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10 extraordinary papers Within days, Watson and Crick had built a identify the full set of codons was completed in forensics, and research into more-futuristic new model of DNA from metal parts. Wilkins by 1966, with Har Gobind Khorana contributing applications, such as DNA-based computing, immediately accepted that it was correct. It the sequences of bases in several codons from is well advanced. was agreed between the two groups that they his experiments with synthetic polynucleotides Paradoxically, Watson and Crick’s iconic would publish three papers simultaneously in (see go..com/2hebk3k). structure has also made it possible to recog- Nature, with the King’s researchers comment- With Fred Sanger and colleagues’ publica- nize the shortcomings of the central dogma, ing on the fit of Watson and Crick’s structure tion16 of an efficient method for sequencing with the discovery of small RNAs that can reg- to the experimental data, and Franklin and DNA in 1977, the way was open for the com- ulate gene expression, and of environmental Gosling publishing Photograph 51 for the plete reading of the genetic information in factors that induce heritable epigenetic first time7,8. any species. The task was completed for the change. No doubt, the concept of the double The Cambridge pair acknowledged in their genome by 2003, another milestone helix will continue to underpin discoveries in paper that they knew of “the general nature in the history of DNA. for decades to come. of the unpublished experimental results and Watson devoted most of the rest of his ideas” of the King’s workers, but it wasn’t until career to education and scientific administra- Georgina Ferry is a writer based in The Double Helix, Watson’s explosive account tion as head of the Cold Spring Harbor Labo- Oxford, UK. A revised edition of her biography of the discovery, was published in 1968 that ratory in Long Island, New York, and serving Dorothy Crowfoot Hodgkin has just been it became clear how they obtained access to (briefly) as the first head of the US National published by Bloomsbury Reader. those results. Franklin had died of a Center for Human Genome Research, now the 1. Watson, J. D. & Crick, F. H. C. Nature 171, 737–738 (1953). decade previously; her death prevented her National Human Genome Research Institute. 2. Avery, O. T., MacLeod, C. M. & McCarty, M. J. Exp. Med. 79, from sharing the Nobel prize awarded to Always outspoken, he was eventually removed 137–158 (1944). Watson, Crick and Wilkins in 1962. from his emeritus position at Cold Spring Har- 3. Hershey, A. D. & Chase, M. J. Gen. Physiol. 36, 39–56 The immediate reception of the double-he- bor when he repeatedly aired controversial (1952). 4. Pauling, L., Corey, R. B. & Branson, H. R. Proc. Natl Acad. 9 lix model was surprisingly muted ,perhaps opinions about genetics, race and intelligence. Sci. USA 37, 205–211 (1951). because there was no obvious mechanism Crick continued to tackle hard problems in 5. Cochran, W., Crick, F. H. & Vand, V. Acta Crystallogr. 5, to explain its role in protein synthesis. In a science, moving in 1977 from Cambridge to the 581–586 (1952). 6. Vischer, E. & Chargaff, E. J. Biol. Chem. 176, 703–714 landmark talk in 1957, Crick proposed that Salk Institute in La Jolla, California, where he (1948). the sequence encoded the sequence spent the rest of his working on the neural 7. Wilkins, M. H. F., Stokes, A. R. & Wilson, H. R. Nature 171, of amino in a protein, and that protein basis of consciousness17 and, specifically, of 738–740 (1953). 8. Franklin, R. E. & Gosling, R. G. Nature 171, 740–741 (1953). production involved RNA both as a template visual perception. He died in 2004, aged 88. 9. Olby, R. Nature 421, 402–405 (2003). and as an ‘adaptor’ that would enable amino The double helix put genetics on a 10. Brenner, S. Proc. Natl Acad. Sci. USA 43, 687–694 (1957). acids to be attached to one another in the right physical footing that would shed on 11. Crick, F. H. C. Symp. Soc. Exp. Biol. 12, 138–163 (1958). 12. Meselson, M. & Stahl, F. W. Proc. Natl Acad. Sci. USA 44, order. He also supported the suggestion — almost every aspect of modern biology and 671–682 (1958). originally made informally by the physicist medicine. Examples include the migration of 13. Lehman, I. R., Bessman, M. J., Simms, E. S. & Kornberg, A. George Gamow to the members of the ‘RNA human populations throughout history; ecol- J. Biol. Chem. 233, 163–170 (1958). Tie Club’ convened by Gamow and Watson, ogy and ; cancer-causing muta- 14. Nirenberg, M. W. & Matthaei, J. H. Proc. Natl Acad. Sci. USA 47, 1588–1602 (1961). but also independently proposed by biolo- tions in tumours and their drug treatment; 15. Crick, F. H. C., Barnett, L., Brenner, S. & -Tobin, R. J. gist Sydney Brenner10 — that triplets of bases surveillance of microbial drug resistance in Nature 192, 1227–1232 (1961). (which Brenner called codons) encode the hospitals and the global population; and the 16. Sanger, F., Nicklen, S. & Coulson, A. R. Proc. Natl Acad. Sci. USA 74, 5463–5467 (1977). 20 amino acids commonly found in proteins. diagnosis and treatment of rare congenital dis- 17. Crick, F. H. C. The Astonishing Hypothesis: The Scientific Finally, Crick expounded what he called the eases. DNA analysis has long been established Search for the Soul (Simon & Schuster, 1994). ‘central dogma’ of biology: that information can flow from nucleic acids to proteins, but High- not the other way round11. These predictions were confirmed by experiment in the next few years. In 1958, the biochemists Matthew Meselson and Franklin Detection of a Stahl showed that one DNA strand acts as a template for the formation of a new strand12. strange The same year, Arthur Kornberg and his colleagues published their discovery of the Taku Yamanaka enzyme DNA polymerase13, which adds bases to newly forming strands. Messenger RNA, In 1947, scientists found a previously unseen particle, which transfer RNA and ribosomal RNA were all is now called a neutral . This led to the discovery of quickly identified. elementary known as , and ultimately to the In 1961, Marshall Nirenberg and Heinrich Mat- thaei were the first to crack part of the genetic establishment of the of . code, demonstrating that bacterial extracts synthesize only the amino phenyl­alanine from RNA that contains just one type of RNA In the late 1940s, the physicists George gap between the lead plate and the vertex of base14 (uracil; U). The same year, Crick, his indis- Rochester and Clifford Butler1 observed the tracks indicated that an invisible neutral pensable female technician Leslie Barnett and something unusual in their charged-particle particle had been produced in the plate, had their co-workers reported mutation studies that detector. They were studying­ the inter­actions travelled for a short distance and had then confirmed the existence of the triplet-based between high-energy cosmic rays and a lead decayed into two visible charged particles. code15, and which therefore suggested that the plate in the detector when they spotted The of the was about codon for phenylalanine was UUU. The race to V-shaped particle tracks (Fig. 1a). The small 1,000 that of an , implying

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a b

0 + – K K – ds us ddu uud

– η π0 + – 0 0 + – π – – π – Σ Σ Λ Σ du – – – uu, dd ud sdd suu uu, dd, ss η′ sdu

– – su sd ssd ssu – K– K0 Ξ– Ξ0 Charge

Figure 1 | Particle detection that led to a better understanding of fundamental of many more particles following Rochester and Butler’s work led to a model12,13 physics. a, In 1947, Rochester and Butler1 analysed the particles produced in which all of the known mesons and baryons (two classes of particle) consist of when high-energy cosmic rays hit a lead plate (the broad central stripe) in a elementary particles called up (u), down (d) and strange (s) quarks, along with their charged-. In certain photographs, they spotted evidence of a (denoted by overbars). The η, η′ and π0 mesons comprise mixtures previously undetected, invisible neutral particle decaying into two visible charged of pairs. The mesons and baryons are arranged by their strangeness particles, which were identified by tracks (labelled with arrows). b, The discovery (a quantity that is related to the presence of strange quarks) and .

that it must be a previously unreported type However, a that has S = –1, applies a charge-conjugation transformation of particle. This discovery paved the way for for example, cannot decay into particles that (in which particles are replaced by their many puzzles and surprises in particle physics have S = 0 through the strong , because antiparticles), the right-handed in the decades that followed. strangeness would not be conserved. Instead, becomes a right-handed antineutrino, which At the of Rochester and Butler’s work, this decay must occur much more slowly does exist. The weak force therefore seemed , , and particles through the weak , which allows to conserve CP symmetry (symmetry under called (short for π mesons) had been total strangeness to change. a combined charge-conjugation and identified, and were known to be sufficient As the accuracy of accelerator-based transformation), until such symmetry was to form . Pions were proposed2 in 1935 measurements increased, it became clear found to be broken in neutral-kaon decays. — to explain how protons and neutrons are held that the τ and θ mesons had extremely similar A neutral kaon is a mixture of K0 and K0 together in small atomic nuclei by the strong and lifetimes. Scientists concluded states, and can exist as the CP-even state

nuclear force, and were found experimen- that these mesons must be the same parti- Keven or the CP-odd state Kodd. The lifetime of 3,4 tally in 1947. cle, which is able to decay into two or three Kodd is much longer than that of Keven, so these

While searching for a in cosmic rays, pions. The mess of strange mesons was finally particles were named KL (for ‘K-long’) and KS scientists discovered a different particle5, cleaned up into four particles dubbed (for ‘K-short’), respectively. A useful conse- which is now called a . A heavy charged (short for K mesons): K+ and K0 and their anti- quence of such lifetimes is that, if neutral kaons — particle was then found6 in 1944, followed by particles K– and K0. are produced by firing protons at a target, the

Rochester and Butler’s unstable neutral parti- However, accepting that the τ and θ mesons CP-even KS component quickly decays, leaving

cle. But the discovery of unexpected particles were the same particle raised another prob- only the CP-odd KL component. In 1964, such 11 did not stop there. Then came the τ , lem. A state of two pions has even parity, which KL particles were observed to decay into the which decays into three pions; the θ meson, means that its wavefunction does not change CP-even state of two oppositely charged pions decaying into two pions; the κ meson, decay- sign under a parity transformation (in which (π+π–). Therefore, despite expectations, CP ing into a muon and an invisible particle; the spatial coordinates are flipped). By contrast, symmetry was shown to be broken. Λ0 particle, decaying into a proton and a pion; a state of three pions has odd parity. If the In that same year, physicists proposed a and the list goes on. same particle could decay into two or three model12,13 to explain all of the known mesons In the early 1950s, researchers began pions, did that mean that, contrary to all con- and baryons — a family that includes protons, producing these rare particles in large ventional wisdom, parity is not conserved by neutrons and the Λ0 particle. In the model, quantities by firing protons at targets in particle the weak force? This question, known as the these mesons and baryons consist of elemen- accelerators. The τ, θ and κ mesons and Λ0 parti- τ–θ puzzle, led to the discovery, in 1957, of tary particles known as quarks, which come cle were peculiar, because, although they were such parity-symmetry breaking in cobalt-60 in three types: up, down and strange (Fig. 1b). generated by the strong force, their decay times decays9 and in pion decays10. In 1973, a theoretical model14 showed were much longer than those expected for this A consequence of parity-symmetry breaking that the breaking of CP symmetry could be force. To explain these observations, physicists by the weak force is that elementary particles explained by introducing three more quarks:

proposed a quantity, known as strangeness (S), called can be only left-handed, , top and bottom. In this framework, KL 7,8 that is conserved by the strong force . which means that their and intrinsic can have a small component of Keven that can Protons and neutrons have S = 0, and angular are in opposite directions. decay into the CP-even π+π– state. But unlike through the strong force, can produce a Under a parity transformation, a left-handed other theoretical models, this framework also

pair of strange particles that have S = –1 and neutrino becomes a right-handed neutrino, allows Kodd to decay into the CP-even state S = +1, so that total strangeness is conserved. which does not exist. However, if one then (direct CP violation).

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10 extraordinary papers Many generations of experiments then were carried out to see whether direct CP violation Neuroscience exists. The measurement required extremely high precision, and after many improvements over 25 years, direct CP violation was finally confirmed15,16. Together with the observation Neuronal signals of CP-symmetry breaking in B mesons (mesons that contain a )17,18, the theoreti- thoroughly recorded cal model was confirmed, and helped to estab- lish the standard model of particle physics, Alexander D. Reyes which is the current explanation of the Uni- verse’s particles and . Originally developed to record currents of flowing However, the standard model is not through channel proteins in the membranes of cells, the complete. For instance, it cannot explain why patch-clamp technique has become a true stalwart of the the contains so little , nor what the mysterious substance called dark neuroscience toolbox. is. Researchers are therefore trying to search for a hint of particle physics beyond that of the standard model. For example, Information in the brain is thought to be were obtained by Neher and Sakmann using experiments in Japan19 and Europe20 are using encoded as complex patterns of electrical patch clamp. extremely rare kaon decays to search for such impulses generated by thousands of neuronal The patch-clamp technique is conceptually a hint. cells. Each impulse, known as an action poten- rather simple. Instead of impaling the cells, In retrospect, Rochester and Butler’s tial, is mediated by currents of charged ions a pipette with a relatively large diameter is V-shaped particle tracks are thought to have flowing through a neuron’s membrane. But how pressed against the cell membrane. Under the been caused by a KS, produced in the lead plate, the ions pass through the insulated membrane right conditions, the pipette tip ‘bonds’ with decaying into the π+π– state. Since their work, of the neuron remained a puzzle for many the membrane, forming a tight seal. This sub- kaons have been used to discover strangeness years. In 1976, Erwin Neher and Bert Sakmann stantially reduces the noise compared with that and the breaking of parity and CP symmetries, developed the patch-clamp technique, which encountered using sharp electrodes, because to build the and the standard showed definitively that currents result from the small patch of membrane encompassed model, and now to search for previously the opening of many channel proteins in the by the pipette tip is electrically isolated from unseen particle physics. Could Rochester membrane1. Although the technique was the rest of the cell’s membrane and from the and Butler have ever imagined that they had originally designed to record tiny currents, it environment surrounding the cell (Fig. 1). opened such a treasure chest? has since become one of the most important The tiny currents passing through the few tools in neuroscience for studying electrical channels in the patch were thus observed for Taku Yamanaka is in the Department signals — from those at the molecular scale to the first time. The recording confirmed key of Physics, Osaka University, Toyonaka, the level of networks of neurons. channel properties: when channels open, Osaka 560-0043, Japan. By the 1970s, current flowing through the there is a step-like jump in the current trace e-mail: [email protected] cell was generally accepted to result from and, when they close, a step-like back the opening of many channels in the membrane, to baseline. It was now possible to determine although the underlying mechanism was details such as the statistics of the opening and 1. Rochester, G. D. & Butler, C. C. Nature 160, 855–857 (1947). unknown. At that time, current was commonly closing of channels, the amplitude of the cur- 2. Yukawa, H. Proc. Phys.-Math. Soc. Jpn 17, 48–57 (1935). recorded by impaling tissue with a sharp elec- rents they mediate and the optimal stimuli that 3. Perkins, D. H. Nature 159, 126–127 (1947). trode — a pipette with a very fine point. Unfor- trigger their opening. For this work, Neher and 4. Lattes, C. M. G., Muirhead, H., Occhialini, G. P. S. & Powell, C. F. Nature 159, 694–697 (1947). tunately, however, the signal recorded in this Sakmann were awarded the 1991 Nobel Prize in 5. Neddermeyer, S. H. & Anderson, C. D. Phys. Rev. 51, way was excessively noisy, and so only the large, Physiology or Medicine. 884–886 (1937). ‘macroscopic’ current — the collective current Improvements in patch clamp made it 6. Leprince-Ringuet, L. & L’Héritier, M. C.R. Acad. Sci. 219, 618–620 (1944). mediated by many different types of channel — feasible to study channels in various prepa- 7. Gell-Mann, M. Phys. Rev. 92, 833–834 (1953). that flows through the tissue could be resolved. rations4 to finally address long-standing 8. Nakano, T. & Nishijima, K. Prog. Theor. Phys. 10, 581–582 2 (1953). In 1972, Bernard Katz and Ricardo Miledi , questions. There was particular interest in ver- 5 9. Wu, C. S., Ambler, E., Hayward, R. W., Hoppes, D. D. & pioneers of the biology of the synaptic connec- ifying a model for action-potential generation Hudson, R. P. Phys. Rev. 105, 1413–1415 (1957). tions between cells, managed to infer from the proposed by Nobel laureates Alan Hodgkin and 10. Garwin, R. L., Lederman, L. M. & Weinrich, M. Phys. Rev. 105, 1415–1417 (1957). macroscopic current certain properties of the Andrew Huxley in the 1950s. Specific predic- 11. Christenson, J. H., Cronin, J. W., Fitch, V. L. & Turlay, R. membrane channels, but only after a heroic tions of the model could now be tested directly Phys. Rev. Lett. 13, 138–140 (1964). effort to exclude all possible confounding fac- by examining the current through individual 12. Gell-Mann, M. Phys. Lett. 8, 214–215 (1964). 13. Zweig, G. CERN Rep. No. CERN-TH-401 (1964). tors. The problem was that the macroscopic channels and by observing the changes in cur- 14. Kobayashi, M. & Maskawa, T. Prog. Theor. Phys. 49, current could be influenced by factors not rent that occur when the molecular structure 652–657 (1973). directly related to channel activity, such as of the channel is modified6. Ultimately, the 15. Alavi-Harati, A. et al. (KTeV Collaboration) Phys. Rev. Lett. 83, 22–27 (1999). cell geometry and modulatory processes that model was shown to be mostly correct and 16. The NA48 Collaboration. Eur. Phys. J. C 22, 231–254 regulate cell excitability. Also troublesome was remains the gold standard for computational (2001). that interpretations of macro­scopic-current neuroscientists today. 17. Aubert, B. et al. (BABAR Collaboration) Phys. Rev. Lett. 87, 4 091801 (2001). features were based on unverified assumptions One of the several variants of patch clamp 18. Abe, K. et al. (Belle Collaboration) Phys. Rev. Lett. 87, about the statistics of individual channel activ- — the whole-cell configuration — found an audi- 091802 (2001). ity2,3. Despite Katz and Miledi’s careful analyses, ence with neuroscientists studying electrical 19. Ahn, J. K. et al. (KOTO Collaboration) Phys. Rev. Lett. 122, 021802 (2019). there was a lingering doubt about whether their phenomena in neurons beyond the channel 20. The NA62 Collaboration. Phys. Lett. B 791, 156–166 (2019). conclusions were correct. The crucial data level. To achieve whole-cell recording, the

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