2.1. How Can a Developed Physical Difference Make a Difference by Functionality?
When thinking about the proposed question, most probably the first thought is about particles and particulate structures and how they can change their form and disposed properties by plastic deformation and chemical reactions. What kind of influence can structurally disposed properties in a particle have on the course of evolution of the particle’s maintenance in its environment? Can those properties be self-referential to their own state? There exist already good models for how a particulate structure can self-organize relying on some kind of coding and modularity—as is the case in nucleic acids, amino acids and living organisms. To explore the explanatory power of the maintenance account, the notion of function is used as a tool to discover self-referentiality in objects that at first are not believed to show such. We are going to consider the wave dynamic formation of transiently stable and mildly predictable parcels of force and information inside energy density fields, no matter whether the carrying medium is the electromagnetic vacuum or matter, in any state of condensation (gaseous, liquid, solid and intermediaries). Non-dispersive wave packets or localized pulses are special for maintaining their identities even when they undergo collisions with each other. This particle-like behavior gave them the name soliton. However, solitons are also special for showing that particle-like behavior of packets of wave-frequency components demands a compensation of natural wave dispersion
5 behavior, which—in contrast to stability of atoms and elementary particles—appears to be a property of the medium in which the wave is excited at least as much as it is a property of the wave itself. A soliton cannot be viewed separately from its medium.
Solitons became known by an observation of
Russell (1808–1882) in water (Union Canal system). One might already know of the narrative of him observing the generation of a wave by a canal boat pulled by horses stopping suddenly, realizing the special character of the wave and then following its course over more than a mile on horseback. After this observation, Russell built his own “soliton generator” to further understand and analyze the interesting phenomenon (see for example [
20]). The canal was in fact—and shallow canals tend to be in general—one of the structural media that support solitons: from observations in open waters such as ponds where one throws in a pebble to generate cyclic wave fronts spreading out (For the sake of completeness: in addition to dispersion, the inverse square law is important for this effect), one would expect excited waves to quickly lose their form, dispersing into more and more disconnected diminishing wiggles on the surface due to different frequency components having different velocities. Then the character of an “object” with a form or an entity of coupled components normally is lost. When non-linear media such as the shallow body of water in Russell’s canal enable excitation of localized pulses, or “wave packets”, they somehow counteract dispersion respectively diffraction, eliminating phase differences between the components. How can a medium eliminate mutual phase differences in wave packets?
Korteweg and
de Vries realized that the phenomenon described by Russell required an unusually large amplitude and that the medium’s non-linearity must be grounded in a different behavior to waves of different amplitudes [
21]. The ship’s speed is the decisive factor because for speeds of water dragged along by the ship which are much lower than a critical threshold speed, i.e., slower than waves radiated from the ship, those linear waves will effectively carry away energy, not allowing the steepening to higher amplitudes [
22]. However, if the ship’s propagation speed
6 reaches the critical threshold, a local radiation wave can grow as the energy acquired from a local fluid at the rate of work by its motion keeps accumulating. Local waves with a small initial amplitude thus are fueled by energy from the disturbance over a relatively long time. If a local wave reaches a certain threshold magnitude, the increase in phase speed with increasing amplitude—enabled by the non-linear behavior of the medium to different amplitudes—is then sufficient to make the wave break away from the disturbance, thus freeing it as a new solitary wave propagating forward with a phase velocity dependent on the amplitude it gained. What is particularly interesting in the case of the excitation of such a discrete “precursor soliton” entity is that it has been generated by a steadily moving disturbance in the medium (i.e., the moving ship or the accelerated flow of water propagating after the ship had stopped). It even has been observed that many solitons may be generated subsequently ([
23] and references therein). What the non-linearity of the medium enables in the case of Russell’s soliton is therefore the following. Out of a forcing
steady flow, a
continuous and periodic sequence of solitary waves or solitons can be generated, i.e., some kind of differential enhancement or perpetuation effect on the excitation [
23]. Due to its topological structure, the canal enhanced the amplitude of some frequencies and dampened the amplitude of others, leading to a distribution of energy in a non-averaged, frequency-selective manner. The mutual phase differences in components of the wave packet that would in the linear case have led to an averaging out of distinct rises in the amplitude of certain frequencies are eliminated in an indirect way: features of its geometry forbid certain frequencies
7 If the topological structure was different in critical places, the same excitation event would allow the frequencies that are forbidden in the canal to develop sufficient amplitude to be measurable. Transformative capacity of structures on intensity distribution and the temporal pacing of gradients and their energy flows into periodic oscillatory motion enabled by their special geometry and topology plays a very important role in thermo-acoustic self-oscillators [
24,
25] or in musical self-oscillators, such as reed instruments and flutes [
24,
26]. In a thermo-acoustic oscillator, the acoustic oscillation of gas is encouraged if heat is injected when the gas is warmed by adiabatic compression, and/or heat is removed when the gas is cooled by adiabatic expansion. Similarly, in a reed instrument such as the clarinet, the reed by its non-linearity lets the high pressure from the breath of the player join the high-pressure part of the sound wave but not the low-pressure part, increasing the strength of the resonance in the cavity and generating a tone at the resonant frequency. In both cases of self-oscillation, the elasticity of a “spring” component in the structure, i.e., of a differentially accelerating component, is varied in such a way that the overall oscillation is fueled by a continuous flow. A differential acceleration or differential enhancement as it is given by the non-linearities of media or artifact structures discussed is a physical basis for selection and selectivity on dynamics. Selecting out different components of wave packets in its effect is not necessarily what selecting different particles from a system would be. When talking about selection, the first intuition is to take away or choose out of... In wave packets or frequency spectra of traveling waves, a selective enhancement or dampening of a frequency has no influence on its potential presence. It does not irreversibly take away but only influences the distribution and local observability of the frequency. Intuition has to first get used to the different selection mechanism and effects in wave dynamics from experience. It is not accustomed to mechanics where disturbing an averaging process by stopping some destructive interference leads to gaining new possibilities here at the cost of elsewhere stopping constructive interference, thus losing possibilities inside a possibility spectrum. The main selective mechanism in wave dynamics is interfering with interference processes. Interference in wave dynamics is a disturbed averaging process of amplitude height given by coherence between waves. It is a linear process; the spectrum is not altered, but the intensities of possibilities (frequencies) are.
In non-linear media, most of the excited waves are changed in their spectra respectively bandwidths. Contrarily, linear mixing in linear media is the superposition of things treated as individuals, which still allows for recognition of each of the individuals and which keeps any individual separable and unchanged. A linear mixing is for example the additive mixing of colors. If the “things” perform cyclically repeating, periodic motions for which a point in the cycle relative to another point in the same cycle can be defined as a phase, such as in waves, the relationship between the cycles becomes important. This relationship, the relative phase between units, can be incoherent, i.e., over a sufficiently large number of units, the regions of local constructive and destructive interference fluctuate so fast that an average value for intensity emerges. The relative phase can also be coherent, enabling a stable pattern of interference regions.
In coherent relative phase, constraining of wave dynamics with structures, the dimensions of which are at the scale of the waves’ wavelengths in the structures, lead to distinct patterns of enhanced and dampened intensity, i.e., fringe patterns (diffraction patterns). Structural objects with this property are usually referred to as diffraction gratings. Interference is also important in the generation of standing waves and cavity resonance. Interfering with interference processes is possible by coupling and decoupling phases, altering the relative phase or by manipulating points of interference nodes and antinodes.
One common differential enhancement mechanism is the resonance amplification of certain frequencies respectively harmonic components of a fundamental frequency in resonant cavities. Influencing resonance is thus possible by altering the node and antinode distribution for waves and altering the fundamental, e.g., by re-scaling the cavity. Another is the manipulation of the decay time of resonances by adding leakage at points where certain excitable frequencies have their antinodes, strengthening amplitudes of others with a node at that spot. Thereby harmonics of a fundamental can also be selectively dampened, without altering the fundamental itself. Both processes are clearly described in [
26].
In the sense of evolutionary biologist
Mayr who developed
Darwin’s “descent with modification” concept of selection [
27] further, embracing the (relatively new knowledge on) genetic information, selection in biology, i.e., natural selection can be defined as “(...) differential perpetuation of genotypes” [
28]. Taking this accepted definition for biological selection into account, differential acceleration or differential enhancement by interfering with interference in physical systems—similar to differential permeability of physical sieves (although working by very different mechanisms as stated above)—can be construed as physical selection. This ascribes a basal selective capacity to processes interfering with interference dynamics in physical systems. Linear processes do not dissipate energy in exchange with surroundings. Absorption and emission events happen only internally and have no influence on the average of ensembles. Non-linear processes are characterized by dissipation and irreversible transformations. Topological features in the medium are altered; they are altered in a spatial pattern that is proportional to the spatio-temporal pattern of intensity (or radiance
8) transported in the wave field. The changes in the medium take place due to (e.g., photochemical) reactions fueled by the spatio-temporally irradiated (photon) energy as power/area- (intensity [J/sm
2 = W/m
2]) or
intensity related available energy. Subsequently, properties important for interactions with fields such as the one that caused the alterations are altered. Those properties comprise absorption, transmission, reflection and the complex medium property refractive index (RI). The RI is mathematically defined as the relation between traveling speed of the phase (in the case of the electromagnetic field being the wave field under consideration: the speed of light in vacuum, c) and the traveling speed inside the medium, v. RI~c/v, and in most known naturally occurring media, it is smaller than 1. The micro-dynamics behind the effect of the RI of a medium on an incoming wave are quantum mechanical by nature and are not delved deeper into here, but a simple macroscopically observable detail is helpful for visualization: Remember that we discussed interference with interference being the main mechanism of altering the intensity distribution structure of a wave field. In classical optics, what is important in a wave field for the average intensity (incoherent relative phase) or the diffraction pattern (coherent relative phase) spatio-temporally “coded” intensity distribution transmitted to a screen is the front hitting the screen at a distance to the field’s source, called the wave front. When a wave front hits a screen, depending on the complex RI of the screen material medium, part of the wave front will be reflected, part of it will be transmitted and other parts of it might be absorbed. In reflection, as in other cases, classical optics uses the model of the so-called Huygens’s elementary wave mechanism. The details can be found in any physics textbook comprising classical optics and are worth deeper study, but for the discussion here, the important message from the model is that it is possible to construe any part of a wave front as a source for an elementary, i.e., spherical wave (in three dimensions). This is valid for the original wave front as well as for its reflection after it hit—and possibly interacted with—the medium. This is the crucial point. If the medium in interaction altered the phase of a reflected wave, the intensity at that point of the medium as a source for the reflected wave front might be altered due to interfering with interference, compared to the wave front that came in. In the case of light, when the light goes from a low-RI medium to a high-RI medium (air to glass), the reflection undergoes a 180-degree phase change. When the light goes from a high-RI medium to a low-RI medium (such as glass to air), it does not undergo a phase change. This is analogous to the case of a vibrating string (from footnote 7) as an example for the generation of a standing wave: At an edge of the medium that is held fixed (i.e., the point is not allowed to displace at amplitude as every other point in the medium), the reflected wave flips over (corresponding to a 180-degree phase change). At an edge of the medium that is free to displace, the reflected wave does not flip over [
30]. This becomes relevant at any point in the medium where there is a sufficiently large region of altered RI while the wave is propagating through. Especially interesting is the case of the incoming wave interfering with its reflected “copy” since this is an example for a coherent relative phase, and the interference defines the image of the reflector, i.e., the incoming wave as a reference wave plus the modulation on the phase done during reflection. In a first summary, it can be said that:
Linear interference influences the intensity distribution between and local observability of frequencies of a given spectrum.
Depending on the relative phase, the intensity of frequencies inside the given spectrum can at a screen at a certain distance to the source of the wave front attain an average value or an image of the primary source modulated by a reflector
9(and possibly a noisy transmission medium, e.g., air) at that frequency as a diffraction pattern.
When a wave front transmitting a diffraction pattern as a spatio-temporally “coded” intensity distribution in the field hits a target surface which is sensitive for some of its frequencies, energy is not simply transmitted but is transmitted with information.
A medium that has been altered by transmission of informed energy can non-linearly change and thereby be altered in properties decisive for subsequent interactions with fields. One possible mechanism for this is that the oscillation of dipoles in molecules induced by a wave affects the momentary local charge distribution (polarization) in the medium and thereby causes local changes in the refractive index.
Thereby non-linear processes plus linear interference can become the means by which an image, which is itself a “non-physical” object, can display a primordial type of self-referentiality. The importance of this finding is further elaborated in this paper, using the maintenance account to functionality. In principle, alterations of the fundamental and the composition of the spectrum are also possible, leading to altered properties as a re-emitting source. This is, for example, possible when the triggered dissipative reaction alters geometries of molecules or the scale of cavities in the receiving material. In this case, the self-referentiality is not given as it is for the process of transmitting an image, but resonances can selectively enhance particular similar frequencies.
Before further elaborating the possible influence of wave-carried images as a primordial physical self-referentiality on the course of evolution and before deepening the discussion of functionality evolving and the importance of the maintenance account, the meaning and importance of non-linearity in general for selective processes transmitted by wave dynamics are further explored.
2.2. Making a Difference by Non-Linear Wave Guiding and Mixing between Frequencies
When modeling the relation between dispersive energy loss (dampening) and non-linearity of amplitude distribution between available modes, such as the steepening to higher amplitude, in a non-linear partial differential equation (e.g., the equation of
Korteweg and
de Vries (1895)), the stabile trade-off that is observable as a soliton is an abstract mathematical solution of the equation. Unfortunately, the lack of human intuition regarding the mathematical link to the physical system is a drawback, often observed when describing motion structures. One understands the soliton phenomenon by being cable of modeling the dynamics and by assuming that the structure associated with the repeatable observation of the phenomenon has as its function (f(x)—being a simple relational function—the generation of the dynamics given the context. Fortunately—while examining more and more occurrences of the phenomenon and the respective contexts using scientific methods to finally arrive at a more intuitive level of understanding—humans can keep inspiring their creativity and those of their peers by beautifully poetic pieces of wisdom such as: “Solitons have the, seemingly, innate ability to solve non-linear system [sic], much like a travelling plane wave seems to solve all the linear ones:) [
20]”. The intuitive rationale given in the quote is that the structure of a soliton mathematically irrespective of its difference to that of a linear traveling wave is similar to the latter in being a stable solution of dynamic equations. Both are describable as solutions to an algorithmic equation. The description of the soliton cannot easily be followed with the Newtonian picture of a largely empty space in which single mass carriers are moving subjected to forces. This picture is what resonates best with our daily routines since we experience the airy space through which we are moving as giving way to our motion, largely independent of its state (maybe there is an exception when we try to move against the direction of the blow of very strong wind). Charges hardly matter macroscopically, and for our motion, the structure of the surface of the runway is more crucial than the state of the airy medium. In the case of the optical soliton traveling the optical fiber, the refractive index of the medium can be locally changed by the action of the electromagnetic wave traveling through, so that the medium becomes the transmitter of light action on light propagation, thus influencing the refraction of follow-up waves and the modulating light wave’s own dispersion by induced change in the refractive index [
21]. This is called wave guiding and is a non-linear process of frequency interaction enabled by photorefractive dielectric and polarizable media.
Non-linear wave interaction is always facilitated by a non-linear medium through which the waves travel. Compared to the initial spectrum (called the reference wave in the following) the altered medium can indeed make waves that have new frequencies and thereby new properties when interacting with matter. Solitons are a stable solution of non-linear partial differential equations, but non-linear media as “simple” facilitators of non-linear mixing of waves are essential for their evolution. In non-linear mixing, the input–output relation is asymmetrically distorted by the medium. Non-linear mixing is a superposition of things where the individual character and the separability (at least transiently) get completely lost. It is irreversible as long as no memory plus a non-adiabatic recovery process are involved. Both mean a considerable amount of action. For non-linear processes to occur, the medium where the process is happening needs to inject into or extract energy from the mixing components, re-distributing system energy.
The range of immediate physical changes through linear superposition and interference possible is limited compared to non-linear mixing processes where substantially new components, e.g., new excitable frequencies can emerge (here, the term emergence can be described mathematically). To better visualize the difference made by the influence of non-linear media compared to purely linear mixing, the example of audible beating is chosen. It is chosen because the sound waves of tuning forks often used to show the beating phenomenon can be easily modeled as simple sinusoid waves, which greatly supports the understanding of the mixing process.
The transition from the interference-borne result of linear mixing in beating to the occurrence of new frequencies due to a non-linear process is discussed. Beating occurs, e.g., when two tuning forks sound together, one being slightly out of tune. Additionally, a non-linear process occurs (where it occurs exactly has been and still is a matter of debate and is discussed below) so that from two sinusoid waves that are almost identical (called f
1 and f
2), new frequencies are generated and can be perceived. When the new frequency which is the difference between the two non-linearly mixed frequencies is slow enough, humans do not hear it as a tone but as a periodic oscillation in the sound intensity of the summation tone, i.e., as a beating. When above ~20 Hz, the human auditory threshold, the difference frequency is heard as a tone too, and the frequency mixing becomes observable. The two similar sine waves oscillating at f
1 and f
2 (colored blue and green, respectively, in
Figure 1) are linearly superposed. Due to constructive and destructive interference in their dynamically evolving phase relation, the amplitude periodically increases and decreases and does so with a frequency (colored orange in
Figure 1) that is the sum frequency of f
1 and f
2. As long as no non-linear medium is distorting the superposition, no signal is generated at the sum frequency. The Fourier transform of the time domain to the frequency domain only shows the two original frequencies f
1 and f
2, and thus this is no new acoustic signal yet. Likewise, the difference frequency (colored red in
Figure 1) is not appearing in the Fourier transform, just the intensity oscillation in the time domain. To arrive at the generation of a sum and a difference frequency signal, a non-linear distortion needs to occur as is shown in
Figure 2. The mathematical function describing the mixing in the non-linear medium, the so-called transfer function, needs to be of quadratic order or higher; that is, it must contain exponents that are at least quadratic.
Interestingly, the beating of the two tuning forks (given the difference frequency is above the auditory threshold of the listener) can be heard. There needs to be a non-linear process happening somewhere facilitating the multiplication between frequencies. The air can be excluded as a source for the mixing since it is assumed to be a largely isotopic, linear medium. The location of the non-linear medium, or, the location where the mixing occurs has been a matter of centuries-long debate [
33]. Hermann von Helmholtz (1821–1894), who was a talented musician and an expert in music theory, modeled the mechanism of the human ear as a Fourier analyzer. He associated the location of the frequency perception on the human basilar membrane with corresponding sinusoidal frequencies. To explain the beating, von Helmholtz associated the transfer of vibrations from the auditory ossicles to the cochlea and its basilar membrane and established the “distortion theory”, an aspect of the theory of the existence of “objective combination tones”. He also did a lot of practical research in generating combination tones (from sum and difference frequencies of combined tones) on instruments and demonstrated their existence independently from the hearing process [
34]. Modern textbooks under the impression of new experimental results emphasize that combination tones occur inside the ear exclusively, often emphasizing theories of purely “subjective combination tones”. Recent experiments by
Lohri at the University of Music and Performing Arts Vienna nevertheless strongly suggest the objective reality of combination tones and lead to the conclusion that materials inside musical instruments with freely vibrating components could be acting as non-linear media [
34]. It has been shown that linear beating also is of importance in non-linear heterodyne
11 detection schemes and that at least in heterodyning “until now it has not been realized that the standard textbook equation for mixing usually fails, as in reality, almost all mixers contain a beating stage at their input [
35]”. It is important to keep in mind that the above simplifying discussion of sum and difference frequencies only touched on one aspect of mixing products of non-linear media when frequencies are combined. Other products comprise integer multiples of the input frequencies, called harmonics and sum and differences between different harmonics, as well as mixtures between harmonics, harmonic combination frequencies and combination frequencies of the fundamental frequencies and harmonics. Higher-order mixing products are called intermodulation frequencies, and their generation cannot be visualized but only calculated using convolution. In non-linearly mixed frequencies, the components from which the carrying frequency emerged lose signal character. In a Fourier transform of the temporal development of the curve (time domain), only the carrier and the modulating frequency can be resolved (in frequency domain). Sum and difference frequencies together with higher-order harmonics of the fundamental frequency and intermodulation products are the products of non-linear frequency mixing in more complex mixing processes, such as in mixers for radio frequencies. In a way, it can be said that non-linear mixing between periodic frequencies is among if not the most basic process in physical evolution in which a dynamic whole can be generated where “the whole is more than the sum of its parts” but with the concession that the original “parts” cannot be easily recovered from the addition as soon as it developed into a non-linear mixing. Probability has been transmitted from the input parts to the output. Non-linearity that originates in the medium based on “own” structural dispositions for the behavior can cause differential amplification and redistribution between amplitudes. Some examples of non-linear behaviors (wave guiding and frequency mixing) and how non-linearity is manifested in mathematical form (in the simplest case of beating and generation of sum and difference frequency components of the fundamental without further higher-order sidebands and harmonics of the fundamental) have been discussed here. Some interesting questions from an evolutionary perspective are, of course, how can mechanisms that “handle” waves of different amplitudes or frequencies in different ways be envisioned? How can mathematical non-linearities be physically effective in structures? What could a structural disposition for the capacity of non-linear frequency mixing possibly look like?
12 According to the research done for the paper, these questions cannot yet be answered by science or at least have not driven interest in a more detailed answer.
2.4. Information in Its Most Basic Physical Representation
Information in its most basic form must be processed—in a basic way—in physical processes, i.e., processes under energy transformations and changes in position. Information is not matter and not energy [
37]. In fact, it is proposed here in reference to
Stonier [
18,
38,
39] and taking into account what has been said about basic (maintenance) functionality to consider information in connection with energy transformation processes. As has been shown in the discussion about a basic form of physical self-referentiality in the coupling of non-linear processes to linear interference, an image of spatio-temporal distribution of energy per period on a stricken surface can be transmitted via fields, or rather, media, by wave dynamics. Connecting to the questions asked in the introduction, we can propose a tentative answer for the physical selective regime of evolution: a difference in physical structures that—from the view of the maintenance account—can make a difference is this basic form of physical self-referentiality. The meaning of an image transmitted via a medium leading to a non-linear dissipative organization of wave-dynamically relevant properties (such as RI) according to the image’s patterning for energy made available as energy per period and area [J/sm
2] can be given by the maintenance account. The function of the otherwise immaterial image is a contribution to the maintenance or repeated generation of distribution functions similar to “itself”. One special property which wave transmission of pacing for local energy availability has is its potential independence from the type of medium it is transmitted by. Naturally in transmission from one medium into another, details of the information of the energy pacing are lost, but the natural relation between electromagnetic waves in the electromagnetic field and moving as well as resting charges (as described by Maxwell’s equations) facilitates cross-medium transmission. Information should be—at least in principle—quantifiable as the amount of discrete possibilities to distribute probability for selection.
When many options to choose from are available, e.g., when in the case of binary coin throws many coins are thrown, information necessary to describe the sequence of decision events will be a lot. Although the result might resemble a random sequence of decision events, information that can be used in communication as quantified by
Shannon’s formula (for information entropy, H on p.14 of [
40]) increases when there exist many mutually independent decision events in a sequence. If there are redundancies such as when many decision events are the same and their relative position in the sequence is not important or can be expressed by a short coded additional information, the amount can decrease. In the extreme case of 10 decision events in favor of heads out of ten throws, the probability for the unbiased result is as low as for any other sequence, but the information could be expressed in algorithmic form quite easily as 10× binary decision event heads provided that the code is available.
A difference that physically makes a difference is primarily something that can accelerate masses or charges; however, this alone is not information but force. A beam of wood that has been mounted so that it can swing when driven under force will oscillate around its resting position back and forth until the energy (force times amplitude of motion away from resting position) is fully transformed into heat and micro motions. In contrast, a pendulum of colliding balls (called Newton’s Cradle) can store the number of initially moved balls until shortly before thermalization. With this system, one could transmit—previously mutually coded—information. That is, a pattern of energy availability in space and time can be transmitted by mutually independent units consolidated via a limiting structure when the coupling between them is altered by applying force differentially.
What about the other form of energy, the potential energy, Epot? It behaves complementary to kinetic energy in that it comprises the position of mass and charges in relation to accelerating influences that potentially can be transformed into kinetic energy during relaxation into their resting position. Ekin and Epot are sufficiently known from physics, but is it possible to logically relate them to the amount of possibilities to choose from for differential acceleration, or, the position of differentially accelerating influences? The soliton wave can conduct energy and the length of its period: if a series of solitons is excited, power and frequency are transmissible in a stable form. The condition for a signal, a wave function that can itself be a discrete sinusoid or comprise discrete elements stable in form, is given. Form stability in waves would have to be translated as stability in energy per frequency. As is widely known, Planck’s formula for quanta of black body radiation (E = hf) gives the smallest unit of discrete waves of stable energy/frequency, the constant h. Interestingly, the physical quantity E/f, that is, E*τ (with τ being the duration for a process from a starting point to an endpoint), has meaning for physics. It is called action (therefore Planck’s constant h is called the quantum of action) and is the main quantity in a natural principle, called the principle of least (in strictly non-dissipative systems replaced by “stationary”) action (PLA). Processes without dissipation according to the PLA happen along trajectories that are the shortest path (in traveling light this can be taken literally as shortest in time) that connects starting point and endpoint, so-called geodesics.
When in linear classical mechanical systems the relation between E
kin and E
pot, quantified in a single number as the Lagrangian temporal integral functional over (E
kin-E
pot) [
39], changes, physical action changes, and the trajectory deviates from the geodesic. The thrilling fact that this quantity, physical action can be expressed using the units of classical translation (distance and time) as well as of classical wave motion (wave number and frequency) is a detail that has been keeping physics busy for quite some time [
41,
42,
43] and that most certainly will be of great relevance for insights regarding physical information processing in evolution. An important question in this context is the importance of the connection between linear and non-linear dynamics for evolution. If the group of
Annila should be right with the theory of a connection between the Second Law of Thermodynamics and the PLA, delineating dispersal of energy along the steepest directional descents in evolution [
44], implications for the understanding of natural processes can hardly be imagined.
According to our considerations of kinetic energy, information changes when a motion structure is reversibly excited; information changes if the input energy makes a difference that manifests as a temporarily stable (almost, given quantum uncertainty) number of correlated medium elements, which potentially can be read out (is potentially communicable) by modulation of an incoming carrier wave. Such a difference can influence further selective processes and lead to further non-linear differential accelerations and enhancements in sensible structures of its surroundings. Information in its basic form can therefore be understood as a Batesonian difference which can be stored (as a relative phase in a field or as in a configuration of chemically bound particles) and which can influence selective processes (differential acceleration, enhancement, delocalization or more generally differential support or weakening of fluctuations present in the receiving system).Translated into action of information on the mechanically relevant kinetic and potential energies, there is:
Kinetic information, which is connected to information contained in kinetic energy. It is the differential enhancement of coherence between mutually independent particle motions in phase space, that is, waves in a relative phase in a wave forming a motion structure with a (communicable) spatio-temporal pattern of interference “coded” intensity related values. In a (projectile) motion of single-particle objects, where Nensemble = 1, speed and direction of propagation are also given by kinetic information, Ikin. If Ekin occurs without Ikin, it plainly transmits an averaged intensity value anywhere into a stricken target, i.e., it is thermalized.
Thereby kinetic information is related to its complementary in a way analogous to the relationship between kinetic and potential energy:
Structural information14 is connected to information contained in potential energy. It amounts to relative position inside a potential as well as to the basic units of potential, charge and mass. Relative position in space and in relation to accelerating (positively or negatively) influences organizes potential energy of correlated densities of mass and correlated densities of charge into spatial networks of distinct geometry. Thresholds for the spatial constraints are defined by topologically influenced restoring forces and local potentials. Subthreshold impacts of energy are reversible due to restoring forces. E
pot without I
Struc is hardly possible. Even the densest packing of mass or charge defines a spatial structure and threshold energies. Collapse into a point is forbidden by the Pauli principle. Maximum random dispersion into free space under thermalized E
kin, splitting all relations that define elementary structure would minimize I
Struc but also E
pot.
High content of structural information in elements of media can severely alter the kinetic information that a wave entering from a medium with maximum phase velocity initially had. Due to the networks between charges and masses, dense partitions of the space into local cavities occur. Cavities of different scales influence properties of (re-)excitable waves by changing fundamentals and associated harmonic spectra of linearly excitable waves. Non-linear effects can also lead to occurrence of new frequencies, and the supply of resonance enhancements for various frequencies from the differently scaled cavities facilitates chaotic developments.
Similarly, motion structures inside a supportive medium can irreversibly alter the structural information of the medium that is carrying them. Optical fibers can be shown to become irreversibly altered in their structure and potentials by propagating solitons in a way that similarly structured solitons out of later incoming light beams will be forming with high probability [
45,
46,
47].
Kinetic information can only interact with kinetic information via structural information. Frequency mixing can only occur from linear superposition of frequencies via non-linear effects of the medium. Structural information can communicate and act on other structural information via kinetic information and kinetic energy, which usually ought to comprise organizing (kinetic) information such as propagation direction and correlation between motions when supposed to be doing work. Structural information imagined in a world with no kinetic information but only subjected to non-directional, non-patterned random thermal motion is most likely to remain incapable of adapting its structure. Kinetic information without structural information to non-linearly support its inherently fluctuating numbers of quanta moving in a correlated phase would thermalize.
Structural information, IStruc, cannot inform a receiver unless the receiver is coupled to it via a field or motion containing Ikin. Sensory functions that can receive information about structure from signals in the field in a structure can improve the transmission.
Motions that do not keep the physical action stationary are connected to prolonged paths, additional events of acceleration and dissipation of energy from and into the surrounding environment, i.e., non-linearity or physical impossibility. They might be made possible for a system but bear risks for the maintenance of structure and structural information when externally input kinetic energy cannot be dissipated into the environment and—following the Second Law of Thermodynamics—is dispersing between all available internal dofs that the structural information is supporting and additionally over further dofs made available by partial or complete disintegration of the structure. Thus they make the system dependent on compensating external, i.e., environmental influences for its motion and possibly for maintenance.
Compared to function, information is not self-referential by itself. While structural information can be maintained comparatively invariant to disturbances from environmental kinetic energies
15, kinetic information is easily destabilized by structures in its environment. Kinetic information too can have a maintenance function, having an influence on being kept largely invariant and potentially re-excited inside its environment. However, different from its structural complementary, it is in need of a balance between the dispersion of motions in a medium (dispersive relation) and the medium’s non-linearity. Examples where this is realized are solitons and localized structures [
45] which are viable exclusively inside supportive media.
2.5. Selection Regimes Guiding and Defining Functionality
In the canal example, the system has the property of coupling the non-linear steepening behavior to the velocity-dependent dispersive behavior for waves of different amplitudes.
The solitary wave is not having a function in the sense of either the etiological or the systemic account. Given the structure of the canal-ship system, the generation of a soliton wave as a means to transport energy in response to a certain kind of excitation and thereby being maintained in its form is simply its relational function, f(x). The system can be excited into this state and return to its initial state—neither ships nor the canal components are structurally changed by the soliton generation process. Generation of solitons is a characteristic, repeatable reaction to a certain type of excitation. Function theory would call this an accidental function, but from an evolutionary perspective, calling it that way is a tool-use-thinking-based hindrance for intuitive thinking
16 about possible mechanisms for prebiotic evolution. The maintenance account cannot do more than acknowledging stability in I
struc17 and a very slight form of self-referentiality between frequencies excited and spatial frequency of cavities in the canal structure that define the fundamental and its harmonic series. Nevertheless, this slight form of self-referentiality in differential enhancement of amplitude for frequencies inside a non-linear process is based on a principle that allows much stronger basic physical self-referentiality in evolution: the linear generation of a pattern or average value in local availability of energy per period and area coupled to a non-linear differential enhancement of amplitude of frequencies in a spectrum.
Consider the observation by Russell as a structurally disposed property of the evolutionary regime of selection based on human intentional decision making (the selection regime of intentional decision making (idm)), a selection regime which evolved late—viewed along the course of evolution from the early days of planet Earth. In this selection regime, some people, such as the individual John Scott Russell, had the individual and cultural background in 1834 for focusing their attention on the solitary wave observation and to realize its special characteristic (maybe immediately having an intuition for affordances). Civil engineer John Scott Russell out of a set of individuals capable of extracting the structurally based function of the canal for future cultural function in the human idm selection regime on this day, together with a portion of a happy accident, enabled the evolution of the function of solitons inside the idm selection regime. The contribution of randomness was, however, strongly reduced already by the ship-canal system structure having the property of generating solitons as an inherent maintenance function and by the cultural human environment that enabled growing up as a naval engineer and having the genetic, phenotypic and experience background for understanding the importance and potential for future affordances of the observed phenomenon.
Thanks to the complex properties of living (human) systems, the soliton motion structure became more than f(x) of the canal or a weak form of self-referentiality. It could be described as an accidental function in accordance with existing accounts of function (etiological and systemic), but hopefully, it was possible to show that description of its function according to the physical-maintenance-based account is adding to the understanding of the function by enabling an evolutionary perspective. The structure became functional as a tool in idm, causing its maintenance and repeated reproduction in a variety of different media. In the idm selection regime, a difference that arises due to a structurally based inherent (physical maintenance or relational) function can be recognized and selected by the intention-based action of individuals in cultural context and societies, causing functionality according to the maintenance account on a higher level. According to systemic and etiological accounts of function, solitons became functional as a tool or expansion of cultural knowledge. According to the maintenance account, solitons evolved in functionality and are in the idm regime reproduced more often and more in diverse contexts compared to the physical selection regime due to techniques only available through idm. Technically generated solitons can be gained using largely different artificially generated structural dispositions. Solitons used in technical communication e.g. are possible in a variety of different non-linear materials [
46]. Only the maintenance account can point out this connection.
Becoming a biologically positively selected (fitness-enhancing) part for a physical structure such as a certain spectral composition or spatiotemporal pattern is highly influential on the probability and frequency of its structural disposition to be maintained or reproduced, according to the maintenance account. The maintenance account focuses on the effect of a potential function regarding its own maintenance by a selective environment. To be maintained by the surrounding environment, a spectrum needs to not trigger non-linear processes that would alter the structural disposition that is bearing it. The biological selective regime evolved many different species and as the systemic and selected effects function accounts, the maintenance account succeeds in recognizing functionality of a structure that is positively selected across species, such as photonic structures [
48] that generate, e.g., interference-based structural coloring that occur in bacteria [
49], insects [
50,
51], plants [
52], birds [
53], mammals [
54] and human artifacts [
55]. Already in this example of a structural disposition that is widely maintained and reproduced in selection regimes of living systems, the ascription of functionality because of the color generation is unclear [
56,
57]. The maintenance account explains the global reoccurrence of structural coloring functionality in biotic and abiotic (e.g., labradorite, opal and technical) structures such as that of unremarkable random patterned structures by the fact that their underlying dispositions do not cause effects that lead to non-linear reorganization under irreversible loss of the effect-bearing disposition—the basis for more complex functionality. What is it that a structure contributes to be stable? Is it not “just existing”? Most of the dispositions leading to chemical transformations seem to be no functions because their cause gets annihilated by their own effect. Most of the chemical dispositions influence the existence of structures in the surroundings more than that of the bearer. From what has been discussed here, we can give four—necessarily incomplete—answers:
In physical selective regimes, images of intensity distribution can be transmitted, influencing the structural information of receiving media. Functional traits for weak self-referentiality support imaging and enhance transfer over different media.
In physico-chemical selective regimes, molecules can aggregate into chemical milieus with stabilized local selective properties, generating closure and micro-environments. Functional traits particularly act on forming a stabilizing environment.
In biological selective regimes, structural genetic information reciprocally couples to biochemical organization in its unit of life, the cell. The body evolves as a complex structured environment of nested environments, enabling sensory functions for its own state and signals in its environment. Individuality of systems emerges.
In intentional selective regimes, senses, nervous systems and storage capacity for experiences in the brain are coupled. This enables an individuality that not only models the environment by the signals it is receiving but also creates a selective regime that can generate individual goals. Cooperation with other individuals is enabled on an unprecedented scale of using information and experiences of multiple generations of conspecifics and foreign species. Functionality is used, analyzed and designed in artifacts.
Individuality increasingly develops the more experiences and individual habits can be stored and transmitted, and this is independent from egoistic or altruistic behavior of individuals. The effect of received information needs to be storable to make a difference in the receiving system. As has been discussed, kinetic information for itself can be stable for some time in its field, but to become distributable into different environments and in-between environments, it needs structural information. Maintenance is therefore a function of material structural dispositions or of a coupling between I
kin and I
Struc. In this paper, the focus has been on the maintenance functionality of the latter, since stability of matter is known from everyday experience. The maintenance account can assist in understanding the contribution of structural dispositions to the coupling between I
kin and I
Struc in the process of evolution. Storability is the basis for the original background of Bateson’s famous quote
18 where the difference that is made can do so as it leads to a change in the receiver’s mindset. With the evolution of robust means of information storage and processing, genetic storage, the human mind and its brain came into existence.
Table 1 shows an overview of selective regimes that can be differentiated based on impossible structurally disposed properties in the previous regime, which mark the transition to the respective subsequent selection regime, when occurring.