Open Access Article
Vanessa V.
Gaensicke
a,
Stephanie
Bachmann
b,
Luca
Craciunescu
c,
Andrew W.
Prentice
c,
Martin J.
Paterson
c,
Dinu
Iuga
b,
Peter J.
Sadler
*a and
Rafael Cavalieri
Marchi
*ad
aDepartment of Chemistry, University of Warwick, Coventry, CV4 7AL, UK. E-mail: P.J.Sadler@warwick.ac.uk; Rafael.Marchi@warwick.ac.uk
bDepartment of Physics, University of Warwick, Coventry, CV4 7AL, UK
cSchool of Engineering and Physical, Heriot-Watt University, Edinburgh, EH14 4AS, UK
dInstitute of Advanced Studies (IAS), University of Warwick, Coventry, CV4 7AL, UK
First published on 3rd March 2025
There is current interest in the anticancer and antimicrobial activities of Ga(III) tris-hydroxyquinolinate complexes, and hence their solution and solid-state chemistry. Here, we have studied the formation, stability and structure of a novel tris-5,7-dibromo-8-hydroxyquinolinate Ga(III) complex [Ga(Br2-HQ)3]. Reactions of 5,7-dibromo-8-hydroxyquinoline with Ga(NO)3 in DMSO were followed using electronic absorption and emission spectroscopy, and revealed the slow but concerted coordination of three chelated ligands, with ligand deprotonation being the apparent rate-limiting step, facilitated by basic Ga(III) hydroxido species. The emissive excited state of [Ga(Br2-HQ)3] in DMSO had a short half-life of 1.2 ns, and the fluorescence (550 nm, λex = 400 nm) was characterized by TDDFT calculations as arising from a ligand-centred singlet S1 state. We compared the structures of [Ga(Br2-HQ)3] and the clinical tris-hydroxyquinolinate complex [Ga(HQ)3] using high-field magic-angle-spinning solid-state 1D and 2D 850 MHz and 1 GHz 1H, 13C and 71Ga NMR spectroscopy. The similarity of their coordination spheres was confirmed by their 71Ga chemical shifts of 101 and 98 ppm, respectively, and quadrupolar coupling constants of 9.265 MHz and 9.282 MHz. 1H-1H 2D NOESY experiments revealed second coordination sphere interactions between an acetic acid solvent molecule and the bound hydroxyquinolinate ligands of [Ga(HQ)3]·0.5CH3CO2H. This finding suggests that carboxylic acids could play a role in modifying the formulation properties of this drug for clinical use.
The first clinical use of Ga(III) in 1970 involved the radioactive isotope 67Ga as an imaging agent. Now both 67Ga and 68Ga (single-photon emission computed tomography and positron emission tomography, respectively)3 are used for, e.g., soft tissue and bone tumours, along with inflammatory abscesses.4 In 2003, a citrate-buffered formulation of Ga(III) nitrate was approved by the US Food and Drug Administration (FDA) as Ganite® for the treatment of malignancy-associated hypercalcaemia,5,6 non-Hodgkin's lymphoma5 and bladder cancer.7 Several other Ga(III) complexes and formulations are undergoing phase I and II clinical trials for cancer treatment.2,8
Ga(III) complexes are also known to possess good antimicrobial activity. Recently, an extensive screening of compounds by the community of open antimicrobial drug discovery (CO-ADD) has shown that the hit-rate for metal complexes (906 complexes screened; 27% active) was higher than for organic compounds (almost 300
000; 2% active) against Gram-negative and Gram-positive bacteria.9 Notably, Ga(III) complexes were highly active, although only a few were screened.9,10
The mechanism of biological action of Ga(III) complexes is believed to involve interference in natural Fe(III) biochemistry. Both ions have similar radii and coordination chemistry, however unlike Fe(III), Ga(III) is not redox-active. For instance, gallium-substituted enzymes and proteins affect the survival of microorganisms since they cannot exert the functions of their iron-dependent counterparts, leading to metabolic distruption.1,11 Ga(III) can contribute to deregulation of cellular iron homeostasis.12
Hydroxyquinolines act as bidentate ligands through coordination of the deprotonated hydroxyl oxygen and the ring nitrogen (Fig. 1). These ligands can inhibit several enzymes including topoisomerase and haspin kinase.13,14 Use of hydroxyquinolines as ligands for Ga(III) can result in a scaffold suitable for drug development. The tris-chelated 8-hydroxyquinoline (HQH) as [Ga(HQ)3] is currently in phase II clinical trials as the oral gallium compound KP46 for treatment of breast, lung, and prostate cancer and bone metastases.15 Interestingly, in vivo trace studies with radioactive (67Ga and 68Ga) KP46, suggest that oral administration can lead to dissociation of the complex in the gut.15
The aqueous solution chemistry of Ga(III) is complicated by hydrolysis and formation of hydroxido/oxido monomers and oligomers, as is the case for Fe(III) and widely studied Al(III).16–20 Equilibria between hydrolysed species can be both thermodynamically and kinetically driven. For aqua Ga(III) complexes, pKa values range from 2.6 (formation of Ga(OH)2+) to 6.3 (formation of Ga(OH)4−).21–23 Hence, hydrolysed Ga(III) species are likely to play a role in the biological chemistry of gallium.
In this work we have studied binding of the 8-hydroxyquinoline derivative 5,7-dibromo-8-hydroxyquinoline (Br2-HQH) to Ga(III). The ligand was chosen to provide the possibility of tracking both Ga(III) and the ligand in biological cells using elemental X-ray imaging, as we have done for an organo-osmium anticancer complex with a brominated chelated ligand.24 This method allows identification of dissociation of a bound Br-labelled ligand from a metal in cells.
We studied the binding of Br2-HQH to Ga(NO3)3 in a variety of organic and aqueous solvents using UV-visible, fluorescence and NMR spectroscopy. The luminescence lifetime of the product was determined, and emissive state was characterised by DFT calculations. Under certain conditions it was possible to isolate [Ga(Br2-HQ)3] which was characterised by multinuclear NMR spectroscopy, including 71Ga and comparison with the clinical drug [Ga(HQ)3], Fig. 1. Although 71Ga is a quadrupolar nucleus (39.89% natural abundance, I = 3/2)25 giving relatively broad resonances in non-symmetrical environments, its resonances are sharper at high fields such as 20 T and 23.5 T since the magic angle spinning (MAS) quadrupolar broadening of the central transition is inversely proportional to the external magnetic field.
:
1 mol ratio of Br2-HQH
:
Ga(III) (0.15 mM).
A second titration was carried out with deprotonated ligand (Br2-HQ) prepared by adding an equimolar concentration of NaOH to Br2-HQH in DMSO with 0.4% DMF solution, and repeating the titration adding Ga(III) to the Br2-HQ solution.
To investigate the time dependence of complex formation, different Ga(III) aliquots (3.4, 6.8, 10.2 μL) from the 44 mM stock solution were added to 3.0 mL of 0.15 mM solution of Br2-HQH in DMSO with 0.4% DMF (v/v) solution in a cuvette. The final mol ratios of Br2-HQH
:
Ga(III) were 1
:
0.33, 1
:
0.67, 1
:
1. The UV-vis spectrum of each solution was recorded every 3 min at 298 K for a total of ca. 2 h.
In each case, the plot of absorbance at 400 nm vs. time gave a reasonable fit to 1st-order kinetics, eqn (1):
![]() | (1) |
In order to determine the influence of ligand deprotonation on the rate of complex formation, we repeated the slowest of these reactions (1 Br2-HQH
:
0.33 Ga(III)) but now using deprotonated ligand (Br2-HQ) prepared as above and adding 0.33 mol equiv. Ga(III). The spectrum of the solution was recorded every 3 minutes at 298 K for a total of 2 h.
:
1 mol ratio of Br2-HQH
:
Ga(III) (0.15 mM). The emission was recorded in the region between 450 nm to 750 nm with λex = 400 nm.
000 ppm certified reference material in 3.6% v/v nitric acid. The correlation coefficient for the linear curve was 0.9998. Solutions of [Ga(Br2-HQ)3] in 3.6% v/v HNO3 were analysed.
In the first titration, aqueous Ga(NO3)3 was added to Br2-HQH (0.15 mM) in 99.6% DMSO/0.4% DMF (v/v) in 0.065 mol equivalent steps to a final 1
:
1 mol ratio. As seen at Fig. 2A, Br2-HQH has absorption maxima at 330 nm and 425 nm. On addition of Ga(III) a new intense band at 390 nm appeared and continued to increase in intensity as further Ga(III) was added. There was a concomitant reduction in intensity of the Br2-HQH band at 330 nm. Notable is the isosbestic point at 355 nm, suggesting that the reaction involves an equilibrium between Br2-HQH and the [Ga(Br2-HQ)3] complex formed.
A similar titration behaviour was observed with monitoring by fluorescence (λex = 400 nm), Fig. 2B. Initially, very weak fluorescence was observed for Br2-HQH at 530 nm, but from the addition of the first Ga(III) aliquot the band maximum red-shifted to 550 nm and increased in intensity with increasing the Ga(III) concentration, Fig. S2.‡
For less than ca. 7 additions of 0.065 mol equiv. Ga(III), giving a Ga(III)
:
Br2-HQH mol ratio > 1
:
3, complete formation of [Ga(Br2-HQ)3] could have occurred, but was not observed. This led us to investigate possible kinetic control of the reaction. In the next set of experiments we added either 0.33, 0.67, or 1 mol equiv. of Ga(NO3)3 to Br2-HQH (0.15 mM) in the same solvents as above (final solvent mixture 0.4% H2O/99.2% DMSO/0.4% DMF v/v), and monitored the reaction by UV-vis every 3 min up to 300 min. In each case, a similar behaviour of decreasing intensity for the Br2-HQH band at 330 nm and increasing intensity of the 390 nm for the [Ga(Br2-HQ)3] product was observed, Fig. 3 and Fig. S3.‡ The final concentration of the product was 0.023 mM, 0.048 mM and 0.051 mM, for 0.33, 0.67, and 1 mol equiv. of Ga(NO3)3 added, respectively, i.e. 45, 95 and 100% formation of [Ga(Br2-HQ)3].
![]() | ||
Fig. 3 (A) Top: time-dependent changes in the UV-vis absorption spectrum when Ga(NO3)3 (1 mol equiv., 0.15 mM) in water was added to Br2-HQH (1 mol equiv., 0.15 mM) solution in 99.6% DMSO/0.4% DMF (v/v). Bottom: variation in absorbance at 341 nm for Br2-HQH, and 389 nm for [Ga(Br2-HQ)3] with time. (B) Top: time-dependent changes in the UV-vis absorption spectrum when Ga(NO3)3 (0.33 mol equiv., 0.05 mM) in water was added to Br2-HQH (1 mol equiv., 0.15 mM) solution in 99.6% DMSO/0.4% DMF (v/v). Bottom: variation in absorbance at 341 nm for Br2-HQH, and 389 nm for [Ga(Br2-HQ)3] with time. The insets show the best fit of log A vs. time (red line), giving the first-order rate constants in Table 1. | ||
The absorption versus time plots show a reasonable fit to first order kinetics (Fig. 3, Table 1 and Fig. S3‡) with the following rate constants: 0.15 mM Ga(III), 0.031 min−1; 0.10 mM Ga(III), 0.014 min−1; 0.05 mM Ga(III), 0.010 min−1, suggesting that the rate-limiting step depends on the Ga(III) concentration.
The next experiment aimed to confirm the nature of the Ga(III) product, in particular the role of Br2-HQH deprotonation in the position of equilibria and in the kinetics of formation of the product. First, we generated deprotonated Br2-HQ ligand by adding NaOH solution to DMSO (0.4% DMF v/v) in steps until no further spectral changes were observed. As shown in Fig. 2C, complete deprotonation and formation of Br2-HQ was evident after addition of ca. 1 mol equiv. of NaOH from the decrease in intensity of the band at 330 nm and formation of two new bands at 355 nm and 425 nm for Br2-HQ, accompanied by an isosbestic point at 348 nm.
Then 20 additions of Ga(NO3)3 were made to a solution of deprotonated ligand to give a final molar ratio of 1 Ga
:
1 Br2-HQ. In this case, the final product was fully formed in less than 0.5 mol equiv. compatible with the formation of [Ga(Br2-HQ)3] with absorption bands at 340 nm and 400 nm, Fig. 2D. To investigate the kinetics of formation of [Ga(Br2-HQ)3], 0.33 mol equiv. of Ga(III) was added to 1 mol equiv. of Br2-HQ and the reaction monitored over time. It was evident that the reaction with deprotonated ligand (Br2-HQ) occurred rapidly (<3 min, Fig. S4‡) in contrast to the reaction with the protonated ligand (Br2-HQH), as described above.
:
32
:
10% v/v), necessary to aid solubility, gave rise to broadening of the peaks within the aromatic region from Br2-HQH over ca. 1 h at 298 K, together with the appearance of low intensity peaks in the same region. Interpretation was complicated by precipitation of a product in the NMR tube.
Next, we attempted to observe the 153 MHz 71Ga-NMR spectrum for a DMSO-d6 solution of [Ga(Br2-HQ)3] at a concentration of 1 mM (highest concentration achievable). However, not surprisingly, in view of the quadrupolar nature of 71Ga (I = 3/2, 39.6% abundant), the low concentration, and the expected broadening for 71Ga in a non-symmetrical environment, no peak was detectable.
Next, we studied 1H, 13C and 71Ga solid-state NMR spectra of [Ga(Br2-HQ)3]. We hoped to take advantage of the sharpening of the multiple spin-half 71Ga (I = 3/2) resonance at high observation frequencies.42 We also compared the 71Ga spectra of [Ga(Br2-HQ)3] and [Ga(HQ)3]·0.5CH3CO2H in view of the clinical use of KP46 for cancer treatment. Such spectra can provide information on the types of coordinated atoms and the coordination geometry.43 No previous 71Ga NMR studies of this class of bioactive complexes appear to have been reported.
Powdered samples were packed in a rotor (diameter of 1.3 mm) and 71Ga solid-state spectra were recorded at 23.5 T (71Ga Lamor frequency of 305 MHz) with 60 kHz MAS for [Ga(Br2-HQ)3] and [Ga(HQ)3], Fig. 4. As expected, at 20 T (260 MHz 71Ga) the resonances were slightly broader (Fig. 4). Fitting the signals to one Ga site for each complex indicated similar isotropic chemical shifts of δ(71Ga) = 101 and 98 ppm, for [Ga(Br2-HQ)3] and [Ga(HQ)3]·0.5 CH3CO2H, respectively. Analysis of line shapes at 20 and 23.5 T gave rise to a quadrupolar coupling constant of CQ = 9 ± 0.5 MHz with a quadrupolar asymmetry parameter of η = 0.5 ± 0.15 for both complexes [Ga(Br2-HQ)3] and [Ga(HQ)3]·0.5 CH3CO2H.
The 1 GHz 1H-DPMAS-NMR spectrum for [Ga(HQ)3]·0.5CH3CO2H showed a distinct pattern of resonances which can be divided into two regions, 4 to 6 ppm attributable to the phenolic region of the complex, and 6 to 10 ppm assignable to pyridyl ring protons, Fig. 5A. The additional peak at −0.8 ppm can be assigned to the methyl group of acetic acid. Aqueous acetic acid was used as solvent in the synthesis, see section 2.3. The presence of acetic acid was also evident from the solution 1H-NMR spectrum, a singlet for the acetic acid methyl protons at 1.8 ppm and another at 11.9 ppm assignable to the carboxylic acid proton, integrating as 0.5 mol acetic acid per mol of [Ga(HQ)3], Fig. S1.‡
For [Ga(Br2-HQ)3], the presence of the two bromide substituents on the hydroquinolinate ligands gives rise to a shift of the phenolic ring protons to low field compared to [Ga(HQ)3], but the resonances for individual protons are unresolved, Fig. 5A.
1H-1H NOESY solid-state NMR spectra were recorded with mixing times of 5 ms and 220 ms, Fig. 6 and Fig. S8.‡ For [Ga(HQ)3]·0.5CH3CO2H with a 5 ms mixing time, two cross peaks for 1H signals at −0.8/5 ppm and −0.8/8 ppm are evident, and indicative of close contact between the acetic acid and hydroxyquinolinate ring protons, as well as less well-resolved cross-peaks between the ring protons. These cross-peaks became broader with a mixing time of 220 ms. For [Ga(Br2-HQ)3] the NOESY cross peaks were poorly resolved with a 5 ms mixing time, but better resolved at 220 ms for contacts between HQ protons.
![]() | ||
| Fig. 6 1H-1H NOESY solid state MAS spectra at 850 MHz of (A) [Ga(Br2-HQ)3] and (B) [Ga(HQ)3]·0.5 CH3CO2H (mixing time of 220 ms). | ||
The 13C CPMAS spectrum of [Ga(HQ)3]·0.5 CH3CO2H (Fig. 5B) also showed sharper peaks than for [Ga(Br2-HQ)3], as for 1H-NMR spectra. The 13C CPMAS spectra of the protonated free ligands HQH and Br2-HQH also showed sharp peaks, Fig. S9,‡ indicating crystalline properties. The resonances of HQH and Br2-HQH were assigned on the basis of reported solution spectra.44,45 Both, 13C and 1H resonances for [Ga(Br2-HQ)3] are broadened compared to [Ga(HQ)3]·0.5CH3CO2H. The broadened resonances for [Ga(Br2-HQ)3] indicate disorder in the sample, whereas the 13C CPMAS spectrum of [Ga(HQ)3]·0.5 CH3CO2H has more than nine resolved peaks showing its high crystallinity and the non-equivalence of the coordinated ligands.
Several DFT functionals (see section 2.11) were employed to calculate UV-Vis absorption spectra, Fig. S12.‡ The best agreement with experiment was obtained using the B3LYP functional with DFT-D3 dispersion correction,46,47 however the character of the S1 transition differed from those predicted by every other method used. Therefore, we calculated vacuum excited state energies with the high-accuracy wave function-based method ADC(2) and arrived at the best theoretical estimate for both absorption and emission by using the ADC(2) S0 → S1 excitation in vacuum and adding the respective hypsochromic and bathochromic shift for solvent and relaxation effects from ωB97X-D348 calculations, Table S1.‡ This resulted in wavelengths of 390 nm for the absorption of the S1 state and a fluorescence at 539 nm out of the same state. These values compare well with the experimentally measured wavelengths of 405 and 550 nm. Therefore, both absorption and emission originate from the S1 state. The T1 state was found at excitation wavelengths longer than 500 nm and phosphorescence above 700 nm for all functionals, therefore it was discounted as the source of luminescence.
Calculations on [Ga(HQ)3] showed qualitatively similar absorption behaviour to [Ga(Br2-HQ)3], with the former exhibiting a slight hypsochromic shift with respect to the Br-substituted molecule, Fig. S13.‡ Additionally, the calculations provided insight into the preferred geometry of [Ga(Br2-HQ)3] for which the meridional isomer is slightly more stable than the facial isomer, in both vacuum and DMSO conditions, Table S2.‡
:
Ga(III) of 1
:
0.33, 1
:
0.67, 1
:
1. Previous reports using potentiometry have shown the high stability of [Ga(HQ)]3 and sulfonated derivative in water,50,51 as well as stepwise formation of the sulfonated complex.51 In general, tris-chelated complexes [Ga(X-HQ)3] are more thermodynamically stable compared to the mono- and bis-chelated species.52 However, such equilibria in aqueous media are complicated by the hydrolytic chemistry of Ga(III) in aqueous media which involves a range of monomeric and polymeric hydroxido/oxido species.21,53 Analogous species have been widely studied for Al(III),54,55 Fe(III)56,57 and In(III).58,59 Here, we have studied the formation of Ga(III) complexes with the brominated hydroxyquinoline ligand Br2-HQH (Fig. 1) with a view to mapping reactions of the tris-chelate [Ga(Br2-HQ)3] in intact cells using X-ray fluorescence. Detection of both Ga(III) and bromine would allow monitoring of possible ligand displacement, as we have shown recently with organo-osmium anticancer agents.24 Such studies may be valuable for identifying the active components (pharmacophores) in cells.
First, we studied the step-wise addition of Br2-HQH to Ga(III) monitored by UV-vis and fluorescence spectroscopy, Fig. 2A and B. These reactions were studied in a variety of mixed aqueous solvents compatible with the solubility of Ga(NO3)3 and Br2-HQH. [Ga(Br2-HQ)3] formed readily in the presence excess Ga(III), however complete formation of the product required a large excess of Ga(III) in the mixed solvent 99.2% DMSO/0.4% DMF/0.4% H2O (v/v). In contrast, titration of deprotonated ligand with Ga(III) led to stoichiometric formation of [Ga(Br2-HQ)3], Fig. 2C and D. This difference can be explained by the presence of basic Ga-hydroxido species in the titration of Br2-HQH which deprotonate the ligand.
The formation of such Ga(III)-hydroxido monomers and polymers has been studied previously.21–23,60 At nanomolar Ga concentrations, mainly monomeric species are formed in aqueous solution with Ga(OH)2+ predominating at pH 3 to 4 with further deprotonation leading to Ga(OH)4− predominating at pH > ca. 4.2.60 At millimolar concentrations, oligomeric species such as Ga4(OH)11+ predominate at pH ca. 4 and Ga(OH)3 at pH 7 and Ga(OH)4− at pH 8.21 Hence, we assume that in our mixed aqueous solvent such hydroxido species will readily form and act as bases to deprotonate the Br2-HQH ligand. The possibility that DMSO and NO3− can also be involved in mixed aqua/ligand complexes and affect the pKa values of bound water cannot be ruled out.61,62 No attempt was made to determine the pH values in our mixed solvents.
UV-vis studies showed that the reaction of Ga(NO3)3 with Br2-HQH is relatively slow taking >2 h to reach completion, Fig. 3 and Fig. S3.‡ For such reactions, a single isosbestic point was observed at 355 nm suggesting an overall conversion of Br2-HQH into a single product.
At the different molar ratios of Ga
:
Br2-HQH, the kinetic plots gave a reasonable 1st-order fit with half-lives of 22.4 min, 49.5 min, 69.1 min, with Ga(III) concentration increasing from 0.33 equiv. to 1 equiv., respectively, showing an approximate linear dependence on Ga(III) concentration (Fig. 3, Fig. S3‡ and Table 1). At equilibrium the overall yield of [Ga(Br2-HQ)3] relative to the initial concentration of Br2-HQH was ca. 100%, 85% and 45% mol equiv. with 1, 0.67 and 0.33 mol equiv. of Ga(III), respectively.
Further detailed kinetic studies of these reactions are warranted, but were beyond the scope of the present work. The reaction mechanism for formation of [Ga(Br2-HQ)3] is complicated and likely to involve sequential binding of three Br2-HQH to Ga(III), perhaps via initial coordination of hydroxyquinoline N to Ga(III), followed by chelate ring formation via deprotonation of the hydroxyl group. The formation of the second and third chelate rings is further complicated by the possible formation of isomers (cis/trans and fac/mer). Since the reaction of deprotonated Br2-HQH with Ga(III) proceeded rapidly (ca. 3 min, Fig. S4‡), it seems likely that the rate-limiting step is ring closure via -OH deprotonation. Basic hydroxido Ga(III) species seem likely to be involved in this step.
There appear to be few reports of kinetics and mechanisms of ligand substitution reactions for Ga(III). Such studies are potentially important for understanding the (dynamic) metallomics of bioactive Ga(III) complexes in biological media.
Initial attempts to isolate [Ga(Br2-HQ)3] using protocols reported in the literature63,64 were unsuccessful, until we discovered that the product readily precipitated in acetonitrile. By dissolving Br2-HQH in DMF followed by addition of acetonitrile and then Ga(NO3)3 in a minimum volume of water, a yellow precipitate readily formed. This protocol is similar to that described for chelation of 5,7-dihalo-8-quinolinoline to Sn(IV)64 (i.e., with no base addition).
In the UV-vis spectrum in DMSO, the band at 400 nm is assignable to ligand–ligand charge transfer (LLCT) as confirmed by DFT calculations, Fig. S12.‡ As is normally the case for nd10(n + 1)s0 metals, no ligand-to-metal (LMCT) band was seen for [Ga(Br2-HQ)3], as reported for isostructural [Al(HQ)3].65,66
Additional characterisation of [Ga(Br2-HQ)3] was obtained from the Fourier-transform infrared (FT-IR) spectrum, Fig. S6.‡ The comparison between the free ligand and complex clearly showed the disappearance of the broad –OH peak of hydroxyquinoline (at ∼3000 cm−1) and the appearance of two new peaks at 950 and 1110 cm−1 assignable to Ga(III)–O bonds, analogous to Al(III) and In(III) complexes.67
The low solubility of [Ga(Br2-HQ)3] made characterisation by NMR in solution difficult. We therefore recorded 71Ga-, 1H- and 13C solid-state NMR spectra for [Ga(Br2-HQ)3] and compared to [Ga(HQ)3] which was synthesized as [Ga(HQ)3] ·0.5CH3CO2H. As seen in Fig. 4, the two complexes have a similar 71Ga chemical shift (101 and 98 ppm, for [Ga(Br2-HQ)3] and [Ga(HQ)3]·0.5CH3CO2H, respectively). These chemical shifts are in the range that might be expected for hexacoordinated Ga(III) complexes.68 Both complexes in this study had a coordination sphere of 3N and 3O. In a similar environment, but with six-coordinated NOTA-type ligands bound to Ga(III), reported 71Ga chemical shifts are in the range +110 to +171 ppm.69 Thus the chemical shifts observed here are within the expected region for 3N and 3O hexacoordinated Ga(III) complexes. This appears to be the first report of 71Ga data for Ga(III) coordinated to hydroxyquinolinate ligands. The reported range of 71Ga shifts is ca. +700 to −700 ppm,70–73 however there are too few to enable a more detailed correlation of chemical shifts with number and/or types of coordinated ligand and the coordination geometry.
It is notable that the 71Ga quadrupole coupling constant observed here (CQ = 9 ± 0.5 MHz) is higher compared to Ga bound to carboxylate groups74 and lower compared to Ga bound to siloxides75 suggesting that the resonance signature is closely dependent on the local symmetry of gallium.76 In the case of [Ga(Br2-HQ)3] and [Ga(HQ)3] the local symmetry is also affected by the different isomers (facial vs. meridional), in the solid and liquid states. Ga(III) preferably adopts the less symmetric but more energetically stable mer-configuration.77 This correlates with the 13C CPMAS and 1H DPMAS data and DFT calculations.
1H-1H NOESY spectra for [Ga(HQ)3]·CH3CO2H (Fig. 6 and Fig. S8‡) indicate spatial proximity of protons in the complexes, including the interaction of quinolinate protons (5 to 10 ppm), with acetic acid methyl protons at – 0.8 ppm. The role of such small molecules in the solid-state structure of this anticancer drug might be important for its formulation for drug use, influencing its rate of dissolution and absorption, and is worthy of further investigation.
In the 13C CPMAS and 1H DPMAS solid-state NMR spectra for both complexes there was an increase in the number of hydroxyquinoline peaks compared to those of the free ligand, Fig. 5 and Fig. S9.‡ From this observation, it can be deduced that these Ga(III) complexes are likely to be to meridional isomers rather than the more symmetrical facial isomers, as in the reported X-ray crystal structure of [Ga(HQ)3].78,79
Fluorescence of [Ga(Br2-HQ)3] was observed at 550 nm (λex = 400 nm) in DMSO solution (Fig. 1). Interestingly, mer-[Al(HQ)3] emits at 525 nm whereas the fac isomer emits at the shorter wavelength of 475 nm.80 Excited state calculations based on energetics, suggested the emission is likely to arise from the S1 state, similar to the experimental findings here, as the triplet T1 state is too low in energy, Table S1.‡
Double hybrid and range-separated functionals predict the S1 state to be a localized, ligand-centred (LC), transition on one ligand (Fig. 7). Whilst B3LYP provides the best agreement with respect to experiment, it shows vastly different character for the S1 state than the other XC functionals, instead predicting S1 to be of ligand–ligand CT (44%) and LC character. A comparison of absorption spectra of [Ga(Br2-HQ)3] in vacuo and in DMSO showed that the solvent causes a blue-shift by ca. 0.2 eV for all tested functionals. In summary, the best theoretical estimate shows that emission in DMSO originates from the S1 state at 539 nm which is a reasonable fit to the experimental emission at 550 nm. DFT calculations showed that mer-[Ga(Br2-HQ)3] is slightly more thermodynamically stable compared to the fac isomer in both DMSO (by ca. 5 to 7 kJ mol−1) and vacuum (by ca. 26 to 30 kJ mol−1), Table S2.‡
Footnotes |
| † This paper is dedicated to Rudi van Eldik on the occasion of his 80th birthday and in celebration of his excellent contributions to inorganic chemistry over many years. |
| ‡ Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5dt00087d |
| This journal is © The Royal Society of Chemistry 2025 |