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Article

Effect of the Substitution of the Mesityl Group with Other Bulky Substituents on the Luminescence Performance of [Pt(1,3-bis(4-Mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl]

by
Giulia De Soricellis
1,2,
Véronique Guerchais
3,
Alessia Colombo
1,*,
Claudia Dragonetti
1,
Francesco Fagnani
1,*,
Dominique Roberto
1 and
Daniele Marinotto
4
1
Dipartimento di Chimica, Università degli Studi di Milano, UdR INSTM di Milano, Via C. Golgi 19, I-20133 Milan, Italy
2
Dipartimento di Chimica, Università di Pavia, Via Taramelli 12, I-27100 Pavia, Italy
3
Univ. Rennes 1, CNRS, ISCR-UMR 6226, F-35000 Rennes, France
4
Istituto di Scienze e Tecnologie Chimiche (SCITEC) “Giulio Natta”, Consiglio Nazionale delle Ricerche (CNR), Via C. Golgi 19, I-20133 Milan, Italy
*
Authors to whom correspondence should be addressed.
Molecules 2025, 30(7), 1498; https://doi.org/10.3390/molecules30071498
Submission received: 28 February 2025 / Revised: 23 March 2025 / Accepted: 24 March 2025 / Published: 27 March 2025
(This article belongs to the Special Issue Feature Papers in Photochemistry and Photocatalysis—2nd Edition)

Abstract

:
The synthesis and characterization of two new complexes, namely [Pt(bis(4-(4-(tert-butyl)phenyl)-pyridin-2-yl)-4,6-difluorobenzene)Cl] and [Pt(bis(4-(3,5-di-tert-butylphenyl)-pyridin-2-yl)-4,6-difluorobenzene)Cl], are reported. Both are highly luminescent in the blue region (Φlum = 0.89–0.95 at 478–480 nm), like the parent complex [Pt(1,3-bis(4-mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl] in degassed diluted dichloromethane solution. An increase in concentration leads to the formation of bi-molecular emissive excited states, as evidenced by a growing structureless band that peaked at 690–697 nm. This formation is more facile for the complex with one tert-butyl group in para of the phenyl group. It appears that the introduction of two tert-butyls in positions 3 and 5 of the phenyl group hampers the neighboring of the monomeric species, although less efficiently than the introduction of methyls in positions 2 and 6.

1. Introduction

Square planar platinum(II) complexes are of prodigious interest in numerous fields of photonics and optoelectronics, such as nonlinear optics [1,2,3,4,5,6,7,8,9,10], artificial photosynthesis [11], photocatalysis [12,13,14], sensing [15,16,17,18,19,20,21,22,23,24,25,26,27,28,29], Organic Light Emitting Diodes (OLEDs) [30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46], bioimaging [47,48,49,50,51,52,53,54,55,56,57,58,59], and photodynamic therapy [60,61,62,63,64,65,66,67]. These complexes are characterized by a strong spin-orbit coupling due to the platinum center, which favors intersystem crossing and emission of light from triplet excited states [68,69]. Besides, their square planar geometry allows the formation of bimolecular states in the ground (dimers) and/or in the excited states (excimers) by means of Pt-Pt or ligand-ligand intermolecular interactions, a precious aspect because, for example, the parallel emissions from mono-molecular and bi-molecular excited states of platinum complexes allow the modulation of the color of luminescent devices [70].
In the last 20 years, a lot of work has been dedicated to platinum(II) chlorido complexes bearing a cyclometalated terdentate 1,3-bis(pyridin-2-yl)benzene ligand because they are among the brightest and most efficient emitters [71]. The parent complex [Pt(1,3-bis(pyridin-2-yl)benzene)Cl] is intensely luminescent in deoxygenated dichloromethane solution at room temperature (Φlum = 0.60 and τ = 7.2 μs) [72], in striking contrast to [Pt(terpyridine)Cl]+, which is essentially non-emissive because it has low-lying d-d states that allow a thermally activated non-radiative decay pathway for the MLCT state [73]. In the complex [Pt(1,3-bis(pyridin-2-yl)benzene)Cl], the presence of the cyclometallating carbon causes an increase in the ligand-field strength and, thus, in the energy of the d-d state, removing this decay pathway [71]. Besides, the rigidity of the tridentate ligand has a beneficial effect on respect to bidentate ligands. In fact, the complex [Pt(ppy)(Hppy)Cl] (ppyH is phenylpyridine) also has a coordination sphere with one cyclometallated benzene ring, two pyridine rings, and one chloride ligand; however, the distortion of the bidentate ligands leads to non-radiative decay at room temperature: the luminescence lifetime is very short at room temperature (641 ns) and increases a lot at 77 K (11.2 μs) [74]. In contrast, the luminescence lifetime of [Pt(1,3-bis(pyridin-2-yl)benzene)Cl] is the same at 77K and at room temperature, showing that the greater rigidity of the tridentate ligand prevents the distortion [71]. Besides, the N^N^C-coordinated [Pt(phenylbipyridine)Cl] isomeric complex has a luminescence quantum yield an order of magnitude lower, although it has a tridentate ligand because the Pt–C bond in [Pt(1,3-bis(pyridin-2-yl)benzene)Cl] is shorter than in [Pt(phenylbipyridine)Cl] leading to a higher ligand-field strength [71].
Remarkably, the absorption and emission maxima of [Pt(1,3-bis(pyridin-2-yl)benzene)Cl] derivatives are influenced by the introduction of electron-donor and/or electron-acceptor substituents on the cyclometallated benzene and on the pyridine rings, offering a versatile method of color tuning. Thus, time-dependent density functional theory (TD-DFT) calculations showed that the frontier orbitals are on different portions of the complex, such that their energies can be modified almost independently [75]. In this class of compounds in which the triplet state at the lowest energy has mainly HOMO→LUMO character, the benzene ring gives the main contribution to the HOMO, whereas the pyridine rings control the LUMO. Therefore, the presence of electron-donor substituents in the benzene ring (which raises the HOMO energy) and electron-acceptor substituents in the pyridine rings (which lowers the LUMO energy, especially when in position para with respect to the N atoms) will lead to a red-shift in the emission, while electron-acceptor substituents in the benzene ring and electron-donor substituents in the pyridine rings will cause a blue-shift. The experimentally observed tendencies follow this design well [48,71,76].
Interestingly, these platinum(II) chlorido complexes with a cyclometalated 1,3-bis(pyridin-2-yl)-benzene ligand show two phosphorescence bands situated in the bluish-green (monomeric emission) and red (excimer/aggregate emission) regions of the visible spectrum, which contributions to the global emission can be chosen by the amount of the platinum complex in the host matrix used for the preparation of the OLED’s blend emissive layer. This represents a precious tool for tailoring the emission color of OLEDs [32].
However, today, the preparation of efficient blue phosphorescent OLEDs remains a challenge [77,78,79]. The idea of filling this gap prompted us to investigate the effect of the introduction of a bulky substituent on position 4 of the pyridine rings of the complex with a fluorinated cycloplatinated 1,3-bis(pyridin-2-yl)-4,6-difluoro-benzene ligand, for which the presence of the fluorine atoms allows a blue monomeric emission. The idea was that the knowledge of such an effect would be of particular interest because excimers or aggregates formation, and, therefore, the phosphorescence properties, could be controlled, achieving the proper spatial arrangement of bulky functional groups, which could decrease Pt-Pt interactions and/or π−π stacking and the concomitant red emission. Promising results were reached recently with the preparation of a chlorido platinum(II) complex bearing a well-designed new N^C^N-cyclometalating ligand, namely 1,3-bis(4-mesityl-pyridin-2-yl)-4,6-difluoro-benzene (Scheme 1, [PtL1Cl]) [44]. Thus, the introduction of the bulky mesityl substituent on the pyridine rings turned out to be a facile strategy to increase the Pt···Pt distance, reaching a value (8.59 Å) much longer than that observed for previously reported chlorido N^C^N-platinum(II) complexes. The [PtL1Cl]) complex, which exhibits intense blue phosphorescence in dilute dichloromethane solution (471 nm, Φlum = 0.97), was used to fabricate a blue OLED with an excellent performance when compared to that reached with blue OLEDs based on other platinum complexes [44]. Clearly, the introduction of bulky substituents in N^C^N Pt(II) complexes represents a springboard for the fabrication of efficient blue OLEDs. For this reason, we designed, prepared, and thoroughly characterized in solution two novel complexes, namely [PtL2Cl] and [PtL3Cl], with one or two tert-butyl groups on the phenyl group in position 4 of the pyridine rings (Scheme 1).

2. Results and Discussion

2.1. Preparation of the Complexes

The new pro-ligands 1,3-bis(4-(4-(tert-butyl)phenyl)pyridin-2-yl)-4,6-difluoro-benzene (HL2) and 1,3-bis(4-((3,5-di-tert-butylphenyl))-pyridin-2-yl)-4,6-difluoro-benzene (HL3) were prepared by cross-coupling the pinacol ester of 1,3-difluoro-4,6-diboronic acid [44] with the suitable 2-chloro-4-Aryl-pyridine (Scheme 2). The reaction of these pro-ligands with K2PtCl4 led to the desired complexes in 41% yield ([PtL2Cl]) and 85% yield ([PtL3Cl]). The complexes were fully characterized by NMR (1H, 13C, and 19F) spectroscopy, mass spectrometry (HRMS), and elemental analysis. Full details of the synthesis and characterization are provided in the Section 3 “Materials and Methods” and in the Supporting Information.

2.2. Photophysical Properties

The absorption spectra of compounds [PtL2Cl] and [PtL3Cl] at various concentrations (1·10−6–2·10−4 M) in CH2Cl2 are shown in Figure 1. There are bands of high intensity in the range 260–320 nm, attributed to intraligand 1π–π* transitions of the N^C^N cyclometalating ligand, and bands of lower intensity at 340–420 nm, caused by charge-transfer transitions concerning the cyclometalating ligand and the metal, as for other N^C^N platinum(II) complexes [39,40,41,42,43,44,70,71,72,73,80]. A weak absorption band at 470 nm is also present in the absorption spectra of both [PtL2Cl] (ε = 310 L mol−1 cm−1) and [PtL3Cl] (ε = 225 L mol−1 cm−1), as shown in the insets of Figure 1, due to the weak transition from the singlet ground state to the lowest triplet state, facilitated by the presence of the platinum center [80].
The normalized emission spectra at room temperature of [PtL2Cl] and [PtL3Cl] in degassed dichloromethane at various concentrations are shown in Figure 2. Upon excitation at 380 nm in dilute solution (1∙10−6 M), the emission spectrum of both complexes is characterized by a vibrationally structured band with a high-energy emission maximum at 480 nm (for [PtL2Cl]) and 478 nm (for [PtL3Cl]), slightly red-shifted with respect to that of [PtL1Cl] (471 nm) [44]. This band can be attributed to the electronic T1 → S0 transition of the monomeric complex [80].
As expected from the behavior of other N^C^N platinum complexes [32,39,40,41,42,43], when the concentration of [PtL2Cl] and [PtL3Cl] is increased up to 2·10−4 M, the emission spectra show a growing structureless band peaked at 690–697 nm, in addition to the vibrationally structured band. This structureless band at lower energy, due to bi-molecular emissive excited states (excimers and aggregates) of the platinum (II) complex formed by means of Pt-Pt or π−π ligand-ligand intermolecular interactions [32], is much more intense for [PtL2Cl] than for [PtL3Cl] (see Figure 2A,B). The formation of aggregates was confirmed by means of excitation spectra (see Electronic Supporting Information). Figure 3 shows the normalized emission spectrum of both complexes with that of [PtL1Cl] in concentrated degassed CH2Cl2 solution (2·10−4 M). It puts in evidence that the low energy band intensity follows the order [PtL2Cl] > > [PtL3Cl] > [PtL1Cl], highlighting that the presence of the tert-butyl group in para of the phenyl group is much less efficient in hampering the formation of dimeric species. The introduction of two tert-butyl groups ([PtL3Cl]) leads to a clear decrease in the intensity of the structureless band, in agreement with an increase in the steric hindrance. It appears that the presence of a mesityl group in para of the pyridine rings is even more efficient in hampering the approach of the monomeric species. In the complex [PtL1Cl], there is a torsion angle of ca 62° between the mesityl groups and the pyridines, as shown from the X-ray structure, which hinders the neighboring of the metal atoms and, therefore, the Pt···Pt interactions; the shortest Pt···Pt distance is 8.59 Å much longer than that observed for the related platinum(II) chlorido complex with a cyclometalated 5-mesityl-1,3-bis(pyridin-2-yl)-benzene ligand (4.4 Å) [44]. Unfortunately, various attempts to obtain crystals of [PtL2Cl] and [PtL3Cl] suitable for X-ray determination failed. In any case, the decrease in the intensity of the structureless band at low energy on going from [PtL2Cl] to [PtL3Cl] is expected upon the introduction of a second tert-butyl group on the phenyl ring. Besides, our results put in evidence the importance of having substituents in the alpha of the carbon linked to the pyridine to better hamper the neighboring of the monomeric species.
In degassed diluted CH2Cl2 solution at room temperature, it is known that [PtL1Cl] is a bright Pt(II) emitter with a luminescence quantum yield (Φlum) of 0.97 [44]. The two new complexes are also characterized by excellent absolute quantum yields, 0.89 and 0.95 for [PtL2Cl] and [PtL3Cl], respectively, as determined with an integrating sphere (Table 1). When the solution of the complexes is air-equilibrated, the Φlum decreases to 0.26 and 0.21 due to oxygen quenching, as expected from the behavior of [PtL1Cl] and similar platinum compounds [44]. Thus, it is worth pointing out that an efficient production of singlet oxygen can be anticipated for these complexes, an interesting aspect of photodynamic therapy [65].
It is known that an increase in the concentration usually leads to a strong decrease in the luminescence quantum yield of N^C^N platinum(II) due to the formation of aggregates and excimers species [71]. As expected, an increase in the concentration of the degassed dichloromethane solution causes a drop in the quantum yield, which, however, remains very high (Φlum = 0.57 and 0.54 at 2·10−4 M, for [PtL2Cl] and [PtL3Cl], respectively) like previously observed for [PtL1Cl]lum = 0.62 [44]). Interestingly, these complexes with a bulky phenyl group on the pyridine rings are suitable for keeping excellent quantum yields even in concentrated solutions.
Excited state decay measurements of the new complexes in degassed CH2Cl2 solutions at different concentrations were performed, exciting at 374 nm at the emission wavelength of 480 and 478 nm for [PtL2Cl] (ESI, Table S2 and Figures S4–S7) and [PtL3Cl] (ESI, Table S4 and Figures S11–S14). The longest lifetime, 4.06–4.09 μs, is observed at the lowest concentration (1·10−6 M, ESI). An increase in the concentration leads to a decrease in the lifetime (Table 1), as expected for the formation of bimolecular states with a diminution of both lifetime and quantum yield. Figures S3 and S10 in the ESI report the excitation spectra in solution at low (1·10−6 M) and high (2·10−4 M) concentrations for [PtL2Cl] and [PtL3Cl], showing the variations of the spectra due to the presence of aggregate species, with a new broadband clearly visible in the region 500–650 nm.
It is worth pointing out that the drop of the lifetime on going from a concentration of 1·10−6 M to 2·10−4 M is much larger for [PtL2Cl] than for [PtL3Cl] (Table 1). This observation would confirm a more difficult formation of excimers/aggregates in the case of [PtL3Cl], reasonably due to the steric hindrance of the two tert-butyl groups on the phenyl linked to the pyridine rings. Such an effect was previously observed for [PtL1Cl] with the pyridines bearing a mesityl group, where the τ value at 2·10−4 M was half that measured at 5·10−6 M (Table 1) [44].
The slightly higher Φlum in the dilute solution of [PtL3Cl] with respect to [PtL2Cl] is reflected by a lower non-radiative rate constant (knr) for the former (Table 1).

3. Materials and Methods

All the reagents and the solvents (dioxane, 1,2-dimethoxyethane, acetonitrile) were used as received from the supplier. Anhydrous toluene was obtained via distillation under argon in the presence of benzophenone. The purifications were performed through column chromatography on silica gel (063–0.200 mm, Merck, Darmstadt, Germany). Grace RevelerisTM with PuriflashTM 40 µm flash cartridges (Buchi, Uster, Switzerland) was used to perform flash chromatography.
The NMR characterizations were obtained by recording on Bruker AV III 300 MHz or AV III 400 MHz spectrometers (Bruker, Billerica, MA, USA). The chemical shifts of 1H, 19F, and 13C NMR spectra are reported in parts per million (ppm), and the coupling constants are measured in Hertz (Hz). The multiplicities of signals are listed as singlet (s), d (doublet), t (triplet), quartet (q), and multiplet (m).
The molecules were analyzed through mass spectrometry at the Centre Régional de Mesures Physiques de l’Ouest, University of Rennes 1, on an LC-MS Agilent 6510 (Agilent, Santa Clara, CA, USA), a Brucker MaXis 4G, or a Thermo Fisher Q-Exactive (Thermo Fisher, Waltham, MA, USA) using ESI and ASAP techniques. Elemental analyses were performed by the Department of Chemistry of the University of Milan.
Electronic absorption spectra in solution were obtained with a UV-3600i Plus UV-VIS-NIR spectrophotometer (Shimadzu Italia S.r.l., Milan, Italy). Luminescence measurements were carried out in CH2Cl2 solution after the Freeze-Pump-Thaw (FPT) procedure to remove dissolved oxygen. Absolute photoluminescence quantum yield, Φ, was measured using a C11347 Quantaurus Hamamatsu Photonics K.K spectrometer (See ESI).

3.1. Procedure for the Synthesis of [PtL2Cl]

3.1.1. Synthesis of HL2

  • 4-(4-(tert-butyl)phenyl)-2-chloropyridine (1):
A round-bottom flask was charged with 4-tert-butylbenzeneboronic acid (1.49 g, 8.4 mmol), 2-chloro-4-iodopyridine (1.00 g, 4.2 mmol), and K2CO3 (1.73 g, 12.5 mmol) under an argon atmosphere. The reagents were solubilized in a 2:1 mixture of 1,4-dioxane and water. An argon needle was placed in the reaction mixture for 30 min to eliminate oxygen traces. Pd(PPh3)4 (0.24 g, 0.2 mmol) was then added, and the reaction vessel was sealed. The mixture was heated under reflux for 72 h and then cooled to room temperature. The organic phase was extracted with toluene, washed three times with 30 mL of water and 20 mL of brine, dried over anhydrous MgSO4, and concentrated in vacuo. Purification via silica gel chromatography (cyclohexane:AcOEt, 20:1, v/v) yielded a colorless oil (547 mg, 53%). 1H NMR (300 MHz, CDCl3, δ): 8.43 (d, J = 5.2 Hz, 1H), 7.48–7.64 (m, 5H), 7.44 (dd, J = 5.2, 1.6 Hz, 1H), 1.39 (s, 9H).13C NMR (75.48 MHz, CDCl3, δ): 153.2, 152.3, 151.4, 150.0, 133.8, 126.7, 126.2, 121.9, 120.4, 34.9, 31.2. HRMS (ESI+): (M + Na)+ calcd for C15H16N35ClNa, 268.0869; found: 268.0863.
  • 2,2′-(4,6-difluoro-1,3-phenylene)bis(4-(4-(tert-butyl)phenyl)pyridine) (HL2):
Compound 1 (0.55 g, 2.2 mmol), the pinacol ester of benzene-1,3-difluoro-4,6-diboronic acid (0.36 g, 0.99 mmol), an aqueous Na2CO3 solution (1 M, 13 mL) and Pd(PPh3)4 (0.19 g, 0.17 mmol) were placed in a Schlenk tube and dissolved in 13 mL of DME. The system was degassed under an argon flow for 10 min before sealing the vessel. The reaction was heated at 100 °C overnight. After cooling, the solvent was evaporated in vacuo, and the oily residue was dissolved in dichloromethane (30 mL) and water (20 mL). The organic layer was collected, dried over anhydrous MgSO4, and concentrated. The crude product was purified by silica gel chromatography (cyclohexane/AcOEt, 16:1) to afford a colorless oil (501 mg, 95%). 1H NMR (300 MHz, CDCl3, δ): 8.77 (d, J = 5.1 Hz, 2H), 8.70 (t, J = 9 Hz, 1H), 8.01 (s, 2H), 7.68 (d, J = 8.5 Hz, 4H), 7.56 (d, J = 8.5 Hz, 4H), 7.51 (dd, J = 5.2, 1.7 Hz, 2H), 7.10 (t, J = 10.7 Hz, 1H), 1.41 (s, 18H).13C NMR (75.48 MHz, CDCl3, δ): 153.1, 152.5, 150.2, 148.9, 135.4, 134.0, 126.9, 126.2, 122.1, 120.6, 105.1, 34.9, 34.7, 34.4, 31.5, 31.3, 30.2, 29.7.1⁹F NMR (282.36 MHz, CDCl3, δ): −112.5 (s, 2F). HRMS (ASAP): (M + H)⁺ calcd for C36H34N2F2 533.2763; found: 533.2764.

3.1.2. Synthesis of [PtL2Cl]

A Schlenk tube was charged with HL2 (0.10 g, 0.19 mmol) and dissolved in 9 mL of acetonitrile. Separately, K2PtCl4 (0.16 g, 0.38 mmol) was dissolved in 1 mL of water and added to the reaction vessel using a Pasteur pipette. The system was degassed for 40 min under an argon stream. The reaction mixture was then sealed and heated at 110 °C for 3 days. The resulting yellow suspension was cooled to room temperature and filtered through a nylon membrane filter. The obtained yellow solid was washed with water and diethyl ether and then dried to afford 77 mg (41%) of the product. 1H NMR (300 MHz, CDCl3, δ): 9.27 (d, J = 5.9 Hz, 3J(1⁹⁵Pt) = 39.3 Hz, 2H), 8.10 (s, 2H), 7.69 (d, J = 8.3 Hz, 4H), 7.58 (d, J = 8.3 Hz, 4H), 7.46 (dd, J = 5.9, 1.9 Hz, 2H), 6.73 (t, J = 11.2 Hz, 1H), 1.41 (s, 18H). 13C NMR (75.48 MHz, CDCl3, δ): 153.7, 151.7, 133.6, 126.7, 126.3, 120.3, 34.7, 31.1, 27.1. 1⁹F NMR (282 MHz, CDCl3, δ): –109.00 (s, 2F). HRMS (ASAP): (M + H2O)⁺ calcd for C36H35N2OF21⁹⁵Pt, 744.2360; found: 744.2367. Elemental Analysis (calcd for C36H33ClF2N2Pt): C, 56.73; H, 4.36; N, 3.68; found: C, 56.77; H, 4.35; N, 3.70.

3.2. Procedure for the Synthesis of [PtL3Cl]

3.2.1. Synthesis of HL3

  • 2-chloro-4-(3,5-di-tert-butylphenyl)pyridine (2):
A round-bottom flask was charged with (3,5-di-tert-butylphenyl)boronic acid (0.88 g, 3.8 mmol), 2-chloro-4-iodopyridine (0.50 g, 2.1 mmol), and K2CO3 (0.87 g, 6.3 mmol) under an argon atmosphere. The reagents were dissolved in a 2:1 mixture of 1,4-dioxane and water. The reaction mixture was degassed by bubbling argon for 30 min. Pd(PPh3)4 (0.24 g, 0.2 mmol) was then added and the vessel was sealed. The reaction was heated at reflux for 72 h, then allowed to cool to room temperature. The organic phase was extracted with toluene, washed three times with 30 mL of water and 20 mL of brine, dried over anhydrous MgSO4, and concentrated in vacuo. Purification via silica gel chromatography (cyclohexane:AcOEt, 20:1, v/v) afforded a colorless oil (847 mg, 67%). 1H NMR (300 MHz, CDCl3, δ): 8.47 (d, J = 5.2 Hz, 1H), 7.55–7.60 (m, 2H), 7.43–7.48 (m, 3H), 1.42 (s, 18H).
  • 2,2′-(4,6-difluoro-1,3-phenylene)bis(4-(3,5-di-tert-butylphenyl)pyridine) (HL3):
Compound 2 (0.42 g, 1.4 mmol), the pinacol ester of benzene-1,3-difluoro-4,6-diboronic acid (0.23 g, 0.6 mmol), an aqueous Na2CO3 solution (1 M, 8 mL), and Pd(PPh3)4 (0.12 g, 0.1 mmol) were placed in a Schlenk tube and dissolved in 8 mL of DME. The system was degassed under an argon flow for 10 min and then sealed. The reaction mixture was heated at 100 °C overnight. After cooling, the solvent was evaporated in vacuo, and the residue was dissolved in dichloromethane (30 mL) and water (20 mL). The organic phase was collected, dried over anhydrous MgSO4, filtered, and concentrated. Purification via silica gel chromatography (cyclohexane/AcOEt, 16:1, v/v) yielded a colorless oil (438 mg, 68%). 1H NMR (300 MHz, CDCl3, δ): 8.79 (d, J = 5.1 Hz, 2H), 8.70 (t, J = 8.9 Hz, 1H), 8.0 (s, 2H), 7.47–7.62 (m, 8H), 7.11 (t, J = 10.6 Hz, 1H), 1.43 (s, 36H). 13C NMR (75.48 MHz, CDCl3, δ): 162.5, 162.1, 158.9, 158.8, 153.0, 151.7, 150.4, 150.0, 137.8, 133.8, 124.7, 123.3, 122.7, 121.6, 121.1, 105.4, 105.1, 104.7, 35.0, 31.5, 30.2, 29.7. 1⁹F NMR (282.36 MHz, CDCl3, δ): −112.92 (s, 2F). HRMS (ESI⁺): (M + H)⁺ calcd for C44H51N2F2, 645.4015; found: 645.4008.

3.2.2. Synthesis of [PtL3Cl]

A Schlenk tube was charged with HL2 (0.17 g, 0.27 mmol) and dissolved in 11.7 mL of acetonitrile. Separately, K2PtCl4 (0.22 g, 0.54 mmol) was dissolved in 1.3 mL water and added to the reaction vessel using a Pasteur pipette. The system was degassed by bubbling argon directly into the solvent for 40 min. The reaction was then sealed and heated at 110 °C for 3 days until a yellow suspension formed. After cooling to room temperature, the mixture was filtered through a nylon membrane filter, yielding a yellow solid. The solid was washed with water, methanol, and diethyl ether and then dried to afford 148 mg (85%) of the product. 1H NMR (300 MHz, CDCl3, δ): 9.34 (d, J = 6.0 Hz, 3J(1⁹⁵Pt) = 39.4 Hz, 2H), 8.13 (s, 2H), 7.63 (s, 2H), 7.45–7.59 (m, 6H), 6.74 (t, J = 11.2 Hz, 1H), 1.43 (s, 36H). 13C NMR (75.48 MHz, CDCl3, δ): 164.3, 153.3, 152.0, 151.7, 136.6, 124.5, 121.5, 121.1, 35.2, 31.4. 1⁹F NMR (282 MHz, CDCl3, δ): −108.48 (s, 2F). HRMS (ESI⁺): (M + Na)⁺ calcd for C44H49N2F23⁵Cl Na1⁹⁵Pt, 896.3092; found: 896.3085. Elemental Analysis (calcd for C44H49ClF2N2Pt): C, 60.44; H, 5.65; N, 3.20; found: C, 60.48; H, 5.66; N, 3.23.

4. Conclusions

In conclusion, two novel complexes, namely [Pt(bis(4-(4-(tert-butyl)phenyl)-pyridin-2-yl)-4,6-difluorobenzene)Cl] and [Pt(bis(4-(3,5-di-tert-butylphenyl)-pyridin-2-yl)-4,6-difluorobenzene)Cl] were easily prepared and thoroughly characterized. In degassed diluted dichloromethane solution, both are highly luminescent (Φlum = 0.89–0.95) in the blue region (478–480 nm) with a lifetime similar to that usually observed for N^C^N platinum(II) complexes (ca 4 µs). Like for the parent complex [Pt(1,3-bis(4-mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl], excellent luminescent quantum yields are obtained even in concentrated solution (Φlum = 0.54–0.57).
An important aspect that this work puts in evidence is the effect on the formation of excimers/aggregates of the substituents on the phenyl group linked in the para position of the pyridines. The steric effect caused by the presence of three methyls in positions 2, 4, and 6 of the phenyl (i.e., the mesityl group) seems the best to hamper the neighboring of monomeric complexes, as evidenced by the lower intensity of the low energy band characteristic of excimers/aggregates in concentrated solutions. The presence of two tert-butyls in positions 3 and 5 of the phenyl group appears slightly less efficient but better than one tert-butyl in the para of the phenyl group. Clearly, it is imperative to have substituents in the alpha of the carbon linked in the para position of the pyridine to hamper better the neighboring of the monomeric species, which would allow Pt-Pt and π−π interactions with concomitant red emission. This observation represents an important guideline for the design of N^C^N platinum complexes as efficient emitters for blue OLEDs.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/molecules30071498/s1. 1H, 13C and 19F NMR spectra of intermediates, ligands and Pt(II) complexes; Table S1: Molar extinction coefficients for [PtL2Cl]; Figures S1 and S2: Absorbance vs Concentration for [PtL2Cl]; Figure S3: Excitation spectra for [PtL2Cl]; Table S2: Lifetimes values for [PtL2Cl]; Figures S4–S7: Lifetime measurements for [PtL2Cl]; Table S3: Molar extinction coefficients for [PtL3Cl]; Figures S8 and S9: Absorbance vs Concentration for [PtL3Cl]; Figure S10: Excitation spectra for [PtL3Cl]; Table S4: Lifetimes values for [PtL3Cl]; Figures S11–S14: Lifetime measurements for [PtL3Cl]; [81].

Author Contributions

Conceptualization, D.R. and V.G.; methodology, D.M., A.C., C.D. and F.F.; investigation, G.D.S., D.M. and F.F.; resources, A.C. and C.D.; data curation, G.D.S., D.M. and F.F.; supervision, D.R. and V.G.; Writing—original draft, F.F.; Writing—review and editing, G.D.S., V.G., D.M., A.C., C.D., F.F. and D.R. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The full characterization of the two complexes (1H, 13C, and 19F NMR spectra, HRMS, elemental analysis, and photophysical characterization) have been included as part of the Supplementary Information.

Acknowledgments

Fondazione Cariplo and Regione Lombardia are acknowledged for the instrumentation bought during the SmartMatLab Centre project (2014). The work was supported by the National Interuniversity Consortium of Materials Science and Technology (Project TRI_25_073 Dragonetti and TRI_25_173 Colombo) and Università degli Studi di Milano (Project PSR2023_DIP_005_PI_FTESS).

Conflicts of Interest

The authors declare no conflicts of interest.

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Scheme 1. Chemical structures of the investigated Pt(II) complexes.
Scheme 1. Chemical structures of the investigated Pt(II) complexes.
Molecules 30 01498 sch001
Scheme 2. Synthesis of complexes [PtL2Cl] and [PtL3Cl].
Scheme 2. Synthesis of complexes [PtL2Cl] and [PtL3Cl].
Molecules 30 01498 sch002
Figure 1. Absorption spectra of [PtL2Cl] (A) and [PtL3Cl] (B) at different concentrations in CH2Cl2 at 298 K. The weak bands at longer wavelengths are shown on an expanded scale for clarity.
Figure 1. Absorption spectra of [PtL2Cl] (A) and [PtL3Cl] (B) at different concentrations in CH2Cl2 at 298 K. The weak bands at longer wavelengths are shown on an expanded scale for clarity.
Molecules 30 01498 g001
Figure 2. Normalized emission spectra of [PtL2Cl] (A) and [PtL3Cl] (B) after excitation at 380 nm, at different concentrations in deaerated CH2Cl2 solution at 298 K.
Figure 2. Normalized emission spectra of [PtL2Cl] (A) and [PtL3Cl] (B) after excitation at 380 nm, at different concentrations in deaerated CH2Cl2 solution at 298 K.
Molecules 30 01498 g002
Figure 3. Normalized emission spectra of [PtL1Cl], [PtL2Cl], and [PtL3Cl] after excitation at 380 nm, in concentrated degassed CH2Cl2 solution (2·10−4 M) at 298 K.
Figure 3. Normalized emission spectra of [PtL1Cl], [PtL2Cl], and [PtL3Cl] after excitation at 380 nm, in concentrated degassed CH2Cl2 solution (2·10−4 M) at 298 K.
Molecules 30 01498 g003
Table 1. Photophysical parameters a of [PtL2Cl] and [PtL3Cl] in comparison with that of [PtL1Cl] [44].
Table 1. Photophysical parameters a of [PtL2Cl] and [PtL3Cl] in comparison with that of [PtL1Cl] [44].
λmax,abs (S0→T1)/nm
[ε/M−1cm−1]
λmax,em/nm b
Monomer
[excimer/Aggregate] c
Φlum d
[Aerated]
τ/µskr e/s−1knr e/s−1
[PtL1Cl]
(5·10−6M)
467
[120]
471
[680]
0.97
[0.18]
4.772.0·1056.3·103
[PtL1Cl]
(2·10−4M)
0.62
[0.12]
2.412.6·1051.6·105
[PtL2Cl]
(5·10−6M)
470
[310]
480
[697]
0.89
[0.26]
3.912.3·1052.8·104
[PtL2Cl]
(2·10−4M)
0.57
[0.23]
1.174.9·1053.7·105
[PtL3Cl]
(5·10−6M)
470
[225]
478
[690]
0.95
[0.21]
3.962.4·1051.3·104
[PtL3Cl]
(2·10−4M)
0.54
[0.17]
2.112.6·1052.2·105
a at 298 K in degassed CH2Cl2. b Excitation at 330 nm. c Excimer/aggregate at 2·10−4 M. d Absolute Φlum measured with an integrating sphere. e Radiative and nonradiative rate constants are calculated from the quantum yields and emission decay lifetimes, according to Φlum = kr·τem = kr/(kr + knr).
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De Soricellis, G.; Guerchais, V.; Colombo, A.; Dragonetti, C.; Fagnani, F.; Roberto, D.; Marinotto, D. Effect of the Substitution of the Mesityl Group with Other Bulky Substituents on the Luminescence Performance of [Pt(1,3-bis(4-Mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl]. Molecules 2025, 30, 1498. https://doi.org/10.3390/molecules30071498

AMA Style

De Soricellis G, Guerchais V, Colombo A, Dragonetti C, Fagnani F, Roberto D, Marinotto D. Effect of the Substitution of the Mesityl Group with Other Bulky Substituents on the Luminescence Performance of [Pt(1,3-bis(4-Mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl]. Molecules. 2025; 30(7):1498. https://doi.org/10.3390/molecules30071498

Chicago/Turabian Style

De Soricellis, Giulia, Véronique Guerchais, Alessia Colombo, Claudia Dragonetti, Francesco Fagnani, Dominique Roberto, and Daniele Marinotto. 2025. "Effect of the Substitution of the Mesityl Group with Other Bulky Substituents on the Luminescence Performance of [Pt(1,3-bis(4-Mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl]" Molecules 30, no. 7: 1498. https://doi.org/10.3390/molecules30071498

APA Style

De Soricellis, G., Guerchais, V., Colombo, A., Dragonetti, C., Fagnani, F., Roberto, D., & Marinotto, D. (2025). Effect of the Substitution of the Mesityl Group with Other Bulky Substituents on the Luminescence Performance of [Pt(1,3-bis(4-Mesityl-pyridin-2-yl)-4,6-difluoro-benzene)Cl]. Molecules, 30(7), 1498. https://doi.org/10.3390/molecules30071498

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