SUMMARY
The fact that sugars, amino acids, and the biological polymers they construct exist exclusively in one of two possible mirror-image forms has fascinated scientists and laymen alike for more than a century. Yet, it was only in the late 20th century that experimental studies began to probe how biological homochirality, a signature of life, arose from a prebiotic world that presumably contained equal amounts of both mirror-image forms of these molecules. This review discusses experimental studies aimed at understanding how chemical reactions, physical processes, or a combination of both may provide prebiotically relevant mechanisms for the enrichment of one form of a chiral molecule over the other to allow for the emergence of biological homochirality.
1. INTRODUCTION
The biopolymers that characterize life on Earth, and the molecular building blocks from which they are constructed, are both chiral and single-handed: that is, they have the potential to exist as either one of two nonsuperimposable mirror-image forms (Fig. 1), and they are selectively biosynthesized in only one of the two forms. Abiotic synthesis of chiral molecules in the absence of some type of chiral directing force produces an equal (racemic) mixture of both mirror-image molecules (enantiomers). The molecular “chirality” (a term originally coined by Kelvin 1904) of biological molecules is thus considered to be a fundamental signature of life (Blackmond 2010). Understanding how modern biology emerged from a presumably racemic prebiotic world represents an important step in understanding the origin of life.
Figure 1.
(A) Mirror-image molecules of alanine, a proteinogenic amino acid, and ribose, a pentose sugar. (B) Right-handed α-helix structures of a peptide from amino acids (left) and RNA from ribonucleotides (right).
In the history of chirality at both the molecular and macroscopic levels, investigations of chemical reactions that produce chiral molecules have been interwoven with studies of their physical properties. Although it is commonly agreed that the concept of molecular chirality was first introduced in Pasteur’s famous 1848 physical separation of the mirror-image crystals of a tartrate salt (Pasteur 1848), the molecular basis of chirality was not in fact established for a further quarter century, when Le Bel and van’t Hoff independently established the tetrahedral carbon atom (Le Bel 1874; van’t Hoff 1874). This finding clarified that such an atom with four different substituents would be a chiral center with two mirror-image forms. Similarly, the physical phase behavior of amino acids was well-studied (Roozeboom 1899) a half century before the macroscopic helicity of biopolymers was characterized (Pauling et al. 1951; Dunitz 2001), which in turn preceded our certain knowledge of which of the two hands of the monomers (called enantiomers) is favored by biology (Cahn et al. 1956).
RNA, DNA, and polypeptides all form supramolecular right-handed α-helix structures, even while the amino acid molecules that make up peptides are designated as left-handed (l), and the molecular building blocks that comprise RNA and DNA—the sugars ribose and deoxyribose—are called right-handed (d) (Fig. 1). Although the focus of RNA world chemistry tends to fall on these macroscopic structures without questioning how single-handedness arose at the molecular level, an important consideration is how the relative amounts of the two hands of the monomers, given as percent enantiomeric excess (ee) (% ee = 100% * (d − l)/(d + l)), influences the production of the biopolymers. Polymerization of RNA is effectively inhibited if a monomeric nucleotide of the wrong chirality is ligated to a growing chain (Joyce et al. 1984). Proteins, in contrast, are rather more promiscuous; incorporation of amino acid residues of opposite chirality in nonribosomal peptides can occur and has even been shown in some cases to add structural and functional diversification as well as to impart chemical robustness. However, this opposite chirality is achieved not by incorporating unnatural d-amino acid molecular building blocks but through posttranslational conversion of the natural hand of an amino acid molecule in a peptide chain to its enantiomer (Kreil 1997). Thus, the establishment of a highly enantioenriched, if not enantiopure (ee = 100%) pool of d-sugar and l-amino acid molecular building blocks would appear to be a prerequisite for formation of the informational polymers implicated in the origin of life.
2. MODELS FOR THE ORIGIN OF HOMOCHIRALITY
Models for how homochirality might have emerged at the molecular level have been proposed since the early 1950s (Frank 1953). Interestingly, theoretical treatments preceded direct experimental investigations by nearly half a century. The question has two parts. The first concerns “symmetry breaking”: What could have served as the original template for biasing production of one enantiomer over the other in the prebiotic world? The second concerns “amplification”: How could a small imbalance of enantiomers be sustained and propagated to give us the biological world of single chirality that surrounds us?
2.1. Symmetry Breaking
Symmetry breaking is a term that has different meanings in different branches of science. To a physicist, it is a phenomenon in which infinitesimally small fluctuations acting on a system decide the system’s fate by choosing which branch of a bifurcation is taken when crossing a critical point. To an outside observer unaware of the fluctuations (or “noise”), the choice will appear arbitrary. To a biologist, symmetry breaking is the process by which uniformity or invariance in a system is broken, linked to functional diversification from molecular assemblies to subcellular structures to cell types. To a chemist, symmetry breaking is the spontaneous generation of an excess of one enantiomer of a chiral molecule over the other in the absence of an external chiral source.
The chemist’s definition of chirality meets that of the physicist’s in the concept of a parity inversion, an operation that transforms a physical phenomenon (or a molecule) into its mirror image. Parity is conserved in electromagnetism, gravity, and strong interactions, but in the mid-20th century, it was discovered that parity is not conserved (“parity violation”) in weak interactions. One of the consequences of parity violation is that a very small energy difference exists between enantiomers that previously had been considered identical. This finding led many to consider possible implications for the origin of biological homochirality. Work aimed at estimating the magnitude of this (exceedingly small) energy difference is ongoing, and although the question is not yet settled (Quack 2002), a relationship between biological homochirality and parity violation energy difference of enantiomers is not yet supported by either theoretical or experimental findings.
2.2. Chiral Amplification
Evidence of small enantiomeric excesses toward l-amino acids found in chondritic meteorite deposits (Elsila et al. 2016) allows the hypothesis that the initial imbalance between enantiomers on earth may have been seeded from an extraterrestrial source. A small imbalance is, however, a necessary but not sufficient condition to explain the emergence of homochirality, which requires some type of amplification or propagation mechanism following symmetry breaking. Thus, whether symmetry breaking to provide an imbalance in enantiomers was preordained or came about by chance, arising on earth or elsewhere, an amplification mechanism remains the key to increasing enantiomeric excess and ultimately to approaching the homochiral state. Experimental studies aimed at uncovering such processes, which began in earnest in the last decade of the 20th century, may be divided into either chemical or physical processes. The remainder of this review will highlight some of these experimental findings.
3. CHEMICAL MODELS
Studies exploring how enantioenrichment may result from chemical transformations fall into a number of categories, including autocatalytic “far-from-equilibrium” chiral amplification (Fig. 2) and reactions mediated by chiral catalysts or chiral auxiliaries (Fig. 3). The latter group of reactions includes the formose carbohydrate synthesis, the Strecker amino acid synthesis, the Powner/Sutherland synthesis of RNA precursors, and chirality transfer reactions such as transaminations, and all involve chemistry that might occur under prebiotically plausible conditions. In contrast, the Soai alkylation of pyrimidyl aldehydes (Soai et al. 1995), which is the sole documented example of chiral amplification via autocatalysis, requires conditions far removed from those thought to exemplify the prebiotic world. However, because this reaction provided the first experimental proof-of-concept of earlier theoretical proposals, its study serves as a model for understanding how homochirality might have emerged and may help us search for prebiotically plausible reactions with similar characteristics.
Figure 2.
Autocatalytic amplification of enantiomeric excess in the Soai alkylation of pyrimidyl aldehydes.
Figure 3.
Prebiotically plausible reactions showing enantioenrichment of either sugars or amino acids.
3.1. Homochirality via Asymmetric Autocatalysis
In 1953 (a good year for research reports related to the origin of life), a mathematical model for the evolution of homochirality was proposed based on a chiral molecule that catalyzes its own self-production and at the same time acts to suppress synthesis of its enantiomer (Frank 1953). The last sentence of this theoretical work, which captivated several generations of chemists, contained an exhortation to experimental chemists: “a laboratory demonstration may not be impossible.” More than 40 years passed before Soai and coworkers met this challenge with a report of the autocatalytic alkylation of pyrimidyl aldehydes with diisopropylzinc (Soai et al. 1995). The rate of the reaction is not only accelerated by addition of catalytic amounts of its own product, but this autocatalytic product may ultimately be formed in very “high” enantiomeric excess starting from a very “low” enantiomeric excess in the original catalyst (Fig. 2). Since this initial discovery, Soai’s group has gone on to present remarkable further observations of asymmetric amplification in the reaction that now bears his name. Enantiomeric excesses as high as 85% were reported for a reaction initiated with a 0.1% ee mixture of chiral molecules produced from exposure to circularly polarized light (Shibata et al. 1998). Asymmetric amplification has also been observed for the reaction initiated by inorganic chiral materials such as quartz (Soai et al. 1999). Most recently, Soai has shown that the reaction may be selectively triggered solely by the minute mirror-image difference provided by isotope chirality of an initiator molecule (Kawasaki et al. 2009), showing that the reaction needs only an extremely small nudge to direct it consistently to the left or to the right.
The first mechanistic rationalization of this extraordinary reaction was reported in 2001 (Blackmond et al. 2001). A kinetic model developed based on highly accurate in situ measurements of the reaction’s progress independently predicted both the temporal degree of asymmetric amplification, confirmed by compositional analysis, and the relative concentrations of the catalyst species, confirmed by nuclear magnetic resonance (NMR) spectroscopy. The reaction product dimerizes stochastically to form the active autocatalyst in the case of homochiral dimers (DD and LL), with the heterochiral dimer (DL) as an inactive reservoir. Figure 4 shows how the kinetic model compares with experimental data for asymmetric amplification in the Soai reaction performed out with two different initial catalyst ee values. This work showed that the Soai reaction couples autocatalysis with a form of “mutual antagonism” between enantiomers, thus evoking the main features of the Frank model. Further mechanistic studies have refined this reaction as a model for symmetry breaking and autocatalytic amplification of ee. The structure and possible role of tetrameric catalysts first proposed by Brown and coworkers (Gridnev and Brown 2004) was supported by kinetic and spectroscopic measurements by Blackmond, Brown, and coworkers (Buono and Blackmond 2003, Quaranta et al. 2010) before Soai and coworkers (Matsumoto et al. 2015) ultimately obtained a crystal structure that confirmed the tetrameric species first proposed by Brown. Most recently, a mechanistic rationalization for the role of isotopically chiral molecules in the Soai reaction has shed light on both the processes of symmetry breaking and asymmetric amplification via autocatalysis (Hawbaker and Blackmond 2018).
Figure 4.
Blackmond/Brown model (left) and product enantiomeric excess as a function of fraction conversion of substrate (right) predicted from reaction rate profiles fit to the kinetic model (blue lines) and corroborated by analysis of experimental enantiomeric excess (ee) data.
Because small-molecule autocatalysis may be thought of as the simplest form of self-replication, it remains an appealing scenario for the RNA community accustomed to believing about macromolecular self-replication. The discovery of a prebiotically relevant reaction, or a network of reactions, that obey the precepts of Frank model autocatalysis remains something of a “Holy Grail” for researchers probing the origin of biological homochirality (Blackmond 2004).
3.2. Reactions Mediated by Chiral Entities
A number of different transformations have been documented that produce enantioenriched sugar or amino acid building blocks under conditions with greater prebiotic relevance than the Soai autocatalytic system discussed above. Two venerable reactions known for more than a century and a half provide routes to the two classes of biological molecules for which chirality is key: the formose sugar synthesis, discovered in 1861 (Butlerow 1861) and unveiled mechanistically by Breslow in 1959 (Breslow 1959), and the Strecker amino acid synthesis discovered in 1850 (Strecker 1850). Although most reports do not address chirality, recent studies have begun to show how chiral catalysts or auxiliaries could provide partial product enantioenrichment. Interestingly, these reactions invoke a kind of synergy between the sugars and amino acids, as one of these two classes of molecule helps to direct enantioselectivity in the synthesis of the other: amino acids act as catalysts to enantioenrich sugars in the formose reaction (Fig. 3A), and sugars enantioselectively resolve amino acid precursors in the Strecker hydration of aminonitriles (Fig. 3B).
The Strecker reaction between aldehydes, cyanide, and ammonia represents a prebiotically plausible route to amino acids, forming first a racemic mixture of aminonitriles. Directing the hydration of these molecules in a dynamic kinetic resolution has been proposed as a pathway for enantioenrichment, and C4-C6 aldehydic carbohydrates can act as catalysts in this transformation. Derivatives of these sugars have been found in meteorites with significant excesses toward the natural d-sugars. Strikingly, mixtures of the natural d-pentoses produce enantioenriched l-aminoamides, which are then further hydrolyzed to the natural l-amino acids (Fig. 3B). This work reiterates the “systems chemistry” aspect of emergence of enantioenrichment from complex mixtures, and it hints at a prebiotic role for other pentose sugars that would have been present in quantities similar to ribose and deoxyribose before these sugars were ultimately chosen for their role in biological polymers (Wagner et al. 2016).
The Powner/Sutherland synthesis of RNA (Powner et al. 2009) represented a leap forward for the RNA world hypothesis because it showed for the first time a synthesis of activated RNA nucleotide monomers from simple prebiotically plausible feedstock molecules. Starting from d-glyceraldehyde, the synthesis bypasses the problematic step of combining ribose with a nucleobase. The work also highlighted “systems chemistry” aspects of emergent reactivity in complex mixtures. Enantioenrichment in this reaction network was established later when it was shown (Hein et al. 2011) that natural l-amino acids preferentially sequester unnatural l-glyceraldehyde, leaving d-glyceraldehyde free for RNA synthesis (Fig. 3C). Even partial enantioenrichment suffices to produce homochiral RNA building blocks; enantiopure crystals of the ribo-amino-oxazoline naturally precipitate from reaction mixtures above 20% ee.
Transfer of chirality from nonracemic meteoritic amino acids to proteinogenic amino acids was shown by Breslow and coworkers (Levine et al. 2008) in transamination reactions catalyzed by Cu ions (Fig. 3D). This work suggests how chirality first seeded extraterrestrially could provide some level of enantioenrichment in the building blocks of life. However, because the enantiomeric excess of the reaction products is lower than that of the molecules from which they are transferred, further amplification mechanisms would be required to produce significant enantioenrichment.
4. PHYSICAL MODELS
Understanding how the physical properties of chiral molecules might be exploited for enantioenrichment requires an understanding of their physical phase behavior—their solubilities and the manner in which they crystallize (Jacques et al. 1994). These concepts, which have been studied extensively for more than a century, are illustrated in Figure 5. When both enantiomers of a molecule are present in solution, crystallization proceeds either with both enantiomers mixed in a single crystal or with enantiomers forming separate crystals. The formation of separate d and l crystals, as in those Pasteur separated with his tweezers, are known as “conglomerates” (Fig. 5, right panel). When the mixed enantiomers form a regular 1:1 d:l matrix, the molecule is called a “racemic compound” (Fig. 5, left panel). The difference in the two types of crystals comes about as a result of characteristics of the molecules that make their solid phase stability greater with heterochiral interactions or homochiral interactions. The former makes up ∼90% of all known chiral compounds, and indeed 17 of the 19 proteinogenic amino acids are racemic compounds.
Figure 5.
Equilibrium between chiral crystals and their saturated solution phases for systems comprised of an unequal number of d and l molecules. (Right) Racemic compound, in which heterochiral interactions are stronger than homochiral interactions; (left) conglomerate, in which homochiral interactions dominate.
When a system containing an unequal number of d and l molecules in a solvent reaches equilibrium between solid and solution phase molecules, the Gibbs phase rule for a ternary system (two enantiomers and one solvent) with three phases (two solid phases and one solution phase) dictates that, at fixed temperature and pressure, the solution composition is fixed at a composition characteristic of that system known as its eutectic composition. An important implication of the phase rule is that a partitioning of enantiomers occurs between the solution and solid in both cases. For conglomerates, because the solubilities of the two enantiomers are identical, the saturated solution will contain an equal number of d and l molecules regardless of how great the overall imbalance between d and l, suggesting the potential for enantioenrichment in the solid phase. For racemic compounds with an unequal number of d and l molecules, the solid phase will form the heterochiral 1:1 d:l solid with all of the minor enantiomer present in the solid phase, while the remaining solid phase molecules of the major enantiomer will be left to form homochiral crystals. The relative solubility of the d:l solid compared with that of the homochiral solid dictates the magnitude of the solution phase imbalance between d and l. In this case, enantioenrichment in the solution phase is common. Below, we discuss models developed for the emergence of homochirality for each type of crystal in turn.
4.1. “Eve Crystal” Model for Conglomerates
It has been known for more than a hundred years that certain molecules such as NaClO3 are achiral in solution but crystallize as conglomerates, typically forming equal amounts of left and right-handed crystals (Kipping and Pope 1898). Under some conditions, the system breaks symmetry during the crystallization and produces more of one hand than the other, even in the absence of a detectable chiral source. The most striking example of this phenomenon was reported by Kondepudi (Kondepudi et al. 1990) who showed that when a homogeneous solution of achiral NaClO3 was cooled to initiate crystallization, the process could be directed if it was accompanied by rapid stirring. In this case, all of the crystals formed were of single chirality, randomly left-handed or right-handed in repeated experiments. This was rationalized by considering the dynamics of crystallization: Formation of the very first crystal (primary nucleation) from a homogeneous supersaturated solution is energetically unfavorable, although crystal growth by adding molecules to crystals already present (secondary nucleation) occurs much more readily. Under rapid stirring, if the first crystal formed, or “Eve” crystal, is broken by into thousands of smaller crystals by impact with the stirring bar, all of these “daughter” crystals are necessarily of the same chiral form, and they grow rapidly by secondary nucleation from solution molecules. If secondary nucleation occurs fast enough before nucleation of any new primary crystals, a single chiral solid state may result (McBride and Carter 1991). This phenomenon, shown in Figure 6 bears resemblance to “far-from-equilibrium” autocatalytic reaction processes such as the Soai reaction discussed earlier.
Figure 6.
Effect of stirring on rates of primary (A) versus secondary (B) nucleation in the “Eve crystal” model of conglomerate-forming NaClO3.
4.2. Attrition-Enhanced Deracemization of Conglomerates
The same achiral salt NaClO3 became the subject of another intriguing process resulting in solid phase homochirality about fifteen years after Kondepudi’s Eve crystal model was introduced. A report by Viedma (Viedma 2005) described a remarkable experiment that starts at what would be the end of a conventional crystallization with an equal number of right- and left-hand crystals of NaClO3 in saturated aqueous solution. Because the system is not supersaturated, no new crystals nucleate; the only processes occurring in the flask are the continual dissolution and reaccretion of NaClO3 molecules to and from existing crystals, and these rates are balanced at equilibrium. Thermodynamics tells us that no net change should occur, and that is exactly what has been found in such experiments for more than a hundred years. Viedma changed all this when he observed that the system evolved over time to “one” of the two chiral solids in a random fashion, provided that he added glass beads to the stirred vial. Attrition by glass beads produces a greater number of smaller crystals, which show higher solubility according to the Gibbs-Thomson rule, causing a slight supersaturation of NaClO3 in solution. Not sufficiently supersaturated to support primary nucleation, the system strives to redress the balance between solid and solution by increasing the rate of reaccretion of solution phase NaClO3 onto existing crystals. A key point is that once a molecule of NaClO3 dissolves from a crystal, it no longer possesses chirality and it retains no memory of the chiral form it previously showed as part of a crystal. Solution-phase NaClO3 thus has no preference for reaccreting to a left- or right-handed crystal. What solution phase molecules do have, however, is a preference for adding to larger crystals over smaller ones, a phenomenon known as Ostwald ripening. If, by chance, the system contains a predominance of large crystals of one hand, solution phase NaClO3 will preferentially add to these crystals, and the quantity of this enantiomorphic solid will increase relative to its mirror-image form (Fig. 7). Evolution of solid phase homochirality in this case requires only a chance imbalance in the crystal size of left versus right-hand crystals, with the solution phase serving as the conduit through which the molecules forget their solid-state chiral history and are free to choose a new solid-state chiral destiny.
Figure 7.
Evolution of solid phase homochirality based on dissolution and reaccretion of molecules from small crystals (shown in blue) of one enantiomer onto larger crystals (shown in purple) of the other enantiomer, through the conduit of solution phase interconversion between enantiomers.
These results led many to consider a possible extension of this process from the achiral NaClO3 to systems more relevant to the origin of life, intrinsically chiral molecules that form conglomerate solids. In this case, the solution conduit between the two solids arises by the process through which chiral molecules rapidly interconvert between their left and right forms, known as racemization. This was successfully shown first for an amino acid derivative (Noorduin et al. 2008) and then for the proteinogenic amino acid aspartic acid (Viedma et al. 2008).
4.3. Crystal Engineering of Racemic Compounds
Morowitz was the first to recognize that solution-phase enantioenrichment is possible for racemic compounds if the heterochiral crystal is relatively insoluble compared with the homochiral crystal (Morowitz, 1969). This work was elaborated by measuring the eutectic composition for a variety of amino acids and nucleosides (Klussmann et al. 2006a; Breslow and Levine 2006; Breslow and Cheng 2009). The degree of chiral amplification is dictated by the thermodynamic properties of the particular compound. The proteinogenic amino acid serine shows a eutectic of 99% ee, meaning that a nearly homochiral solution is achievable even when the overall ee of the solid and solution combined is close to racemic. Valine, on the other hand, shows a eutectic of 47% ee, which means that a much lower level of chiral amplification is possible for this amino acid. Further work discovered that the cocrystallization of a variety of small molecules with amino acids can alter the relative heterochiral/homochiral solubility and thus “engineer” the eutectic composition (Klussmann et al. 2006b; 2007). This finding helped to generalize the eutectic model, revealing a number of prebiotically plausible cocrystallizations that raised the eutectic composition of amino acids. For example, when valine cocrystallizes with fumaric acid, its eutectic increases to 99% ee, affording a path to solution–phase homochirality. Similarly, proline’s eutectic composition increases from 50% ee to 99% ee when chloroform cocrystallizes with the racemic compound (Fig. 8). Similar concepts have been invoked to rationalize enantioenrichment during sublimation of amino acids (Fletcher et al. 2007).
Figure 8.
Cosolvate enriches the solution phase enantiomeric excess by suppressing the solutility of the racemic compound. (Right) Crystal structure of LD proline with CH3Cl.
5. COMBINING PHYSICAL AND CHEMICAL APPROACHES
A number of examples illustrate how prebiotic chemistry resulting in amplification of enantiomeric excesses of amino acids and sugars has been aided by physical processes. The selective thermodynamic partitioning of amino acid enantiomers between solution and solid phases has been invoked as a possible prebiotic mechanism for solution phase amplification of enantiomeric excess.
A combination of these physical and chemical amplification processes was shown for the proline-mediated reaction of glyceraldehyde and concomitant production of enantioenriched ribo-amino-oxazoline (Fig. 4C). Enantioenrichment of 1% ee l-proline was achieved by forming the CHCl3-dl-proline cosolvate (Klussmann et al. 2006b). Nearly enantiopure solution phase proline was recovered and mixed with racemic glyceraldehyde and 2-amino-oxazole in aqueous solution to produce enantioenriched ribo- and arabino-amino-oxazolines in solution, from which enantiopure crystals of the ribo-amino-oxazoline precipitated (Hein et al. 2011). Thus, chemical amplification of ee is augmented by two physical amplification processes: enantioenrichment of the amino acid before the chemical reaction, and the selective crystallization of enantiopure ribo-amino-oxazoline following the chemical reaction.
A likely prebiotic scenario suggests that a complex pool of organic molecules would likely be present in any potential reaction medium. To test the robustness of these chirality amplification processes in multicomponent mixtures, the reaction of racemic glyceraldehyde with 2-amino-oxazole was performed in mixtures of a variety of different amino acids. Enantiopure crystals of ribo-amino-oxazoline were successfully obtained directly from crude reaction mixtures containing as many as fourteen of the nineteen chiral, proteinogenic amino acids (Hein et al. 2011). The emergence of molecules of single chirality from complex, multicomponent mixtures is a proof of “systems chemistry” (von Kiedrowski 2005) and supports the robustness of the processes under potential prebiotic conditions.
6. CONCLUDING REMARKS
The implications of the single chirality of biological molecules may be viewed in the context of increasing complexity at both the molecular and macroscopic levels. In the molecular sciences research, this has been codified as the field of “systems chemistry” (von Kiedrowski, 2005), which seeks to understand the chemical roots of biological organization by studying the emergence of system properties that may be different from those showed individually by the components in isolation. The abiotic construction of homochiral genetic polymers from molecular building blocks implies at least some minimal degree of enantioenrichment at the molecular level, if not molecular homochirality, to ensure efficiency as RNA or peptide chains grow in length. This review has described a variety of work invoking either chemical or physical processes, or both, that might allow the emergence of biological homochirality.
Footnotes
Editors: Thomas R. Cech, Joan A. Steitz, and John F. Atkins
Additional Perspectives on RNA Worlds available at www.cshperspectives.org
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