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| "Physics and Life" Paul Davies in: The First Steps of Life in the Universe Proceedings of the Sixth Trieste Conference on Chemical Evolution. Trieste, Italy, 18-22 September. Editors: Chela-Flores, J., Owen, Tobias and Raulin, F. Kluwer Academic Publishers: Dordrecht, The Netherlands. (In preparation.) Physics and Life Lecture in honour of Abdus Salam Paul Davies Physics Department Imperial College London SW7 2AY Fifty years ago, physicists seemed on the verge of solving the problem of life. Inspired by Erwin Schrödinger's book What is Life? (1944), researchers began unraveling the molecular basis of the living cell, in the belief that a solution to both the nature and the origin of life would soon be found. Today, these hopes seem very naïve. Indeed, physics is regarded by most investigators as not especially relevant to the problem of life. To be sure, physics plays an indirect role in life, in two ways. First, life operates in accordance with the laws of physics, but so does everything else, including, for example, the Italian Constitution. Physics is universal, its laws simple, mathematical and general. But life, like the Italian Constitution, is complex, non-mathematical, and very special. Precisely because physics is universal, it is unusual that its principles are crucial for explaining any particular physical system. The second way in which physics has an indirect bearing on life is by providing the basic 'tool kit' which biology requires. It is well known that the existence of life (at least as we know it) depends rather sensitively on the precise nature of the laws of physics, and particularly on the numerical values that nature assigns to various coupling constants and particle masses. This topic often goes under the name 'the anthropic principle' and has been much reviewed (Barrow & Tipler, 1986). Here I shall restrict myself to two simple examples, the first due to Fred Hoyle (Hoyle, 1954). Life is based on carbon. This element did not exist at the birth of the universe, but was made inside large stars. A carbon nucleus forms from the fusion of three helium nuclei. This reaction has a tiny cross-section, and the carbon yield would be paltry were it not for the fortuitous existence of a resonance at just the right energy to correspond to the temperatures of stellar cores. If the strong interaction did not have the strength it does, the universe could have been largely devoid of this life-giving substance. The second example has been discussed by Freeman Dyson (Dyson, 1971), and also concerns the strength of the strong nuclear force. If it were just two per cent stronger, then it would be possible for two protons to overcome their electric repulsion and bind to form a di-proton. This would soon decay via the weak interaction to a deuteron. Dyson considers the consequences of this for the hot big bang theory of the universe. One second after the origin of the universe, the cosmic material was a soup of free protons, neutrons, electrons, etc. During the subsequent few minutes, about 25 per cent of the nuclear matter was converted into helium, the rest being left as hydrogen. If di-protons were possible, the leftover protons would rapidly convert into deuterons, which would then combine to form more helium. The result would be that all the hydrogen would be consumed, leaving a universe composed entirely of helium. There would then be no stable stars like the sun and no water. Life would almost certainly be impossible in such a universe. There is a long list of similar happy accidents in particle physics that make for a remarkably bio-friendly universe - analogous to what science administrators call 'a well-found laboratory'. All this is well and good, but is physics relevant to life's specific and peculiar properties? One person who was convinced that physics plays a direct role in life, at least in its genesis, was Abdus Salam, in whose honour this paper is delivered. His work on molecular chirality (Salam, 1991, 1992) was a bold attempt to trace the well-known handedness of biological molecules to parity violation in electroweak interactions, a subject that he himself founded. If this link is correct, it provides a key biological role for one the most fundamental aspects of particle physics. Whilst not wishing to revisit the topic of chirality here, I shall argue, in the spirit of Salam's work, that physics may enter into biology at a basic level in a number of important ways. In approaching this problem, it is helpful to be reminded of Jacques Monod's celebrated distinction between chance and law, or necessity as he termed it (Monod, 1972). All physical systems come about from a combination of these factors. Some, like crystals, are almost completely determined in their structure and properties by the laws of physics alone, which embody the relevant crystal symmetries. Others, like clouds in the sky, are shaped mostly by chance. In between are systems such as snowflakes, for which the overall hexagonal structure is determined by physics, but the specific filigree details are a matter of happenstance. Where, on this spectrum from pure chance to pure law, does life lie? Opinions vary widely. Monod himself argued that life was pretty much the product of chance, a stupendous chemical fluke unique in the observable universe. By contrast, Christian de Duve (de Duve, 1995) thinks life is a 'cosmic imperative,' more or less bound to occur wherever earthlike conditions prevail. The belief that life is 'written into' the laws of nature is sometimes called biological determinism (Shapiro, 1986). In its most extreme form, as advocated for example by Sidney Fox (Fox, 1988), it asserts that the laws of the universe are cunningly rigged to coax life into being from lifeless chemicals, by favouring the production of just those molecules that life needs. On this manifestly teleological view, life's information content derives from the physical laws that generate the informational molecules. This view is hard to sustain, since the information content, as measured algorithmically (Chaitin, 1990), of the known laws of physics at least, is demonstrably low (Yockey, 1992). That is why crystals, which are determined by those laws, have low information content, being just regular arrays of atoms. By contrast, DNA is a random string of atoms - the 'aperiodic crystal' famously predicted by Schrödinger (1944) - and so has high algorithmic information content; it is then hard to see how such an entity could be a product of law alone. In this respect it is worth noting that although the backbone structure of DNA is determined by the laws of physics and chemistry, the precise sequence of nucleotides - the 'letters of the genetic alphabet' - are not. There are no chemical bonds between successive nucleotides; chemistry is indifferent to the sequence chosen. Those like de Duve who espouse a less teleological and conspiratorial form of biological determinism argue that because the stuff of life is common in the universe, then so must life be. Oft-cited is the commonness of the life-giving elements C,H,N,O,P,S, and the ubiquity of simple organic building blocks like methane, formaldehyde, alcohol and even amino acids. These molecules are easy to make, and are found across the universe, in meteorites, comet tails and even interstellar clouds. Therefore, the argument goes, life should be common too. This argument is, however, flawed. The building blocks of life are easy to make because their synthesis is thermodynamically favoured. But stringing them together in an aqueous environment into complex molecular chains like proteins and RNA is thermodynamically 'uphill. ' Just as a pile of bricks alone don't make a house, so organic building blocks alone don't make life. Put a stick of dynamite under a pile of bricks, and you don't make a house, you just make a mess. In the same way, merely throwing energy willy-nilly at a collection of amino acids, for example, to drive it against the thermodynamic gradient, won't produce a protein. Just as a house requires the delicate assembly of bricks into an elaborate and specific arrangement, so amino acids need to be carefully linked in a precise way to make a functional protein, rather than gunk. The same goes for nucleic acids. A hundred years ago, it was commonly supposed that life is some sort of magic matter, and that life's origin would be analogous to baking a cake. All it needs is the right ingredients mixed in the right order under the right conditions. Today we know that the living cell is less magic matter, more a supercomputer; i.e. it is an information processing and replicating system. The key property that distinguishes life from other forms of complexity is the informational aspect, the message in the genes. Chemistry cannot explain information. Chemistry is the medium of life, but one must not confuse the medium with the message. In the living cell, nucleic acids and proteins, which are scarcely on nodding terms chemically, deal with each other via an information channel, i.e. using software rather than hardware, written in a triplet mathematical code. The advantage of life 'going digital' in this way is much greater flexibility and fidelity (as is also the case with digitization in electronic devices). The situation can be likened to flying a kite versus a radio-controlled plane. A kite is hard-wired to the controller, and is clumsy to control by pulling on the strings. By contrast, a radio-controlled plane is easier to fly because the controller's instructions are digitized and transmitted to the plane, where they are decoded and used to harness local energy sources. The radio waves themselves do not push and pull the plane around; they merely convey the information. Analogously, nucleic acids do not themselves assemble proteins, they relay the instructions for ribosomes to do it. This frees protein assembly from the strictures of chemistry, and permits life to choose whatever amino acid sequences it needs. So, far from deriving from physics and chemistry, biological information is quasi-independent of it. To explain the origin of this information-based control, we need to understand how mere hardware (atoms) wrote its own software. Note that we must do more than simply explain where information per se came from. A gene is a set of coded instructions (e.g. for the manufacture of a protein). To be effective, there must exist a molecular milieu that can decode and interpret the instructions, and carry them out, otherwise the sequence information in the DNA is just so much gobbledygook. The information is therefore semantic in content, i.e. it must mean something (Küppers, 1985). So we are faced with the task of understanding the nature and origin of semantic, or meaningful, information. Since the very concept of information emerged from communication theory in the realm of human discourse, this is no trivial matter. Information is not like mass or energy: you can't tell by looking whether a molecule has it or not. As yet, there is no 'info-dynamics' comparable to the dynamics of matter, let alone an understanding of how 'meaning' emerges in nature. The central puzzle, as it seems to me (Davies, 1998), is that life possesses two apparently contradictory properties. The first is that the key informational content demands randomness (in the algorithmic sense) since order is by definition low in information content. The second is specificity; arbitrary randomness is no good. A protein, for example, is a specific random sequence of amino acids; any old higgledy-piggledy sequence will almost certainly be biologically useless. Individually, randomness and specificity are not hard to create. Chance (in the form of thermal chaos say) generates randomness, and law generates specificity. But what combination of chance and law generates specific randomness? One solution is Darwinism. Chance mutation and lawlike natural selection has what it takes to produce the right mix of randomness and specificity. But Darwinism kicks in only after life gets going; it cannot be used to explain the origin of life. Some researchers suggest defining life as any system that undergoes replication, variation and selection, and argue for 'Darwinism all the way down'. The system may be simply a collection of replicating molecules that could plausibly form by chance in a prebiotic soup. Can molecular Darwinism explain biogenesis? Maybe, but we have scant idea what those first replicating molecules might be. Examination of real organic replicator systems like RNA/proteins indicates that even the simplest replicators are extremely large and complex molecules, unlikely to form by chance. Moreover, the smaller the molecules the sloppier they copy, suggesting that molecules small enough to form by chance would be very bad at replicating information, and thus subject to Eigen's error catastrophe (Eigen & Schuster, 1979), whereby information is eroded by the inaccurate copying process faster than natural selection can inject it. I concede that if something like the RNA world (Cech, 1986) were given to us ready-made, it has the capacity to evolve into life as we know it. But it strains credulity to suppose that the RNA world sprang into being in one huge chemical transformation. Likely it would be the product of a long series of steps. We can liken the situation to a vast decision tree of chemical reactions, with the RNA world as one tiny twig on the tree. (There is the question of whether there are other twigs that could lead to life, but I shall assume here that the RNA route is the only one.) So we need to understand how a hypothetical class of simple, small replicators navigated through that decision tree and 'found' the RNA twig. Was this just a lucky fluke, or is there something other than a random walk involved? Now searching databases and navigating decision trees is an interesting branch of science that we might term informational physics. I wish to conjecture that some new discoveries in this field just might help explain how life's decision tree was navigated. The first point I want to make is that informational physics encompasses mechanisms capable of converting random motion into directed motion. An example of current interest is the so-called Brownian ratchet, based on a device first studied in detail by Smoluchowski (1912). It consists of a ratchet and pawl connected via a rod to a set of vanes, and immersed in a gas in thermodynamic equilibrium. The ratchet allows the vanes to rotate in one direction, but not the reverse. The random motion of the molecules bombarding the vanes will cause the system to rotate, thereby apparently converting undirected chaotic molecular motion into directed macroscopic motion. This seems to violate the second law of thermodynamics, because the rotation could be used to perform work, e.g. by lifting a weight. The resolution of the paradox was essentially spotted by Smoluchowski (1912) and refined by Feynman (Feynman, Leighton & Sands, 1963) and Abbott (Abbott, Davis & Parrondo, 1999), in which it was pointed out that in thermodynamic equilibrium the position of the pawl will fluctuate due to thermal noise, and allow the ratchet to slip backwards as often as it is driven forwards. There is then no net rotation on average. Moreover, a type of Brownian ratchet that serves to convert random into directed motion has been devised by Magnasco (1993), and studied by Doering (1995) and Harmer & Abbott (1999). In this system, an ensemble of randomly bouncing balls can be made to diffuse uphill if driven by a tilted sawtooth forcing potential that flashes on and off - the so-called flashing ratchet (Ajari & Prost 1993). The ratchet thus drives the system 'the wrong way' from a thermodynamic viewpoint (though there is no violation of the second law because the system is not closed on account of the external potential). The relevance of this discussion to life is that Darwinian evolution is an example of a ratchet, because advantageous random changes are locked in, thus also giving a superficial appearance of going against the second law of thermodynamics. Derived from the physical example of the Brownian ratchet is the curious paradox of Parrondo (Harmer & Abbott, 1999; Parrondo et. al., 2000), involving games of chance. Parrondo has proved that two fair games that individually have an expectation of loss to the player can be played in combination with an expectation of gain! Again, the relevance of this to biological evolution is clear: Darwinism is a type of game of chance in which the winners, driving against the thermodynamic gradient ('climbing Mount Improbable', to use Richard Dawkins' evocative description (Dawkins, 1996)) are the survivors. If chance variations could lead to ordered evolution as opposed to random diffusion, then canalization within the chemical decision tree may result. (Of course, if nature obligingly directs the activity preferentially towards the RNA world we are back to teleology again.) My remaining examples concern the possibility that quantum mechanics may have a more direct role to play in life than merely providing the mechanism of chemical bonding. The founders of quantum mechanics generally believed that life required some extraordinary physics to explain it. Thus Schrödinger wrote (Schrödinger, 1944, p. 81), 'We must be prepared to find a new kind of physical law prevailing.' Several researchers have suggested that quantum mechanics might be biologically relevant. An early conjecture along these lines is Fröhlich's theory (Fröhlich, 1983) that collective vibrational modes (coherent phonons) in biological membranes can create conditions similar to a Bose-Einstein condensate, leading to ordered, cooperative behaviour in which the vibrational energy is concentrated into the lowest mode. A more recent example has been given by McFadden (2000), who points out that certain mutations occur as a result of quantum tunneling events in the pair bonds within DNA. He conjectures that the biological environment might 'select' certain mutations by affecting the tunneling probabilities. Is this credible? Certainly the theory of quantum transitions involving strong coupling to the environment involves some unusual features. For example, in the watchdog or quantum Zeno effect (Itano et. al., 1990), continuous measurement-like interaction with by the environment can serve to paralyze a quantum system in its initial state. The inverse watchdog or Zeno effect (Altenmuller & Schenzle, 1993; Kofman & Kurizki, 2000) can amplify certain transitions and 'steer' a quantum system through a sequence of states by environmental interactions. McFadden conjectures that competing quantum transitions with biochemically very distinct consequences might have very different transition rates, so that adaptive mutations might be quantum mechanically favoured. Applying this to biogenesis, it is possible to imagine that states that are in some sense 'more lifelike' (e.g. more complex, more organized, more information rich) might also be favoured. The trouble is, it's very hard to pin down a precise attribute for 'lifelike' that can exercise a well-defined physical effect. The most obvious candidate is replication, which has a clear physical basis. In a quantum system with feedback, it may be that the production of a replicator in a complicated network of chemical reactions acts like an attractor, with the feedback amplifying, via something like the inverse watchdog effect, the transition probabilities leading to replicating molecules. These ideas hint that maybe quantum mechanics can 'fast-track' a chemical soup to complex biologically-relevant states. Since the object of the exercise is to explain the origin of biological information, the appropriate theoretical framework would seem to be quantum information theory. This subject is currently of intense interest because of the possibility of constructing a quantum computer (Milburn, 1998; Bennett & DiVincenzo, 2000). The key property of quantum information processing is that it is far more powerful than classical information processing. That is because the wavefunction of a collection of entangled particles can store information in the phases. So long as quantum coherence is maintained, transformations of the wavefunction can simultaneously process exponentially more information than the corresponding classical system. Farhi and Gutmann (1998) have applied quantum information theory to decision trees, and found an exponential improvement in the search time. Treating the biogenesis problem as the need to navigate the molecular decision tree to 'find' the RNA world, or something similar, then a quantum search would obviously be vastly quicker. Building upon these ideas, a fruitful line of investigation would be to apply quantum information theory to ratchets. Quantum ratchets might combine quantum search efficiency with the directionality property of ratchets. Another related field under active investigation is quantum game theory (Meyer, 1999; Eisert et. al., 1999). This is closely related to the molecular evolution decision tree problem: if competing chemical reactions are regarded as participants in a game, with the 'winner' being life (or simply a replicator), then quantum strategies are expected to be much more efficient than their classical counterparts. Hameroff (1998), and more recently Nanopoulos (Mershin et. al., 2000), have suggested that quantum information processing may play an important role in protein folding - another famous decision tree problem, where this time the branches of the tree are alternative conformational states. These researchers point out that the protein tubulin can undergo quantum flips between two specific conformational states, and thus form a binary quantum switch - the basic component of a quantum computer. In a microtubule of the sort found within living cells, ordered arrays of tubulin molecules constitute a sort of quantum cellular automaton, potentially capable of prodigious information processing. Penrose and Hameroff (Penrose, 1994) have also suggested that quantum information processing takes place in microtubules, and, more controversially, that this process may be involved in the phenomenon of consciousness. There is some circumstantial evidence in favour of the theory that quantum computation plays a crucial role in life. Grover's algorithm was devised to apply quantum information processing to search an unsorted database of N objects by posing Q yes-no questions. Grover (1999) proved that this would produce a N1/2 improvement in the search time. The relationship between N and Q in Grover's algorithm is (2Q + 1) sin-1(N-1/2) = p/2 which has the intriguing solutions Q = 1, N = 4, and Q = 3, N = 20.2. Patel (2000) has suggested that these numbers could explain the genetic code. N = 4 corresponds to the four nucleotide bases, Q = 3 to the triplet code and N @ 20 to the twenty amino acids life uses. He has developed a scenario of molecular assembly using quantum interrogation in which these numbers may crop up naturally, as a consequence of quantum mechanics. Another hint of quantum physics at work in the genetic code is the discovery that the coding assignments possess a compact description in terms of supersymmetry (Bashford et. al., 1999). Supersymmetry arises in particle physics as a unified description of fermions and bosons, and is a subject to which Salam made important contributions. To find supersymmtery appearing in a biological context is remarkable, and still somewhat mysterious. Unless it is a weird coincidence, it points to a deep link between the quantum realm of particle physics and the quasi-classical realm of protein assembly. Exciting though these various quantum conjectures may be, they all come up against a major obstacle - decoherence. Explicitly quantum effects may be manifested only so long as the phase relationships between various branches of the wave function are maintained. But these phase relationships are exceedingly delicate, and will be disrupted by even slight interactions with a noisy environment (Zurek, 1991). A simple-minded calculation (Tegmark, 1999) for the conditions inside a living cell, for example, indicates decoherence timescales of 10-13 s or less - too fast to be biochemically relevant, and far too fast to navigate a decision tree of significant complexity. If this obstacle is to be circumvented, there have to be special reasons why certain organic systems are screened from decohering influences. There is a claim that water and proteins could have a shielding effect on electromagnetic disturbances (Mershin et. al., 2000). Moreover, most decoherence calculations assume linear, near-equilibrium systems. In biology one is dealing with highly nonlinear systems involving strong feedback loops, often driven far from equilibrium by an energy throughput. The quantum theory of such systems is more or less nonexistent; greatly extended decoherence times may not be impossible under such conditions. Also, decoherence calculations are applied primarily to electromagnetic disturbances on charged particles. In the case of coherent vibrational modes of bio-polymers and membranes, phonons are the relevant quantum particles, and these are likely to have much longer decoherence times than electrons and ions. Although the case for quantum information processing in living systems is far from proved, I think Salam would have approved of the following philosophical observation. Given that quantum mechanics provides the possibility of stupendous information processing power, why does nature have need of it? To what use is it put? Does this extraordinary power just go to waste, or is it harnessed somewhere? I believe it is indeed harnessed, in bringing life into existence, and maybe mind too. That is not a scientific conclusion, of course, but the history of science does show that what can happen in physics usually does happen somewhere in nature. If quantum computation turns out to technologically feasible, I would find it hard to believe that nature didn't get there first. Acknowledgements I should like to thank Derek Abbott, Carlton Caves, Johnjoe McFadden, Peter Jarvis, Gerard Milburn, Lee Smolin and Duncan Steel for their help and encouragement in preparing this paper. References Abbott, D., Davis, B. and Parrondo, J.M.R. (1999) The problem of detailed balance for the Feynman- Smoluchowski engine (FSE) and the multiple pawl paradox, in Proceedings of the Unsolved Problems of Noise (UpoN99), American Inst. Phys. 511, 213. Ajari, A. & Prost, J. (1993) Mouvement induit par un potentiel periodique de basse symmetrie: dielectrophorese pulsee, C.R. Acad. Sci. Paris II 315, 1635. Altenmuller, T.P. & Schenzle, A. (1993) Dynamics of measurement: Aharonov's inverse quantum Zeno effect, Phys. Rev. A48, 70. Barrow, J.D. & Tipler, F.J.(1986) The Anthropic Cosmological Principle, Clarendon Press, Oxford. Bashford, J.D., Jarvis, P.D. & Tsohantjis, I. (1998) Supersymmetry in the genetic code, in Physical Applications and Mathematical Aspects of Geometry, eds. H.-D. Doebner, P. Nattermann, W. Scherer and C. Schulte, World Scientific Press, Singapore. Bennett, C.H. & DiVincenzo, D.P. (2000) Quantum information and computation, Nature 404 (2000). Cech. T. (1986) RNA as an enzyme, Scientific American 255, No. 5, 64. Chaitin, G. (1990) Information, Randomness & Incompleteness: Papers on Algorithmic Information Theory, second edition, World Scientific Press, Singapore. Davies, P. (1998) The Fifth Miracle: The Search for the Origin of Life, Penguin, London. Dawkins, R. (1996) Climbing Mount Improbable, Viking, London. De Duve, C. (1995) Vital Dust, Basic Books, New York. Doering, C.R. (1995) Randomly rattled ratchets, Nuovo Cimento, 17D, 685. Dyson, F. (1971) Scientific American 225 (September issue), 25. Eigen, M. & Schuster, P. (1979) The Hypercycle: The Principle of Natural Self-Organization, Springer-Verlag, Berlin.. Eisert, J., Wilkens, M. & Lewenstein, M. (1999) Quantum games and quantum strategies, LANL preprint quant-ph/9806088. Farhi E. & Gutmann, S. (1998) Quantum computation and decision trees, Phys. Rev. A58, 915. Feynman, R.P., Leighton, R.B. and Sands, M. (1963) The Feynman Lectures on Physics, Addison-Wesley, Reading, Mass., vol. 1, sec. 46.1. Fox, S. (1988) Prebiotic roots of informed protein synthesis, in The Roots of Modern Biology, ed. H. Kleinkauf et.al., de Gruyter, Berlin, p. 897. Fröhlich, H. (1983) Coherent Excitations in Biological Systems, Springer-Verlag, Berlin. Grover, L. (1999) Quantum computing, The Sciences, July/August edition, 24. Hameroff, S.R. (1998) Quantum computation in brain microtubules? The Penrose-Hameroff "Orch OR" model of consciousness, Phil. Trans. Royal Soc. (London) A356, 1869. Harmer, G.P. & Abbott, D. (1999) Parrondo's paradox, Statistical Science, 14, 206. Hoyle, F. (1954) Astrophys. J. Supplement 1, 121. Itano, W.M., Heinzen, D.J., Bollinger, J.J. & Weinland, D.J. (1990) Quantum Zeno effect, Phys. Rev. A41, 2295. Kofman, A.G. & Kurizki, G. (2000) Acceleration of quantum decay processes by frequent observations,' Nature 405, 546. Küppers, B.-O. (1985) Molecular Theory of Evolution, Springer-Verlag, Berlin. Magnasco, M.O. (1993) Forced thermal ratchets, Phys. Rev. Lett. 71, 1477. Mershin, A., Nanopoulos, D.V. & Skoulakis, E.M.C. (2000) Quantum brain?, LANL preprint quant-ph/0007088n. McFadden, J. (2000) Quantum Evolution, HarperCollins, London. Meyer, D.A. (1999) Quantum strategies, Phys. Rev. Lett. 82, 1052. Milburn, G. (1998) The Feynman Processor, Perseus Books, Reading, Mass. Monod, J. (1972) Chance and Necessity, trans. A. Wainhouse, Collins, London. Parrondo, J.M.R., Harmer, G.P. & Abbott, D. (2000) New paradoxical games based on Brownian ratchets, Phys. Rev. Lett. 85, 3386. Patel, A. (2000) Quantum algorithms and the genetic code, LANL preprint quant-ph/0002037. Penrose, R. (1994) Shadows of the Mind, Oxford University Press, Oxford. Salam, A. (1991) The role of chirality in the origin of life, J. Mol. Evol. 33, 105. Salam, A. (1992) Chirality, phase transitions and their induction in amino acids, Phys. Lett. B288, 153. Schrödinger, E. (1944) What is Life?, Cambridge University Press, Cambridge. Shapiro, R. (1986) Origins: A Skeptic's Guide to the Creation of Life on Earth, Summit Books, New York. Smoluchowski, M. (1912) Experimentall nachweisbare, der üblichen Thermodynamic widersprechende Molekularphänomene, Phys. Z. 13, 1069. Tegmark, M. (1999) The quantum brain, LANL preprint quant-ph/9907009. Yockey, H. (1992) Information Theory and Molecular Biology, Cambridge University Press, Cambridge. Zurek, W.H. (1991) Decoherence and the transition from quantum to classical, Physics Today, 44, No. 10, 36. |
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| Laurent wrote: [snip 608 lines of soft science social situational brainpuke] IF YOU HAVE NOTHING TO SAY, DON'T. Or at least put it on a Web page and post a link that can be efficiently ignored. Read a psychology journal. Everything has been perfectly explained at the nine sigma level. Alas, the Harvard Law of Animal Interaction pulls trump: When all experimental variables have been frozen, the test animal will still do what it damned well pleases. The idiot psychologists, who cannot be incorrect, then shift their leaden derrieres and shout "HETEROSKEDASTICITY!!!" Uncle Al says, "Let's take a vote on the nature of physical reality." -- Uncle Al [Only registered users see links. ] [Only registered users see links. ] (Do something naughty to physics) |
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| Laurent: Do you do anything but cut-and-paste excerpts from articles? |
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| Uncle Al wrote: We do. We see what we believe to be there. Belief shapes reality and we all have a vote at all times. John |
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| <snip> Flagle's Law is otherwise known as the Law of Perversity of Inanimate Objects: "Any inanimate object, regardless of its composition or configuration, may be expected to perform at any time in a totally unexpected manner for reasons that are either entirely obscure or else completely mysterious. " I Believe THAT! I saw it posted on the wall of the Instrument Design and Repair shop (AKA "Instruments: Resign in Despair") where I was once employed. Tom Davidson Richmond, VA |
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| John Sefton wrote: Belief divorced from physical action changes not one atom of the kosmos outside of our skins. Reality does not need sentients in order to be what it is. Bob Kolker |
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| davies , life , paul , physics |
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