Modulation of the water exchange rates in [Gd–DO3A] complex by formation of ternary complexes with carboxylate ligands

Silvio Aime *a, Mauro Botta b, James I. Bruce c, Valentina Mainero d, David Parker c and Enzo Terreno a
aDipartimento di Chimica IFM, Università di Torino, Via P. Giuria 7, I-10125, Torino, Italy.. E-mail: aime@ch.unito.it
bDipartimento di Scienze e Tecnologie Avanzate, Università del Piemonte Orientale, ‘Amedeo Avogadro’, C.so Borsalino 54, I-15100, Alessandria, Italy
cDepartment of Chemistry, University of Durham, South Road, Durham, UK DH1 3LE
dLaboratorio Integrato di Metodologie Avanzate, Bioindustry Park Canavese, Via Ribes 5, I-10010, Colleretto Giacosa (TO), Italy

Received (in Cambridge, UK) 29th September 2000 , Accepted 20th November 2000

First published on 15th December 2000


Abstract

Ternary complexes of formula [Gd–DO3A–L–(H2O)] (where L is a carboxylate-containing ligand) display exchange lifetimes of the metal-coordinated water that can be modulated as a function of L.


Paramagnetic Gd(III) chelates are currently under intense scrutiny for their use as contrast agents (CAs) for magnetic resonance imaging (MRI).1 Their efficiency is usually expressed in terms of relaxivity (r1), which represents the relaxation enhancement of the water protons at mmol concentration of the paramagnetic agent. The relaxivity is the result of a complex interplay of several structural, dynamic and electronic parameters. Recently, it has been shown that the exchange lifetime of the coordinated water, τM, may have a key role in determining the relaxivity of a Gd(III) complex.2 In fact,it has been found that τM covers a whole range of values ranging from few ns in the aqua-ion3 up to several μs in complexes of octadentate neutral macrocyclic ligands.4 In systems containing one coordinated water only (q = 1) it has been shown that the exchange process occurs through a dissociative mechanism and the relative exchange rate is dependent upon the energy difference between the nona-coordinate ground state and the octa-coordinate transition intermediate.5 Thus, an increased encumbrance in the ground-state structure results in a smaller energy jump to reach the intermediate state with a consequent increase in the water exchange rate.6 Moreover, it has been found that in DOTA-like systems, the isomer possessing a twisted antiprismatic structure displays an exchange rate of the bound water that is ca. 50 times faster than that observed for the isomer endowed with a more compact square antiprismatic geometry.7,8 Thus, minor structural variations may have remarkable effect on the exchange lifetime of the coordinated water in lanthanide(III) chelates.

As far as the use as CA for MRI is concerned, optimal values of τM for the attainment of high relaxivities [once the Gd(III) is part of a slowly moving macromolecular substrate] fall in the range of few tenths of ns.9 Thus, it is relevant to gain more insight into the structural factors which are responsible of the exchange rate of the coordinated water. Recently, it has been shown that coordinatively unsaturated Gd(III) chelates with q > 1 are able to readily form ternary complexes with suitable ligands such as carboxylates. The formation of such adducts involves the replacement of one or more Gd-bound water molecules by the ligand.10,11 Herein, we show that the mixed complexes [Gd–L–L′–(H2O)], where L is the heptadentate ligand DO3A12 and L′ is a carboxylate-containing ligand, display exchange lifetimes of the metal coordinated water which can be modulated as a function of the added ligand.

The formation of ternary adducts has been followed by analyzing the changes of relaxivity upon L′ concentration. The [Gd–DO3A] complex has a relatively high r1 value (6.0 mM−1 s−1 at 20 MHz and 25 °C14) as the largely dominant isomer13 displays two metal-bound water molecules (average q value = 1.8). Upon adding sodium propionate or L-alanine to a solution of [Gd–DO3A], a progressive decrease of r1 was observed (Fig. 1). This effect is related to the replacement of one Gd-coordinated water molecule by the entering ligand. The fitting of these data according to the PRE (proton relaxation enhancement) theory15 allowed us to estimate either the relaxivities of the ternary complexes, which are consistent for Gd(III) chelates of the expected molecular size and q = 1, or the binding constant between the paramagnetic complex and the ligand (Table 1).



          PRE titration of a 1.15 mM solutions of 
[Gd–DO3A–(H2O)2] with 
l-alanine (■) and sodium propionate (●); 0.235 
Tesla, pH 7, 25 °C.
Fig. 1 PRE titration of a 1.15 mM solutions of [Gd–DO3A–(H2O)2] with L-alanine (■) and sodium propionate (●); 0.235 Tesla, pH 7, 25 °C.
Table 1 Relaxivities, 1∶1 association constants and hydration numbers (q) for [Ln–DO3A–L′–(H2O)] (Ln = Gd or Tb) ternary complexes (20 MHz, 25 °C)
[Gd–DO3A–L′] [Tb–DO3A–L′]
 
L′ r 1/mM−1 s−1 K A/M−1 K A/M−1 q
Propionate 3.7 17 25 1.0
L-Alanine 4.7 19 <50 1.35


As a further check, we evaluated, by luminescence measurements, the metal complex–substrate affinity as well as the hydration state of the resulting mixed complexes. The comparison between the rate constants of the luminescence decay for [Tb–DO3A] adducts in H2O and D2O assures about the presence of a residual lanthanide bound water molecule, whereas by looking at the changes in the intensity of the emission spectra at 545 nm [corresponding to the ΔJ = 1 transition of Tb(III) ion] upon the addition of the substrates, KA values in agreement with those measured by the PRE analysis were obtained (Table 1).

The exchange rate of the metal bound water molecule in this class of paramagnetic complexes may be conveniently determined by measuring the temperature dependence of water 17O-R2p.

In fact, the R2p values are basically a function of q, τM and the electronic relaxation times of the metal ion Tie (i =1,2). Two different regimes can be met, one occurring at low temperatures, in which the changes in R2p are mainly determined by τM (slow exchange region) and one at higher temperatures, essentially dominated by Tie (fast exchange region). For many systems displaying τM in the range of few hundreds of nanoseconds R2p displays a bell-shaped curve (as shown in Fig. 2 for [Gd–DO3A–(H2O)2] at 7.05 T, τM298 = 80 ns). The 17O-R2p values for the ternary complexes [Gd–DO3A–propionate–(H2O)] and [Gd–DO3A–alanine–(H2O)] are significantly smaller than those of the parent chelate owing to the reduction of q in the ternary adduct. Interestingly, the observed behaviour is consistent with the occurrence of a fast exchange of the metal bound water molecule in the case of [Gd–DO3A–propionate–(H2O)] (τM298 = 8 ns). Thus on going from [Gd–DO3A–(H2O)2] to [Gd–DO3A–propionate–(H2O)] there is a considerable shortening of the residence lifetime of the inner sphere water molecule. Furthermore, the observed τM is much shorter than that of [Gd–DOTA–(H2O)] and, interestingly, it is in the range of optimal values for providing the highest relaxivities for MRI applications.9



          
            17O-R2pvs. T of 27.3 
mM solutions of [Gd–DO3A–(H2O)2] 
(◆), 
[Gd–DO3A–propionate–(H2O)]− 
(●), [Gd–DO3A–alanine–(H2O)] (■), 
[Gd–DO3A–α-aminobutyrate–(H2O)] 
(□) and 
[Gd–DO3A–β-aminobutyrate–(H2O)] (○); 
7.1 Tesla, pH 7.
Fig. 2 17O-R2pvs. T of 27.3 mM solutions of [Gd–DO3A–(H2O)2] (◆), [Gd–DO3A–propionate–(H2O)] (●), [Gd–DO3A–alanine–(H2O)] (■), [Gd–DO3A–α-aminobutyrate–(H2O)] (□) and [Gd–DO3A–β-aminobutyrate–(H2O)] (○); 7.1 Tesla, pH 7.

Surprisingly, the profile for the [Gd–DO3A–alanine–(H2O)] adduct displays a different shape, indicative of a longer τM value (τM298 = 180 ns). This may reflect the occurrence of a hydrogen-bonding interaction between the metal bound water molecule and the positively charged α-amino group of the amino-acid, which could also be mediated by a solvent water molecule (Scheme 1).



          Proposed representations of the ternary 
[Ln–DO3A–alanine–(H2O)] adduct. The elongation 
of the residence lifetime of the metal bound water molecule may result from 
the occurrence of the hydrogen bonding network.
Scheme 1 Proposed representations of the ternary [Ln–DO3A–alanine–(H2O)] adduct. The elongation of the residence lifetime of the metal bound water molecule may result from the occurrence of the hydrogen bonding network.

In order to further check this hypothesis 17O-R2pvs. T profiles of the adducts between [Gd–DO3A–(H2O)2] and aminobutyrate anions differing in the position of the protonated amino group were recorded (Fig. 2).

The 17O-R2p values for the adduct with α-aminobutyrate are similar to those of the L-alanine adduct (τM298 = 120 ns). However, when the –NH3+ group is shifted to the β-position, the exchange lifetime decreases significantly (τM298 = 80 ns).

Therefore, these results clearly suggest that the position of the protonated amino group plays a key role for controlling the water exchange rate of the metal bound water molecule.

In summary, though it is difficult to foresee a MRI application for the Gd(III) based ternary complexes investigated in this work, the results here reported indicate a novel route to the modulation of the exchange rate of the coordinated water in Gd(III) complexes. Moreover, one may seek for the formation of ternary complexes between suitably functionalized Gd(III) chelates and endogenous substrates containing carboxylate functionalities.

Acknowledgements

Financial support from MURST and CNR (Biotechnology PF and L. 95/95) is gratefully acknowledged. This work was carried out under the framework of the COST-D18 action.

Notes and references

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