Highly fluorescent guanosine mimics for folding and energy transfer studies.

Guanosines with substituents at the 8-position can provide useful fluorescent probes that effectively mimic guanine residues even in highly demanding model systems such as polymorphic G-quadruplexes and duplex DNA. Here, we report the synthesis and photophysical properties of a small family of 8-substituted-2'-deoxyguanosines that have been incorporated into the human telomeric repeat sequence using phosphoramidite chemistry. These include 8-(2-pyridyl)-2'-deoxyguanosine (2PyG), 8-(2-phenylethenyl)-2'-deoxyguanosine (StG) and 8-[2-(pyrid-4-yl)-ethenyl]-2'-deoxyguanosine (4PVG). On DNA folding and stability, 8-substituted guanosines can exhibit context-dependent effects but were better tolerated by G-quadruplex and duplex structures than pyrimidine mismatches. In contrast to previously reported fluorescent guanine analogs, 8-substituted guanosines exhibit similar or even higher quantum yields upon their incorporation into nucleic acids (Φ = 0.02-0.45). We have used these highly emissive probes to quantify energy transfer efficiencies from unmodified DNA nucleobases to 8-substituted guanosines. The resulting DNA-to-probe energy transfer efficiencies (η(t)) are highly structure selective, with η(t)(duplex) < η(t)(single-strand) < η(t)(G-quadruplex). These trends were independent of the exact structural features and thermal stabilities of the G-quadruplexes or duplexes containing them. The combination of efficient energy transfer, high probe quantum yield, and high molar extinction coefficient of the DNA provides a highly sensitive and reliable readout of G-quadruplex formation even in highly diluted sample solutions of 0.25 nM.

INTRODUCTION

From the early days of structural biology, DNA was recognized as having the ability to adopt alternate folds (1). In addition to A-, B- and Z-form double helices, DNA can fold into a variety of hairpin, triplex, G-quadruplex and i-motif structures that contain non-canonical base pairs (2,3). While the exact biological relevance of these structures remains an open question, DNA sequences with the ability to fold into G-quadruplex structures have been implicated in regulating gene transcription (4–6), recombination (7), chromosome stability (8–10) and programmed cell death (11). In all cases, open questions still remain about the exact folding pathways and biologically active conformation(s) of these DNA sequences (12).

A wide variety of biophysical techniques have been used to characterize DNA folding in vitro. These include NMR (13–15), circular dichroism (CD) (16), UV absorption (17,18), X-ray crystallography (19), FRET (20–22) and immunostaining (23). Most of these methods require pure DNA samples and are not compatible with conformational analyses in living cells. While fluorescence spectroscopy has the potential for conformational analyses in vivo, techniques involving high-affinity fluorescent probes or DNA molecules conjugated to large fluorescent tags can perturb the structure and/or stability of the DNA itself (21,24,25). Further development of fluorescence-based methods is needed to provide highly sensitive, non-perturbing tools to characterize DNA folding in vitro and in vivo. Due to their small size and predictable location, internal fluorescent probes offer some advantages over linker-attached chromophores, such as the ability to report subtle structural changes with single nucleotide resolution (26–29).

Modification of the 8-position of guanosine is an attractive avenue to fluorescent derivatives because it is not directly involved in base-pairing interactions within G-quadruplex or duplex structures (R2, Figure 1A). Derivatization of this position can generate fluorescent products (Figure 1B) (30–34) with emission properties that are sensitive to DNA folding (34). While the addition of bulky groups to the 8-position of guanosine can shift the conformational equilibrium of the glycosidic bond from ‘anti’ to ‘syn’ (35–38), DNA folding can force 8-modified guanosines to adopt anti conformations with relatively small energetic penalties to DNA folding (ΔΔG ≤ 1 kcal mol−1) (37,38).

Figure 1.

(A) Structures and numbering of 8-substituted-2′-deoxyguanosines and an ion-containing G-tetrad (gray). (B) Wavelengths of maximal absorbance (λabs) and emission (λem) in water, and quantum yield (Φ) of each nucleoside in acetonitrile, water or D2O.

We recently reported 8-(2-pyridyl)-2′-deoxyguanosine ‘2PyG’ (Entry 2, Figure 1B) as a ‘turn-on’ fluorescence probe of G-quadruplex folding and energy transfer (34). Upon its incorporation into G-tetrads, 2PyG was minimally disruptive to intramolecular G-quadruplex folding where it exhibited higher quantum yields (Φ = 0.04–0.15) than the corresponding nucleoside () in water (Φ = 0.02). Using 2PyG, we discovered efficient energy transfer reactions involving unmodified guanosines in G-quadruplex structures (DNA-to-probe energy transfer efficiency, ηt = 0.11–0.41) that depended on the presence and identities of cations coordinated to the O6 positions of the guanine residues. It was unclear from these studies, however, if the reported intramolecular energy transfer reactions resulted from unusual intrinsic properties of G-quadruplexes, the unusual photophysical characteristics of 2PyG, or some combination thereof. To help address this question, we have synthesized oligonucleotides containing 8-(2-phenylethenyl)-2′-deoxyguanosine (StG) and 8-[2-(pyrid-4-yl)-ethenyl]-2′-deoxyguanosine (4PVG, Figure 1B) and evaluated their ability to report DNA folding and internal energy transfer reactions in G-quadruplex, single-stranded and duplex structures derived from the human telomeric repeat sequence. As compared to 2PyG, both of the vinyl-bridged derivatives 4PVG and StG exhibit red-shifted excitation and emission maxima, lower potentials for perturbing DNA structure, and higher quantum yields (Φ = 0.03–0.44) in the context of folded DNA. For all three 8-substituted guanosines, DNA-to-probe energy transfer efficiencies were much higher in G-quadruplex structures (ηt = 0.12–0.30) than the same oligonucleotides folded into B-form duplexes (ηt = 0.02–0.06). The unusual photophysical properties of cation-containing G-quadruplexes are therefore responsible for the efficient energy transfer reactions within these structures (34). These phenomena together provide a reliable and highly sensitive means for deciphering the folded state of the DNA (duplex versus quadruplex) even in highly diluted sample solutions of ≤250 pM.

MATERIALS AND METHODS

Synthesis of 8-substituted-2′-deoxyguanosine nucleosides and phosphoramidites

The 2PyG nucleoside () and corresponding β-cyanoethyl phosphoramidite were synthesized according to published procedures (34). The phosphoramidites of 8-(2-phenylethenyl)- and 8-[2-(pyrid-4-yl)-ethenyl]-2′-deoxyguanosine were synthesized according to Scheme 1. The 8-bromo-O6-protected-2′-deoxyguanosine derivative 6 is a highly versatile intermediate for palladium catalyzed cross-coupling reactions including Suzuki, Stille and Heck. The 8-(2-phenylethenyl)-derivative 7 was synthesized by Suzuki–Miyaura cross-coupling of 6 with commercially available trans-styryl boronic acid pinacol ester to yield the trans isomer of 7. The analogous pyridine derivative 9, was made by first preparing the vinyl derivative 8 via Stille coupling of 6 with tributyl(vinyl) tin, followed by addition of the pyridine group via Heck coupling. The resulting trans derivatives 7 and 9 were deprotected with tetrabutylammonium fluoride (TBAF) to furnish free nucleosides (3 and 4, Figure 1B), or they were carried forward into phosphoramidite synthesis using standard methodologies for N(2) protection with isobutyryl chloride (10 and 11), followed by deprotection with TBAF (12 and 13) and the addition of dimethoxytrityl to the 5′OH groups (14 and 15). The detailed synthetic procedures and characterization of these intermediates are available in the supporting information. Slightly different procedures were needed for introducing the cyanoethyl phosphoramidite on the 3′OH of each compound (16 and 17). In the case of 17, a base catalyzed reaction with 2-cyanoethyl diisopropylchloro phosphoramidite was successful, while compound 16 was prepared by an acid catalyzed reaction of 14 with 2-cyanoethyl tetraisopropyl phosphordiamidite by 5-ethylthio-(1 H)-tetrazole. All new compounds were characterized by NMR and mass spectrometry (Supplementary Data), except for compound 16 that was carried directly into oligonucleotide synthesis without isolation (39).

Scheme 1.

Synthesis of the 8-(substituted)-2′-deoxyguanosine phosphoramidites 16 and 17.

Oligonucleotide synthesis

Modified oligonucleotides were synthesized on a 1-µmol scale using a Millipore Expedite 8909 DNA synthesizer according to the standard Trityl-off procedure, except that 5% dichloroacetic acid in CH2Cl2 was used for Trityl deprotection. Manual coupling reactions were used for the site-specific introduction of 16 and 17 into oligonucleotides. These phosphoramidites (0.02 mmoles) were dissolved into 200 µl of 0.25 M 5-ethylthio-(1 H)-tetrazole in dry acetonitrile and added to DNA columns via syringe for 10 min. Upon completion of each sequence, oligonucleotides were cleaved from the solid support and deprotected by treatment with 1.5 ml of 33% aqueous ammonium hydroxide at 55°C for 17 h in a 1.7-ml screw-top cap tube. The resulting products were dried, dissolved into water and purified by using C-18 reversed phase HPLC with a mobile phase of 0.1 M triethyl ammonium acetate (pH 7) and acetonitrile. Following lyophilization, oligonucleotide stock solutions were prepared in pure water and quantified using ε(260 nm) = 244 300 cm−1M−1. MALDI-TOF MS hTeloG9: G9 = StG (m/z) calcd, 7676.4; found 7684.5; G9 = 4PVG (m/z) calcd, 7677.4; found 7680.4; hTeloG23: G23 = StG (m/z) calcd, 7676.4; found 7678.4; G23 = 4PVG (m/z) calcd, 7677.4; found 7677.8. The synthesis and characterization of the 2PyG-containing oligonucleotides were reported elsewhere (34). See Supplementary Figures S1–S6 for analytical HPLC chromatograms and MALDI-MS spectra.

DNA folding and buffer conditions

Duplex DNA samples were prepared in the presence of 100 mM NaCl and 1.1 equivalents of the complementary strand. G-quadruplex structures were prepared from single-stranded oligonucleotides in 100 mM of NaCl or KCl-containing buffers. Unfolded, single-stranded DNAs were prepared in 100 mM LiCl. Buffers were prepared as 10 mM cacodylic acid solutions containing the indicated salt, and the pH was adjusted to 7.4 by neutralization with KOH, NaOH or LiOH. The final buffers had the following compositions: (K+): 10 mM potassium cacodylate buffer + 100 mM KCl; (Na+): 10 mM sodium cacodylate buffer + 100 mM NaCl; (Li+): 10 mM lithium cacodylate buffer + 100 mM LiCl; duplex sample (DS): 10 mM sodium cacodylate buffer + 100 mM NaCl. Oligonucleotides were diluted into buffer to final concentration of 2 µM and heated for 5 min at 95°C, and slowly cooled to room temperature overnight before use.

CD and thermal denaturation studies

CD spectra were collected on a Jasco model J-715 spectropolarimeter equipped with a Julabo FS 18 temperature control system and a 1.0-cm path length thermo-controlled CD quartz cell. Spectra were collected at 25°C between 220 and 400 nm with 0.1 nm steps, 2 nm band width and scanning rate of 50 nm min−1. Three scans were averaged for each reported spectrum. For DNA-melting experiments, 2 μM solutions of pre-folded DNA were equilibrated for 15 min at 10°C and slowly ramped to 95°C at a rate of 30°C h−1. The ellipticity of each sample was monitored at 290 nm for the hTelo derived G-quadruplexes and 260 nm for the corresponding duplexes. Reverse temperature scans showed no hysteresis.

Photophysical measurements

Energy transfer efficiencies and quantum yields were calculated as previously reported (34,40,41). Absorption and emission spectra were recorded using a Molecular Devices SpectraMax M5 instrument in a 1-cm path-length quartz cuvette. Instrument settings were maintained for all reported fluorescence measurements, allowing for direct comparisons of fluorescence intensities (Figure 2). For measurements of nucleoside quantum yields (Figure 1B), optical densities were adjusted to 0.1 ± 0.01 at the indicated λex of each nucleoside and corresponding standard. As the standard for 2PyG (λex = 300 nm), 2-aminopyridine in 0.1 N H2SO4 (Φ = 0.6) was used, and quinine sulfate in 0.1 M H2SO4 (Φ = 0.56) was used as a reference for StG (λex = 340 nm) and 4PVG (λex = 355 nm). Quantum yields of each probe in the context of oligonucleotides were determined as above except that the corresponding nucleosides in water were used as references. The excitation spectra of each probe in the context of DNA were collected using the following wavelengths of emission: 415 nm for 2PyG, 450 nm for StG and 475 nm for 4PVG. For all measurements involving oligonucleotides, 2 μM solutions of pre-folded DNA were used. This allowed for direct comparisons of CD and fluorescence spectra, but the relatively high absorbance of DNA samples at 260 nm (∼0.4 AU) caused a significant attenuation of the excitation beam that reduced the fluorescence intensities from each probe. This was evidenced by non-linear relationships between raw fluorescence intensities Fraw(λex) and DNA concentrations above 50 nM when samples were photoexcited at 260 nm (Supplementary Figure S7A). Fraw(λex) values at each excitation wavelength λex were therefore corrected by multiplication with the following correction factor (CF) to obtain corrected F(λex) values (40). Where A(λex) is the absorbance of the sample at each wavelength of excitation.

Figure 2.

Excitation spectra of 2 µM of StG (A), 4PVG (B) or 2PyG (C) in the presence of 100 mM KCl (K+), 100 mM NaCl (Na+) or 100 mM LiCl (Li+). Excitation spectra of hTeloG23(StG) (D), hTeloG23(4PVG) (E) and hTeloG23(2PyG) (F) were collected using emission at 450, 475 and 415 nm, respectively. Emission spectra of hTeloG23(StG) (G), hTeloG23(4PVG) (H) and hTeloG23(2PyG) (I) were collected using excitation at 260 nm. Double-stranded samples ‘DS’ included 1.1 equivalents of the complementary strand and were prepared in 100 mM NaCl. All samples contained 2 µM of DNA or 8-substituted-2′-deoxyguanosine nucleoside () in an aqueous 10 mM cacodylate buffer (pH 7.4).

All fluorescence spectra (Figure 2) and ‘F(260)/F(X)’ ratios (Table 1) were measured using 2-µM solutions of DNA and corrected according to Equation (1). To check the validity of this approach, serial dilutions of StG-containing duplex and G-quadruplex DNAs were analyzed for fluorescence intensity as a function of sample concentration (Supplementary Figure S7). When the samples were excited at 260 nm, linear relationships were observed only after the application of the CF in Equation (1) (Supplementary Figure S7A–B). At DNA concentrations of 50 nM and below, the fluorescence intensities and F(260)/F(X) ratios for the CF-corrected and uncorrected fluorescence measurements converged to the same values due to the low absorbance of the samples. These results validate the use of Equation (1). It should be emphasized that this CF is not needed for dilute DNA samples (<50 nM) having minimal optical densities (OD ≤ 0.01) at 260 nm.

Table 1.

Quantum yield (Φ), DNA-to-probe energy transfer efficiency (ηt) and the ratio of fluorescence intensities obtained upon excitation at 260 nm [F(260)] and at 360 nm [F(360)] for StG, 375 nm [F(375)] for 4PVG and 325 nm [F(325)] for 2PyG

Name	Cond.	StG			4PVG			2PyG
		Φ	ηt	F(260)/F(360)	Φ	ηt	F(260)/F(375)	Φ	ηt	F(260)/F(325)
hTeloG9	Li+	0.45	0.06	2.0	0.05	0.17	2.0	0.04	0.09	2.3
	K+	0.44	0.21	3.5	0.04	0.28	3.3	0.09	0.24	4.0
	Na+	0.37	0.18	3.9	0.03	0.36	3.7	0.08	0.30	4.7
	DS	0.32	0.02	0.9	0.03	0.04	1.0	0.03	0.03	1.1
hTeloG23	Li+	0.35	0.03	1.9	0.07	0.16	1.8	0.05	0.11	1.8
	K+	0.33	0.12	3.3	0.04	0.24	2.9	0.05	0.19	3.0
	Na+	0.37	0.12	3.3	0.06	0.31	3.0	0.10	0.26	3.3
	DS	0.20	0.02	1.3	0.02	0.05	1.2	0.04	0.06	1.4

Fluorescence spectra of these same samples are shown in Figure 2. Cond.: Measurements were performed in the presence of 100 mM KCl (K+), 100 mM NaCl (Na+) or 100 mM LiCl (Li+) in an aqueous 10 mM cacodylate buffer (pH 7.4). Double-stranded samples (DS) included 1.1 equivalents of the complementary strand and 100 mM NaCl.

RESULTS AND DISCUSSION

Cis–trans conformational analyses of nucleosides 3–4

Derivatives of 8-vinyl guanosine, including 8-(2-phenylethenyl)-2′-deoxyguanosine (), were recently reported to be cis–trans photoisomerizable switches capable of influencing DNA conformation (39,42–44) Nucleoside 3 photoisomerizes upon irradiation at 370 nm to reach a photostationary E:Z ratio of 6:94, while irradiation at 254 nm caused the reverse photoisomerization and reached a E:Z ratio of 80:20. According to HPLC and NMR analysis, we were able to reproduce these results with nucleoside 3 in our laboratory (42). Replacing the phenyl ring of 3 with a pyridine group generates a new fluorescent nucleoside derivative trans-8-(4-pyridyl-vinyl)-2′-deoxyguanosine () that exhibits little, if any photoswitching (45). This feature allows simplified interpretation of CD and fluorescence data collected using compound 4 in the context of oligonucleotides.

Syn–anti conformational analyses of nucleosides 2–4

Introducing bulky substituents to the C8 position of a purine residue is known to shift the conformational preference of the N9-C1′ glycosidic bond towards syn (36–38). This can be evaluated using 1H and 13C NMR. A conformational change from anti to syn correlates with a downfield shift of H2′, C1′, C3′ and C4′ and an upfield shift of the C2′ signal (46,47). According to this analysis, the 2PyG nucleoside 2 prefers a syn conformation. In contrast, the C8 vinyl bridged compounds 3 and 4 exhibit chemical shifts consistent with an anti conformational preference of the glycosidic bond (Supplementary Table S1). These preferences were confirmed by 2D-ROESY experiments, where strong cross peaks were observed between the phenyl/pyridyl rings and 5′OH, H5′, H3′ and H2′ of compounds 3 and 4, but were absent in 2PyG (Supplementary Figures S8–S10). These results confirm a syn conformational preference for 2PyG, and anti preference for StG and 4PVG. These conformational preferences might be important in the context of oligonucleotides, where StG and 4PVG are generally less disruptive to DNA folding than 2PyG.

Global structure and thermal stabilities of oligonucleotides

In K+-containing solutions, the human telomeric repeat DNA sequence [G3(T2AG3)3] ‘hTelo’ can fold into several distinct G-quadruplex conformations in populations that are largely determined by the 5′- and 3′-flanking nucleotides (3,48–50). The sequence studied here (TT[G3(T2AG3)3]A) mostly adopts a ‘(3+1) parallel–anti-parallel hybrid’ topology in the presence of K+ (49). In Na+-containing solutions this same sequence folds into a ‘anti-parallel’ topology in solution (50,51). Each of these structures contain a characteristic mixture of syn and anti glycosidic conformations of guanosines involved in G-tetrad formation (3).

Folding of single-stranded hTelo oligonucleotides was controlled by variation of alkali metal salts in the buffer. The global structures and stabilities of the resulting mixtures were assessed using temperature-dependent CD. In Li+-containing solutions, CD data were consistent with mostly unfolded, G-stacked single-stranded DNA (Figure 3A). Similar results were obtained for all modifications introduced at positions G9 and G23 of hTelo in Li+ buffer. In buffers containing 100 mM KCl, hTelo adopts a ‘(3 + 1) hybrid’ structure that exhibits a positive CD peak at 288 nm with a shoulder at 270 nm and a minimum at 242 nm (49). The same characteristic CD spectrum was observed when G9 was replaced with 2PyG, StG and 4PVG, suggesting the presence of wild-type folds (Figure 3B). In K+ buffers, 2PyG caused a larger thermal stabilization of the ‘(3 + 1) hybrid’ structure (10°C) as compared to StG and 4PVG (5°C and 8°C, Table 2). In contrast, replacing G9 with T caused very large changes to the global structure of hTelo in K+ (Figure 3B) that were accompanied by a dramatic decrease in thermal stability (ΔTm = −23°C, Table 2). We interpret these spectral changes and decreased stability as the loss of one G-tetrad and formation of a G-quadruplex containing only two G-tetrads with ‘head-to-head’ heteropolar stacking orientation (52). These results suggest that position G9 is sensitive to mutation, and that 2PyG, StG and 4PVG are incorporated directly into the G-tetrads of natively folded hTelo in the presence of K+.

Figure 3.

CD spectra of single-stranded hTeloG9 and hTeloG23 derivatives in 100 mM LiCl (A), 100 mM KCl (B and C) or 100 mM NaCl (D). Double-stranded DNA samples ‘DS’ included 1.1 equivalents of the complementary strand and were prepared in 100 mM NaCl (E and F). All samples contained 2 µM of DNA in an aqueous 10 mM cacodylate buffer (pH 7.4).

Table 2.

Thermal denaturation melting temperatures (Tm) of single-stranded oligonucleotides in K+ or Na+, and duplex samples (DSs) in Na+ as determined by temperature-dependent CD

Name	X	Tm in K+ (ΔTm)	Tm in Na+ (ΔTm)	Tm of DS (ΔTm)
hTelowt	G	67.7	53.5	66.0
hTeloG9	StG	73.1 (5.4)	60.6 (7.1)	63.0 (−3.0)
	4PVG	75.9 (8.2)	61.1 (7.6)	64.6 (−1.4)
	2PyG	77.5 (9.8)	61.8 (8.3)	61.2 (−4.8)
	T	44.6 (−23)	39.2 (−14)	57.8 (−8.2)
hTeloG23	StG	59.5 (−8.2)	52.7 (−0.8)	66.5 (0.5)
	4PVG	61.5 (−6.2)	47.5 (−6.0)	66.9 (0.9)
	2PyG	59.3 (−8.4)	51.6 (−1.9)	66.2 (0.2)
	T	45.2 (−23)	45.1 (−8.4)	64.5 (−1.5)

CD spectra of these same samples are shown in Figure 3. ΔTm = Tm(modified oligo) − Tm(wild type).

The substitution of G23 with 2PyG caused hTelo to fold into an ‘anti-parallel’ topology even in K+ solutions (Figure 3C). This structure, where G23 adopts a syn conformation, is normally only observed in Na+-containing solutions (50,51). hTeloG23(2PyG) was therefore characterized in Na+ buffer, where it exhibited nearly the same global structure and thermal stability as the wild-type sequence in Na+ (ΔTm = −2°C, Figure 3D and Table 2). StG and 4PVG, in contrast, did not force hTeloG23 to fold into an ‘anti-parallel’ structure in K+ solutions, and, like the wild-type sequence, two maxima in the region between 270 and 305 nm, and a minimum at ∼240 nm were observed (Figure 3C). StG and 4PVG were also compatible with the formation of the ‘anti-parallel’ hTelo structure in Na+ solutions (Figure 3D). Taken together, these results suggest that single-stranded hTelo oligonucleotides containing StG and 4PVG exhibit folding behavior more similar to wild-type hTelo than 2PyG or T-containing variants.

In contrast to the mutation-sensitive folding of single-stranded hTelo, the substitution of position G9 or G23 with 2PyG, StG, 4PVG or T resulted in little impact on the global structure of the corresponding duplex DNAs (Figure 3E and F). Due to the close proximity of G23 to the end of the oligonucleotide, these modifications had little impact on thermal stability of the duplex (Table 2). Duplexes containing modifications at the central G9 position, in contrast, exhibited thermal stabilities that were highly sensitive to mutations. T incorporation at G9 caused a ΔTm = −8°C as compared to the wild type hTelo duplex (Table 2). The 8-substituted guanosines caused much less loss in thermal stability than T, with ΔTm = −5°C, −3°C and −1°C for 2PyG, StG and 4PVG, respectively (Table 2). Consistent with our results from hTelo G-quadruplexes, these data suggest that duplex oligonucleotides containing StG and 4PVG exhibit duplex-folding equilibria more similar to wild-type hTelo than either 2PyG or T mutations.

Photophysical properties of 8-substituted guanosines 2–4

2PyG, StG and 4PVG, exhibit large Stoke’s shifts (>100 nm) and broad, almost featureless, excitation and emission spectra (Figures 1B and 2 A–C). Due to their larger conjugated π systems, StG and 4PVG are red shifted by 35–75 nm as compared to 2PyG. The quantum yields of all three nucleosides () approached unity in acetonitrile (Φ = 0.57–0.74), while 2PyG and 4PVG exhibited much lower quantum yields in water (Φ = 0.02 and 0.16). Interestingly, 2PyG and 4PVG exhibited 2-fold higher quantum yields in D2O than in H2O (Figure 1B). StG, in contrast, exhibited approximately the same quantum yields in H2O, D2O and acetonitrile (Figure 1B). Taken together, these results suggest that water-mediated quenching of 2PyG and 4PVG involves proton transfer between photoexcited pyridyl nitrogens and bulk solvent. According to molecular modeling of known structures (49,51), the pyridyl nitrogen of 2PyG should be partially protected from bulk solvent upon its incorporation into positions G9 and G23 of hTelo. This may explain the higher quantum yields of 2PyG in the context of G-quadruplex folded DNA (34). The same modeling studies suggest that the pyridyl nitrogen of 4PVG will remain fully solvated in both quadruplex and duplex DNA. No enhancement in the quantum yield of 4PVG was therefore predicted upon its incorporation into DNA.

Quantum yields of 8-substituted guanosines in modified oligonucleotides

The vast majority of fluorescent guanosine analogs, such as 2-aminopurine (2AP), 6-methylisoxanthopterin (6-MI) and 3-methylisoxanthopterin (3-MI) are quenched by close proximity and collisions with unmodified purine residues (53,54). These result in large (10–300-fold) decreases in quantum yield upon their incorporation into duplex DNA (55–57). In contrast, 8-substituted guanosines exhibit relatively little, if any quenching upon their incorporation into G-quadruplex, single-stranded or duplex DNA. The quantum yield of 2PyG in water (0.02) increases to Φ = 0.03−0.05 upon its incorporation into single-stranded or duplex hTelo DNA, and it increases to Φ = 0.05−0.15 when the same oligonucleotides were folded into G-quadruplex structures (34). In the case of 4PVG (Φ = 0.16), somewhat lower quantum yields were obtained upon its incorporation into single-stranded and quadruplex structures (Φf = 0.03−0.07) and still lower quantum yields were observed in the context of duplex DNA (Φf = 0.02−0.03). Upon its incorporation into DNA, StG exhibited quantum yields that were much higher than both 2PyG and 4PVG (Table 1). The values measured for the single-strand and G-quadruplex samples containing StG (Φf = 0.33−0.45) were higher than the values obtained for duplex DNA (Φf = 0.20−0.32). The quantum yields of StG are ∼10- to 100-fold higher than all previously reported fluorescent guanine mimics in the context of well-folded nucleic acids with strong base-stacking interactions (53–57).

Energy transfer properties of modified oligonucleotides

The excitation spectra of the oligonucleotides containing 8-substituted guanosines exhibit two maxima corresponding to direct excitation (330–400 nm) and indirect excitation via unmodified nucleobases (260 nm). The ratio of these excitation peaks weighted by the absorbance properties of the DNA and quantum yields of the probe can be used to calculate energy transfer efficiencies (ηt) (34,40,41). Here ηt is defined as the number of photons transferred from active nucleobase energy donors to each energy acceptor, divided by the total number of photons absorbed by all nucleobases at 260 nm. Due to distance and geometry constraints, many of the unmodified nucleobases will be inactive donors, so the reported efficiencies (Table 1) provide a lower limit for the transfer efficiencies of the active donors.

Energy transfer efficiencies from unmodified bases to 2PyG, StG and 4PVG were ∼2–20-fold higher in G-quadruplexes (ηt = 0.12–0.36) as compared to the same oligonucleotides in duplex DNA (ηt = 0.02–0.06). Single-stranded samples in Li+ exhibited intermediate efficiencies (Table 1). While the calculation of energy transfer efficiencies requires numerous measurements and data processing, a simple comparison of fluorescence intensities resulting from DNA excitation versus selective probe excitation can provide a simple and highly sensitive readout of G-quadruplex formation. According to this approach, the intensity of probe fluorescence upon DNA excitation at 260 nm F(260) is divided by the fluorescence intensity upon selective probe excitation F(X), where X = 325 nm for 2PyG, 360 nm for StG and 375 nm for 4PVG. Consistent with the trends in energy transfer efficiencies (ηt), duplex DNA exhibited the lowest F(260)/F(X) ratios of 0.9–1.4, single-stranded DNA in Li+ exhibited intermediate F(260)/F(X) ratios of 1.8–2.3, while G-quadruplex structures have the highest F(260)/F(X) ratios with 3.0–4.7. These values were similar for all three 8-substituted guanosines, and were independent of the exact structural features and thermal stabilities of the G-quadruplexes or duplexes containing them (Table 1). To evaluate the sensitivity of this F(260)/F(X) ratiometric analysis, serial 2-fold dilutions of hTeloG9 duplex and G-quadruplex DNA containing StG were performed (Supplementary Figure S7). The ratios in F(260)/F(X) were concentration independent (quadruplex ≈ 4, and duplex ≈ 1) and could be readily measured with a standard fluorimeter and sample holder (1-cm path length) using 250 pM solutions of StG-labeled DNA (Supplementary Figure S7). This approach therefore provides a simple and highly sensitive fluorescence readout of G-quadruplex folding that is compatible with extremely diluted sample mixtures.

CONCLUSIONS

Fluorescence phenomena enable powerful and readily accessible technologies for probing biomolecule folding and activity (26). Fluorescence-based assays involving fluorescent nucleobase analogs typically assess conformational changes using probes that exhibit lower quantum yields when base-stacked with neighboring residues (58–62). Probes that remain highly emissive when involved in base-stacking interactions will increase the sensitivity of nucleic acid folding studies, and may provide a means to differentiate DNA/RNA folds where alternative base-stacking interactions are present (eg. duplex versus quadruplex). Here, we demonstrate how highly emissive probes that mimic guanine residues can be used to differentiate DNA secondary structures by estimating energy transfer efficiencies between unmodified nucleobases and 8-substituted guanines. To the best of our knowledge, this represents a new paradigm in detecting conformational changes in nucleic acids. While FRET-based studies using large ‘external’ probes are frequently reported (21), interpretations of the resulting data are limited to changes in probe-to-probe distances, whereas the use of an ‘internal’ fluorescent base analog can provide a direct readout of the characteristic photophysical properties of secondary structures of nucleic acids containing them. Notably, this can be accomplished by introducing a very small modification (e.g. a single styrene or pyridine group) into the oligonucleotide at a strategic location to provide a highly sensitive and minimally perturbing fluorescent readout of structure.

Polymorphic G-quadruplex structures derived from the human telomeric repeat (hTelo) provide demanding model systems to evaluate internal fluorescent probes for their potential impact on DNA folding and stability. To effectively mimic guanosine in G-quadruplexes, both the Watson–Crick and Hoogsteen hydrogen bonding faces must be maintained. Previous studies have demonstrated that subtle changes to either face (e.g. 7-deazaguanine, 6-thioguanine or inosine) result in large losses in G-quadruplex folding kinetics and stability (63). Indeed, single base mutations (G→T) in hTelo DNA resulted in large losses to intramolecular G-quadruplex thermal stabilities ranging from 8°C to 24°C, while duplexes containing the same mutations lost only from 2°C to 8°C of thermal stability (Table 2). On DNA folding and stability, 8-susbtituted guanosines exhibited context-dependent effects but were generally well-tolerated in both G-quadruplex and duplex oligonucleotides.

2PyG was the first reported example of a fluorescent guanine mimic that exhibits the same or higher quantum yield when base-stacked with neighboring purine residues (34). As a nucleobase analog, however, 2PyG suffers from some limitations including a syn glycosidic conformational preference, a relatively low-quantum yield in water (Φ = 0.02–0.15), and an excitation maximum in the UV. For these reasons, a second generation of 8-substituted-2′-deoxyguanosines with expanded pi-systems was developed. One known derivative, 8-(2-phenylethenyl)-2′-deoxyguanosine (StG, Figure 1B) was previously reported to exhibit an anti glycosidic conformational preference and the ability to exhibit photoswitching about the vinyl double bond (39,42,44). Here, we report a related derivative 8-[2-(pyrid-4-yl)-ethenyl]-2′-deoxyguanosine (4PVG, Figure 1B) that also exhibits a preference for an anti glycosidic conformation, but due to the presence of a pyridyl nitrogen atom, it does not act as a photoswitch. As compared to 2PyG, both of these vinyl-bridged derivatives exhibit red-shifted excitation and emission maxima, lower perturbations of DNA structure/stability, and higher quantum yields. To the best of our knowledge, StG displays the highest quantum yield of all reported purine base analogs in the context of folded nucleic acids (Φ = 0.20–0.45). The quantum yield of StG is not as environmentally sensitive as 2PyG and 4PVG, but it can still report DNA folding due to its ability to serve as an emissive energy acceptor for unmodified nucleobase donors.

Previous studies have suggested that the enhanced quantum yields of unmodified guanine residues upon O6 ion coordination are responsible for the unusually efficient energy transfer reactions mediated by G-quadruplex structures (34). It was not clear from these results, however, if efficient energy transfer resulted from the intrinsic properties of G-quadruplexes, the unusual photophysical characteristics of 2PyG, or some combination thereof. Here we report a similar range of transfer efficiencies for all three 8-substitued guanosines evaluated in G-quadruplexes (ηt = 0.12–0.31), suggesting that efficient energy transfer results from the intrinsic properties of G-quadruplex structures, not the probes. In all cases, the energy transfer efficiencies were structure dependent, with ηt(duplex) < ηt(single strand) < ηt(G-quadruplex). In the case of G-quadruplex structures, the combination of efficient energy transfer, high-probe quantum yields, and high molar extinction coefficient of the oligonucleotide (ε260nm ≈ 250 000 cm−1M−1) results in very bright fluorescence emissions that allow for the detection of G-quadruplex conformations at oligonuclotide concentrations of 250 pM or lower using a standard fluorimeter and sample holder. Even in such dilute solutions, a simple comparison of emission intensities resulting from selective probe excitation versus excitation of the DNA provides a highly convenient, sensitive and reliable means to characterize the folded states of oligonucleotides. The trends from these ratiometric analyses matched those from detailed analyses of energy transfer efficiencies. In both cases, the trends were independent of the exact structural features of the G-quadruplex or 8-substituted guanosine probe used. Given the simplicity and sensitivity of this approach, we expect that it will be compatible with conformational analyses using fluorescence microscopy and single molecule spectroscopy.

SUPPLEMENTARY DATA

Supplementary Data are available at NAR Online.

FUNDING

University of Zürich Forschungskredit (57131901); Swiss National Science Foundation (130074). Funding for open access charge: Swiss Federal Grant.

Conflict of interest statement. None declared.