Intrinsic fluorescence of B and Z forms of poly d(G-m5C).poly d(G-m5C), a synthetic double-stranded DNA: spectra and lifetimes by the maximum entropy method.

A study has been made of the fluorescence of poly d(G-m5C).poly d(G-m5C), a synthetic double-stranded DNA, in buffered neutral aqueous solution at room temperature, excited by synchrotron radiation at 280 nm and 250 nm and by a frequency-doubled pulse dye laser at 290 nm. Exciting at 280 nm, the B form shows a uni-modal UV spectrum with lambdaf(max) approximately 340 nm. The Z form has in addition a visible emission lambdaf(max) at 450 nm. The spectral positions remain unchanged on exciting at 250 nm but the relative intensities change considerably. Decay profiles have been obtained at 360 nm and 450 nm for both the B and Z forms and have been analyzed by fitting to a pseudo-continuous distribution of 100 (and occasionally 200) exponentials, ranging from 10 ps to 20 ns, by optimizing the 'entropy' of the signal (the method of maximum entropy). We find the mean lifetimes for both wavelengths of emission and for both structural forms fall into three well-separated regions in the ranges indicated tau1 approximately 0.04-0.21 ns, tau2 approximately 0.9-1.26 ns, and tau3 approximately 5.1-6.5 ns. The UV emission, from its spectral position and half-width, correlates with monomeric emission from m5C (and from C for poly d(G-C)). However the lifetime tau1 is approximately 2 orders of magnitude longer than the monomers and points to an involvement of protonated guanosine (GH+, tauf approximately 200 ps) in the overall absorption/emission sequence. In the UV the tau3 emission is predominant, with fractional time-integrated emission approximately 86% for B DNA and approximately 64% for Z. We suggest it results from exciton (stacked) absorption followed by dissociative emission. For Z DNA the visible (450 nm) emission is dominated by a tau3 species (approximately 91%) with a lifetime of 6.5 ns and we suggest it represents a hetero-excimer emission consequent upon absorption by the strongly overlapped base-stacking, which differs from that in B DNA. The weak emission corresponding to tau2 is made more apparent by scanned gated detection of the emission from laser excitation (290 nm) of single-crystal d(m5C-G)3. A central role is attributed to the tight stacking of the bases in the Z form which correlates with enhanced hypochromism at 250 nm vs. 280 nm and with the reversal of the fluorescence intensity ratios UV-visible between these wavelengths.     

Influence of dA X dT and d(2aminoA) X dT base pairs on the B in equilibrium Z transition of DNA fragments. 1H-NMR study of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G)

The Helical structures of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G) were studied in aqueous solution at various salt concentrations and temperatures by 1H-NMR spectroscopy. In 0.1 M NaCl solution only the B form was evidenced for these DNA fragments whereas in 4 M NaCl both B and Z forms, in slow exchange on the NMR time scale, were observed. Under these conditions the Z form accounted for less than 60% of the decamer conformation; conversely d(C-G)3 hexamers containing methylated cytidines were predominantly in the Z form (greater than 90%) [Tran-Dinh et al. (1984) Biochemistry 23, 1362; Cavaillès et al. (1984) J. Biomol. Struct. Dyn. 1, 1347-1371]. On the other hand, d(C-2aminoA-C-G-T-G) in which the d(2aminoA) X dT base pair forms three hydrogen bonds, was found to adopt the Z conformation in 4M NaCl solution which was not the case for d(C-A-C-G-T-G) (unpublished results). The present study shows that the B in equilibrium Z transition in solution is highly sequence-dependent and that correlation exists between the stability of the duplexes (essentially governed by the number of hydrogen bonds between complementary bases) and their ability to adopt the Z conformation.     

Base tilt of poly[d(A)]-poly[d(T)] and poly[d(AT)]-poly[d(AT)] in solution determined by linear dichroism

We have measured the CD, isotropic absorption, and LD of poly[d(A)]–poly[d(T)] and poly[d(AT)]–poly[d(AT)] in the vacuum-uv spectral region. The reduced dichroism (LD divided by isotropic absorption) varied as a function of wavelength and was independent of shear gradient. Thus, the bases are not perpendicular to the helix axis in solution. Since the directions of the transition dipoles are known, the orientations of the bases in the polymers can be calculated from the reduced dichroism spectra. The results show that the base normals are tilted at angles greater than 25°, with respect to the helix axis, and thymine is tilted more than adenine for both polymers. The tilt axes of adenine and thymine are not parallel, indicating a large propeller twist. Space-filling models of poly[d(A)]–poly[d(T)] and poly[(AT)]–poly[d(AT)] are built based on our results, and the conformations of the two (A + T) polymers in solution are discussed.     

A temperature-dependent Z to B to single-strand transition in d(CGCG)

A thermally induced left- to right-handed helical interconversion for the self-complementary tetradeoxynucleotide d(CGCG) has been observed in the presence of NaCl at concentrations from 1.5 to 2.25M. Analysis of the Raman spectrum of d(CGCG) in aqueous solution as a function of temperature indicates that at low temperature a left-handed Z-helical form is the predominant species. An increase in temperature results in a decrease in the population of the left-handed form and an increase in the population of the right-handed form. Further elevation in temperature results in extensive disruption of base stacking and a loss of secondary structure. This unstacking presumably represents dissociation to a single-stranded structure. The data suggest that a temperature-dependent Z to B to single-strand transition occurs under the conditions employed. A direct Z to single-strand conversion was not identified. In contrast to previous examples, the thermally induced left- to right-handed helical conversion for d(CGCG) can occur in the absence of chemically modified nucleic acid bases, alcohol solutions, or divalent ions.     

Hairpin formation of d(CGCG-TA-CGCG), d(CGCG-TG-CGCG) and their cytosine methylated analogs

Hairpin formations of decamers d(CGCG-TA-CGCG), d(CGCG-TG-CGCG), and their m5dC analogs are evidenced by the existence of biphasic absorbance melting profiles in which the lower transition temperature increases with increasing oligomer concentration, whereas the higher melting temperature is concentration independent. The corresponding temperature dependent CD intensity at 285 nm exhibits a maximum around 55 degrees C. These observations are consistent with the interpretation that the lower temperature transition corresponds to the duplex to hairpin transformation while the melting of hairpins into single strands constitutes the higher temperature transition. The CD spectrum of the hairpin conformation appears to be characterized by a couplet with nearly equal positive and negative intensities at 285 and 255 nm, respectively, while a significantly smaller intensity at 285 nm is apparent for the duplex form. The hairpin conformation is suspected to contain a two-nucleotide loop. Titrations with NaCl further suggest that, in contrast to the TA sequence, the TG sequence with wobble base pairing favors Z formation under high salt conditions.     

Hairpin Formation of d(CGCG-TA-CGCG), d(CGCG-TG-CGCG) and Their Cytosine Methylated Analogs

Abstract

Hairpin formations of decamers d(CGCG-TA-CGCG), d(CGCG-TG-CGCG), and their m⁵dC analogs are evidenced by the existence of biphasic absorbance melting profiles in which the lower transition temperature increases with increasing oligomer concentration, whereas the higher melting temperature is concentration independent. The corresponding temperature dependent CD intensity at 285 nm exhibits a maximum around 55°C. These observations are consistent with the interpretation that the lower temperature transition corresponds to the duplex to hairpin transformation while the melting of hairpins into single strands constitutes the higher temperature transition. The CD spectrum of the hairpin conformation appears to be characterized by a couplet with nearly equal positive and negative intensities at 285 and 255 nm, respectively, while a significantly smaller intensity at 285 nm is apparent for the duplex form. The hairpin conformation is suspected to contain a two-nucleotide loop. Titrations with NaCl further suggest that, in contrast to the TA sequence, the TG sequence with wobble base pairing favors Z formation under high salt conditions.     

Delta V0 of the Na(+)-induced B-Z transition of poly[d(G-C)] is positive

The equilibrium between the right- and left-handed conformations of poly[d(G-C)] in aqueous NaCl shifts towards the right-handed (B) form with increasing pressure. The optical density at 290 and 260 nm was determined at 50 and 180 MPa for solutions in which approximately equal amounts of the two conformations were present at 0.1 MPa (atmospheric pressure). Interpretation of the observed changes in terms of a two-state unimolecular reaction mechanism results in an average molar reaction volume (delta V0) equal to 26 cm3 mol-1 at 22 degrees C; that is, the partial molar volume of B form poly[d(G-C)] is smaller than that of the left-handed (Z) form. Based upon the thermodynamics of ion-pair formation in polar solvents, it is proposed that the positive delta V0 reflects a favorable entropy change for the reaction toward the Z conformation. The larger entropy change of the Z form may derive from the release of water molecules from the hydration spheres of the cation and the poly[d(G-C)] due to the formation of ionic interactions with the Z conformer. The delta V0 of the transition is similar in sign and magnitude to the calculated molar volume change of the interaction of Na+ with H2PO4- in water.     

Structure of a pleiomeric form of poly d(AT):poly d(AT)

A chemically simple polynucleotide duplex, poly d(AT):poly d(AT), has been trapped in a fibrous form with a complex helical secondary structure with a large (7.4 nm) axial repeat 24 nucleotides long. The motif which is repeated by the symmetry elements is a hexanucleotide in which two residues (both TpA) have the less common gauche minus conformation at C3'-O3' and consequently distinctive phosphate orientations. This reinforces earlier conclusions that PypPu nucleotides tend to have different shapes from PupPy nucleotides and that DNA surfaces may signal what base sequences lie beneath them. The morphological differences between this pleiomeric DNA polymer and closely-related, but more symmetrical allomorphs are just as great as those observed in short DNA fragments in crystals.     

Structure of d(CACGTG), a Z-DNA hexamer containing AT base pairs.

The left-handed Z-DNA conformation has been observed in crystals made from the self-complementary DNA hexamer d(CACGTG). This is the first time that a non disordered Z form is found in the crystal structure of an alternating sequence containing AT base pairs without methylated or brominated cytosines. The structure has been determined and refined to an agreement factor R = 22.9% using 746 reflections in the resolution in the resolution shell 7 to 2.5 A. The overall shape of the molecule is very similar to the Z-structure of the related hexamer d(CG)3 confirming the rigidity of the Z form. No solvent molecules were detected in the minor groove of the helix near the A bases. The disruption of the spine of hydration in the AT step appears to be a general fact in the Z form in contrast with the B form. The biological relevance of the structure in relation to the CA genome repeats is discussed.     

Linear dichroism demonstrates that the bases in poly[d(AC)] · poly[d(GT)] and poly[d(AG)] · poly[d(CT)] are inclined from perpendicular to the helix axis

Flow linear dichroism is used to measure specific inclinations for each of the four bases in poly[d(AC)]·;poly[d(GT)] and poly[d(AG)]·poly[d(CT)] in both the B and A forms. For the B form in solution the bases are found to have a sizable inclination. Inclination is increased in the A form, as expected. In all cases the pyrimidines are more inclined than the purines. © 1993 John Wiley & Sons, Inc.     

Molecular mechanical studies of base-pair opening in d(CGCGC):d(GCGCG), dG5·dC5, d(TATAT):d(ATATA), and dA5·dT5 in the B and Z forms of DNA

Molecular mechanical energy refinement of double-helical pentanucleotide tetra-phosphates, d(CGCGC):d(GCGCG), dG₅·dC₅, d(TATAT):d(ATATA), and dA₅ ·dT₅ geometries, are presented in order to examine the energy required to open the Nl(purine) …? N3(pyrimidine) distance (base-pair opening) of a Watson-Crick base pair from its normal value of 3 Å to a value of 6 Å. The structural consequences of forcing base-pair opening is sequence dependent. For both dA₅ ·dT₅ and d(TATAT):d(ATATA), forcing the Nl (AdeKN3 (Thy) distance of the central base pair to a value of 6 Å slides the bases perpendicular to the helix axis forming a low-energy non-Watson-Crick base pair having an adenine amine hydrogen …? thymine carbonyl oxygen hydrogen bond. The two GC sequences behave differently from both AT sequences and differently from each other. Forcing the Nl(Gua) …? N3(Cyt) distance to 6 Å leads to unconventional structures in which hydrogen bonds are formed between the separated bases and the bases above or below them. These structures appear to be trapped in true local minima 6–10 kcal/mol higher in energy than the Watson-Crick structures. Preliminary simulations on d(CGCGC):d(GCGCG) in the Z geometry suggest the reason the Z form may be more refractory to proton exchange than the B form, consistent with experimental observations.     

Elsamicin A can convert the Z-form of poly[d(G-C)] and poly[(G-m5C)] back to B-form DNA.

The interaction of poly[(G-C)] and poly[d(G-m5C)] with the antitumor antibiotic elsamicin A, which binds to alternating guanine + cytosine tracts in DNA, has been studied under the B and Z conformations. Both the rate and the extent of the B-to-Z transition are diminished by the antibiotic, as inferred by spectroscopic methods under ionic conditions that otherwise favor the left-handed conformation of the polynucleotides. Moreover, elsamicin converts the Z-form DNA back to the B-form. The circular dichroism data indicate that elsamicin binds to poly[d(G-C)] and poly[d(G-m5C)] to form a right-handed bound elsamicin region(s). The transition can be followed by changes of the molar ellipticity at 250 nm, thus providing a convenient wavelength to monitor the Z-to-B conformational change of the polymers as elsamicin is added. The elsamicin A effect might be explained by a model in which the antibiotic binds preferently to a B-form DNA, playing a role as an allosteric effector on the equilibrium between the B and Z conformations, thus favoring the right-handed one.     

Base tilt of B-form poly[d(G)]-poly[d(C)] and the B- and Z-conformations of poly[d(GC)]-poly[d(GC)] in solution

We have measured the CD, isotropic absorption, and linear dichroism (LD) in the vacuum-uv spectral region for the B-conformations of poly[d(G)]-poly[d(C)] and poly[d(GC)]-poly[d(GC)], and for the Z-conformation of poly[d(GC)]-poly[d(GC)] formed in 70% trifluoroethanol. The reduced dichroism (LD divided by isotropic absorption) for all conformations varied with wavelength, indicating that the bases are not perpendicular to the helix axis. Since the directions of the transition dipoles are known, the inclinations and axes of inclination of each base can be determined from the wavelength dependence of the reduced dichroism spectra. The results indicate that the base normals of the (G + C) polymers in the B- and Z-conformations are tilted at angles greater than 19° with respect to the helix axis. The guanine and cytosine bases have different inclinations, and the tilt axes are not parallel. Therefore, the bases for all the (G + C) polymer conformations studied are buckled and propeller twisted.     

Structure of the alpha-form of poly[d(A)].poly[d(T)] and related polynucleotide duplexes

The alpha-form of poly[d(A)].poly[d(T)], observed in fibers at high (greater than 80%) relative humidity, is a 10-fold double-helical structure of pitch 3.2 nm. This new X-ray analysis shows that the two strands of the double helix are of the same kind conformationally and both B-like in containing C-2'-endo-puckered deoxyribose rings. Nevertheless, the two strands are different enough for the overall morphology of the duplex to resemble that of the heteromerous model for the drier (beta) form of poly[d(A)].poly[d(T)] in which one strand has C-2'-endo rings and the other C-3'-endo. Since the orientations of the bases in poly[d(A)].poly[d(T)] are persistently different from those of classical B-DNA it is likely that there will be local bending (about 10 degrees) at the junctions between general sequence tracts and the oligo[d(A)].oligo[d(T)] tracts that occur in some native DNAs. The conclusions about the structure of alpha-poly[d(A)].poly[d(T)] are reinforced by independent analyses of similar X-ray diffraction patterns from poly[d(A)].poly[d(U)] and poly[d(A-I)].poly[d(C-T)].     

Mercury-induced transitions between right-handed and putative left-handed forms of poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)]

Poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)], each dissolved in 0.1 M NaClO4, 5 mM cacodylic acid buffer, pH 6.8, experience inversion of their circular dichroism (CD) spectrum subsequent to the addition of Hg(ClO4)2. Let r identical to [Hg(ClO4)2]added/[DNA-P]. The spectrum of the right-handed form of poly[d(A-T).d(A-T)] turns into that of a seemingly left-handed structure at r greater than or equal to 0.05 while a similar transition is noted with poly[d(G-C).(G-C)] at r greater than or equal to 0.12. The spectral changes are highly cooperative in the long-wavelength region above 250 nm. At r = 1.0, the spectra of the two polymers are more or less mirror images of their CD at r = 0. While most CD bands experience red-shifts upon the addition of Hg(ClO4)2, there are some that are blue-shifted. The CD changes are totally reversible when Hg(II) is removed from the nucleic acids by the addition of a strong complexing agent such as NaCN. This demonstrates that mercury keeps all base pairs in register.     

A duplex of the oligonucleotides d(GGGGGTTTTT) and d(AAAAACCCCC) forms an A to B conformational junction in concentrated salt solutions

The coexistence of both A form and B form tracts and formation of an A-B junction in the oligomer d(GGGGGTTTTT).d(AAAAACCCCC) in saturated sodium chloride solution have been detected by Raman spectroscopy. The entire duplex adopts the familiar B-form conformation in aqueous solution at low salt concentrations (0.1M NaCl). In 6M NaCl the adoption of an A form is observed within the G,C tract while a B-form is maintained in the A.T tract. The experimental results indicate that two different helical forms can co-exist in a rather short oligonucleotide and that formation of an A-B junction can occur over a fairly small span of bases. This is in agreement with recent rules governing the relation between base sequence and secondary structure of DNA published from this laboratory. The conformational preferences of each of the individual oligomers d(AAAAACCCCC) and d(GGGGGTTTTT) have also been investigated. The oligomer d(AAAAACCCCC) is single stranded but some evidence for base stacking is observed at 2 degrees C. In contrast, a double stranded B-form structure characterized by wobble G-T base pairing is observed for d(GGGGGTTTTT) in 0.1M and 6M NaCl.     

Interaction of lac repressor with alternating poly d (A-T) and poly d (G-C). Circular dichroism studies

The binding of lac repressor to poly d(A-T) and poly d(G-C) has been studied using circular dichroism. The results indicate that the binding induces the same conformational change of both polynucleotides and perturbs the same number of nucleic acid bases (28 bases). It is shown that in 0.1 M phosphate buffer the CD measurement can be used to determine the binding constant of lac repressor to poly d(A-T). Competition experiments performed at various salt concentrations show that the stronger interaction of lac repressor for poly d(A-T) than for poly d(G-C) is based on difference in the dissociation rate of the complexes whereas the association rate for both polymers are similar.     

Poly[d(A.T)] and other synthetic polydeoxynucleotides containing oligoadenosine tracts form nucleosomes easily.

Synthetic double-stranded polydeoxynucleotides of the general form poly[d(AnT).d(ATn)], with n ranging from 3 to 11, have been synthesized. The conformation of the polymers was investigated by circular dichroism spectroscopy and the polymers were examined for their ability to form nucleosomes. Although spectra show that a circular dichroism band characteristic of poly[d(A.T)] appears in the polymer family for n greater than 7, we demonstrate that even polynucleotides with the longest tracts of contiguous adenosine bases (n = 11) are able to form nucleosomes when reconstituted using a histone exchange procedure. Thus resistance to nucleosome formation does not coincide with the appearance of features similar to that of poly[d(A.T)] over the bulk of the nucleosomal DNA. Furthermore, we show that an approximately 150 base-pair poly[d(A.T)] itself, long thought to be refractory to nucleosome formation, can assemble into such a protein-DNA complex when reconstituted by a low-salt exchange procedure. Competitive assays show that the homopolymer reconstitutes about as well as heterogeneous sequences DNA. Our work, therefore, suggests that highly adenosine-rich sequences in vivo apparently have a function that operates at a level other than that of nucleosome structure.     

Synthesis and characterization of poly[d(G-z5C)]. B-Z transition and inhibition of DNA methylase

Deoxy-5-azacytidine 5'-triphosphate was synthesized and used as a substrate for the enzymatic synthesis of the polynucleotide poly[d(G-z5C)]. Whereas the triphosphate decomposes in solution, the azacytosine analogue incorporated into DNA is stable under conditions preserving the double-helical structure. Poly[d(G-z5C)] undergoes the transition to the left-handed Z conformation at salt (NaCl and MgCl2) concentrations approximately 30% higher than those required for unsubstituted poly[d(G-C)]. However, the incorporation of azacytidine potentiates the formation at room temperature of the Z helix stabilized by the transition metal Mn2+; in the case of poly[d(G-C)], a heating step is required. The spectral properties of the two polymers in the B and Z forms are similar. Both left-handed forms are recognized by anti-Z DNA immunoglobulins, indicating that the DNAs bear common antigenic features. Poly[d(G-z5C)] is not a substrate for the DNA cytosine 5-methyltransferase from human placenta. It is a potent inhibitor of the enzyme when tested in a competitive binding assay. These results are compatible with a very strong, possibly covalent, mode of interaction between methyltransferases and DNA containing 5-azacytosine.