© 1990 Oxford University Press Nucleic Acids Research, Vol 18, No. 6 1559 DNA with adenine tracts contains poly(dA).poly(dT) conformational features in solution Sabine Brahms and J.Georges Brahms Institut Jacques Monod, CNRS, Universite Paris VII Tour 43, 2 Place Jussieu, 75251 Paris Cedex 05, France Received November 2, 1989, Revised and Accepted January 4, 1990 ABSTRACT The conformation of DNA's with adenine-thymine tracts exhibiting retardation in electrophoretic migration and considered as curved were investigated in solution by CD and RAMAN spectroscopy. The following curved multimers with adenine tracts but of different flanking sequences d(CA5TGCC)n, d(TCTCTA 6 TATATA 5 ) n , d(GA4T4C)n yield CD spectroscopic features indicating a non-B structure of the dA.dT tract with similarities to polyd(A).polyd(T). We suggest that adenine-thymine bases in these multimers contain some of the distinctive conformational features of polyd(A).polyd(T) probably with large propeller twist found by NMR (Behling and Kearns, 1987) and by X-ray diffraction on oligonucleotides containing a tract of adenines (Nelson et al. 1987, Coll et al; 1987; DiGabrlele ef al. 1989). Some elements of distinctive CD features of the contiguous adenines run are also observed in the straight multi-9-mer d(CA5GCC)n which lacks in-phase relation to the helical repeat. Despite the presence of the TpA step in the straight multimer d(GT4A4)n, the altered dA.dT conformation is not completely destroyed. Interruption of adenine tract by a guanine in d(CAAGAATGCC)n leads to a B-like conformation and to a normal electrophoretic mobility. The Raman spectra reveal a rearrangement of the sugar-phosphate backbone of dA.dT tract in the multimer d(CA5TGCC)n with respect to that of polydA.polydT. This is reflected in the presence of an unique Raman band associated to C2'-endo sugar with a predominant contribution of C1'-exo puckering which is exhibited by the multimer whereas two distinct Raman bands characterize poly(dA).poly(dT) backbone conformation. INTRODUCTION DNA curving has been observed experimentally in a variety of DNA containing homopolymeric (dA).(dT) tracts essentially by anomalously slow electrophoretic migration on polyacrylamide gels (1-5). In addition sequence directed curving has been observed by electron microscopy (6, 7) and by demonstration of higher circularization probabilities of ohgomers (8). Up to now curved DNA structures were found composed essentially of short runs of oligo(dA) ohgo(dT) spaced in phase with helical repeat. Previously a weak periodicity of some dinucleotides was detected in eukaryotic DNA which suggested that periodic positioning of small bends could lead to unidirectional curvature (9). There is a general agreement that the curvature is coming from the differences in the roll angles of a sequence e.g. of An tract and the roll angles in remaining DNA at a period equal to helical repeat (14b). Different authors provide various models to interpret the curvature (10, 11, 3, 12-14). Poly(dA).poly(dT) has distinct structural and functional properties; it adopts a modified B* form (15) and cannot undergo a B - A transition upon lowering of relative humidity, as shown by infrared dichroism and X-ray diffraction on DNA fibers (15, 16). Poly (dA). poly (dT) cannot be reassociated into nucleosomes (17, 18). Results of X-ray diffraction on single crystal of ohgomers with adenine tracts indicate that run of (dA).(dT) forms a high propeller twist at each base pair facilitating the formation of an additional bifurcated hydrogen bond (19-21). A large propeller twist was also observed in poly(dA).poly(dT) in solution (34). The results of crystallographic analysis of Nelson et al. (19) and DiGabnelle (21) indicate that the A-tract exhibits very small (close to zero) roll angles and the A-tract is straight. According to the crystallographic results curving must occur outside of the A tract (19). It appears that more detailed studies of curved DNA structure in solution are necessary to understand the structure of curved sequences. We report here the investigation of the conformation of curved repetitive DNA's with A-tracts in solution by spectroscopic methods (far UV circular dichroism (CD) and Raman scattering measurements). It is shown that the considered curved DNA's d(CA5TGCC)n, d(TCTCTA6TATATA5)n and d(GA4T4C)n display in solution some of the CD spectral characteristics of poly(dA).poly(dT) homopolynucleotide reflecting conformational similarity of the oligo(dA).oligo(dT) runs of the different curved multimers. We have also investigated A tract containing multimers which do not exhibit retardation in gel electrophoresis either because of incorrect phase relation or because of the presence of T4pA sequence or because of interrupted A tract. Raman spectra show the rearrangement of the sugar puckering of dA.dT tract to one main C2'-endo conformation with predominance of Cl '-exo conformation in the multimer. 1560 Nucleic Acids Research MATERIALS AND METHODS Preparation of synthetic oligomers and of corresponding muitimers Different oligomers and their complementary strands were prepared on Applied Biosystems and Cruachem synthesizers. Each oligonucleotide was synthesized at least twice using two different solid state synthesizers. The correctness of the sequence of one of the synthesized oligonucleotide CA5TGCC was checked by direct sequencing. These oligomers were purified by gel electrophoresis and by FPLC on a Mono Q anion exchange chromatography (Pharmacia) following the instructions of the manufacturer. The majority of oligomers were first submitted to reverse phase C 18 HPLC chromatography, prior to detntylation, with the generous help of Dr Ronald Frank (G.B.F. Braunschweig). Each of the oligomers was phosphorylated using T4 polynucleotide kinase during 1 hour at 37°C. The oligomers were hybridized with their complementary strands heated to 60°C and slowly cooled to room temperature to form double stranded self ligated muitimers with sticky ends and left for 2 - 4 hours at 4°C. The enzymatic ligation reaction was carried out with T4 ligase (Pharmacia) at 12°C during 16 hours. It appeared of importance in our approach to achieve a high degree of ligation of different oligomers. The concentration of oligonucleotides in the ligation reaction was at least 2 mg/ml in the presence of 10% of ethylene glycol. After ligation the samples were deproteinized by phenol followed by twofold chloroform-isoamylalcohol extraction. Finally the muitimers were precipitated by ethanol. Under these conditions the average size of ligated oligomers was estimated -6- 1 6 0 M O 2 2 0 2 4 0 260 250 300 Figure 1. CD spectra of d(A 5 TGCQ n (dotted line) which exhibits retardation in electrophoretic mobility and of d(CAAGAATGCC), (full line) of normal mobility. The CD spectrum of B-form pBR322 (dashed line) is shown for comparison. The spectra were measured at 20°C For preparation of muitimers and other details see materials and methods at about 500 to 700bp from gel electrophoresis The products of ligation were run on 6% polyacrylamide gels in 75 mM Trisborate 1.2 mM EDTA pH 8 at room temperature. A center of a band was excised from the gel and an additional electrophoresis was performed in denaturating medium (formamide). The mobilities of these muitimers were compared with fragments of pBR322 digested separately with HaelTJ, Bgll and TaqI used as size markers and with those of ligated products of 10 bp BamHI linker. Raman scattering spectra Raman spectra were measured with a computer controlled Raman spectrophotometer assembled from a Jarrel-Ash double monochromator with an argon ion laser at 514 5 nm as a source (22). The Raman spectrum represents an average over 40 scans at a dwell time of 1 sec cm" 1 and is represented after a simple base-line adjustment procedure. The multimer samples consist of 100 ng of DNA in 5 ^1 of 40 mM KF pH 7 in either H2O or 2H2O. The sample was held in a quartz capillary held in a thermostated brass block at about 5°-10°C. Circular dichroism spectra Circular dichroism spectra were measured in the spectral range from 170nm to 320 nm using the vacuum UV dichrograph constructed in the laboratory (23). The sample absorbances were about 0 25 to 0.50 at 260nm in 40 mM KF, 5 mM potassium phosphate buffer pH 7. A CD spectrum of each mutimer represents an average over three different DNA samples measured at 20°C. RESULTS AND DISCUSSION Conformation of A.T bases of curved and straight muitimers with adenine tracts We have investigated the conformation of synthetic DNA's with repetitive adenine-thymine sequences which may or may not exhibit retardation of electrophoretic mobility. In figure 1 we compare the CD spectra of d(CA5TGCC)n known to produce retardation of mobility and considered as curved (2) and of d(CAAGAATGCC)n in which bending is eliminated by interruption of the adenine tract by a single guanine residue and exhibits normal mobility in electrophoresis (3). Figure 1 shows that the curved multimer d(CA5TGCC)n display in near UV a particular CD spectrum with four characteristic bands at about 245nm, 258nm, 272nm and at 282nm (dotted line) which shape is distinct from a normal B-conformation CD spectrum (dashed line). The bands at 258nm at 272nm in the curved muitimers d(CA5TGCC)n are distinct and particularly weak compared to the CD of an average DNA like pBR322 of B-form (fig. 1). The bands at 258nm and 272nm were assigned to adenine and thyrrune respectively (24). hi contrast the spectrum of the straight multimer d(CAAGAATGCC)n (fig. 1, full line) is of entirely different shape and indicates a conformation approaching that of a normal type B-DNA when compared to the CD spectrum of pBR322 of 'conservative' character composed of two bands at 275nm and 245nm of positive and negative sign and of nearly equal rotational strength (fig. 1 dashed line). We may consider that the CD spectrum of the muitimers is composed quite closely of two contributions i.e. of dA.dT base pairs of the adenine tract and of the base pairs of flanking sequences. The presence of the 295nm band of negative sign is related to the GC flanking sequences outside of the dA tract and appears similar in the two muitimers. The difference in the two muitimers CD spectra on Nucleic Acids Research 1561 (TCTCTA TATATA ) 9M O 220 2<0 260 w«v«l*noth 300 < n Figure 2. Comparison of CD spectra of poly(dA) poly(dT) (dashed line) with that of two curved multimers (full line) (A) dfTCTCTAjTATATAj),, and (B) d(CA 5 TGCQ n both exhibiting retardation of electrophorctK mobility. The conditions are as in figure 1. figure 1 mainly results from the presence of a guanine which interrupts the A-tract and should be the main cause of the collapse of the fine structure and of a significant modification in CD shape. The intense far U V bands below 200 nm are indicative of good base pairing and stacking in a right handed helix in all these multimers. The CD shape of the curved multimer suggests that the adenine tract may produce a distinguishable fine structure in the CD of curved multimers. To obtain more information on conformational features of curved DNA two multimers of different sequences dCTCTCTAfiTATATAj),, (ref. 8) and d(CA5TGCC)n were compared (Fig. 2). Figure 2 shows that the CD shape of these two multimers d(CA5TGCC)n and d(TCTCTA<;TATATA5)n resemble that of poly(dA).poly(dT) but their CD fine structure is attenuated as compared to the homopolymer partly as a result of superposition of the two CD contributions: of adenine tract and of flanking base pairs. Nevertheless the CD spectra indicate that some of the essential features like the particularities of basebase arrangement of poly(dA).poly(dT) already exist to some extent in adenine tracts in both curved DNA's dCTCTCTA^TATATA,),, (Fig. 2A) and d(CA5TGCC)n (Fig. 2B). This presumably gives rise to a CD shape (dotted line) with splitted 285nm-245nm region into four positive and negative bands different from the B-type spectra. Haran and Crothers (31) have shown a cooperativity in building of an A-tract structure which is in agreement with our results. In the straight ohgonucleotide d(CAAGAATGCC)n the required minimum of three A:T base pairs is no longer present to satisfy the cooperativity of the adenine tract which may explain the observed difference in conformation (Fig. 1). In the straight multimer the interruption of the adenine tract by a single guanine residue causes a transition to a B-like conformation. According to their respective CD (Fig. 2), the tracts of six and five adenines in both multimers considered as curved have conformational features different from a B-DNA. We suggest that the A-tract of the multimers shown in Figure 2 adopts a structure approaching that of poly (dA). poly (dT). Our results are in agreement with recently reported data on CD of poly d(An).poly dCTJ composed of ohgodA.oligodT of various lengths (35). The authors observed a rapid change and increase of the 258nm band intensity with an increase of the number of contiguous adenine residues starting from the tnmer. It was of interest to compare the conformation of multimers in which oligomeric components were propagated in phase with the helical repeat to that propagated out of phase. Stable axial curvature is expected to have inherent phase relation to the helical repeat. In contrast the 9-mer multimer d(CA5GCC)n in which such phasing is absent migrates with normal mobility. Figure 3 shows the CD spectrum of the 9-mer multimer which to some extent resembles that of the decamer d(GA5TGCC)n displayed on figure 2, both exhibiting a non-B-type structure of the A-tract. Despite the existence of certain conformational features of the adenine tract susceptible to generate a local alteration of the helix direction, the 9-mer multimer is not producing a macroscopic curvature as a consequence of the absence of phase coherence. An example of sequence dependent differences concerns two multimers, d(GA4T4C)n showing retardation in electrophoretic migration and d(GT4A4C)n which have normal mobility (5b). Differences between df^GA^C),, and d(GT4A4Qn were also observed in cutting reactivity by the hydroxyl radical and were interpreted on the basis of differences in the narrow minor groove width of the former and of normal width of the latter as a consequence of TpA step (25). The comparison of the CD spectra of the curved multimer d(GA4T4C)n with the straight multimer d ^ T ^ Q n shows that both multimers exhibit a conformation different from B-form DNA (Fig. 3). The two spectra show some differences, but one can observe in both CD the presence of the specific conformation of the adeninerthymine tract reflected in the maxima at about 258nm, 272nm and 282nm. In both multimers the dA.dT tract seems to be in a non-B conformation as shown by the presence of the 258nm band which is much strongly attenuated in d(GT4A4C)n. The contribution of G-C sequences are reflected by the presence of the negative band at about 295nm. 1562 Nucleic Acids Research 1000 800 >, 600 'm c 4) £ 400 200 65O 7OO 75O BOO S5O cm-1 180 200 220 240 250 280 300 Figure 3. Circular dichroism spectra of d(GA4T4C)n (dotted line) exhibiting anomalously slow electrophoretic migration and of dfGT^C),, (dashed line) with normal migration Trie nanomer multimer d(CAjGCC)n (full line) is lacking macroscopic curvature and does not show retardation in electrophoretic mobility The experimental conditions are as in figure 1 Calorimetric measurements show that the 5'TpA step has lower energy of stacking interaction (AH= 6.0 kcal/mol) than ApT (AH= 8.6 kcal/mol) (27). This difference in stability is most probably a consequence of a smaller stacking overlap for TpA than for ApT (28, 29,30a). Possibly the TpA step destrabilizes also the spine of hydration of poly(dA).poly(dT) structure (30b). We found (fig. 3) that the TpA step does not destroy completely the adenine-thymine tract structure in d(GT4A4C)n which maintains some conformational features of a modified B-DNA form. Our results are also in good agreement with NMR data of base pair lifetime determination of adenine lmino-protons of d(A4T4) and d(T4A4) oligomers (26). The exchange time of adenine iminoprotons of d(A4T4) was found to be long whereas in dC^A,,) even if appeared much shorter was found also anomalous. The interpretation of Gu6ron et al. is very similar to ours i.e. in 'dOVA*) also the non-B structure is formed either incompletely or only part of the time' (26). Measurements of anomalous migration of multimers containing TnAn tracts and A,,Tn tracts reported by Haran and Crothers (31) also lead to an existence of a structure different from B within the components of TnAn blocks. The specific CD band shape in the 250nm-280nm range suggests that some of the particular features of adenine-thymine base-pairing of a modified B-DNA form found in poly(dA).poly(dT) tend to be adopted by the adenine-thymine tract in all investigated curved DNA. We suggest that oligodA.oligodT tract in curved multimers adopt in solution a non-B conformation approaching polyd(A).polyd(T) type. The CD spectrum of poly(dA).poly(dT) (Fig. 2) of unusual shape with sphtted three bands in the region 255nm-3OOnm is not encountered in any other DNA. We may Figure 4 Raman scattering spectra of curved multimer (CA5TGCC)n (dashed line) and of poly(dA) poly(dT) (full line) in the frequency range 500cm~' — 900cm of base and sugar-phosphate backbone vibrations The spectra were normalized with respect to the 1094cm ~' phosphate vibrations band (data not shown) assume that this particular shape of the homopolydeoxynucleotide results from stacking of bases with relatively large propeller twist. A large propeller twist of adenine thymine tracts (18° -24°) was found by X-ray diffraction analysis of single oligomers crystals (19-21). The presence of a large propeller twist is also confirmed by energy calculation from fiber diffraction and NMR data in solution (32, 33, 34). Interruption of the adenines tract e g. by a guanine residue in a straight d(CAAGAATGCC)n restores a B type conformation. Our interpretation is also in agreement with the recent results of CD spectra investigation of a series of oligomers ohgod(A)n.oligod(T)n (35). The authors observed an abrupt change between ohgod(A)2.oligod(T)2 and higher oligomers which subsequently generate continuously changing spectra for higher oligomers. This was interpreted as reflecting appearance and change of propeller twist at AT base pairs with increasing length of contiguous adenosines (35) starting from the trimer. The presence to some degree of a type of conformation poly(dA) poly(dT)-like in the adenine tract of the 9-mer multimer d(CA5TGC)n supports the idea that the structural elements of the distortion of the helical axis do exist but sine they are not propagated in phase with the helical repeat the macroscopic curvature can not occur. Our data clearly show that despite the low conformational stability at the TpA step probably resulting from its lower energy of stacking interaction (27-30) in d(GT4A4C) the non-B structure of the adenine tract is not destroyed but less complete. This interpretation of our results on d(T4A4)n is in good agreement with NMR data of base pair lifetime determination (26). To some extent this specific structure is retained in the adenine run of the 9-mer d(CA5GCC)n and in d(GT4A4C)n both with normal electrophoretic mobility. The spectra of straight d(CAAGAATGCC)n have lost the spectral features of polyd(A).polyd(T). In d(CAAGAATGCC)n the presence of a Nucleic Acids Research 1563 guanine may interrupt the A-tract structure presumably the network of propeller twisted adenines (19-21). Sugar-phosphate backbone and bases conformation — Raman scattering investigation Raman scattering spectrum of d-(CA 5 TGCC) n in the conformationally sensitive region of base and of phosphate-sugar backbone vibrations 620cm" 1 -900cm" 1 is shown in Fig. 4 (dotted line) where it is compared to that of the homopolymer polyd(A) polyd(T) (Fig. 4 full line). In the frequency range characteristic of sugar-phosphate backbone vibrations the multimer yields one main broad band at 828cm"1. This band approximately corresponds to the frequency of vibrations of sugar in C2'-endo furanose ring pucker family (36, 37). The displacement of this band from 835cm~' typical of C2'-endo furanose pucker to a band centered at 828cm "' suggests a distribution of sugar comformations around C2'-endo family presumably including a main contribution of Cl'-exo deoxyribose pucker. These results in solution are in agreement with crystallographic analysis data on a similar sequence containing A-tract d(CGCA6GCG) by Nelson et al (19). In this frequency range polyd(A).polyd(T) exhibits clearly two distinct bands contribution at 816 cm" 1 and at 841cm"1 (Fig. 4; ref. 38). This may suggest that in polyd(A).polyd(T) two populations of deoxynbose conformations contribute i.e. one at 816"' closely related to 04'-endo and the second at 841 cm" 1 of the C2'-endo family. The band at 816cm"1 is tentatively assigned to an intermediate conformation presumably to O4'-endo deoxyribose pucker since it occur between 809cm" 1 characteristic of C3'-endo ring pucker and 835cm"1 assigned to C2'-endo (36, 37). The O4'-endo pucker is intermediate between C2'-endo and C3'-endo puckering in terms of pseudorotation angle (39). This comparison suggests the occurrence of a rearrangement of the backbone conformation of adenine tract from two distinct furanose pucker populations in poly(dA).poly(dT) homopolymer to one main population of the C2'-endo family with Cl'-exo deoxyribose conformer contribution in the curved multimer of d(CA5TGCC)n. Further indications of the sugar-phosphate backbone rearrangement of the A-T tract of the multimer are also suggested by the changes of the Raman band at 750cm"1 of thymine which is sensitive to sugar C2'-endo/T conformation (40). The relative intensity of the 750cm"1 band sharply decreases in the spectrum of the multimer d(CA5TGCG)n with respect to that of poly(dA).poly(dT) (Fig. 4). Other differences concern the band at 728cm"1 of adenine in plane vibrations of the multimer d(CA5TGCC)n which exhibits Raman hyperchromism (Fig. 4). This suggest that short tracts of five adenines in the multimer d(CA5TGCC)n are slightly less stacked with respect to the continuous dA.dT pairs in the homopolymer. The Raman band at 670cm"1 assigned to thymine is well resolved and of intermediate intensity between poly(dA) poly(dT) and DNA, as one could expect from the dependence of intensity on A-T base content (40). The contribution of G-C bases is reflected by the presence of a 682cm"1 band assigned to guanine and at 782cm~' assigned to cytosine. Raman scattering is particularly sensitive for detection of short life states of the order of 10"12sec. The contributions of 841cm"1 and of 816cm"1 bands in polyd(A).polyd(T) may represent two families of deoxynbose conformations and/or may reflect rapid interconversion of furanose puckering which may not be observed by other methods e.g. NMR, particularly nuclear Overhauser effect which measures over 10~3sec. As noted previously (38) it is not surprising why NMR studies on polyd(A).polyd(T) report only one C2'-endo sugar conformation (34) whereas Raman scattering may detect contribution of two populations of furanose puckering. Our results about the backbone flexibility of DNA containing adenine tracts are in general agreement with the data of X-ray diffraction analysis of Dickerson et al. (41, 42) and their recent refinements by Westhof (43). The variability of furanose pucker in DNA was also observed in solution of supercoiled and relaxed pBR322 (44) and of DNA's (40) from the analysis of band shape. It is to be noticed that our present method is direct since DNA's with adenine tracts yielded Raman bands with well defined maxima (Fig. 4). The Raman spectra reveal rearrangement of sugar-phosphate backbone of the dA.dT tract of the multimer d(CA5TGCG)n from two Raman bands in poly(dA).poly(dT) to one band at 828cm"1 assigned to C2'-endo family with predominant Cl'-exo sugar pucker. 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