systems are interesting because the Ir(C∧C*)2 subunit functions as a robust platform for the development
of efficient emitters whose properties can be tuned by incorporating
different chromophoric C∧N or N∧N ligands.When
compared with other d6 metal ions, the photophysical
properties of Pt(IV) complexes have received much less attention.
In previous studies, we have shown that cyclometalated Pt(IV) complexes
with 2-arylpyridine ligands may exhibit very efficient and long-lived
phosphorescence,[43−48] which makes them potentially useful as luminescence-based sensors,
photosensitizers, or photocatalysts. Their emissive excited states
are essentially 3LC in character, with very little metal
orbital participation in the form of an MLCT admixture. Because of
the high oxidation state of the metal, unoccupied dσ* orbitals
have relatively low energies and, in some derivatives, electronic
promotions to these orbitals, i.e., ligand-to-metal charge-transfer
(LMCT) excited states, may become thermally accessible from the emissive
state. Such states have dissociative character because dσ* orbitals
are strongly antibonding, providing a pathway for nonradiative deactivation
or photochemical reactivity.[49,50] Therefore, an indispensable
requirement for Pt(IV) complexes to reach high emission efficiencies
is the presence of suitable strong σ-donor ligands, which induce
a large ligand-field splitting and raise the energy of LMCT states.Recently, we reported Pt(IV) complexes of the types [PtCl2(C∧C*)(C∧N)] and [PtCl(C∧C*)(C∧N∧C)],
where C∧C* is a cyclometalated, mesoionic aryl-NHC ligand of
the 1,2,3-triazolylidene subclass, which constituted the first examples
of Pt(IV) emitters bearing a carbene ligand.[51,52] Derivatives of the type [PtCl2(C∧C*)(C∧N)]
exhibited strong 3LC emissions involving the C∧N
ligand, with significantly higher quantum efficiencies with respect
to the homologous C2-symmetrical [PtCl2(C∧N)2] complexes as a consequence of the
electronic effects of the carbene moiety. However, their synthesis
presented problems associated with the difficult cyclometalation of
the aryl-NHC ligand, resulting in relatively low yields. Herein, we
present a straightforward methodology involving two consecutive cyclometalations
of aryl-NHC ligands that has allowed the synthesis of complexes of
the type [Pt(C∧C*)2(C∧N)]+. These
species are the first Pt(IV) tris-chelates bearing cyclometalated
aryl-NHC ligands and show intense phosphorescent emissions that can
be modulated through the variation of the C∧N ligand, demonstrating
the usefulness of the Pt(C∧C*)2 subunit as a platform
for the design of efficient emitters.
Results and Discussion
Synthesis and Characterization
The synthetic route
to the target tris-cyclometalated Pt(IV) complexes is shown in Scheme . The reaction of
the dimeric platinum precursor (Pr4N)2[Pt2Cl6] with 4 molar equiv of the in situ-prepared
silver carbene intermediate “AgI(trzH)” (trzH = 4-butyl-3-methyl-1-phenyl-1H-1,2,3-triazol-5-ylidene) in 1,2-dichloroethane at 80 °C
led to the selective formation of trans-[PtCl2(trzH)2] (1), which could be isolated
in 85% yield. The trans geometry of 1 was established from an X-ray diffraction analysis (see below).
The reason for the exclusive formation of this isomer is probably
that, upon coordination of the first trzH ligand, the Pt–Cl
bond trans to the carbenic carbon becomes highly labile and is rapidly
abstracted by the silver ion, resulting in the coordination of a second
trzH ligand in this position. Consistent with this, the attempts to
obtain a complex with only one trzH ligand by employing a 1:2 molar
ratio (dimeric platinum precursor to carbene) were unsuccessful, resulting
always in the formation of 1. Similar results have been
previously observed for the reactions of K2[PtCl4] with other silver carbenes.[53−57]
Scheme 1
Synthetic Route to the Target Tris-cyclometalated Pt(IV) Complexes
(i) Ag2O,
1,2-dichloroethane
(DCE), 50 °C; (ii) (Pr4N)2[Pt2Cl6], DCE, 80 °C; (iii) PhICl2, CH2Cl2; (iv) Na2CO3, 1,2-dichlorobenzene
(DCB), 120 °C; and (v) 2 AgOTf, N∧CH, DCB, 120 °C.
Synthetic Route to the Target Tris-cyclometalated Pt(IV) Complexes
(i) Ag2O,
1,2-dichloroethane
(DCE), 50 °C; (ii) (Pr4N)2[Pt2Cl6], DCE, 80 °C; (iii) PhICl2, CH2Cl2; (iv) Na2CO3, 1,2-dichlorobenzene
(DCB), 120 °C; and (v) 2 AgOTf, N∧CH, DCB, 120 °C.The 1H and 13C NMR spectra
of complex 1 show two sets of resonances for the trzH
ligand in very
similar proportions (Figure S1), pointing
to the presence of two different conformational isomers that interconvert
very slowly at room temperature as a consequence of restricted rotation
about the Pt–C bond. This possibility was confirmed by a variable-temperature
NMR study in DMSO-d6, which showed that the different pairs
of aromatic and aliphatic signals coalesce in the range 35–60
°C (Figure S2). Using the Eyring equation,[58] a free energy of activation of ΔG‡ = 15.0 kcal/mol was calculated for
this process at the coalescence temperature of the NCH2 protons (60 °C). Several examples of restricted rotation of
NHC ligands about the metal–C bond have been previously reported.[53,59−61]The crystal structure of 1 is
shown in Figure .
The crystal analyzed corresponded
to the conformer with an antiparallel orientation of the phenyl and
butyl substituents of the trzH ligands. The Pt–Cl bonds lie
along a crystallographic 2-fold axis and therefore the coordination
around the metal is strictly planar. The mean plane of the triazolylidene
ring is rotated by 68.85° with respect to the coordination plane.
The Pt–C1 bond distance of 2.027(2) Å is typical of Pt(II)
complexes with mutually trans NHC ligands.[53−55,62−64]
Figure 1
Structure of complex 1 (thermal
ellipsoids at 50%
probability). Hydrogen atoms are omitted. Selected bond distances
(Å) and angles (°): Pt–C1, 2.027(2); Pt–Cl1,
2.3253(8); Pt–C12, 2.3132(7); C1–Pt–Cl1, 90.35(6);
C1–Pt–Cl2, 89.65(6); and Cl1–Pt–C12, 180.0.
Structure of complex 1 (thermal
ellipsoids at 50%
probability). Hydrogen atoms are omitted. Selected bond distances
(Å) and angles (°): Pt–C1, 2.027(2); Pt–Cl1,
2.3253(8); Pt–C12, 2.3132(7); C1–Pt–Cl1, 90.35(6);
C1–Pt–Cl2, 89.65(6); and Cl1–Pt–C12, 180.0.Treatment of a CH2Cl2 solution
of 1 with PhICl2 led to the oxidation to Pt(IV)
and the electrophilic
metalation of the pendant aryl group of one of the trzH ligands, resulting
in the formation of the monocyclometalated species [PtCl3(trz)(trzH)] (2), which was isolated in 96% yield. The 1H NMR spectrum of 2 shows an aromatic resonance
flanked by 195Pt satellites at δ = 6.99 ppm (JPtH = 37 Hz), arising from the proton ortho
to the metalated carbon of a phenyl ring. The crystal structure (Figure ) corroborated the
presence of a cyclometalated trz and a coordinated trzH and revealed
that the carbenic moieties remain mutually trans, resulting in a mer disposition of metalated carbons or chloride ligands.
Figure 2
Structures
of complexes 2 (a) and the cations of 4b (b) and 4d (c) (thermal ellipsoids at 50%
probability). Hydrogen atoms are omitted. Selected bond distances
(Å) and angles (°): 2: Pt–C1, 2.046(2);
Pt–C9, 2.032(2); Pt–C14, 2.089(2); Pt–Cl1, 2.4509(5);
Pt–C12, 2.3190(5); Pt–Cl3, 2.3395(5); C1–Pt–C9,
80.95(8); and C1–Pt–C14, 173.90(8). 4b:
Pt–C1, 2.037(3); Pt–C9, 2.071(3); Pt–C14, 2.043(4),
Pt–C22, 2.065(4); Pt–N7, 2.094(3); Pt–C31, 2.087(3);
C1–Pt–C9, 80.22(14); C14–Pt–C22, 79.79(14);
and N7–Pt–C31, 79.69(13). 4d: Pt–C1,
2.034(2); Pt–C9, 2.0414(19); Pt–C14, 2.0393(19), Pt–C22,
2.0837(19); Pt–N40, 2.1164(17); Pt–C31, 2.0790(19);
C1–Pt–C9, 80.06(8); C14–Pt–C22, 80.05(8);
and N–Pt–C31, 79.46(7).
Structures
of complexes 2 (a) and the cations of 4b (b) and 4d (c) (thermal ellipsoids at 50%
probability). Hydrogen atoms are omitted. Selected bond distances
(Å) and angles (°): 2: Pt–C1, 2.046(2);
Pt–C9, 2.032(2); Pt–C14, 2.089(2); Pt–Cl1, 2.4509(5);
Pt–C12, 2.3190(5); Pt–Cl3, 2.3395(5); C1–Pt–C9,
80.95(8); and C1–Pt–C14, 173.90(8). 4b:
Pt–C1, 2.037(3); Pt–C9, 2.071(3); Pt–C14, 2.043(4),
Pt–C22, 2.065(4); Pt–N7, 2.094(3); Pt–C31, 2.087(3);
C1–Pt–C9, 80.22(14); C14–Pt–C22, 79.79(14);
and N7–Pt–C31, 79.69(13). 4d: Pt–C1,
2.034(2); Pt–C9, 2.0414(19); Pt–C14, 2.0393(19), Pt–C22,
2.0837(19); Pt–N40, 2.1164(17); Pt–C31, 2.0790(19);
C1–Pt–C9, 80.06(8); C14–Pt–C22, 80.05(8);
and N–Pt–C31, 79.46(7).The metalation of the pendant phenyl group of the
remaining trzH
ligand in 2 was achieved by heating at 120 °C in 1,2-dichlorobenzene in the presence
of a base (Na2CO3), which resulted in the formation
of the bis-cyclometalated complex [PtCl2(trz)2] (3, 78% yield). Its 1H NMR spectrum shows
a single set of resonances arising from equivalent cyclometalated
trz ligands. In addition, the proton ortho to the metalated carbon
of the phenyl ring is strongly shielded (δ = 6.49 ppm, JPtH = 52 Hz), indicating that it is affected
by the diamagnetic current of an orthogonal aromatic ring. These data
demonstrate a C2-symmetrical configuration
with mutually cis chloride ligands.The introduction of different
cyclometalated 2-arylpyridines (C∧N)
as the third chelating ligand was accomplished by reacting 3 with 2.4 equiv of AgOTf (OTf– = trifluoromethanesulfonate)
and an excess of the 2-arylpyridine in 1,2-dichlorobenzene at 120
°C, which afforded complexes [Pt(trz)2(C∧N)]OTf
in 72–80% yields [C∧N = dfppy (4a), ppy
(4b), tpy (4c), thpy (4d),
flpy (4e)]. The 1H NMR spectra of these complexes
show three distinctive aromatic resonances flanked by 195Pt satellites arising from the protons ortho to the metalated aryls,
which are significantly shielded because they are directed toward
orthogonal aromatic rings (δ = 7.04–6.29 ppm).The crystal structures of complexes 4b and 4d were solved by X-ray diffraction analyses (Figure ) and are completely analogous. The carbene
moieties are mutually trans, and the coordinated nitrogen and metalated
carbon of the C∧N ligand are trans to each of the metalated
aryls of the trz ligands. Therefore, they retain the disposition of
trz ligands found in their precursor, resulting in a mer configuration of metalated aryl rings. In the case of 4d, the positions of the thiophene and pyridine rings were found disordered,
with one of the orientations presenting a much higher occupancy factor
than the other (ca. 81:19). Hence, the Pt–C9
or Pt–C22 bonds in 4d can be considered as predominantly
trans to the pyridyl or thienyl rings, respectively (Figure ), the latter being significantly
longer because of the stronger trans influence of the metalated carbon.
However, in 4b the positions of the pyridyl and phenyl
rings of the ppy ligand were not distinguished by the refinement model,
resulting in very similar Pt–C9 and Pt–C22 bond distances.
Photophysical Properties
The electronic absorption
spectra of 4a–e in CH2Cl2 solution (Table , Figure ) show structured
absorptions in the 250–400 nm range that can be ascribed to
primarily 1LC transitions within the ligands. The shapes
and energies of the observed bands are very similar to those of complexes
[PtMe(Cl)(C∧N)2][44] and
[PtCl2(trz)(C∧N)][52] with
the respective 2-arylpyridine ligands, implying that the spectra are
dominated by C∧N-centered absorptions, whereas those involving
the trz ligands must be obscured. The lowest-energy absorption maximum
shifts from 321 to 370 nm along the sequence 4a → 4e, as the expected energies of the lowest π–π*
transition of the C∧N ligand decrease. As observed for [PtMe(Cl)(flpy)2],[44] complex 4e presents
a significantly higher molar absorptivity (25900 M–1 cm–1) with respect to the rest of the derivatives
(8100–12100 M–1 cm–1).
Intense absorptions are advantageous for applications such as photocatalysis
or bioimaging.
Table 1
Electronic Absorption Data for the
Studied Complexes in CH2Cl2 Solution (ca. 5 × 10–5 M) at 298 K
Electronic absorption spectra of complexes 4a–e in a CH2Cl2 solution at 298 K.
Electronic absorption spectra of complexes 4a–e in a CH2Cl2 solution at 298 K.Before examining their luminescence, the photostability
of 4a–e was checked by irradiating their solutions
in
CD3CN in quartz NMR tubes with UV light (310 nm) for 6
h at room temperature. Only in the cases of 4a–c were traces of decomposition products observed in the 1H NMR spectra (ca. 2% of the initial concentration; Figures S15–S19). This behavior is noteworthy
because certain tris-chelate Pt(IV) complexes with a mer configuration of metalated aryl groups, mer-[Pt(C∧N)3]+ (C∧N = dfppy, ppy, tpy), isomerize to
the fac complexes under iradiation with UV light
as a consequence of the population of LMCT excited states.[43,45] Instead, complexes 4a–e produce significant
luminescent emissions, which were characterized from deaerated CH2Cl2 solutions and poly(methyl methacrylate) (PMMA)
matrices (2 wt %) at 298 K and frozen butyronitrile (PrCN) glasses
at 77 K. The emission data at 298 K are summarized in Table , and the emission spectra in
CH2Cl2 solution are shown in Figure . The data at 77 K and the complete series of excitation and
emission spectra are included in the Supporting Information. Vibronically structured emissions are observed
in all cases, characterized by large Stokes Shifts and lifetimes in
the hundreds of microseconds range, which demonstrate a 3LC emissive state. Given that emission energies decrease in the same
order as the lowest-energy absorption, the involved ligand is clearly
the cyclometalated 2-arylpyridine, and therefore the trz ligands play
a supporting role. In the case of the flpy derivative 4e, a secondary emission band at a higher energy is assigned as fluorescence
on the basis of its very short lifetime (<0.2 ns). This band represents
a very small fraction of the emitted photons, with a quantum yield
of ΦF ≈ 0.005 in both CH2Cl2 and PMMA. We have previously reported dual fluorescent/phosphorescent
emissions from Pt(IV) complexes bearing flpy[65] or other C∧N ligands with extended π systems,[45,46] which are due to a relatively less efficient intersystem crossing
to the triplet manifold as a consequence of a lower metal orbital
contribution to the involved excited states and the reduced spin–orbit
coupling effects induced by the metal. Excitation spectra monitored
at the phosphorescent emission band correlate with the corresponding
absorption profiles in all cases. The excitation spectrum of 4e monitored at the fluorescence band coincides with the one
monitored at the phosphorescence band in the lower-energy region but
shows some differences at higher energies that we tentatively attribute
to relatively inefficient internal conversion between higher-lying 1LC(trz) states and the lowest 1LC(flpy) state (see Figure S21 for details). Compared with fac-[Pt(C∧N)3]+,[43] [PtMe(Cl)(C∧N)2],[44] and [PtCl2(trz)(C∧N)],[52] the phosphorescent emissions of 4a–e are somewhat blue-shifted, probably as a consequence of the stronger
π-acceptor character of the trz ligands relative to 2-arylpyridines,[66] leading to a lower energy of metal dπ
orbitals and hence a lower MLCT contribution to the emissive excited
state.
Table 2
Emission Data of Complexes 4a–e at 298 K
complex
medium
λem (nm)a
ΦPb
τ
(μs)c
kr × 10–3 (s–1)d
knr × 10–3 (s–1)e
4a
CH2Cl2
431, 459, 486
0.34
118
2.9
5.6
PMMA
431, 458, 486
0.68
348
1.9
0.9
4b
CH2Cl2
443, 474, 499
0.25
132
1.9
5.7
PMMA
443, 473, 500
0.77
341
2.3
0.7
4c
CH2Cl2
450, 481, 507
0.24
169
1.4
4.5
PMMA
450, 480, 508
0.77
433
1.8
0.5
4d
CH2Cl2
507, 523, 545, 588
0.15
148
1.0
5.7
PMMA
507, 523, 545, 589
0.44
514
0.9
1.1
4e
CH2Cl2
400, 511, 550, 592
0.10
117
0.8
7.7
PMMA
395, 509, 547, 592
0.39
750
0.5
0.8
The most intense peak is italicized.
Phosphorescence quantum yield.
Lifetime.
Radiative rate constant, kr = ΦP/τ.
Nonradiative rate constant, knr = (1 – ΦP)/τ.
Figure 4
Emission spectra of complexes 4a–e in CH2Cl2 at 298 K.
Emission spectra of complexes 4a–e in CH2Cl2 at 298 K.The most intense peak is italicized.Phosphorescence quantum yield.Lifetime.Radiative rate constant, kr = ΦP/τ.Nonradiative rate constant, knr = (1 – ΦP)/τ.Quantum yields vary in the range 0.10–0.34
in CH2Cl2 and 0.39–0.77 in PMMA matrix
and reach the
highest values for the derivatives bearing a ppy-based ligand (4a–c). The only previously reported luminescent Pt(IV)
tris-chelates with a mer arrangement of metalated
aryl rings contain at least one C∧N ligand of a relatively
low energy for the π–π* transition, namely, mer-[Pt(flpy)3]+[65] and the heteroleptic derivatives mer-[Pt(ppy)2(flpy)]+[65] and mer-[Pt(C∧N)2(C′∧N′)]+ with C∧N = dfppy, ppy, C′∧N′
= thpy, 1-phenylisoquinoline (piq),[45] and
their quantum yields were in the range from 0.03 (for mer-[Pt(ppy)2(piq)]+) to 0.08 (for mer-[Pt(flpy)3]+).The radiative and nonradiative
rate constants (kr and knr, respectively) for
the phosphorescent emissions were calculated assuming that the triplet
emissive state is formed with unit efficiency. This assumption introduces
a negligible error in the case of 4e because the fluorescence
emission has a very low quantum yield.[65] The kr values are similar to those of
complexes fac-[Pt(C∧N)3]+ and [PtCl2(trz)(C∧N)] with the same C∧N
ligands. The lower quantum yields of 4d and 4e are mainly attributable to their lower radiative rates, which are
typically found for Pt(IV) complexes bearing thpy[45,46,52] and flppy[65] ligands
and can be explained by a relatively poor metal-ligand orbital overlap,
leading to decreased MLCT contributions to the emissive state. The knr values are drastically reduced in PMMA matrix
in all cases, resulting in significantly higher quantum yields. This
indicates that nonradiative deactivation in CH2Cl2 solution occurs mainly through molecular motion and collisions with
solvent molecules.
Electrochemistry
The cyclic voltammograms of complexes 4a–e were registered in MeCN solution
and are shown in Figure . The potentials of the observed redox processes and estimations
of highest occupied/lowest unoccupied molecular orbital (HOMO/LUMO)
energies are listed in Table . A single irreversible oxidation wave is observable within
the accessible potential window for all complexes except 4e, which produces two irreversible waves. The anodic peak potentials
decrease in the sequence 4a → 4e,
corresponding to increasing HOMO energies as the C∧N ligand
becomes more electron donating. Therefore, the HOMO is essentially
a π orbital of the C∧N ligand in all cases, which agrees
with the density functional theory (DFT) calculations on 4c (see below). The estimated HOMO energies are similar to those of
other Pt(IV) complexes with the respective C∧N ligand in a
similar coordination environment, i.e., homoleptic mer-[Pt(C∧N)3]+ or heteroleptic mer-[Pt(C∧N)2(C′∧N′)]+ complexes,[45] whereas the fac isomers[43,46,65] and the bis-cyclometalated complexes [PtCl2(C∧N)(trz)][52] show lower values.
Figure 5
Cyclic voltammograms
of complexes 4a–e in MeCN at 100
mV s–1.
Table 3
Electrochemical Dataa and HOMO/LUMO Energy Estimationsb for Complexes 4a–e
complex
Ep,ac
Ep,cd
E1/2e
EHOMO
ELUMO
ΔEHOMO-LUMO
4a
2.11
–1.92, −2.17
–2.04, −2.46
–6.63
–2.90
3.73
4b
1.89
–1.99, −2.23
–2.08, −2.35, −2.52
–6.46
–2.82
3.64
4c
1.79
–1.99
–2.16, −2.34, −2.55
–6.37
–2.81
3.56
4d
1.68
–1.92, −2.03, −2.29
–2.48
–6.28
–2.86
3.42
4e
1.58, 1.94
–1.88, −2.07, −2.27, −2.39
–6.18
–2.88
3.30
In V vs SCE, registered in a 0.1
M solution of (Bu4N)PF6 in dry MeCN at 100 mV
s–1.
In
eV.
Irreversible anodic
peak potentials.
Irreversible
cathodic peak potentials.
For the reversible waves.
Cyclic voltammograms
of complexes 4a–e in MeCN at 100
mV s–1.In V vs SCE, registered in a 0.1
M solution of (Bu4N)PF6 in dry MeCN at 100 mV
s–1.In
eV.Irreversible anodic
peak potentials.Irreversible
cathodic peak potentials.For the reversible waves.The first reduction wave is observed at very similar
potentials
for all complexes and is irreversible, except for 4e,
which shows a quasi-reversible wave (Figure S24). Additional reversible processes are observed at more negative
potentials, corresponding to the reduction and subsequent reoxidation
of species arising from the first reduction. The very similar LUMO
energies indicate that this orbital is the same for all complexes
and is not affected by the C∧N ligand. On the basis of DFT
calculations on complex 4c, the LUMO is composed of the
combined lowest π* orbitals of the trz ligands.
Computational Study
For a more precise understanding
of the properties of complexes 4, DFT and time-dependent
DFT (TD-DFT) calculations have been carried out for the tpy derivative 4c. Complete details are presented in the Supporting Information,
including fragment contributions to the frontier orbitals (Table S2). Figure shows an orbital energy diagram, including selected
isosurfaces. The HOMO is mainly composed of the highest π orbital
of the tpy ligand with some dπ orbital contribution from the
metal (ca. 3%), whereas the LUMO is made of the lowest
π* orbital of the trz ligands and is similarly distributed over
them. The LUMO+1 is the lowest π* orbital of the tpy ligand.
The lowest molecular orbital with dσ* character is LUMO+4.
Figure 6
Molecular
orbital energy diagram from DFT calculations and selected
isosurfaces for complex 4c.
Molecular
orbital energy diagram from DFT calculations and selected
isosurfaces for complex 4c.The TD-DFT results predict essentially LC transitions
within the
tpy ligand as the most intense, lowest-energy singlet excitations
(Table S3), in agreement with the above
interpretation of the experimental absorption spectrum. Analogous
transitions involving the trz ligand are predicted at higher energies
and have lower oscillator strengths. Ligand-to-ligand charge-transfer
(LLCT) transitions between the tpy and trz ligands are predicted to
occur at low energies, but their oscillator strengths are extremely
low and therefore they cannot be identified in the experimental spectrum.
The first three triplet excitations correspond to LC transitions within
each of the cyclometalated ligands (Table S4), the lowest one involving the tpy, which is consistent with the
assignment of the emissive state. The lowest triplet LMCT excitation
involving an electronic promotion to LUMO+4 is 1.26 eV above the emissive
state (T15, Table S4; cf. 0.64 or 0.78 eV for the lowest 3LMCT excitation
in [PtCl2(tpy)2] or [PtCl2(trz)(tpy)],
respectively),[52] and is not expected to
significantly contribute to nonradiative excited-state decay through
thermal population.A geometry optimization of the lowest triplet
excited state of 4c was carried out for additional insight.
The calculated
spin density distribution (Figure ) essentially corresponds to a π–π*
transition within the tpy ligand, which agrees with the above assignment
of the emissive state as a primarily 3LC(tpy) excited state.
The calculated natural spin density of 0.010 on the metal atom is
comparable to those found for heteroleptic complexes of the type mer-[Pt(C∧N)2(C′∧N′)]+ (range 0.004–0.009)[45,65] and can be
interpreted as a very small MLCT contribution to the excited state.
The adiabatic T1–S0 energy difference
is 2.68 eV (463 nm), in good agreement with the observed emission
energy.
Figure 7
Spin density distribution (0.0008 e bohr–3) of
the optimized lowest triplet excited state of 4c.
Spin density distribution (0.0008 e bohr–3) of
the optimized lowest triplet excited state of 4c.
Conclusions
A method to obtain the C2-symmetrical,
bis-cyclometalated species [PtCl2(trz)2] (3) has been developed, involving an oxidation of the Pt(II)
bis-carbene complex, trans-[PtCl2(trzH)2] (1), and the successive electrophilic metalations
of the pendant phenyl groups of the trzH ligands. Complex 3 is an excellent precursor for the preparation of cationic tris-cyclometalated
complexes [Pt(trz)2(C∧N)]OTf (4) via
chloride abstraction with AgOTf in the presence of 2-arylpyridine
ligands. These are the first reported Pt(IV) tris-chelates bearing
cyclometalated aryl-NHC ligands. Despite presenting a mer configuration of metalated aryls, they are significantly photostable
under irradiation with UV light, in sharp contrast with most of the
homologous mer-[Pt(C∧N)3]OTf complexes
with the same C∧N ligands, which undergo photoisomerization
reactions. In addition, they show significant phosphorescent emissions
in different media, arising from 3LC states involving the
C∧N ligands. The computational results show that the energies
of deactivating 3LMCT states are high enough not to have
an adverse effect on the emissions via thermal population from the
emissive state, which is consistent with the observed photostabilities
and can be explained by the strong σ-donation from the NHC moieties.
Hence, the Pt(trz)2 subunit is demonstrated as a suitable
platform upon which phosphorescent Pt(IV) tris-chelates with tunable
emission energies can be built by incorporating different cyclometalated
2-arylpyridines as chromophoric ligands, opening the way to the development
of new classes of emissive Pt(IV) complexes by employing other chromophoric
bidentate ligands.
Experimental Section
General Considerations and Instrumentation
Preparations
were carried out under atmospheric conditions, except for those that
required silver reagents, which were conducted in the dark under an
N2 atmosphere. Synthesis grade solvents were employed in
all cases. The triazolium iodide salt,[67] (Pr4N)2[Pt2Cl6],[68] and PhICl2[69] were synthesized according to reported procedures. All other reagents
were obtained from commercial sources. Elemental analyses were carried
out with a LECO CHNS-932 microanalyzer. Electrospray ionization high-resolution
mass spectra (ESI-HRMS) were recorded on an Agilent 6220 Accurate-Mass
time-of-flight (TOF) LC/MS. NMR spectra were registered on a 600 MHz
Bruker Avance spectrometer at 298 K. The variable-temperature NMR
spectra of 1 were registered on a 300 MHz Bruker Avance
spectrometer. Chemical shifts (δ) were referenced to residual
signals of nondeuterated solvent and are given in ppm downfield from
tetramethylsilane. Abbreviations: s, singlet: d, doublet; t, triplet,
q, quartet; p, pentet; sext, sextet; and m, multiplet.
Preparation of trans-[PtCl2(trzH)2] (1)
The triazolium salt (250 mg, 0.73
mmol) and Ag2O (110 mg, 0.47 mmol) were mixed in 1,2-dichloroethane
(15 mL), and the resulting suspension was stirred at 50 °C for
14 h and then filtered through Celite. (NPr4)2[Pt2Cl6] (178 mg, 0.18 mmol) was added to the
filtrate, and the mixture was stirred for 14 h at 80 °C and filtered
through Celite. The filtrate was evaporated to dryness, and the residue
was triturated with MeOH (3 × 4 mL) to give a white solid, which
was recrystallized from CH2Cl2/Et2O and vacuum-dried to give 1. Yield: 217 mg (85%). 1H NMR (600 MHz, CD2Cl2): δ = 8.47
(d, JHH = 7.8 Hz, 2H, CH), 8.29 (d, JHH = 7.8 Hz, 2H, CH), 7.58–7.51 (m, 4H,
CH), 7.43 (t, JHH = 7.7 Hz, 2H, CH), 4.05
(s, 3H, NCH3), 4.04 (s, 3H, NCH3), 3.22 (t, JHH = 8.0 Hz, 2H, CH2), 3.04 (m, JHH = 8.0 Hz, 2H, CH2), 2.01 (p, JHH = 7.7 Hz, 2H, CH2), 1.79 (p, JHH = 7.7 Hz, 2H, CH2), 1.57 (sext, JHH = 7.3 Hz, 2H, CH2), 1.45 (sext, JHH = 7.4 Hz, 2H, CH2), 1.04 (t, JHH = 7.4 Hz, 3H, CH3), 0.97 (t, JHH = 7.4 Hz, 2H, CH3). 13C APT NMR (150 MHz, CD2Cl2): δ = 157.3
(C), 157.0 (C), 147.2 (C), 147.0 (C), 140.7 (C), 140.5 (C), 129.6
(CH), 129.4 (CH), 129.3 (CH), 129.0 (CH), 125.5 (CH), 125.2 (CH),
36.6 (2 NCH3), 31.9 (CH2), 31.7 (CH2), 25.7 (CH2), 25.4 (CH2), 23.5 (CH2), 23.4 (CH2), 14.34 (CH3), 14.29 (CH3). Anal. Calcd for C26H34Cl2N6Pt: C, 44.83; H, 4.92; N, 12.06. Found: C, 44.71, H, 4.72,
N, 12.12.
Preparation of [PtCl3(trz)(trzH)] (2)
To a solution of 1 (198 mg, 0.28 mmol) in
CH2Cl2 (25 mL) was added PhICl2 (94
mg, 0.34 mmol), and the mixture was stirred at room temperature for
1 h. Partial evaporation of the resulting solution under reduced pressure
(2 mL) and addition of Et2O (10 mL) led to the precipitation
of a white solid, which was collected by filtration and vacuum-dried
to give 2. Yield: 200 mg (96%). 1H NMR (600
MHz, CD2Cl2): δ = 7.81–7.79 (m,
2H, CH), 7.65 (dd, JHH = 7.8, 1.5 Hz,
1H, CH), 7.48–7.44 (m, 1H, CH), 7.39–7.35 (m, 2H, CH),
7.19 (td, JHH = 7.6, 1.2 Hz, 1H, CH),
7.14 (td, JHH = 7.6, 1.5 Hz, 1H, CH),
6.99 (dd with satellites, JHH = 7.8, 1.3
Hz, JPtH = 37 Hz, 1H, CH), 4.22 (s, 3H,
NCH3), 4.10 (s, 3H, NCH3), 3.54 (ddd, JHH = 14.1, 11.0, 5.3 Hz, 1H, CH2),
3.35 (ddd, JHH = 14.6, 12.6, 4.5 Hz, 1H,
CH2), 3.10 (ddd, JHH = 14.1,
11.0, 5.4 Hz, 1H, CH2), 2.74 (ddd, JHH = 14.6, 12.3, 4.3 Hz, 1H, CH2), 1.97–1.90
(m, 1H, CH2), 1.80–1.73 (m, 1H, CH2),
1.65–1.57 (m, 2H, CH2), 150–1.43 (m, 2H,
CH2), 1.40–1.29 (m, 2H, CH2), 0.96 (t, JHH = 7.4 Hz, 3H, CH3), 0.89 (t, JHH = 7.4 Hz, 3H, CH3). 13C APT NMR (150 MHz, CD2Cl2): δ = 148.5
(JPtC = 44 Hz, C), 146.0 (C), 142.1 (C),
141.0 (C), 140.2 (C), 139.4 (C), 135.1 (CH), 130.5 (CH), 130.3 (CH),
129.5 (JPtC = 40 Hz, CH), 127.2 (CH),
126.4 (CH), 123.9 (C), 116.4 (CH), 37.2 (NCH3), 36.9 (NCH3), 32.0 (CH2), 31.7 (CH2), 27.1 (CH2), 23.7 (CH2), 23.2 (CH2), 23.1 (CH2), 14.13 (CH3), 14.06 (CH3). Anal. Calcd
for C26H33Cl3N6Pt: C,
42.72; H, 4.55; N, 11.50. Found: C, 42.66, H, 4.47, N, 11.60.
Preparation of [PtCl2(trz)2] (3)
A Carius tube was charged with complex 2 (75
mg, 0.10 mmol), Na2CO3 (54 mg, 0.51 mmol), and
1,2-dichlorobenzene (3 mL), and the mixture was stirred at 120 °C
for 14 h. After cooling down to room temperature, Et2O
(10 mL) was added, and the precipitate was collected by filtration.
The product was extracted with CH2Cl2 (5 ×
5 mL). Partial evaporation of the combined extracts under reduced
pressure (2 mL) and addition of Et2O (10 mL) led to the
precipitation of a white solid, which was collected by filtration
and vacuum-dried to give 3. Yield: 56 mg (78%). 1H NMR (600 MHz, CD2Cl2): δ = 7.62
(dd with satellites, JHH = 7.9, 1.4 Hz, JPtH = 9 Hz, 2H, CH), 7.09 (ddd, JHH = 7.8, 7.5, 1.2 Hz, 2H, CH), 6.86 (td, JHH = 7.7, 1.4 Hz, 2H, CH), 6.49 (dd with satellites, JHH = 7.8, 1.2 Hz, JPtH = 52 Hz, 2H, CH), 4.25 (s, 6H, NCH3), 3.48 (ddd, JHH = 14.2, 10.1, 5.8 Hz, 2H, CH2),
3.24 (ddd, JHH = 14.3, 10.2, 6.1 Hz, 2H,
CH2), 1.86–1.74 (m, 4H, CH2), 1.50 (sext, JHH = 7.4 Hz, 4H, CH2), 0.97 (t, JHH = 7.4 Hz, 6H, CH3). 13C APT NMR (150 MHz, CD2Cl2): δ = 149.3
(JPtC = 802 Hz, C), 146.8 (JPtC = 58 Hz, C), 142.2 (C), 133.4 (JPtC = 25 Hz, CH), 129.8 (JPtC =
54 Hz, CH), 126.1 (JPtC = 814 Hz, C),
125.8 (CH), 116.1 (JPtC = 30 Hz, CH),
37.0 (NCH3), 32.0 (CH2), 24.0 (CH2), 23.2 (CH2), 14.1 (CH3). Anal. Calcd for
C26H32Cl2N6Pt: C, 44.96;
H, 4.64; N, 12.10. Found: C, 45.03; H, 4.74; N, 12.09.
General Procedure for the Preparation of [Pt(trz)2(C∧N)]OTf (4)
A Carius tube was charged
with complex 3 (60 mg, 0.09 mmol), AgOTf (54 mg, 0.21
mmol), the N∧CH ligand (0.45 mmol), and 1,2-dichlorobenzene
(2 mL), and the mixture was stirred at 120 °C for 14 h. After
cooling down to room temperature, CH2Cl2 (10
mL) was added, and the mixture was filtered through Celite. An excess
of NaOAc was then added, and the suspension was stirred for 30 min
and filtered through Celite. Partial evaporation of the filtrate and
addition to Et2O (10 mL) led to the precipitation of a
white solid, which was collected by filtration and vacuum-dried to
give the corresponding complex 4.
Authors: Jaesang Lee; Hsiao-Fan Chen; Thilini Batagoda; Caleb Coburn; Peter I Djurovich; Mark E Thompson; Stephen R Forrest Journal: Nat Mater Date: 2015-10-19 Impact factor: 43.841
Authors: Rebecca E Karmis; Serena Carrara; Amy A Baxter; Conor F Hogan; Mark D Hulett; Peter J Barnard Journal: Dalton Trans Date: 2019-07-09 Impact factor: 4.390
Authors: David C Powers; Diego Benitez; Ekaterina Tkatchouk; William A Goddard; Tobias Ritter Journal: J Am Chem Soc Date: 2010-10-13 Impact factor: 15.419