Molecular states in single-stranded adenylate chains by relaxation analysis

The single-strand helix-coil transition in various oligo- and polyadenylates is characterized by means of an improved cable temperature-jump technique. In all the polymers studied {poly(rA), poly(dA), poly[A(m^2′)] and poly[A(e^2′)]} helix-coil relaxation is observed in the time range from 30 to 1000 nsec. Relaxation-time constants observed at wavelengths λ<280 nm (τ_α) are different from those found at λ >280 nm (τβ), indicating the presence of more than two conformational states. The time constants τ_α increase in the series poly(dA), poly[A(m^2′)], constants τ_β/τ_α is approximately 2.5, except in poly(dA) where τ_β/τ_α ≈ 9. Relaxation measurements with r(A)_n- oligomers show a decrease in conformational mobility with increasing chain length. The relaxation curves also demonstrate that “internal” residues have lower reaction rates than residues at the ends of the oligomer chain. Measurement in D₂O reveal a solvent isotope effect for τ_α of +87% for poly(rA), and of +53% for poly(dA), whereas no isotope effect is found in τ_β. The absence of “slow” relaxation processes in the model compound 9,9′ -trimethylenebisadenine shows that the relatively low rate of the single-strand helix-coil transitions is due to the coupling of base stacking with the folding of the sugar–phosphate chain. The absence of a seprate relaxation process (corresponding to τ_β) in 9,9′-trimethylenebisadenine, as well as in the dinucleotides ApC and CpA, suggests that this relaxation process is dependent upon the presence of both the sugar–phosphate chain and of adjacent adenine bases. The experimental data provide evidence that there is more than one ordered conformation in various single-stranded oligo- and polyadenylates and that the transition between these conformations is influenced by the sugar conformation.     

A UV resonance Raman investigation of poly(rI): Evidence for cation-dependent structural perturbations

Poly(rI) stabilized by either Na⁺ or K⁺ was investigated using uv resonance Raman (UVRR) spectroscopy. Raman excitation profiles of inosine 5′-monophosphate demonstrated the 250 nm excitation selectively enhances base stacking interactions, while ribose and carbonyl stretching vibrations are preferentially enhanced with 210 nm excitation. These wavelengths were used to examine the structure of poly(rI) in the presence of either K⁺ or Na⁺ as a function of temperature. UVRR studies revealed that the K⁺ stabilized form is more thermally stable, yielding a T_m of ∼ 47°C compared to a T_m of ∼ 30°C for the Na⁺ stabilized form. We observed that both the ribosyl conformation and the coordination of the carbonyl groups depend on the nature of the cation. The C₆O stretching frequency indicates that Na⁺ coordinates much more strongly to the carbonyl groups than K⁺ (1672 cm⁻¹ Na⁺ vs 1684 cm⁻¹ K⁺ at 4°C). Conformationally sensitive modes of the phosphate backbone and the ribosyl ring indicate that Na⁺ stabilized poly(rI) predominantly exists in a C_3′-endo ribose conformation, whereas K⁺ stabilized poly(rI) adopts a C_2′-endo conformation possibly as a consequence of the larger ionic radius of the K⁺ ion. © 1998 John Wiley & Sons, Inc. Biopoly 46: 475–487, 1998     

A vibrational spectroscopic study of the self-association of polyinosinic acid and polyguanylic acid in aqueous solution

We have studied by Raman and ir spectroscopy the structure of self-associated polyinosinic acid and polyguanylic acid in aqueous solution. The results are consistent with the formation of a four-stranded complex, which melts cooperatively near 60°C in the case of poly (I) in the presence of K⁺ ions. The conformation of the ribose in both systems is mixed C2′-endo/C3′-endo, giving a structure that is intermediate between the extremes proposed previously from x-ray diffraction studies. Characteristic Raman bands for the C2′-endo ribose conformation in polyribonucleotides are identified. The four-stranded structure of poly (I) appears to be very flexible, with ≈15% of the tetrameric segments being disrupted and ≈30% of the ribose units adopting a disordered conformation prior to melting. This disordering process increases to ≈75% above the melting transition, with the remaining ≈25% of the ribose units keeping an ordered C2′-endo or C3′-endo conformation. © 1994 John Wiley & Sons, Inc.     

A Raman spectroscopic study of the interaction between nucleotides and the DNA binding protein gp32 of bacteriophage T4

Raman spectra of the bacteriophage T4 denaturing protein gp32, its complex with the polynucleotides poly(rA), poly(dA), poly(dT), poly(rU), and poly(rC), and with the oligonucleotides (dA)₈ and (dA)₂, were recorded and interpreted. According to an analysis of the gp32 spectra with the reference intensity profiles of Alix and co-workers [M. Berjot, L. Marx, and A. J. P. Alix (1985) J. Ramanspectrosc., submitted; A. J. P. Alix, M. Berjot, and J. Marx (1985) in Spectroscopy of Biological Molecules, A. J. P. Alix, L. Bernard, and M. Manfait, Eds., pp. 149–154], 1 gp32 contains ≈ 45% helix, ≈ 40% β-sheet, and 15% undefined structure. Aggregation of gp32 at concentrations higher than 40 mg/mL leads to a coordination of the phenolic OH groups of 4–6 tyrosines and of all the sulfhydryl (SH) groups present in the protein with the COO^? groups of protein. The latter coordination persists even at concentrations as low as 1 mg/mL. In polynucleotide–protein complexes the nucleotide shields the 4–6 tyrosine residues from coordination by the COO^? groups even at high protein concentration. The presence of the nucleotide causes no shielding of the SH groups. With Raman difference spectroscopy it is shown that binding of the protein to a single-stranded nucleotide involves both tyrosine and trytophan residues. A change in the secondary structure of the protein upon binding is observed. In the complex, gp32 contains more β-sheet structure than when uncomplexed. A comparison of the spectra of complexed poly(rA) and poly(dA) with the spectra of their solution conformations at 15°C reveals that in both polynucleotides the phosphodiester vibration changes upon complex formation in the same way as upon a transition from a regular to a more disordered conformation. Distortion of the phosphate–sugar–base conformation occurs upon complex formation, so that the spectra of poly(rA) and poly(dA) are more alike in the complex than they are in the free polynucleotides. The decrease in intensity of the Raman bands at 1304 cm^?1 in poly(rA), at 1230 cm^?1 in poly(rU), and at 1240 and 1378 cm^?1 of poly(dT) may be indicative of increased stacking interactions in the complex. No influence of the nucleotide chain length upon the Raman spectrum of gp32² in the complex was detected. Both the nucleotide lines and the protein lines in the spectrum of a complex are identical in poly(dA) and (dA)₈.     

Interaction of Purine Nucleotides with Cobalt-Hexammine,Cobalt-Pentammine and Cobalt- Tetrammine Cations. Evidence for the Rigidity of Adenosine and Flexibility of Guanosine and Deoxyguanosine Sugar Conformations

Abstract

The interaction of adenosine-5′-monophosphate (5′-AMP), guanosine-5′-monophosphate (5′-GMP) and 2′-deoxyguanosine-5′-monophosphate (5′-dGMP) with the [Co(NH₃)₆]³⁺, [CO(NH₃)₅C1]²⁺ and [CO(NH₃)₄C1₂]⁺ cations has been investigated in aqueous solution with metal/nucleotide ratios (r) of 1/2, 1 and 2 at neutral pH. The solid complexes have been isolated and characterized by FT-IR and ¹H-NMR spectroscopy.

The complexes are polymeric in nature both in the crystalline solid and aqueous solution. The binding of the cobalt-hexammine cation is indirectly (via NH₃) through the N-7 and the PO₃ ^2- groups of the AMP and via O-6, N-7 and the PO₃ ^2- of the GMP and dGMP anions (outer-sphere). The cobalt-pentammine and cobalt-tetrammine bindings are through the phosphate groups (inner-sphere) and the N-7 site (outer-sphere) of these nucleotide anions. The ribose moiety shows C2′-endo/anti conformation, in the free AMP and GMP anions as well as in the cobalt-ammine - AMP complexes, whereas a mixture of the C2′-endo/anti and C3′-endo/anti sugar puckers were observed for the Co(NH₃)₆-GMP, Co(NH₃)₅-GMP and a C3′-endo/anti conformer for the Co(NH₃)₄-GMP complexes. The deoxyribose showed an O4′-endo/anti conformation for the free dGMP anion and a C3′-endo/anti for the Co(NH₃)₆-dGMP, Co(NH₃)₅-dGMP and Co(NH₃)₄-dGMP complexes.     

Conformational Analysis of a Hybrid DNA-RNA Double Helical Oligonucleotide in Aqueous Solution: d(CG)r(CG)d(CG) Studied by 1D- and 2D-1H NMR Spectroscopy

Abstract

The double helical structure of the self-complementary DNA-RNA-DNA hybrid d(CG)r(CG) d(CG) was studied in solution by 500 MHz ¹H-NMR spectroscopy. The non-exchangeable base protons and the (deoxy)ribose H1′, H2′ and H2″ protons were unambiguously assigned using 2D-J-correlated (COSY) and 2D-NOE (NOESY) spectroscopy techniques. A general strategy for the sequential assignment of ¹H-NMR spectra of (double) helical DNA and RNA fragments by means of 2D-NMR methods is presented.

Conformational analysis of the sugar rings of d(CG)r(CG)d(CG) at 300 K shows that the central ribonucleotide part of the helix adopts an A-type double helical conformation. The 5′- and 3′-terminal deoxyribose base pairs, however, take up the normal DNA-type conformation. The A-to-B transition in this molecule involves only one (deoxyribose) base pair. It is shown that this A-to-B conformational transition can only be accomodated by two specific sugar pucker combinations for the junction base pair, i.e. N·S (C3′-endo-C2′-endo, 60%, where the pucker given first is that assigned to the junction nucleotide residue of the strand running 5′ → 3′ from A-RNA to B-DNA) and S·S (C2′-endo-C2′-endo, 40%).     

The Structure of Poly(dA)· poly(dT) as Revealed by an X-ray Fibre Diffraction

Abstract

X-ray diffraction in fibres revealed that the calcium salt of poly(dA) · poly(dT) is a 10-fold double helix with a pitch of 3.23 nm. The opposite sugar-phosphate chains in the refined model are characterized by a complete conformational equivalence and contain sugars in a conformation close to C2′-endo.

As a result a new model of the sodium salt of poly(dA) · poly(dT)has been constructed, which is different from the Heteronomous DNA proposed earlier (S. Arnott et al., Nucl. Acids Res. 11, 4141 (1983)). The new model of Na-poly(dA) · poly(dT) has conformationally similar opposite chains; it is a structure of the B-type, rather like that of Ca-poty(dA) · poly(dT).     

Untenability of the Heteronomous DNA Model for Poly(dA) · Poly(dT) in Solution. This DNA Adopts a Right-Handed B-DNA Duplex in Which the Two Strands are Conformationally Equivalent. A 500 MHz NMR Study Using One Dimensional NOE

Abstract

ID NOE ¹H NMR spectroscopy at 500 MHz was employed to examine the structure of poly(dA)·poly(dT) in solution. NOE experiments were conducted as a function of presaturation pulse length (50, 30, 20 and 10 msec) and.power (19 and 20 db) to distinguish the primary NOEs from spin diffusion. The 10 msec NOE experiments took 49 hrs and over 55,000 scans for each case and the difference spectra were almost free from diffusion.

The spin diffused NOE difference spectra as well as difference NOE spectra in 90% H₂O + 10% D₂O in which TNH3 was presaturated enabled to make a complete assignment of the base and sugar protons. It is shown that poly(dA) ·poly(dT) melts in a fashion in which single stranded bubbles are formed with increasing temperature.

Extremely strong primary NOEs were observed at H2′/H2″ when AH8 and TH6 were presaturated. The observed NOEs at AH2′ and that AH2″ were very similar as were the NOEs at TH2′ and TH2″. The observed NOEs at AH2′ and AH2″when AH8 was presaturated were very similar to those observed at TH2′ and TH2″ when TH6 was presaturated. In addition, presaturation of H1′ of A and T residues resulted in similar NOEs at AH2′/H2″ and TH2′/H2″ region and these NOEs at H2′ and H2″ were distinctly asymmetric as expected in a C2′-endo sugar pucker. There was not a trace of NOE at AH8 and TH6 when AH3′ and TH3′ were presaturated indicating that C3′-endo, × = 30–40° conformation is not valid for this DNA. From these NOE data, chemical shift shielding calculations and stereochemistry based computer modellings, we conclude that poly(dA)·poly(dT) in solution adopts a right- handed B-DNA duplex in which both dA and dT strands are conformationally equivalent with C2′-endo sugar pucker and a glycosyl torsion, ×, of ?73°, the remaining backbone torsion angles being φ′ = 221°, ω′ = 212°, ω = 310°, φ = 149°, ψ = 42°, ψ′ = 139°. The experimental data are in total disagreement with the heteronomous DNA model of Arnott et. al. proposed for the fibrous state. (Arnott, S., Chandrasekaran, R., Hall, I.H., and Puigjaner, L.C., Nucl. Acid Res. 11, 4141, 1983).     

Syn-anti effects on the spatial configuration of polynucleotide chains

Semiempirical energy calculations have beeb performed on model nucleic acid systems to assess the preferred conformation of the rotation χ about the glycosidic linkage and also the effect of this rotation on the spatial configuration of the sugar-phosphate chain backbone. The rotation angle ?? about bond C_5′–C_4′ in purine polyribonucleotides and 5′-monoribonucleotides is found to depend on whether the conformational range of χ is syn or anti. The preferred conformation of χ in these molecules is also found to depend upon the nature of the attached base. The orientation of χ in poly rA chains is predicted to be predominantly anti, whereas in poly rG the syn conformer is expected to occur in significant proportions. The syn conformer is preferred almost exclusively in certain unusual purine polynucleotides, such as poly 8Br-rA. It is noted that the preferred conformation of x in polynucleotides is not necessarily the same as that calculated for 5′-mononucleotides and nucleosides. On the basis of these calculations, the influence of the orientation and nature of a purine base on the spatial configuration of a polynucleotide chain as a whole has been examined. The random coil dimensions of a syn polynucleotide chain are found to be larger than those of an anti chain as a consequence of the effect of a syn base on the local conformation of the chain skeleton. Finally, it is found that the occurrence of a syn base in an ordered polynucleotide chain may prevent the formation of normal stacking with the preceding base.     

Influence of ribose 2′-O-methylation on GpC conformation by classical potential energy calculations

Potential energy calculations were employed to examine the effect of ribose 2′-O-methylation on the conformation of GpC. Minimum energy conformations and allowed conformational regions were calculated for 2′MeGpC and Gp2′MeC. The two lowest energy conformations of 2′MeGpC and Gp2′MeC are similar to those of GpC itself. The helical RNA conformation (sugar pucker-C(3′)-endo, ω′ and ω,g^?g^?, bases-anti) is the global minimum, and a helix-reversing conformation with ω′, ω in the vicinity of 20°, 80° is next in energy. However, subtle differences between the three molecules are noted. When the substitution is on the 5′ ribose (Gp2′MeC), the energy of the helical conformation is less than that of GpC, due to favorable interactions of the added methyl group. When the substitution is at the 3′ ribose (2′MeGpC) these stabilizing interactions are outweighed by steric restrictions, and the helical conformation is of higher energy than for GpC. Furthermore, the statistical weight of the 2′MeGpC g^? g^? helical region is substantially less than the corresponding weight for Gp2′MeC. In addition, 2′MeGpC′s methoxy group is conformationally restricted to a narrow range centered at 76°. This group has a broadly allowed region between 50 and 175° in Gp2′MeC. These differences occur because the appended methyl group in 2′MeGpC is located in the interior of the helix cylinder, as it would be in polynucleotide, while it hangs unimpeded in Gp2′MeC. These findings suggest that 2′-O-methylation has both stabilizing and destabilizing influences on the helical conformation of RNA. For 2′MeGpC the destabilizing steric hindrance imposed by the nature of the guanine base dominates.     

Examination by the molecular orbital method of the intrinsic conformation preferences of nucleic acid sequence]

This paper reports a systematic PCILO study of the conformation of the nucleic acid backbone. The authors principally studied the ω′ and ω phosphodiester torsion angles of the disugar triphosphate model as a simultaneous function of (1) the sugar nature, ribose or deoxyribose, (2) the different combinations of the sugar ring puckers C(2′)-endo-C(2′)-endo, C(3′)-endo-C(3′)-endo, C(3′)-endo-C(2′)-endo, and C(2′)-endo-C(3′)-endo, and (3) the different conformations around the ψ(C4′–C5′) exocyclic bond. The dependence of the (ω′,ω) conformational energy maps upon these different factors, is discussed. The results are in very good agreement with the observed structures of ribonucleic (RNA10, RNA11, A′-RNA12, tRNA^Phe) and deoxyribonucleic acids (D-DNA, C-DNA 9.3, B-DNA 10, A-DNA 11). Thus the validity of this model, the disugar triphosphate unit, is ensured. The main conclusions that can be drawn from this systematic study are the following:

• 1 The torsion around P-05′ (angle ω) is, as a general rule, more flexible than the torsion around P-03′ (angle ω′).
• 2 There is no notable difference between the ribose–triphosphate units and the deoxyribose–triphosphate units for the C(3′)-endo–C(3′)-endo and C(3′)-endo–C(2′)-endo sugar puckers.
• 3 The deoxyribose–triphosphate units with C(2′)-endo–C(2′)-endo and C(2′)-endo–C(3′)-endo sugar puckers show much more ω′ flexibility than the ribose–triphosphate units with the same sugar puckers and cis position for the 2′hydroxyl group.
• 4 The preferred values of ω′ are independent of the sugar nature (ribose or deoxyribose) and of ψ values; they are correlated with the sugar pucker of the first sugar-phosphate unit:
  • C(3′)-endo-C(3′)-endo and C(3′)-endo-C(2′)-endo puckers ? ω′ ? 240° (g^? region)
  • C(2′)-endo-C(2′)-endo and C(2′)-endo-C(3′)-endo puckers ? ω′ 180° (t region)
• 5 The preferred values of ω are independent of the nature and the puckering of the sugars; they are correlated with the rotational state of the torsion angle ψ(C4′–C5′): ψ ? 60° (gg) ? ω ? 300° (g^?), ψ ? 180° (gt) or 300° (tg) ? ω ? 60° (g⁺)

     

Poly(rA) • Poly(rU) with Ni2+ Ions at Different Temperatures: Infrared Absorption and Vibrational Circular Dichroism Spectroscopy

Abstract

Phase transitions were studied of the sodium salt of poly(rA) ?poly(rU) induced by elevated temperature without Ni²⁺ and with Ni²⁺ in 0.07 M concentration in D₂O (～0.4 [Ni]/[P]). The temperature was varied from 20° C to 90° C. The double-stranded conformation of poly(rA)?poly(rU) was observed at room temperature (20° C—23° C) with and without Ni²⁺ ions. In the absence of Ni²⁺ ions, partial double- to triple-strand transition of poly(rA) ?poly(rU) occurred at 58° C, whereas only single-stranded molecules existed at 70° C. While poly(rU) did not display significant helical structure, poly(rA) still maintained some helicity at this temperature. Ni²⁺ ions significantly stabilized the triple-helical structure. The temperature range of the stable triple-helix was between 45° C and 70° C with maximum stability around 53° C. Triple-to single-stranded transition of poly(rA) ?poly(rU) occurred around 72° C with loss of base stacking in single-stranded molecules. Stacked or aggregated structures of poly(rA) formed around 86° C. Hysteresis took place in the presence of Ni²⁺ during the reverse transition from the triple-stranded to the double-stranded form upon cooling. Reverse Hoogsteen type of hydrogen-bonding of the third strand in the triplex was suggested to be the most probable model for the triple-helical structure. VCD spectroscopy demonstrated significant advantages over infrared absorption or the related electronic CD spectroscopy.     

A vibrational spectroscopic study of the metastable form of associated polyinosinic acid

We have studied by Raman and ir spectroscopy the metastable complex formed by the self-association of polyinosinic acid in aqueous solution. The complex is easily prepared by quickly cooling to ca. 0°C a warm solution of the polyribonucleotide to which a small amount of rubidium salt has been added. Upon heating, this metastable form melts cooperatively near 13°C, well below the dissociation temperature of a stable four-stranded complex, which occurs at 47°C in the same conditions. The presence of several components in the stretching-mode region of the carbonyl groups in the vibrational spectra of the metastable complex suggests that it also has a parallel four-stranded structure. The difference in structure between the two forms is believed to be caused by the presence of fewer metal ions in the central channel of the metastable complex, in agreement with conclusions reached in previous investigations. The Raman spectra further show that the ribose units in the metastable form have a C3′-endo conformation, in contrast with the stable form, for which we have previously suggested a mixed C2′-endo/C3′-endo conformation. © 1996 John Wiley & Sons, Inc.     

New Strategies for the Chemical Synthesis of Biologically Important Nucleic Acid Derivatives

Abstract

This paper describes general methods for the synthesis of N-phosphorylated ribonucleosides and oligonucleotides containing a 2′-O-phosphorylated or 2′-O-thiophosphorylated ribonucleoside. The NMR-based conformational analysis and computational molecular dynamics simulation of the 2′-O-phosphorylated ribonucleoside residue in such modified oligonucleotides suggested that the ribose residue existed preferentially in a C2′-endo conformation. It was also found that simple heating of 2′-O-phosphorylated oligonucleotides resulted in rapid dethiophosphorylation.     

Structural and Conformational Studies on Deoxyguanosyl-3′,5′-Deoxyadenosine Monophosphate and Its Ethyl Phosphotriester Analogs - Left-Handed Dimers

Abstract

The mode of base-base stacking, the handedness and the sugar(dGpA)phosphate backbone conformation of deoxyguanosyl 3′-5′ deoxyadenosine and its diastereomeric ethyl phosphotriester analogs were studied by ¹H NMR, UV and CD spectroscopy. The results indicate the three dimers are left-handed, while the sugar phosphate backbone is comprised predominantly of C_2′-endo, gg (C_4′-C_5′) and g′g′ (C_5′-O) conformers. The two bases are extensively stacked and interact about 90° along the dyad axes. The extent of base overlap in dGpA is slightly greater than in either ethyl phosphotriester analog. The absolute configurations of the two ethyl phosphotriester diastereoisomers of dGpA can be assigned by one-dimensional and two-dimensional ¹H NMR nuclear Overhauser enhancement experiments.     

The conformational properties of α,β‐dehydroamino acids with a C‐terminal ester group

α,β‐Dehydroamino acid esters occur in nature. To investigate their conformational properties, a systematic theoretical analysis was performed on the model molecules Ac‐ΔXaa‐OMe [ΔXaa = ΔAla, (E)‐ΔAbu, (Z)‐ΔAbu, ΔVal] at the B3LYP/6‐311+ + G(d,p) level in the gas phase as well as in chloroform and water solutions with the self‐consistent reaction field‐polarisable continuum model method. The Fourier transform IR spectra in CCl₄ and CHCl₃ have been analysed as well as the analogous solid state conformations drawn from The Cambridge Structural Database. The ΔAla residue has a considerable tendency to adopt planar conformations C5 (?, ψ ≈ ? 180°, 180°) and β2 (?, ψ ≈ ? 180°, 0°), regardless of the environment. The ΔVal residue prefers the conformation β2 (?, ψ ≈ ? 120°, 0°) in a low polar environment, but the conformations α (?, ψ ≈ ? 55°, 35°) and β (?, ψ ≈ ? 55°, 145°) when the polarity increases. The ΔAbu residues reveal intermediate properties, but their conformational dispositions depend on configuration of the side chain of residue: (E)‐ΔAbu is similar to ΔAla, whereas (Z)‐ΔAbu to ΔVal. Results indicate that the low‐energy conformation β2 is the characteristic feature of dehydroamino acid esters. The studied molecules constitute conformational patterns for dehydroamino acid esters with various side chain substituents in either or both Z and E positions. Copyright © 2011 European Peptide Society and John Wiley & Sons, Ltd.     

Theoretical studies of DNA-RNA hybrid conformations.

Molecular modelling has been used to probe the conformational preferences of double stranded DNA-RNA hybrids. As might be expected, the sugars of the DNA strand have higher conformational flexibility, but, for the majority of the repetitive sequences studied, these sugars prefer a C2-endo pucker, while ribose sugars uniformly adopt a C3-endo pucker. This gives rise to a strongly heteronomous duplex conformation. One exception to this rule involves the thymidine strand of poly(dT).poly(rA), which marginally prefers a C3-endo pucker. Our study further indicates that the DNA strands of the hybrids favour backbone torsions in the canonical B domain, rather than the modified values proposed on the basis of fibre diffraction studies. Backbone conformational transitions can nevertheless be induced leading to an alpha gamma-flip (alpha:gamma, g-/g(+)-->t/t) or to the alpha beta gamma-flip form proposed from fibre studies (alpha:beta:gamma, g-/t/g(+)-->t/g+/t). The latter transition is also found to be linked to BI-->BII transitions (epsilon:zeta, t/g(-)-->g-/t).