Lifen
Chen‡
a,
David J.
Hayne‡
*a,
Egan H.
Doeven
a,
Johnny
Agugiaro
b,
David J. D.
Wilson
b,
Luke C.
Henderson
a,
Timothy U.
Connell§
c,
Yi Heng
Nai
a,
Richard
Alexander
a,
Serena
Carrara
b,
Conor F.
Hogan
b,
Paul S.
Donnelly
d and
Paul S.
Francis
*a
aDeakin University, School of Life and Environmental Sciences, Centre for Regional and Rural Futures (CeRRF), Institute for Frontier Materials (IFM), Geelong, Victoria 3220, Australia. E-mail: paul.francis@deakin.edu.au; d.hayne@deakin.edu.au
bDepartment of Chemistry and Physics, La Trobe Institute for Molecular Sciences (LIMS), La Trobe University, Melbourne, Victoria 3086, Australia
cCommonwealth Scientific and Industrial Research Organisation (CSIRO), Clayton, Victoria 3168, Australia
dSchool of Chemistry, Bio21 Molecular Science and Biotechnology Institute, The University of Melbourne, Victoria 3010, Australia
First published on 31st July 2019
Translation of the highly promising electrogenerated chemiluminescence (ECL) properties of Ir(III) complexes (with tri-n-propylamine (TPrA) as a co-reactant) into a new generation of ECL labels for ligand binding assays necessitates the introduction of functionality suitable for bioconjugation. Modification of the ligands, however, can affect not only the photophysical and electrochemical properties of the complex, but also the reaction pathways available to generate light. Through a combined theoretical and experimental study, we reveal the limitations of conventional approaches to the design of electrochemiluminophores and introduce a new class of ECL label, [Ir(C^N)2(pt-TOxT-Sq)]+ (where C^N is a range of possible cyclometalating ligands, and pt-TOxT-Sq is a pyridyltriazole ligand with trioxatridecane chain and squarate amide ethyl ester), which outperformed commercial Ir(III) complex labels in two commonly used assay formats. Predicted limits on the redox potentials and emission wavelengths of Ir(III) complexes capable of generating ECL via the dominant pathway applicable in microbead supported ECL assays were experimentally verified by measuring the ECL intensities of the parent luminophores at different applied potentials, and comparing the ECL responses for the corresponding labels under assay conditions. This study provides a framework to tailor ECL labels for specific assay conditions and a fundamental understanding of the ECL pathways that will underpin exploration of new luminophores and co-reactants.
Fig. 1 (a) The parent luminophore, tris(2,2′-bipyridine)ruthenium(II); and examples of (b) disubstituted33,34 and (c) monosubstituted6,8,35,36 derivatives suitable for bioconjugation. The single binding group separated from the luminophore by an alkyl chain is the approach that has been adopted in commercial ECL systems. Carboxylic acid functionality is common, but other groups, such as amines, maleimides, hydrazides, and phosphoramidites have also been used.37 (d, e) The carboxylic acids are converted to more reactive N-hydroxysuccinimide (NHS) esters for binding to amines (such as lysine units of proteins).35 |
The underlying principles of this detection chemistry were established through an extensive series of investigations that included the inception of ‘co-reactant’ ECL,4 in which the oxidation of a sacrificial species such as tri-n-propylamine (TPrA) forms the chemi-excitation source (Scheme 1a), and the elucidation of an alternative pathway to the excited luminophore (Scheme 1b)5 that has been shown to be the dominant light-producing mechanism within typical ECL-based assays immobilised on microbeads.6,7 ECL labels for bioconjugation were created by adding suitable functional groups to one or both pyridine rings of a single ligand (see Fig. 1), which exert, in this case, only minor influence on the electrochemical and photophysical properties of the luminophore.8
Scheme 1 Co-reactant ECL mechanisms involving (a) electrochemical oxidation the tri-n-propylamine co-reactant (TPrA) and metal complex (M; [Ru(bpy)3]2+), or (b) oxidation of the co-reactant only,5,21 where TPrA+˙ is an aminium radical cation, TPrA˙ is a neural α-amino alkyl radical, and P is its subsequent products. The additional ‘catalytic route’ involving oxidation of TPrA by M+, and an ‘annihilation’ pathway, in which the excited state is generated from the reaction of M+ (from a) with M− (from b), are shown in Scheme S1 in the ESI.† |
Cyclometallated iridium(III) complexes (e.g., Fig. 2a–c) have emerged as promising candidates for a new generation of ECL labels.2,9,10 Compared to the traditional Ru(II) polypyridine chelates, the Ir(III) complexes exhibit much greater quantum yields (offering enhanced analytical performance) and their emission wavelengths and electrochemical potentials can be readily manipulated through changes in ligand structure,11 creating exciting opportunities for multi-colour and/or potential-resolved multiplexed ECL systems.12–15 However, despite more than a decade of exploration of co-reactant ECL of Ir(III) complexes with these goals in mind, the properties of the most promising luminophores have not been effectively translated into ECL labels for the extensive range of possible assays, which we attribute to several major limitations:
Fig. 2 The conceptual development of [Ir(C^N)2(L)]+ complex ECL labels from the early promising examinations of (a) neutral heteroleptic Ir(III) complexes such as Ir(C^N)2(acac), where C^N = 2-phenylpyridine (ppy), 2-phenylbenzo[d]thiazole (bt), 2-phenylisoquinoline (piq) or various other ligands.9,16,17 (b) A representative example of the wider class of cationic [Ir(C^N)2(N^N)]+ complexes, the co-reactant ECL of many of which has also been examined.40,41 (c) More recently reported analogues incorporating a 1-substituted-4-(2-pyridyl)-1,2,3-triazole ligand, which show promising properties for ECL.22,23,29 (d) The most common approach to convert neutral and cationic Ir(III) complexes into ECL labels has been to substitute one ligand for the same bipyridine derivative as that used in Ru(II) labels (see Fig. 1).15,18,19 (e) As with the Ru(II)-based labels shown in Fig. 1, the carboxylic acids are converted to the corresponding NHS esters for binding to amines. (f) The alternative design for ECL labels described herein. |
(1) The available Ir(III) complexes are generally far less soluble in water than [Ru(bpy)3]2+, and so their ECL properties have almost exclusively been evaluated under conditions that are not compatible with common assay formats.9,16,17
(2) Most ligands utilised in Ir(III) complexes do not have readily available derivatives with functional groups suitable for bioconjugation and consequently, very few of the promising Ir(III) complexes have been adapted into labels. Of the few that have been created, the predominant approach has been to replace one ligand with the same bipyridine derivatives that have been used in the [Ru(bpy)3]2+-based labels (e.g., Fig. 2d).15,18,19 However, this appears to limit the range of electrochemical potentials, emission wavelengths and ECL intensities of the complexes.
(3) The two dominant ECL reaction pathways (Scheme 1a and b) elucidated for [Ru(bpy)3]2+ (with TPrA as co-reactant)5 are not necessarily both feasible for all Ir(III) complexes,20 which has implications for their effectiveness under assay conditions. This has not been considered in the previous development of Ir(III)-based ECL labels.
We sought to devise a framework for the development of ECL labels from Ir(III) complex luminophores in which each of the above challenges are addressed. With this in mind, we selected a pyridyltriazole ancillary ligand (Fig. 2c) as the scaffold for the novel ECL labelling complexes. This ligand class exhibits several favourable properties for ECL detection,22–24 including simple ‘click chemistry’ preparation25 that provides a versatile point for derivatisation or attachment.26
De Cola and co-workers have previously explored various [Ir(C^N)2(pt-R)]+ complexes (Fig. 2c; where C^N = ppy or df-ppy, and R = methyl, phenyl, benzyl, adamantyl, β-cyclodextrin and other groups) for photoluminescence,27 light emitting electrochemical cells28 and ECL22 applications. The [Ir(df-ppy)2(pt-R)]+ species exhibited a deeper blue emission than most charged Ir(III) complexes, and intense co-reactant ECL under aprotic and aqueous conditions. Similarly, we have shown that [Ir(df-ppy)2(ptb)]+ (Fig. 2c; C^N = df-ppy; R = Bn) exhibits more intense co-reactant ECL than related blue luminophores Ir(df-ppy)3 and [Ir(df-ppy)2(ptp)]+ (where ptp = 3-phenyl-1,2,4-triazol-5-ylpyridinato) in acetonitrile,23 which we exploited in foundational investigations of multi-colour annihilation ECL.29,30 Using an analogous synthetic strategy, we prepared a highly water-soluble derivative [Ir(df-ppy)2(pt-TEG)]+ (Fig. 2c; C^N = df-ppy; R = tetraethylene glycol (TEG)) that provided more intense co-reactant ECL24,31 and chemiluminescence32 than related Ir(III) complexes in buffered aqueous solution.
Although most prior studies of the ECL of [Ir(C^N)2(pt-R)]+ complexes have focused on developing blue luminophores (such as [Ir(df-ppy)2(ptb)]+; λem = 453, 481 nm),22–24 we have previously observed efficient red photoluminescence (λem = 592, 632 nm) from [Ir(piq)2(ptb)]+ (where piq = 1-phenyl-isoquinoline),38 indicating that the emission of these complexes can be tuned over a wide range via simple modifications to the C^N ligands. Moreover, in our previous development of luminescent Ir(III) complexes for live cell imaging,39 we explored several strategies for their covalent attachment to biomolecules, involving the introduction of maleimide, N-hydroxysuccinimide activated ester, or squarate ethyl ester (Fig. 2f; C^N = ppy or 2-phenylquinoline (pq)) functional groups.
We now draw together these advances to overcome several barriers to the adoption of promising Ir(III)-complex electrochemiluminophores to labelling in binding assays. This includes an in-depth examination of the influence of bioconjugation ligands on Ir(III) complex luminophores, a simple synthetic approach to prepare analogues suitable for organic solvents or aqueous conditions, the creation of novel ECL labels, and the evaluation of the new labels within two common ECL-based assay formats.
To understand these effects, we initially conducted an experimental and theoretical study of the relevant properties of twelve Ir(III) complexes. This included: (i) four commercially available Ir(C^N)2(acac) complexes (Fig. 2a), where C^N = piq, bt, ppy and df-ppy, which exhibit red, yellow, green and blue luminescence, respectively; (ii) four [Ir(C^N)2(dm-bpy)]+ complexes (Fig. 2b; R1 and R2 = Me), with the same C^N ligands, as the parent luminophores of complexes with bpy-based ligands for bioconjugation (Fig. 2e), and (iii) four [Ir(C^N)2(ptb)]+ complexes (Fig. 2c; R = Bn) containing the parent luminophore of the proposed [Ir(C^N)2(pt-TOxT-Sq)]+ labelling complexes. The model luminophores were employed because they were commercially available or readily synthesised and they avoided complications from the reactive peripheral functionality of their labelling derivatives8 when assessing the properties of the luminophore. The [Ir(C^N)2(dm-bpy)]+ and [Ir(C^N)2(ptb)]+ complexes containing piq, ppy and df-ppy ligands have previously been reported,23,28,38,45 but the two bt analogues were prepared in this study for the first time.
The properties of the Ir(C^N)2(acac) complexes (Table S1† and Fig. 3, 4, S1–S6†) were in good agreement with those reported across prior studies.17,46 DFT calculations on Ir(C^N)2(acac) complexes indicate that the HOMO is predominantly localised on the phenyl ring of the C^N ligands and the metal centre, the LUMO is on the C^N ligand (Fig. S7†), and the observed luminescence (Fig. 3) originates from mixed metal-to-ligand and intra-ligand charge transfer (3MLCT/3ILCT) excited states.47 As the acac ligand has minimal direct involvement in the frontier molecular orbitals, trends in spectroscopic and electrochemical properties across the four complexes mirror those of their homoleptic Ir(C^N)3 counterparts.17,23,48
Ir(ppy)2(acac) exhibits green luminescence (Fig. 3a) and the highest LUMO energy of the four complexes, which is reflected in it having the most negative reduction potential (Fig. 4). The electron-withdrawing fluoro substituents of Ir(df-ppy)2(acac) strongly stabilise the HOMO and to a lesser extent the LUMO, with corresponding positive shifts in associated electrochemical potentials and a hypsochromic shift to give its characteristic blue emission. The bt ligand also lowers the energy of the frontier orbitals compared to ppy, but with a slightly lesser effect on the HOMO, resulting in a yellow emission. The resolved band structure in the emission spectrum can be attributed to the greater proportion of the LUMO on the phenyl ring of the C^N ligands. The extended aromaticity of the piq ligand greatly stabilises the LUMO through its low lying π* orbital, but the HOMO energy is relatively unchanged, resulting in a large bathochromic shift in emission.
If the ancillary acac ligand is replaced by dm-bpy, the HOMO is stabilised by ∼0.4 eV (observed as commensurate increases in the oxidation potentials; Fig. 4) but remains located on the metal and C^N ligands (Fig. S7 and Table S6†). The low-lying π* orbital of the dm-bpy ligand, however, is now the dominant contributor to the LUMO of the df-ppy, ppy, and bt complexes, although both the dm-bpy and two piq ligands contribute to the LUMO of the [Ir(piq)2(dm-bpy)]+ complex. This results in a similar reduction potential for all four [Ir(C^N)2(dm-bpy)]+ complexes at −1.83 ± 0.03 V vs. Fc+/0 (Fig. 4). As Ir(ppy)2(acac) has the highest energy LUMO, the influence of the dm-bpy ligand on the emission spectra is most prominent for [Ir(ppy)2(dm-bpy)]+. This changes the order of emission energy from df-ppy > ppy > bt > piq in Ir(C^N)2(acac) complexes (Fig. 3a) to df-ppy > bt > ppy > piq in [Ir(C^N)2(dm-bpy)]+ complexes (Fig. 3b). Moreover, the near identical LUMO energies of the four complexes narrows the difference in their emission wavelengths, reducing the possible selectivity of multi-colour ECL systems.
The HOMOs calculated for the [Ir(C^N)2(ptb)]+ complexes had similar energies to those of their [Ir(C^N)2(dm-bpy)]+ counterparts (Fig. 4), and were again distributed on the metal centre and C^N ligands. The LUMOs, however, were intermediate in energy between those of the Ir(C^N)2(acac) and [Ir(C^N)2(dm-bpy)]+ complexes. The order of emission energies matched that of the Ir(C^N)2(acac) complexes (Fig. 3c). The difference in the λmax between the blue and red emitters is 151 nm (or 140 nm if the highest energy peaks are compared), which is much greater than that of the [Ir(C^N)2(dm-bpy)]+ complexes (71 nm), and similar to that of the Ir(C^N)2(acac) complexes (142 nm).
The red and yellow luminophore Ir(C^N)2(acac) complexes exhibited greater ECL intensities (2.05 and 0.81, vs. [Ru(bpy)3]2+ = 1, see Table S1†) than the green and blue emitters (0.015 and 0.17), but it should be noted that the CCD detector provides a fairly even response across the wavelength range and other commonly used photodetectors (such as photomultiplier tubes) exhibit much greater sensitivity in the blue and green regions. The ECL intensities of the [Ir(C^N)2(dm-bpy)]+ and [Ir(C^N)2(ptb)]+ complexes were distributed over narrower ranges (0.27–0.89 and 0.10–0.43, respectively).
The above characterisations allow us to assess the feasibility of the ECL reaction pathways shown in Scheme 1a and b for these Ir(III) complexes. This is critical, because studies of the ECL of [Ru(bpy)3]2+ with TPrA co-reactant have shown that the conditions of some assays heavily favour one ECL pathway over others.5–7,49 The requirements can be visualised using the graphs shown in Fig. 5a–d,20 in which the electrochemical potential for oxidation and reduction of the metal complex is plotted against the excited state energy (shown as the λmax from low temperature emission spectra).
Fig. 5 (a–d) Redox potentials vs. low-temperature emission wavelengths (λmax) for (a) Ir(C^N)2(acac), (b) [Ir(C^N)2(dm-bpy)]+, (c) [Ir(C^N)2(ptb)]+, and (d) [Ir(C^N)2(pt-TEG)]+, on graphs depicting the redox potential requirements of the ECL mechanisms shown in Scheme 1a and b, indicating which ECL pathway(s) are feasible for each complex. Lines (i)–(iv) show the redox potential requirements for reactions (1)–(4), respectively. (e and f) Normalised ECL intensity during an applied potential sweep from 0 V to 1.8 V and back to 0 V (vs. Ag|AgCl) for (e) [Ir(bt)2(pt-TEG)]+ and (f) [Ir(df-ppy)2(pt-TEG)]+ at 1 μM (blue lines) and 0.1 μM (red lines) in buffer (ProCell) solution containing TPrA as a co-reactant (plots for [Ir(piq)2(pt-TEG)]+ and [Ir(ppy)2(pt-TEG)]+ are shown in ESI†), providing experimental confirmation of the predictions made in (d) under the aqueous conditions commonly used in ECL assays. The concentration of TPrA in the Procell solution is higher than that typically used in comparisons of ECL intensities in buffered aqueous solutions (for example, see Table 1), which will favour the ‘first wave’ of ECL.5 The absence of the first wave in (f) therefore indicates that it will not be observed for this complex with any relevant concentration of TPrA. |
Overlaid on the graphs in Fig. 5a–d are the redox potential requirements of the two ECL pathways. Line (i) is the oxidation potential of TPrA. For complexes with an oxidation potential above this line, reaction (1) is favourable. This ‘catalytic route’5 provides an efficient means to generate TPrA+˙,50 but it is not essential for ECL, because TPrA is also electrochemically oxidised. Line (ii) represents the oxidation potential that the metal complex requires to attain its electronically excited state via reaction (2) (from Scheme 1a). As can be seen in the curve of this line, the energy demands become greater as the emission wavelength becomes shorter (i.e., blue-shifted luminophores must possess higher oxidation potentials to generate ECL viaScheme 1a). This requirement for Scheme 1a, which we referred to in our previous work as the ‘ECL wall of energy sufficiency’,51 was met by all of the metal complexes under investigation.
M+ + TPrA → M + TPrA+˙ | (1) |
M+ + TPrA˙ → M* + P | (2) |
To generate ECL viaScheme 1b, the metal complex must first be able to be reduced by TPrA˙ (reaction (3)) and then react with TPrA+˙ with sufficient excess energy to generate the electronically excited luminophore (reaction (4)). These requirements are met in complexes with a reduction potential above line (iii) and below line (iv) in Fig. 5a–c (i.e., the green coloured region of the graph).
M + TPrA˙ → M− + P | (3) |
M− + TPrA+˙ → M* + TPrA | (4) |
Of the Ir(C^N)2(acac) and [Ir(C^N)2(dm-bpy)]+ complexes (Fig. 5a and b), only the red emitters with piq ligands clearly satisfy the criteria for generating ECL with TPrA viaScheme 1b. It should be noted, however, that there are numerous sources of error in these predictions20 and borderline cases (such as [Ir(bt)2(dm-bpy)]+ and [Ir(ppy)2(dm-bpy)]+) should be treated with caution. Of the [Ir(C^N)2(ptb)]+ complexes, both [Ir(piq)2(ptb)]+ and [Ir(bt)2(ptb)]+ satisfy the criteria for generating ECL viaScheme 1b. Moreover, whilst the data depicted in Fig. 5a–d enable evaluation of which mechanisms are thermodynamically feasible, the intensity of ECL generated through the available pathways is dependent on the efficiency of both excitation (determined by the relative rates of ground and excited state product formation52) and emission (which is equivalent to the photoluminescence quantum yield).
The electrochemical potentials of the [Ir(C^N)2(pt-TEG)]+ complexes matched those of [Ir(C^N)2(ptb)]+ in acetonitrile (Fig. S6†) and the oxidation potentials of the [Ir(C^N)2(pt-TEG)]+ complexes in buffered aqueous solution (vs. Ag|AgCl) exhibited a similar trend (Table 1). The luminescence λmax of [Ir(C^N)2(pt-TEG)]+ in water and [Ir(C^N)2(ptb)]+ in acetonitrile at ambient temperature were near identical, as was their λmax at low temperature in 4:1 ethanol:methanol (Fig. S4 and S5,†Tables 1 and S1†). The ECL intensities of the [Ir(C^N)2(pt-TEG)]+ complexes in buffered aqueous solution, however, were greater than those of [Ir(C^N)2(ptb)]+ in acetonitrile, relative to that of [Ru(bpy)3]2+ under each set of conditions.
Photoluminescence | Electrochemical potentials | ECL | ||||||
---|---|---|---|---|---|---|---|---|
λ max , /nm | λ max , (85 K)/nm | E 0–0 /eV | ϕ PL (%) | E ox /V (vs. Ag|AgCl) | E ox /V (vs. Fc+/0) | E red /V (vs. Fc+/0) | I ECL | |
a Metal complexes at 10 μM in water at ambient temperature. b Corrected for the change in instrument sensitivity over the wavelength range. c Metal complexes at 5 μM in ethanol:methanol (4:1) at 85 K. d Energy gap between the zeroth vibrational levels of the ground and excited states, estimated from the highest energy peak of the low-temperature emission spectrum. e Photoluminescence quantum yield in ‘ProCell’ phosphate buffer used in commercial ECL instruments. f Metal complexes at 0.5 mM in 0.1 M phosphate buffer solution (pH 7.5); squarewave voltammetry; 5 mV step, 0.02 amplitude, 25 Hz. g Metal complexes at 0.25 mM in acetonitrile with 0.1 M TBAPF6; cyclic voltammetry; scan rate: 0.1 V s−1. h ECL intensities relative to [Ru(bpy)3]2+ (10 μM metal complex in phosphate buffer (pH 7.5) with 10 mM TPrA; 10 s pulse, 10 Hz). | ||||||||
[Ru(bpy)3]2+ | 625 | 581, 629 | 2.13 | 3 | 1.09 | 0.89 | −1.73, −1.92, −2.15 | 1 |
[Ir(piq)2(pt-TEG)]+ | 596, 628 | 580, 629, 684 | 2.14 | 9 | 1.15 | 0.86 | −2.01, −2.23 | 0.86 |
[Ir(bt)2(pt-TEG)]+ | 526, 562 | 515, 557, 604, 659 | 2.41 | 23 | 1.28 | 1.01 | −2.08 | 2.76 |
[Ir(ppy)2(pt-TEG)]+ | 475, 505 | 471, 506, 536 | 2.63 | 14 | 1.08 | 0.86 | −2.20 | 1.57 |
[Ir(df-ppy)2(pt-TEG)]+ | 452, 481 | 448, 480, 507 | 2.77 | 19 | 1.44 | 1.20 | −2.13 | 0.26 |
Due to the similar properties of the [Ir(C^N)2(ptb)]+ and [Ir(C^N)2(pt-TEG)]+ complexes, the same predictions (Fig. 5d) were made for the feasibility of the two ECL reaction mechanisms (Scheme 1a and b), where [Ir(piq)2(pt-TEG)]+ and [Ir(bt)2(pt-TEG)]+ are anticipated to generate ECL (with TPrA co-reactant) via both pathways, whereas [Ir(ppy)2(pt-TEG)]+ and [Ir(df-ppy)2(pt-TEG)]+ are limited to Scheme 1a. We sought validation for these predictions using the ‘two-wave’ ECL experiment utilised by Bard and co-workers5 in their elucidation of Scheme 1b for [Ru(bpy)3]2+, in which the ECL intensity is monitored during a voltammetric sweep from low to high anodic potentials. Scheme 1b is initiated at the oxidation potential for TPrA, whereas Scheme 1a also requires electrochemical oxidation of the metal complex, which in the case of the [Ir(C^N)2(pt-TEG)]+ complexes, occurs at considerably higher potentials (Fig. 5d).
The two ‘waves’ of ECL intensity corresponding to the oxidation of TPrA and the metal complex (Table 1) for [Ir(bt)2(pt-TEG)]+ (Fig. 5e) and [Ir(piq)2(pt-TEG)]+ (Fig. S8b†), and the single wave of ECL associated with the oxidation of [Ir(df-ppy)2(pt-TEG)]+ (Fig. 5f) and [Ir(ppy)2(pt-TEG)]+ (Fig. S8a†) in aqueous buffered solution support the prediction made for each complex based on electrochemical potentials and emission energies. Bard and co-workers observed that a lower concentration of [Ru(bpy)3]2+ favoured the first wave of ECL (viaScheme 1b), which we also observed for [Ir(bt)2(pt-TEG)]+ (Fig. 5e) adding further evidence of the competing ECL pathways of this complex.
We note here that interpretation of ECL intensity profiles during voltammetric experiments without considering the energy requirements of the competing ECL pathways (as depicted in Fig. 5a–d) can be misleading, as other factors can contribute. The ECL of Ir(ppy)3 with TPrA, for example, is strongly inhibited at high over-potentials,13,14 which has been attributed to oxidative quenching of the excited state Ir(ppy)3* by TPrA˙+. Moreover, De Cola and co-workers16 observed more than two maxima in the ECL of Ir(pph)2(pic) (where pph = phenylphenanthridine; pic = picolinate) and TPrA, which is yet to be understood.
ECL labela | Photoluminescence | Electrochemical potentials | |||
---|---|---|---|---|---|
λ max , /nm | ϕ PL , (%) | τ , /ns | E ox /V (vs. Fc+/0) | E red /V (vs. Fc+/0) | |
a The chemical structure of [Ru(bpy)2(mbpy-COOH)]2+ is shown in Fig. 1c; the [Ir(C^N)2(mbpy-COOH)]+ labels are depicted by Fig. 2d, except that the piq complex does not contain the 4-methyl group, and the bt complex contains a 4′-carboxy instead of 4′-carboxypropyl group on the bpy-based ligand (due to the availability of the different commercial labels at the time of the study); and the [Ir(C^N)2(pt-TOxT-Sq)]+ labels are depicted by Fig. 2f. b The ECL labels were dissolved in DMF (1 mM) and diluted to 10 μM in a 0.1 M PBS solution (pH 7.4). c Corrected for the change in instrument sensitivity over the wavelength range. d Photoluminescence quantum yield. e Emission lifetime; excitation wavelength at 344 nm or 451 nm using Nanoled light sources. f ECL labels at 0.25 mM in acetonitrile with 0.1 M TBAPF6; cyclic voltammetry; scan rate: 0.1 V s−1. Peaks associated with the counter ion or labelling functional group not listed. | |||||
[Ru(bpy)2(mbpy-COOH)]2+ | 632 | 4.9 | 311 | 0.84 | −1.78, −1.96, −2.24 |
[Ir(piq)2(bpy-COOH)]+ | 592(sh), 640 | 10.4 | 378 | 0.85 | −1.90, −2.17 |
[Ir(bt)2(mbpy-COOH)]+ | 530(sh), 572, 615(sh) | 5.9 | 174 | 1.04 | −1.87, −2.28 |
[Ir(ppy)2(mbpy-COOH)]+ | 606 | 2.0 | 398 | 0.84 | −1.87 |
[Ir(df-ppy)2(mbpy-COOH)]+ | 533 | 2.7 | 392 | 1.16 | −1.84, −2.49 |
[Ir(piq)2(pt-TOxT-Sq)]+ | 590(sh), 632 | 11.8 | 927 | 0.87 | −2.01, −2.22, −2.56 |
[Ir(bt)2(pt-TOxT-Sq)]+ | 526, 564 | 26.7 | 1051 | 1.01 | −2.11, −2.35, −2.56 |
[Ir(ppy)2(pt-TOxT-Sq)]+ | 476, 503 | 8.8 | 308 | 0.86 | −2.22 |
[Ir(df-ppy)2(pt-TOxT-Sq)]+ | 453, 483, 515 | 15.7 | 559 | 1.16 | −2.14 |
As a proof-of-concept demonstration of the influence of the electrochemical and spectroscopic properties on the ECL of Ir(III) complexes in the context of the reaction pathways available to each luminophore, we compared the relative ECL intensities of the bioconjugated [Ir(C^N)2(pt-TOxT-Sq)]+ and [Ir(C^N)2(mbpy-COOH)]+ labels in two different modes of binding assay (Fig. 6). The first was a sandwich hybridisation RNA assay on magnetic bead support, and the second was a C-reactive protein (CRP) sandwich immunoassay with the capture monoclonal antibody (mAb) immobilised on a gold electrode.
In the sandwich RNA hybridisation assay, the target was mixed with capture probe-functionalised magnetic beads (2.8 μm diameter, streptavidin coated) and a detection probe with ECL label attached, and heated to 45 °C for 15 min. The beads were then washed, resuspended in ProCell solution (a phosphate buffer enriched with TPrA and various surfactants with a confidential specific chemical composition, which was specially designed and optimised for ECL assays in commercial systems), and dispersed above a screen-printed electrode in a custom-made holder (Fig. S10†) containing a magnet to move the beads to the electrode surface. The ECL was initiated by applying 1.4 V vs. Ag|AgCl at the working electrode for 10 s and measured using a silicon photomultiplier detector (Fig. S11†).
Bard and co-workers' elucidation of an alternative ECL reaction pathway of the [Ru(bpy)3]2+ luminophore with TPrA co-reactant5 revealed Scheme 1b as the dominant light-producing pathway of the magnetic bead-supported assays used in commercial ECL instruments. In these assays, only an infinitesimal fraction of ECL-labels are held within the nanometric electron tunnelling distance from the electrode surface required for their direct oxidation (required for Scheme 1a).5,7,54 Diffusion of the TPrA radicals, however, allows excitation via homogeneous electron transfer to the [Ru(bpy)3]2+ luminophores (Scheme 1b) at much greater (micrometric) distances from the electrode surface.
Based on the above considerations of the parent luminophores of the ECL labels (Fig. 5), the reaction pathway depicted in Scheme 1b should only be feasible for the novel red and yellow emitters ([Ir(piq)2(pt-TOxT-Sq)]+ and [Ir(bt)2(pt-TOxT-Sq)]+) and the commercial red emitter ([Ir(piq)2(bpy-COOH)]+).
As shown in Fig. 7a, comparison of the ECL signal-to-blank (S/B) ratios for the different labels for the same target RNA concentration and assay conditions shows that these labels gave the greatest response. The commercial bt analogue, for which the parent luminophore was considered a borderline case (Fig. 5b), also showed a minor response. The two [Ir(C^N)2(pt-TOxT-Sq)]+ labels gave superior S/B ratios than their commercial counterparts, but the response with [Ir(piq)2(pt-TOxT-Sq)]+ was still 3-fold poorer than that of [Ru(bpy)2(mbpy-COOH)]2+.
For the [Ir(piq)2(pt-TOxT-Sq)]+, [Ir(bt)2(pt-TOxT-Sq)]+, [Ir(piq)2(bpy-COOH)]+ and [Ru(bpy)2(mbpy-COOH)]2+ labels, the reactions depicted in Scheme 1b are exergonic, but considerable variation in ECL responses were observed in the RNA assay due to differences in the efficiencies of (i) excitation (dependent on the relative rate of reactions leading to the excited state in addition to various ‘dark’ reactions), and (ii) emission (which can be estimated from the photoluminescence quantum yield, although the excited state may also be vulnerable to quenching from reactive oxidation products of the co-reactant in some cases13).
As the quantum yield of the labels decreased in the order: [Ir(bt)2(pt-TOxT-Sq)]+ > [Ir(piq)2(pt-TOxT-Sq)]+ > [Ir(piq)2(bpy-COOH)]+ > [Ru(bpy)2(mbpy-COOH)]2+ (Table 2), the excitation efficiency appears to be the dominant factor. It is therefore not surprising that most Ir(III) complexes reported to exhibit the greatest ECL intensities to date have exhibited red luminescence and reduction potentials that would place them in the same regions of Fig. 5 as the [Ru(bpy)3]2+ complex, even though they were not evaluated under bead-based assay conditions that would limit the ECL pathway to that depicted in Scheme 1b. Examples include Ir(pq)2(acac) (λem = 609 nm, E0′ = 0.57 V and −2.05 V vs. Fc+/0),40 Ir(pph)2(pic) (λem = 649 nm, E0′ = 0.61 V and −1.94 V vs. Fc+/0),16 and [Ir(dmpq)2(mbpy-COOH)]+ (λem = 590 nm, E0′ = 0.78 V and −1.66 V vs. Fc+/0),19 where dmpq = 2-(3,5-dimethylphenyl)quinoline.
For assays in which the Ru(II)/Ir(III) complex luminophore can diffuse to the electrode or is immobilised in very close proximity to the electrode surface, co-reactant ECL with TPrA is feasible viaScheme 1a (with possible involvement of Scheme S1a†), but only if a sufficient potential is applied to oxidise the metal complex, and the reaction between the oxidised complex and TPrA˙ is sufficiently exergonic to populate the excited state responsible for emission (reaction (2)). As illustrated by Fig. 5a–d, all metal complexes examined in this study meet this requirement. The potentials required to oxidise these metal complexes are generally greater than that for TPrA, and so the pathway depicted in Scheme 1b (and Scheme S1b†) may also contribute to the overall ECL intensity for complexes meeting its requirements (described above).
In our second assay, the capture antibody was covalently immobilised on a monolayer of 16-mercaptohexadecanoic acid on a gold electrode, which was incubated with the target CRP and then the detection antibody. The electrode was then introduced to an electrochemical cell containing ProCell solution and the ECL was initiated using a voltammetric sweep (0.05 V s−1) from +0.5 V to +1.5/1.6 V (vs. Ag|AgCl) and measured using a photomultiplier tube (S20 multi-alkali photocathode) module. The ECL labels in this assay are much closer to the electrode than the vast majority of those in the bead-based approach, but still outside the typical electron tunnelling region.5,54 O'Reilly et al.,55 however, showed that the dominant ECL mechanism of a similar assay (CRP by sandwich immunoassay; capture antibody absorbed on a Pt electrode; detection antibody with an [Ru(bpy)2(N^N)]2+-type ECL label) involved oxidation of the label (Scheme 1a) and the catalytic oxidation of TPrA (Scheme S1a†). As noted by the authors,55 electron hopping between ECL luminophores49,54 is unlikely in this system due to their relatively low concentration, but multi-step electron transfer through proteins via their redox active side chains is well known.56
As shown in Fig. 7b, comparison of the ECL signal-to-blank (S/B) ratios for the different labels under the same CRP assay conditions shows that the two blue emitter labels ([Ir(df-ppy)2(pt-TOxT-Sq)]+ and [Ir(df-ppy)2(mbpy-COOH)]+), which both require oxidation to generate ECL, gave the greatest response. Moreover, the S/B ratio for the novel [Ir(df-ppy)2(pt-TOxT-Sq)]+ ECL label was only 15% lower than that of [Ru(bpy)2(mbpy-COOH)]2+.
For the characterisation of [Ir(C^N)2(pt-TOxT-Sq)]+ and other ECL labels, the complexes were dissolved in DMF (1 mM) and diluted to 10 μM in a 0.1 M PBS solution (pH = 7.4). Steady-state emission spectra were collected on a Nanolog (HORIBA Jobin Yvon IBH) spectrofluorometer. A 450 W xenon-arc lamp was used to excite the complexes using a 1200 g mm−1 grating blazed at 330 nm excitation monochromators, a 1200 g mm−1 grating blazed at a 500 nm emission monochromator, and a thermoelectrically cooled TBX picosecond single-photon detector. Emission and excitation spectra were corrected for source intensity, gratings, and detector response. Lifetimes were measured using the time correlated single photon counting (TCSPC) option on the spectrometer and correlated by a time-to-amplitude converter (TAC) in forward TAC mode. A Nanoled laser (λex = 344 nm or 451 nm) was pulsed at 100 kHz, signals were collected using a FluoroHub counter and the data was analysed using DAS6 software (HORIBA Jobin Yvon IBH). Spectra for absolute quantum yields were measured at room temperature (22 ± 2 °C) with a Quanta-phi HORIBA Scientific 6 in. diameter integrating sphere connected to the Nanolog via optical fibres. The complexes were excited using a 450 W xenon lamp and detected with a liquid nitrogen cooled Symphony II (Model SII-1LS-256−06) CCD.
Adaption of promising Ir(C^N)2(acac) complexes for ECL labelling through the common approach of replacing the ancillary ligand with 2,2′-bipyridine derivatives introduces a low-lying π* LUMO that contracts the spread of emission colours over a series of complexes, which will be detrimental for multi-colour applications. The change is most prominent in complexes with the furthest negative reduction potentials (i.e., the highest LUMO energies). Of the Ir(C^N)2(acac) complexes examined in this study, this was the ppy complex, and the change in ancillary ligand to dm-bpy visibly switched the order of emission energies with the Ir(bt)2(acac) complex. These effects can be largely ameliorated with alternative ancillary ligands such as pyridyltriazole ligands, which are prepared by simple click chemistry procedures to access more water-soluble analogues and functionality suitable for labelling, without significant modification to the properties of the luminophore.
Graphical representations of the key energy requirements of the competing ECL reactions elucidated for the [Ru(bpy)3]2+ complex with TPrA as a co-reactant show fundamental limits on the redox potentials and emission wavelengths of complexes that can generate ECL through a mechanism involving oxidation of only the TPrA co-reactant (Scheme 1b). Most importantly in the context of developing multi-colour ECL systems, the ‘window’ of reduction potentials enabling this pathway becomes narrower as emission energy increases, and it does not extend across the entire visible region. Plotting the redox potentials and (low-temperature) emissions of the Ir(III) complexes on these graphs enables simple prediction of the feasible ECL pathways, which for the [Ir(C^N)2(pt-TEG)]+ complexes was supported by the relative ECL intensity at different applied potentials under aqueous conditions relevant to binding assays.
The practical outcome of this limitation is seen in the bead-based assay, in which only some of the Ir(III) complexes (those for which Scheme 1b is feasible) result in a significant ECL signal for the target analyte. This provides the simplest experimental verification of Bard and co-workers' reasoning5 (supported by a range of experiments and simulations by other groups7,54,67) of the dominant ECL reaction pathway for bead-based assays using [Ru(bpy)3]2+ with TPrA as co-reactant. Examination of a greater range of electrochemiluminophores with this approach will enable the energy boundaries (carrying considerable error due to the difficulty in establishing the redox potentials of TPrA and TPrA˙) to be clarified. Moreover, this approach will be valuable for the evaluation of alternative co-reactants in conjunction with various metal complexes (which may provide an analogous pathway to Scheme 1b for ECL in the blue region of spectrum), as previous studies68 have predominantly focused on [Ru(bpy)3]2+, and not under bioconjugated assay conditions. Assays in which the metal complex can diffuse to the electrode surface, or is immobilised within a few nanometres of the electrode, or where electrons can be transferred over greater distances from the metal complex to the electrode, are not subject to the above limitations. In these cases, the effectiveness of the label is defined only by the efficiency of its excitation and emission under the specific assay conditions, and the relative sensitivity of the photodetector towards that luminophore.
The novel [Ir(C^N)2(pt-TOxT-Sq)]+ ECL labels were obtained through a more convenient and versatile synthetic approach and provided superior ECL responses to the commercial [Ir(C^N)2(mbpy-COOH)]+ analogues in both assays. In both assays, the ECL was less intense than that of the conventional [Ru(bpy)2(mbpy-COOH)]2+ label, but assay conditions have been optimised specifically for the [Ru(bpy)3]2+-based labels since the inception of the technique, and there is considerable scope to improve the relative performance of the Ir(III) complex labels, in areas such as TPrA concentration and electrochemical pulse time.17 Despite a few alternative co-reactants providing greater ECL intensities with [Ru(bpy)3]2+ under specific conditions, TPrA remains the ‘gold standard’ co-reactant for ECL assays. Other co-reactants, however, may provide superior ECL performance from various Ir(III) complexes. Finally, the ability through DFT calculations to predict the influence of changes in ligand structure on the redox and luminescence character of the complex, and consider these changes with respect to the energy requirements of various ECL pathways, will enable the design of superior Ir(III) complex ECL labels with specific emission colours and targeting different reaction pathways.
Footnotes |
† Electronic supplementary information (ESI) available: Synthesis and characterisation of ligands, Ir(III) complexes and ECL labels. Additional data: absorption and emission spectra; cyclic voltammograms; tabulated spectroscopic and electrochemical properties in acetonitrile; calculated MO energies, contributions to the respective MOs, and contour plots; primers and NASBA amplicon fragment sequences. See DOI: 10.1039/c9sc01391a |
‡ These authors contributed equally. |
§ Present address: RMIT University, Melbourne, Victoria 3001 Australia. |
¶ Commercial sources of chemicals: tris(2,2′-bipyridine)ruthenium(II) hexafluorophosphate ([Ru(bpy)3](PF6)2) and tetrabutylammonium hexafluorophosphate (TBAPF6; electrochemical grade) were purchased from Sigma-Aldrich (NSW, Australia). Tris(2,2′-bipyridine)ruthenium(II) chloride hexahydrate ([Ru(bpy)3]Cl2·6H2O) and bis(cyclopentadienyl)iron (ferrocene; Fc) were purchased from Strem Chemicals (MA, USA). The four Ir(C^N)(acac) complexes and five ECL labels (bis(2,2′-bipyridyl)(4-methyl-4′-carboxypropyl-2,2′-bipyridyl)ruthenium(II) hexafluorophosphate ([Ru(bpy)2(mbpy-COOH)](PF6)2), bis(4,6-difluoro-2-(2-pyridyl)phenyl-C2,N)(4-methyl-4′-carboxypropyl-2,2′-bipyridyl)iridium(III) chloride ([Ir(df-ppy)2(mbpy-COOH)]Cl), bis(2-phenylpyridine-C2,N)(4-carboxypropyl-2,2′-bipyridyl)iridium(III) hexafluorophosphate ([Ir(ppy)2(mbpy-COOH)](PF6)), bis(2-phenylbenzothiazole-C2,N)(4-methyl-4′-carboxy-2,2′-bipyridyl)iridium(III) chloride ([Ir(bt)2(mbpy-COOH)]Cl), bis(1-phenylisoquinoline)(4-methyl-4′-carboxypropyl-2,2′-bipyridyl)iridium(III) chloride ([Ir(piq)2(bpy-COOH)]Cl)) were purchased from SunaTech (Jiangsu, China). |
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