Fernaldo Richtia
Winnerdy‡
a,
Blaž
Bakalar‡
a,
Poulomi
Das‡
a,
Brahim
Heddi
ab,
Adrien
Marchand
c,
Frédéric
Rosu
d,
Valérie
Gabelica
c and
Anh Tuân
Phan
*a
aSchool of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371, Singapore. E-mail: phantuan@ntu.edu.sg
bLaboratoire de Biologie et de Pharmacologie Appliquée, CNRS, Ecole Normale Supérieure Paris-Saclay, Gif-sur-Yvette 91190, France
cLaboratoire Acides Nucléiques: Régulations Naturelle et Artificielle, Université de Bordeaux, Inserm & CNRS (ARNA, U1212, UMR5320), IECB, Pessac 33600, France
dInstitut Européen de Chimie et Biologie, Université de Bordeaux, CNRS & Inserm (IECB, UMS3033, US001), Pessac 33607, France
First published on 26th April 2021
Cations are critical for the folding and assembly of nucleic acids. In G-quadruplex structures, cations can bind between stacked G-tetrads and coordinate with negatively charged guanine carbonyl oxygens. They usually exchange between binding sites and with the bulk in solution with time constants ranging from sub-millisecond to seconds. Here we report the first observation of extremely long-lived K+ and NH4+ ions, with an exchange time constant on the order of an hour, when coordinated at the center of a left-handed G-quadruplex DNA. A single-base mutation, that switched one half of the structure from left- to right-handed conformation resulting in a right–left hybrid G-quadruplex, was shown to remove this long-lived behaviour of the central cation.
Cations are considered an integral part of DNA structures. They interact with and shield the negative charges of the phosphate backbone,15 thus aiding the condensation of DNA structures.16 The residence time of sodium ions around the phosphate backbone was found to be on the nanosecond timescale based on 23Na nuclear relaxation experiments as well as molecular dynamics simulations.17,18 G-quadruplex structures are formed by stacking of square-planar structures, termed G-tetrads, and are highly polymorphic.19–22 Cations have been found within G-quadruplex structures, where they coordinate with the carbonyl oxygens and help stabilize the G-tetrad core.23,24 While some G-quadruplexes do not undergo significant structural changes in various cation solutions,25 structures such as human telomeric G-quadruplexes are particularly sensitive to the cations present in solution.26–36 Cations are either coordinated between stacked G-tetrads or in the plane of a G-tetrad, depending on their respective ionic radius and charge.20,37–39 Previous studies using 15NH4+ ions have shown that they dynamically exchange between binding sites as well as with the bulk ions present in solution.38,40–45 The residence times determined for the coordinated cations span several orders of magnitude, from sub-millisecond,41,42,46,47 millisecond,38,40 to 1.7 seconds, the longest time observed so far.44
The first left-handed G-quadruplex structure (named Z-G4) has been reported for a natural DNA sequence.48 The left-handedness of Z-G4 does not pertain to its stereochemistry, but rather to the base stacking and phosphate backbone progression. While investigating the effects and behaviors of cations in the context of left-handed G-quadruplexes, we unexpectedly found extremely long-lived cations, K+ and/or NH4+, residing inside the channel of the Z-G4 structure, as detected by NMR spectroscopy and mass spectrometry. The idea of G-quadruplexes as targets for therapeutics was described before.49–51 The Z-G4 structure was shown to be specifically recognized by a chiral ligand.52 This work implies a steadfast Z-G4 conformation with respect to time, which may be important for its potential biological functions as an aptamer or drug target. The combination of unique structural features of Z-G4 and long-lasting cations in the channel can be useful in G-quadruplex engineering and nanotechnology.53,54
Spectral assignments of Z-G4 in NH4+ solution were obtained using both site-specific labeling method57 and NOESY spectral analysis (Fig. S3†). NMR spectral analysis indicated that the same G-quadruplex fold (Fig. 1C)—two bi-layered left-handed G-quadruplex blocks (Block1 and Block2)—was preserved in both K+ and NH4+ solutions. This conclusion is also supported by D2O solvent exchange experiments, where only imino protons peaks of inner G-tetrads were preserved (Fig. S2†).
We correlated the coordination positions of the ammonium ions with the neighboring protons by using NOESY and 15N–1H HSQC experiments (Fig. 2). The upfield ammonium ion peak at 6.57 ppm was correlated with a single 15N–1H HSQC cross-peak and had NOE cross-peaks only with the inner G-tetrad imino protons (Fig. 2, cyan line). We concluded that this ammonium ion occupied the inner binding site, between the two blocks of Z-G4 (Fig. 2, cyan sphere). The downfield ammonium ion peak at 6.87 ppm was resolved in 2D experiments, giving rise to two discrete cross-peaks in the 15N–1H HSQC spectrum. Each proton showed eight distinct NOE cross-peaks, four with outer tetrad imino protons and four with inner tetrad imino protons (Fig. 2, purple lines). These results indicated that both downfield ammonium ion peaks are coordinated within the two outer binding sites of the Z-G4 structure (Fig. 2, purple spheres). Based on the imino proton assignments, we determined that O1 corresponds to the ion in Block1 and O2 to the ion in Block2.
A 2D NzEx-HSQC experiment38 with 100 ms mixing time was performed for Z-G4 folded in 15NH4+ at pH 5.1 and 293 K. The introduction of a mixing time allowed the exchange process between the 15NH4+ ions in the binding sites and in solution to be observed via correlation cross-peaks in the NMR spectrum. We observed that the outer ions produced cross-peaks with the bulk 15NH4+ (Fig. S6†). On the other hand, the inner ion did not produce any cross-peaks, with either the outer ions or the bulk 15NH4+, indicating that its exchange time was much longer than the mixing time.41 Further variations of the mixing time and temperature provided us with a rough estimate of the outer ion exchange time with bulk ammonium to be on the order of 100 ms.
To further study this novel behavior of the inner ion, we investigated the exchange between NH4+ and K+ ions. Titration of K+ in a sample containing 100 mM NH4+ revealed three states of the inner ammonium ion, with outer ions being either 2 NH4+, 1 NH4+ + 1 K+, or 2 K+, corresponding to proton peaks at 6.57, 6.53 and 6.49 ppm respectively (Fig. S7†). Note that in the presence of both 100 mM NH4+ and 100 mM K+, the species containing 2 K+ at the outer binding sites predominates, indicating a higher affinity of K+ to these sites.
A sample of Z-G4 was folded in 100 mM 15NH4+ and subsequently dialyzed against H2O for 10 minutes in order to remove most of the bulk 15NH4+ ions in solution. It was flash frozen and lyophilized. In dried condition, the sample was re-suspended in a buffer containing 100 mM K+ ions and immediately tracked with time-series 15N-filtered 1H NMR experiments. The outer 15NH4+ ions were quickly replaced by K+ ions. We observed the area of the inner 15NH4+ peak disappearing with a time constant of τ = (55 ± 1) min (Fig. 3B), which can be attributed to the exchange process of the inner 15NH4+ with K+. Concurrently, the imino proton spectra showed the disappearance of the initial species (NH4+ form) and the appearance of a new species (K+ form) (Fig. S8†). The time constants for the appearance and disappearance of the corresponding imino protons were found to be consistent with that of the decreasing inner ammonium ion peak. These values directly correspond to the residence time of the inner 15NH4+ ion in Z-G4. Any reassociation process of 15NH4+ ion was ruled out due to the huge abundance of bulk K+ counterions, leaving the concentration of released 15NH4+ ions negligible. As a control experiment, 15NH4+ to K+ ion exchange was also performed with the sequence TG4T,58 which forms a tetrameric right-handed G-quadruplex. The results displayed fast exchange of channel ions, further highlighting the uniqueness of the ion with long residence time in Z-G4 (Fig. S9†). This control experiment is also supported by previous ion-exchange experiments on various right-handed G-quadruplexes.41,42,59
To determine the specificity of the unprecedented slow exchange rates towards the type of the ion, we conducted the experiment in reverse. We prepared a sample of Z-G4 folded in K+ then re-suspended it in 100 mM 15NH4+. Over the course of 3 hours, we observed the emergence of two inner ammonium ion peaks (Fig. 3C) corresponding to different configurations of the outer ion occupancies. The peak at 6.53 ppm corresponded to Z-G4 with one of each ion type (15NH4+ and K+) as outer ions, while the peak at 6.49 ppm corresponded to Z-G4 with K+ as both outer ions (Fig. S7†). By tracking the area of both inner ion peaks over time (Fig. 3C) we observed time constants of τ = (49 ± 2) min and τ = (44 ± 2) min respectively. These time constants are slightly shorter than those observed in the previous experiments, where K+ was replacing 15NH4+. In addition, NMR spectrum of Z-G4 at time t = 210 min after resuspension in 15NH4+ solution indicated the presence of multiple conformations (Fig. S10†), corresponding to different combinations of bound ions as observed in 15N-filtered experiments (not shown). This observation is consistent with NH4+ ions having lower affinity to the Z-G4 binding sites compared to K+: in similar experiments K+ can almost fully replace NH4+, while NH4+ can only partially replace K+ at the binding sites of Z-G4. To further support this claim, we performed non-competition-based control experiments, whereby we re-suspended the Z-G4 samples prepared in K+ or 15NH4+ with deionized H2O (Fig. S11†). The results supported the long-lived properties of both ions in Z-G4.
The different estimated values of the NH4+ time constants in the two methods discussed above could be partly attributed to the different ions that were present in each experiment. Previously, adding Na+ to NH4+-containing solvent was shown to accelerate the movements of the NH4+ inside the G-quadruplex channel.59
To probe the structural impact on the long residence time of the inner channel ions, mutation studies of Z-G4 were performed. Mutations that preserve the left-handed G4 structure, such as the sequence 2xBlock2Δ,55 were found to possess similar property of long-lived inner ions (Fig. S12 and S13†). Another mutated sequences, ZG4-T4mod, which has a right–left hybrid G4 conformation (Fig. S14†),60 was unable to fold in NH4+ (Fig. S15†) and thus the K+ to NH4+ ion exchange experiment could not be performed. Hence, we opted to perform mass spectrometry experiments to detect the exchange between the channel 41K+ and bulk 39K+ isotopes (Fig. S16†). The results are further described in the mass spectrometry section.
A sample of Z-G4 was prepared in 10 mM KCl and 90 mM trimethylammonium acetate, heated to 90 °C, slowly cooled to room temperature, and stored for 7 days. A control mass spectrum was recorded by diluting the stock sample to 1 mM KCl and 99 mM TMAA. We detected three specifically bound K+ ions (Fig. 4A). Then, the same stock sample was diluted with ammonium acetate, to final concentrations of 1 mM KCl, 9 mM TMAA and 90 mM NH4OAc, and the spectra were recorded at several time points (Fig. 4B). Within the dead time of the experiment (2 min), two K+ ions were replaced by NH4+ ions. A few extra adducts were observed (total of four cations bound), and these were presumably nonspecific adducts to outer sites (NH4OAc is less good than TMAA to suppress nonspecific adducts).61 We monitored the slow disappearance of the complex with 1 K+ and 2 NH4+ (blue arrow) and the appearance of the complex with 3 NH4+ (red arrow). The distribution of nonspecific adducts was estimated from the time point at 24 h, and this contribution was mathematically subtracted to construct the decay curves (Fig. 4C). The slow emergence of the 3 NH4+ species (τ = 44 min) agrees with our NMR observations where we also observed the fast exchange of the outer ions followed by an extremely slow exchange of the inner ion.
We also checked the gas-phase ion mobilities of the complexes with 3 K+, 1 K+ + 2 NH4+ and 3 NH4+. The arrival time distributions for the ion mobility separation in helium, here converted to collision cross section (CCS) distributions for comparison with theoretical values, were superimposable and relatively narrow, indicating no structural change upon cation replacement. The histogram of calculated CCS values overlaps very well with the experimental distributions (Table S3† and Fig. 4D). The gas-phase simulated structures, obtained by PM7 semi-empirical molecular dynamics, differ from the X-ray crystal structure mainly by: (1) the thymine loop rearrangements and (2) the narrower grooves due to hydrogen bond formation between the partially neutralized phosphate groups. The latter phenomenon, previously described for B-DNA duplexes,62 does not significantly perturb the G-tetrad core of Z-G4 (Fig. S17†).
Mass spectrometry experiments were also performed to compare the K+ → K+ ion exchange process in Z-G4 (left-handed) and its single-base mutated sequence ZG4-T4mod (right–left hybrid). The molecules were initially folded in presence of 41K+ isotopes then were diluted in 39K+ solvent. The results showed that the exchange times for the two outer ions for both constructs were fast, while the inner ions stayed longer for the Z-G4 construct (Fig. S16†). By 25 minutes, almost all the 41K+ inner ions in Z-G4 were still present, while around 50% of the 41K+ inner ions in ZG4-T4mod were already exchanged out. After 3 days, the Z-G4 construct still contained most of its inner 41K+ ions, while ZG4-T4mod construct lost all the inner 41K+ ions. Due to different experimental conditions, the approximation of the residence time of the central cation in this experiment is not to be compared with the NMR results for exchange between K+ and NH4+. However, in relative terms, we observed that the residence time of cations residing in the pure left-handed structure (Z-G4) was much longer compared to the ones in the right-left hybrid structure (ZG4-T4mod). These data show that certain structural features the left-handed G-quadruplex is required for the long residence time of the central ion, as a single-base mutation which affected the left-handed conformation could alter the residence time.
In general, G4 conformations are highly dependent on the presence and type of cations. Crowding conditions and the presence of counterions can affect the stability of G4 structures, with some divalent ions being able to even disrupt the G4 structures entirely.67–71 Therefore, the long-lasting property of the ions in the Z-G4 could potentially be useful in nanotechnology. For example, G-tetrads could be used as the basis for construction of artificial nanopores/ion channels72 and the ability to control the ion residence times might find useful applications.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1sc00515d |
‡ Authors F. R. W., B. B. and P. D. contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2021 |