Abstract
Abiogenesis, life arising from non-living matter, is reconsidered. A historic account is given from Darwin to the present with special consideration of the incipient relationship between quantum theory and life processes. Recent ideas relating to the spontaneous emergence of life are considered and evaluated, including the work on self-organizing systems by Ilya Prigogine and the Brussels-Austin School. The second law is commensurate with chemical evolution, but is incapable of explaining the mechanism behind the selection of specific polymers from an infinitude of molecular specimens. We attest abiogenetic life processes originating from a quantum chemical material world. A Gibbs free energy formulation is derived ab initio conceding non-equilibrium evolutions and open system self-organization. Correlated Dissipative Structures, CDS, combine quantum-thermal correlations at precise temperatures commensurate with their adaptive time scales, constituting CDE, a Correlated Dissipative Ensemble. The theory suggests an objective communication principle reminding of a Call-Centre-Poisson point process. The self-referential structure applies directly to biological systems, suggesting a fundamental quantum-chemistry life-principle incorporating evolution of the whole biosphere without contradicting the objectivity of physical laws.
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Notes
- 1.
See e.g. an interesting discussion of Darwin’s stance on spontaneous generation in [1].
- 2.
The story is quoted in Brown’s Bernal biography, see Ref. [5].
- 3.
According to the reviewer [13], the book comes as a real surprise to those comfortable with the view that the scientific problems of abiogenesis are mostly resolved.
- 4.
These thermally excited modes are identified as Jordan blocks, converting states to sequences of transitions.
- 5.
Mayr introduced teleonomic processes, on par, but thus far not accounted for, by known physical laws, as follows: A teleonomic process or behaviour is one that owes its goal-directedness to the influence of an evolved program.
- 6.
Monod struggled with an epistemological contradiction, i.e. objectivity set against the need for teleonomy in biology stating: In fact the central problem of biology lies within this contradiction.
- 7.
The discussion took place at the Canary Islands in 2004, while the transcripts did not appear in print until 2008, see [25] and in particular the contributions by Paul Davies and Howard Wiseman.
- 8.
In the foreword to [25] Sir Roger Penrose asks the question: Is it merely the complexity of biology that gives living systems their special qualities and if so, how does this complexity come about? Or are the special features of strongly quantum-mechanical system in some way essential? Penrose’s answer is well-known, but we will not discuss his “Orch OR” theory, nor in detail Tegmark’s decoherence argument.
- 9.
By many considered the father of quantum chemistry, see [26] for rationales.
- 10.
The debate whether the Nobel Prize awarded work on density functional theory, DFT, should be considered ab initio will not be discussed here. Yet, DFT is definitely epistemic in nature.
- 11.
Bishop has analysed the work of the Brussels-Austin Group [29] with particular focus on the definitions and mathematical extensions to rigged Hilbert spaces and its applications to concrete mathematical systems.
- 12.
Bricmont refers to Lanford’s original derivation of Boltzmann’s equation [33].
- 13.
Lanford’s theorem in the case of N hard spheres was extended in [34]. The review [35] nevertheless concludes: Boltzmann’s 1872 effort, to conciliate microscopic time-reversible dynamics with increase of entropy and trend to equilibrium, still remains as a source of challenging mathematical problems.
- 14.
It is hard to evaluate general statements made here, since the fundamental difference between CM and QM at the end of the day turns out to be significant.
- 15.
The non-Hermitian extension permits higher order singularities affecting the time evolution of the CES.
- 16.
See e.g. Wiseman in [25].
- 17.
Cf. the Koopman representation employed in the Prigogine sub-dynamics. For more details see [29].
- 18.
The original Technical Note, dated May 1, 1962, from the Uppsala Quantum Chemistry Group is available on internet and authenticated as ASTIA DOCUMENT No: AD No. 296970. The story behind the lost manuscript and the progress of ODLRO has been told at numerous occasions, see [26] for more details.
- 19.
Other physical areas represented in the book were also laser physics, quantum optics, quantum information and subatomic physics.
- 20.
Ref. [45] was originally published in 2005 in different form in German by C. Bertelsmann. Germany, as Einstein Spuk: Teleportation und weitere Mysterien der Quantenphysik.
- 21.
Cf. the statements by Paul Davies in [25].
- 22.
Note that the notion of microscopic reversibility means different things in CM and QM.
- 23.
Cf. Bricmont’s comments in the previous section and associated footnotes.
- 24.
Although the complete state space dimension might be infinite, the relevant degrees of freedom using partitioning technique turns out to be finite. Employing the thermodynamic limit is another source of irreversibility.
- 25.
The limit is usually interpreted as the course-grained limit with the time being smaller than a process-defined relaxation time, \(\tau_{\text{rel}}\), but still large enough to randomize the phases. The Prigogine sub-dynamics does not contain this assumption.
- 26.
- 27.
Wiener, the father of Cybernetics, introduced feed-back and learning as mechanisms for information and communication in evolving organizations. See more on Communication Simpliciter in later sections.
- 28.
Stated by the Swedish Chemistry Nobel Laureate The Svedberg, see also the AIM magazine in Phase below.
- 29.
The graduate program, producing 35 Ph.D’s, was sponsored by the Swedish Foundation for Strategic research. The AIM Magazine, InPhase: Bridging the Gap between Academia and Industry is available from the author on request.
- 30.
The nature of these degrees, paired fermionic or bosonic etc., will be discussed later.
- 31.
This might appear as an unnecessary limitation. However, assigning instead \(g\) degrees of freedom, the result becomes simply that \(n\) will be replaced by \(n/g\) in Eq. (4.6). Without restricting the formulation one might refer to \(n^{\prime} = n/g\) as the relevant degrees of freedom defining \(UD\left( {n^{\prime}} \right)\), provided \(n^{\prime}/4\pi \gg 1\).
- 32.
Note that \(\sigma_{\text{tot}}\) cancels out in the final relation and that the factor \(4\pi\) occurs since the outgoing flux of \(UD\left( n \right)\) is defined per solid angle. In biological systems the number \(n\) gets important since it conveys crucial information regarding the performance of each CES. In such cases the quality index \(n\) will be explicitly denoted separating it from other technological or artificial intelligence devices.
- 33.
This is usually referred to as analytic continuation onto the second unphysical Riemann sheet.
- 34.
For instance the relation between kinetic and potential energies, see relevant discussions in Ref. [26].
- 35.
Cf. the concept of star-unitary transformations introduced by the Brussels-Austin School.
- 36.
This imparts the occurrence of the irreducible Jordan normal form of the operator representation, where the order of the largest block defines the Segrè characteristics corresponding to the actual degeneracy.
- 37.
Any matrix can be brought to complex symmetric form.
- 38.
Note that a resonance may come arbitrarily close to the real axis and still be classified as being located on the second sheet.
- 39.
The partition of the propagator into its retarded-advanced parts will be crucial as it imposes a separation of positive-negative times corresponding to the lower-upper parts respectively of the complex energy plane.
- 40.
The Swedish mathematician Torsten Carleman extended the Fourier transformation by splitting the integral into two parts with the variable \(z\) being complex. This generalization is well described in Lützens’s Studies in the History of Mathematics and Physical Sciences No. 7 [67].
- 41.
For a simple introduction see Ref. [68] and footnote 36.
- 42.
- 43.
The proof involves the notion of quasi-isometry. The problem is due to the fact that the numerical range of a complex scaled attractive Coulomb potential cannot be proven to be restricted to the lower complex halfplane, a necessary and a sufficient condition for the fulfillment of the Hille-Yosida theorem [20].
- 44.
The discussions occur in an interdisciplinary poll [74] that concerns the reconciliation of profoundly conflicting facts regarding time and the fundamental processes going on in the world.
- 45.
The evolution of \(UD\left( n \right)\) turns out to be Poissonian the loss of memory is here implicit.
- 46.
See the definitions introduced by Husimi [41].
- 47.
In the reduced representation one could employ the reduced Hamiltonian [44], and in a thermalized picture one might also include the chemical potential.
- 48.
We will denote the spatial coordinates with a vector notation, i.e. \(\vec{x}_{k}\).
- 49.
- 50.
The normalization factor is not explicitly shown in the antisymmetric wedge product symbolized by \(\wedge\).
- 51.
In fact \(\lambda_{T} = \lambda_{S}\), displaying that all eigenvalues are degenerate except \(\lambda_{L}\).
- 52.
The transformation \(\varvec{B}\) becomes a key quantity, see also footnote 55 and the next section.
- 53.
The story is detailed in Ref. [78].
- 54.
As can also be deduced from statistical arguments [77], one finds \(\lambda_{S} = \frac{{N\left( {N - 2} \right)}}{{4n\left( {n - 1} \right)}}; \lambda_{L} = \frac{N}{2} - \frac{{N\left( {N - 2} \right)}}{4n}\).
- 55.
- 56.
Cf. a random phase system.
- 57.
- 58.
The present mapping appears incompatible since in general \(N < 2n\). This is automatically taken care of by the mirror theorem, since the extra eigenvalues in the larger space dimension are filled out by zeros.
- 59.
- 60.
The stringent philosopher, Rosenberg [87], views biological issues within the same epistemological framework as the philosophy of physics, primarily based on the second law. It is of course beyond this summary to render a fair and ample account of the detailed ingredients that goes into such a stance.
- 61.
For the Poisson distribution the variance equals the mean.
- 62.
- 63.
Note that different situations lead to various Jordan forms and their Segré characteristics as well as differing magnitudes of \(\lambda_{L} , \lambda_{S}\). For simplicity we have made the choice (6.22).
- 64.
Communication taken in a restricted sense, i.e. without semantics employing only syntax and pragmatics.
- 65.
- 66.
The matrix (8.12) has a direct link with Gödel’s self-referential paradox, see footnote 65.
- 67.
- 68.
- 69.
- 70.
- 71.
The mirror relation between N, the number of fermions, and n, the number of nuclear centers naturally disappears in the QBH, but a bosonic analysis nevertheless yields a number, see [77].
- 72.
Penrose discusses space-like futures with massless particles calling our Universe an aeon in an endless sequence of aeons.
- 73.
In this formulation concepts such as Hawking radiation and the Bekenstein-Hawking entropy have not been considered here. Whether and how they might become applicable also in a quantum theoretical description remain a topic for the future.
- 74.
- 75.
- 76.
Note that Chalmers’ concept of the Hard Problem presupposes a dualistic attitude. Various recent suggestions display ‘the long and winding road’ from monism to dualism.
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Acknowledgements
I am grateful to the Chair of QSCP XXIII, Prof. Liliana Mammino, and the Co-Chair Jean Maruani for generously allowing me to present this work in the present proceedings from the meeting. My indebtedness for constructive suggestions and recommendations goes to Prof. Alia Tadjer and Prof. Jean Maruani. This work has over time been supported by the Swedish Natural Science Research Council, the Swedish Foundation for Strategic Research, The European Commission and the Nobel Foundation.
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Brändas, E.J. (2020). Abiogenesis and the Second Law of Thermodynamics. In: Mammino, L., Ceresoli, D., Maruani, J., Brändas, E. (eds) Advances in Quantum Systems in Chemistry, Physics, and Biology. QSCP 2018. Progress in Theoretical Chemistry and Physics, vol 32. Springer, Cham. https://doi.org/10.1007/978-3-030-34941-7_15
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