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On the Carrier of Inertia Patrick Grahn1, Arto Annila2* and Erkki Kolehmainen3 1COMSOL, FI-00560 Helsinki, Finland 2Department of Physics, University of Helsinki, FI-00014 Helsinki, Finland 3Department of Chemistry, University of Jyväskylä, FI-40014 Jyväskylä, Finland *email: [email protected] Inertia is described as a reaction taken by vacuum to an action. The vacuum is perceived as a physical substance that embodies photons in pairs without net electromagnetic field. In this form the free space houses mere energy density in balance with average energy density of matter in the whole Universe. Therefore any local change in momentum will invariably perturb the all-embracing vacuum, whose reaction manifests itself as inertia. Accordingly, the vacuum energy density is also in a local balance with energy that is bound in a body. This manifests itself as a local gravitational potential energy. In this way gravity can be understood as an energy difference between the local and universal potential energy, and hence gravitational and inertial masses are identical. By the same token, gravity and electromagnetism share the similar form of force, since both are carried by the photons. Keywords: free energy, gravity, mass, quantum, photon, the principle of least action, vacuum 1. Introduction How does mass out there influence motions here? The question concerns the carrier of inertia whereas the cause of inertia itself has been understood to be the gravitational action due to the total mass of the Universe [1,2,3,4]. The universal gravitational potential experienced here builds up with distance r from the bodies out there, since their number increases as r2 and gravitational potential falls as 1/r. Thus, the most distant matter in the Universe contributes most to the inertial reaction. It is puzzling only how the inertial reaction due to the bodies out there acts at once here. Yet, despite being instantaneous, the inertial reaction has all the hallmarks of a radiative interaction that propagates at the speed of light. In other words, gravity and electromagnetism share the same functional form of force [5]. Thus, it is perplexing how the inertial reaction can on one hand be an action at a distance and on the other hand display the same characteristics as light? Put differently, how inertia can on one hand result from the most distant bodies out there and on the other hand manifest itself instantaneously here, just like a local field? Pieces of the puzzle do not fit to each other, or do they? Mathematically it is possible to combine waves that propagate forward in time with those that propagate backward in time to make up an instantaneous effect [6]. However, this solution by symmetry appears in a logical contradiction with time’s asymmetry, that is, with the universal arrow of time resulting from the Universe’s diluting expansion [7,8]. In other words, future does not match the past, and hence it is hard to imagine how the postulated pairing of gravitational waves for instantaneous effects could possibly be universally perfect. The problem is not only irreversibility but also pathdependence. The Universe displays history that accrues along its evolutionary course from all the past states in a non-determinate manner, not solely from the initial state along a deterministic course. Already the most distant observation of universal evolution, namely cosmic microwave background CMB radiation [9,10] reveals that low multipoles of its angular decomposition are not independent but anomalously correlated [11,12,13]. In general, subsequent states are correlated along the path of a non-holonomic process [8,14]. When history matters, the timeand path-dependent trajectories are at variance with constant-energy equations of motions that can, at least in principle, be transformed to a time-independent frame [15]. Then again, the postulated local field, as a means for the immediate inertial reaction, ought to be physical and have its sources, just like any other field. This implies a substance that embodies the universal gravitational potential in balance with its sources, that is, with all bodies in the Universe. Such a postulated physical vacuum seems to invite a return of the aether, which, in turn, has been abandoned since Michelson-Morley experiment [16,17]. To avoid this conflict, various transient or virtual fields have been suggested [18,19,20,21], thereby picturing the vacuum as an exceptional medium that possesses energy density about nJ/m3 without any substance [22]. Thus, the prevailing perception of vacuum appears to be inconsistent in one way or the other. To find a way out of the deadlock we bring forward the recently reconsidered possibility that the vacuum is after all a physical medium, not sustaining photon propagation, but embodied by the photons themselves [23,24,25]. 1 2. The photon-embodied physical vacuum According to the proposed percept the photons do not propagate exclusively in the form of single quanta of light, but in pairs so that electromagnetic fields of the two photons sum up to zero, and hence cancel each other exactly (Fig. 1). This phenomenon is also familiar from an anti-reflection coating that does not actually prevent the photons from reflecting but combines reflected rays to destructive interference, and hence a coated lens appears perfectly transparent. In the out-of-phase configuration the paired photons display no electromagnetic fields, but carry only energy density. Therefore, the natural free energy minimum state is dark and inert as observed. action as an integral part of matter will become a free quantum as an integral part of immaterial surrounding space [24,33,34]. We remind right away that this view of the photon as the elementary constituent was abandoned shortly after being introduced [31], because it was thought to be at variance with radiative decay via two or more alternative paths. Namely, the conservation of quanta seems to be violated when an initial state decays to the same ground state either directly by a single photon emission or via two intermediate states yielding three photons in succession. However, to reject the conservation of quanta by this reasoning does not appear to us full proof, because the quanta in the form of paired photons are not considered and counted. Therefore, it is of interest to see what can be explained and understood by the photon-embodied vacuum. 3. Comprehension by the physical vacuum (a) (b) Figure 1. When two photons, whose electromagnetic fields are shown in blue and red, co-propagate exactly out-of-phase, there is no net electromagnetic field, and hence the photon pair carries mere energy density (a). When the phase configuration departs from the complete destructive interference, e.g., near a charge, electromagnetic fields will manifest (b). This portrayal of vacuum in terms of the paired photons explains both radiative and seemingly instantaneous attributes of inertia. The vacuum’s radiative character is formalized in the equality c2oo = 1 that relates the speed of light to the free space properties of permittivity o and permeability o. Although the photon as the force carrier has its characteristic finite speed, the inertial reaction appears as instantaneous, because the vacuum is all-around. Then again, balance between the vacuum’s energy and the universal gravitational potential energy is given by the renowned zero-energy principle Mc2 – GM2/R = 0 [26,27] which can be written also as the unitary condition GM/c2R = 4Gt2 = 1 where the universal mass M is within radius R = ct of the Universe at its current age t = 13.8 billion years and G is the gravitational constant and is the average density of matter [22]. In the evolving Universe c and G cannot be constants but functions of the decreasing universal energy density [28,29]. In the other words, the properties of the diluting vacuum are changing, just as those of any other evolving substance. The idea of photon-embodied vacuum entails that the photon is an indestructible entity [30,31]. This means, for instance, that the total number of quanta is a constant in an isolated system [32]. Conversely, when the system opens up for radiative emission, at least one bound quantum of 3.1. Inertia’s radiative and instantaneous character There is no dilemma with inertial reaction appearing as if instantaneous despite the finite speed of light, because the photon-carried energy density is already present everywhere, and hence it will react to any action. In other words, the inertial reaction in fact propagates at the finite speed of light, but the universal gravitational potential here is highly invariant by summing up gravitational potentials of all bodies out there. Only a massive dematerialization out at a distant galaxy could momentarily perturb inertia here. Such a perturbation would arrive here at the speed of light, and hence could, at least in principle, be detected also by a measurement of the inertial reaction, not only by means of an interference detector. The perturbation on inertia would be minute, since the power of this propagating vector potential [4] will decrease inversely to the squared optical distance and directly to the frequency that shifts down due to expansion of the Universe [35,36]. Likewise, when the action perturbs the photon-embodied vacuum here, the energy density perturbation will start to propagate the Universe over and eventually it will reach distant bodies out there. By the same token, when the Universe is regaining its balance after the perturbation here, any one of its bodies out there will be tossed hardly at all. Any change in momentum dtp will inevitably couple to some dissipation. The change will manifest itself also relative to the universal vacuum. For instance, our motion along with the Milky Way is inescapably somewhat asymmetric, i.e., non-inertial relative to bodies in the rest of the Universe, and hence dtp displays itself in the cosmic microwave background radiation as a dipolar temperature gradient across the sky. Likewise, acceleration relative to the physical vacuum will manifest itself as Unruh effect [37]. In fact no motion along a piece of an open trajectory is truly non-dissipative, because the moving body will in- 2 variably keep changing its state relative to some other bodies whose distribution is asymmetric, albeit uniform on the largest scale. 3.2. Rotational inertia By the same token, rotational inertia is understood as the reaction taken by the universal vacuum to balance the action due to the body moving along the orbit. Only over a complete period absorption and emission relative to the whole Universe will sum up to zero. The quadratic dependence r2 of rotational inertia on the distance r from the axis of rotation follows from the same reasoning that the larger the radius of rotation, the larger realm of surrounding energy density is perturbed. Thus, the gravitational effect of distant bodies via the physical vacuum manifests itself as Coriolis and centrifugal forces, e.g., as a spinning body being oblate and as a meniscus of water spinning along with a bucket being curved [38]. 3.3. Equivalence principle When both the universal vacuum and the local gravitational potential are understood to embody the paired photons that can be regarded as gravitons, equivalence between the inertial and gravitational mass is inescapable. In other words, the equivalence principle is inevitable. The equivalence can be comprehended by considering mass as a measure of the total geodesic curvature of a quantized action. This measure, defined by Euler for curves, expresses how much a photon, bound in matter as an inter-action, or a particle, as a quantized action, is more curved than the freely propagating photons that constitute the reference vacuum. [39,40,41,42]. Of course, it will be only after eons of expansions that the tiny reference curvature 1/R will be flattened markedly from that it is today. Therefore mass appears as an invariant attribute of a body rather than being the measure relative to the whole Universe. By the same token, also charge and magnetic moment are understood as manifestations of the particle’s quantized geometry. When everything is understood in terms of the quantized actions, then the quanta of light propagating in the vicinity of a body will increase in energy density, i.e., blueshift by assuming paths of increased curvature to attain thermodynamic balance with the body’s mass, i.e., to adapt to the body’s curvature. According to this physical portrayal of everything in terms of actions the curved spacetime is an excellent mathematical model for the photon-embodied vacuum [43]. 3.4. Gravity When the local and universal energy densities are not in balance, the energy difference, i.e., the force manifest itself as gravity. When the surrounding energy density is sparser than the gravitational potential energy density within the system of bodies, then quanta will escape along the energy gradient from the system to its surroundings, and hence the bodies will move toward each other. Conversely, when the surrounding energy density is higher than that within the system of bodies, then quanta will enter the system from the rich surroundings, and hence the bodies will move apart. Most notably, distant galaxies move away from us, because the Universe shines quanta, albeit mostly in the invisible pairs of photons, between us and the distant bodies. Thus, gravity is not exclusively an attractive force but repulsive when the surroundings is rich energy. This character of gravity is no different from that of the electrostatic force. Neither two charges of opposite sign are exclusively attracted to each other, but move apart when the surrounding medium increases with energy. This repulsion of ions is obvious when a salt crystal dissolves in water. 3.5. Manifestations of universal gravity On cosmological scale the quantized physical vacuum when emerging from quanta that are emitted from matter, spans an energy density gradient across the Universe. The contemporary surroundings is sparse whereas the distant nascent environ is dense in energy. This gradient manifests itself as the universal gravitational force. The resulting acceleration, ao = c/t = cH in terms of Hubble constant H, is on the order of 10-10 ms-2. It is balanced by motions that display themselves in galaxy rotation and velocity dispersion of galaxies [25,44,45]. In general, the arrow of time relates to consumption of energy gradients [7]. The expansion of the Universe is by the physical portrayal of vacuum understood to result from the incessant combustion of matter-bound high-energy quanta to those free quanta of low-energy embodying the vacuum [46,47]. The current rate of expansion, i.e., on-going vacuum genesis, depends on mechanisms of combustion, most notably on contemporary stars of various kinds including black holes. Likewise, the nascent rate is understood to have depended on primordial mechanisms that produced ingredients for baryogenesis along with the dissipated quanta that constitute space. 3.6. Appearance of electromagnetic force carriers According to the textbook physics it seems a bit of a puzzle from where the photons of electromagnetic field appear instantaneously when an atom ionizes. In contrast there is no mystery, when the photons are understood to have been around all the time but paired in the out-of-phase configuration. Electromagnetic fields will appear instantaneously when an atom ionizes and induces a phase shift away from the paired-photon minimum-energy configuration (Fig. 1). Clearly, the photon can be detected easily when it is no longer exactly at the opposite phase to its co-propagating partner. Also the textbook’s virtual photon comes to existence only when it is detected. Thus, consequences of considering the vacuum as being physically embodied by the paired photons is not formally that different from picturing the vacuum comprising of virtual particles. 3 3.7. Casimir effect The photon-embodied vacuum can account for Casimir effect [48] as well. Instead of imagining virtual photons making up a field, the real but paired photons of vacuum generate a net force, attractive just as repulsive depending on the energy density difference between adjacent plates and their surroundings. In other words, the formalism remains the same, but the tangible interpretation substitutes the abstract construct of virtual photons. Furthermore, the dynamical Casimir effect [49] can be understood so that when the vacuum is subject to high-frequency perturbation, the photons in pairs will shift away from the perfect out-of-phase balance, and hence the single photons will emerge for detection at microwave band that covers most of the vacuum’s spectrum. Moreover, fluctuations in the photon-embodied vacuum can be understood to result in the Lamb Shift in the same way as quantum electrodynamics attributes fluctuations to field-theoretic vacuum [50,51]. The paired quanta fluctuate about the free energy minimum state, and hence their phases shift transiently away from the perfect cancelation. This perturbative potential gives rise to a small but detectable effect on electron orbits. The interdependency between electromagnetism and gravity due to their common force carrier is inevitable. The inseparable paired-photon phase and density can be qualitatively understood to manifest, for instance, as a difference in the measured proton charged radius depending on whether an electron or a much heavier muon is circulating the nucleus [52,53,54]. 3.8. Double-slit experiment Conceptual conundrums of the double-slit experiment resolve with ease when photons and other projectiles on their way to detector are understood to perturb and interfere with the paired photons that embody the vacuum. Put differently, when the physical vacuum is ignored, the projectiles are erroneously assumed to propagate in an imaginary emptiness, and hence the troublesome conceptual constructs. The Aharonov–Bohm effect [55], in turn, demonstrates that the surrounding energy density is a sum of an added vector potential and the omnipresent vacuum potential. The increase in energy density along the particle’s path of propagation, as usual, displays itself as a phase shift. 3.9. Field exclusion and phase-locking The Meissner effect [56] can be understood to display the physical character of vacuum so that a superconductor, as a closed system without coupling to its surroundings, cannot accept quanta from the applied field, but excludes them. Conversely, the Tajmar effect [57] can be interpreted so that when a ring cools down to the superconductive state, it will enclose the surrounding quanta as an integral part of its stationary state. Thus, when the superconductive ring is set to rotation, the phase-locked quanta in the immediate surroundings will follow. Nearby optical gyroscopes sense that the quanta that are next to the ring, will track the superconductor put in rotation. Conversely, when the ring is in a normal state, the quanta of vacuum are not locked but free, and hence the adjacent gyroscopes do not register such a marked inertial reaction when the ring is put in rotation. 4. Formalism of the physical vacuum Physics communicates by equations of motion its quantitative comprehension about nature. Specifically, when energy is conserved, the equation of motion accounts for the system in a steady-state thermodynamic balance in its surroundings or eventually decoupled from its surroundings altogether. In general, when energy is not conserved, the equation of motion describes the system in evolution from one state to another by either absorbing or emitting quanta with energy to gain balance with its surroundings in least time. We apply the same reasoning for the vacuum. 4.1. Vacuum at stationary-state dynamic balance When the vacuum’s photons are shifted away from the perfect out-of-phase configuration, typically due to presence of charges, and hence are readily detectable as electromagnetic fields, the familiar Lorenz gauge [58] Α 1 t 0 c2 (1) that links mathematically the electric potential and magnetic vector potential A, can be recognized as the physical equation of motion for the photon-embodied vacuum. For example, will decrease with time when the photons move away from a dense locus to sparser surrounding down along the spatial gradient of A, and vice versa, to maintain the thermodynamic balance. An energy density gradient due to a charge will manifest itself as the electric field E = – – ∂tA embodied by the vacuum’s photons. Accordingly a steady-state circulation due to an electric current will manifest itself as the magnetic field B = A. When the vacuum’s photons are in the perfect out-of-phase configuration, and hence hard to detect merely as gravitational fields, the same equation (Eq. 1) applies describing mere changes in energy density. The motion of vacuum at thermodynamic balance, where net dissipation vanishes, is no different from the changes in momentum p that keep leveling off sporadic gradients of potential energy U U t p 0 (2) to maintain the system in its thermodynamic balance. It is straightforward to show that Eq. 2 transcribes to Eq. 1 via 4 c∙ = ∂t and = U/ and |A| = |p|/ when the scalar potential U and the momentum p are divided by charge density . The to-and-fro flows of energy at thermodynamic balance are obtained explicitly when Eq. 2 is multiplied with velocity v to give v U t 2K 0 . (3) where changes in kinetic energy 2K = p∙v direct down along the gradients of potential energy U. The equation 3 applies equally to the stationary-state vacuum whose density perturbations level off at the speed of c, and hence Eq,. 3 reduces to Eq. 1. The steady-state circulation of vacuum about a body that is spinning with angular momentum L, is similar to magnetism, and hence it will manifest itself as gravito-magnetism due to the divergence-free part of the gravitational potential, i.e., vector potential A = GL × r/c2r3 [59,60]. The flows of energy density without electromagnetic fields are difficult, but not impossible to detect. Recently density waves originating from black hole mergers were picked up by sensitive interferometers [36]. Those huge collisions out there did not rock much anything here. It is worth emphasizing that according to the physical percept of vacuum, the gravitational wave is not a temporal distortion of an abstract metric, but a tangible density wave whose passage will amount to an increased index along the optical path of a diffractometer. 4.2. Vacuum in evolution When the vacuum is perturbed away from the free energy minimum state by accelerating charges, the familiar Poynting’s theorem [8,61] e v E e v 0c2 E B (4) describes the charge density e in acceleration down along the electric field E, and thereby consuming the potential energy , that couples to dissipation of photons along Poynting vector S = E B to the surrounding vacuum. This is to say that the universal vacuum acquires quanta from the local potential that keeps diminishing due to the decreasing separation of charges. When all material densities in energy have transformed to mere radiation, i.e. → 0 and v → c, Eq. 4 will reduce to Eq. 1 of equilibrium [8]. When the electromagnetic fields are not apparent for detection, but a net neutral body with mass m is falling down along the gradient of gravitational potential energy U = GmM/r due to mass M, the general equation of motion is dt 2K v U idt Q (5) where dtQ = c2dtm is annotated with i to denote that dissipation is orthogonal to U just as S in Eq. 4 is orthogonal to . When recalling that the change in kinetic energy dt2K = dt(p∙v), the integral form of Eq. 5 is recognized as the principle of least action in its original dissipative form by Maupertuis [62,63]. Thus, emergence and evolution of the vacuum is no different from other natural processes [8,64,65,66]. Accordingly, dispersion of vacuum energy, just like that of any other system, is skewed about the average energy kBT given by the Planck’s radiation law. 4.3. State equations of a single quantum In addition to the equation of motion for the vacuum as a physical substance there is the equation for the single quantum itself. The quantum of action in propagation carries energy E within its (period of) time t, and hence measures up to Planck’s constant h = Et. Likewise, ħ = E applies, when the quantum’s circulates within period = 2t. The vacuum’s photon-embodiment displays itself also in the invariant measure h = 2eΦ0 that relates the magnetic flux quantum Φ0 of a current loop, whose circulation amounts to 2e in units of the elementary charge e. These forms of Planck’s constants are, of course, mathematically identical to those in the textbooks where h appears only as a proportionality factor rather than being the measure of the indivisible basic constituent of nature. All in all, the familiar equations describe the physical vacuum without revision but with re-vision. The proposed photon-embodied vacuum provides merely a tangible account on various phenomena that inevitably involve the vacuum, most notably the inertial reaction. 5. Discussion The physical vacuum in the form of paired photons without net electromagnetic fields is such a trivial thought that one would expect it to have appeared already a long time ago to account for the universal gravity that manifests itself as inertia. It might well have surfaced, but presumably when luminiferous aether as a medium for the propagation of light was abandoned, also the idea of a photon-embodied vacuum submerged. Still today, the photons may seem like innumerable when appearing from the vacuum as if from nowhere and disappearing to the vacuum as if to nothingness. This superficially non-conserved character of photons is solidified by theory that introduces creation and annihilation operators without bookkeeping of quantized actions. The field-theoretic vacuum of quantum electrodynamics, albeit compliant with data, appears to us as a contrived abstraction. Virtual photons or other ephemeral embodiments of gravity and electromagnetism strike a contrast with the tangible thought that fields require sources. Therefore, we reason that the actual photons embodying the physical vacuum are precisely the field quanta of both electromagnetic and gravitational fields whose sources are the 5 charged and neutral bodies. Thus, the proposition of photon-embodied vacuum to explain gravity and electromagnetism in general and inertia specifically does not necessitate revision in the mathematical forms of modern physics, and hence matches measurements alike, but still provides a tangible interpretation of observations. The physical vacuum makes no categorical distinction between local and universal, because the quantized energy density permeates everything. For instance, the photons embody gravitational and Coulomb potential within an atom, and the photons embody likewise the surrounding vacuum. Thus, the quanta that are material as inter-actions, are not fundamentally distinct from the quanta that are radiative, i.e., immaterial. This revelation sheds light on Newton’s thinking [67]. Gravity must be caused by an agent, acting constantly according to certain laws; but whether this agent be material or immaterial, I have left to the consideration of my readers. [1] [17] Herrmann S., Senger A., Möhle K., Nagel M., Kovalchuk E. V., Peters A., 2009, Rotating optical cavity experiment testing Lorentz invariance at the 10−17 level, Physical Review D 80, 105011, arXiv:1002.1284 [18] Haisch B., Rueda A., Puthoff H. E., 1994, Inertia as a zero-point-field Lorentz force. Physical Review A 49, 678–694 [19] Carroll S. M., 2001, The Cosmological Constant. Living Rev. Relativity 4, 1 [20] Peebles P. J. E., Ratra B., 2003, The cosmological constant and dark energy. Reviews of Modern Physics 75, 559–606 [21] Bush J. W. M., 2015, The new wave of pilot-wave theory. Phys. Today 68, 47–53 doi: 10.1063/PT.3.2882. [22] Unsöld A., Baschek B., 1983, The New Cosmos. Translated by Smith R. C., Hein C. Springer-Verlag, New York, NY, USA, ISBN 978-1-4757-1791-4 [23] Annila A., 2010, All in action. Entropy 12, 2333–2358. [24] Annila A. Natural thermodynamics. Physica A 2016 444, 843–852. doi:10.1016/j.physa.2015.10.105 [25] Annila A. 2016, Rotation of galaxies within gravity of the Universe. Entropy 18, 191–205 [26] Tryon E. P., 1973, Is the Universe a Vacuum Fluctuation? Nature 246, 396–397 [27] Feynman R. P., Morinigo F. B., Wagner W. G., Hatfield B., 1995, Feynman Lectures on Gravitation. AddisonWesley, Reading, MA, USA [28] Urban M., Couchot F., Sarazin X., Djannati-Atai A., 2013, The quantum vacuum as the origin of the speed of light. Eur. Phys. J. D 31, 281–282 [29] Leuchs G., Villar A. S., Sánchez-Soto L. L., 2010, The quantum vacuum at the foundations of classical electrodynamics. Applied Physics B 100, 9–13 [30] Newton I., 1704, Opticks, 1979, Dover, New York, NY, USA: [31] Lewis G. N., 1926, The Conservation of Photons. Nature 118, 874–875 [32] Noether E., 1918, Invariante Variationsprobleme, in: Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen, Math.-Phys. Kl. 235–257. Translation: Noether E., 1971, Invariant variation problem. Transport Theory Statist. Phys. 1, 183–207 [33] Pernu T. K., Annila A., 2012, Natural emergence. Complexity 17, 44–47 [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] Mach E., 1883, The Science of Mechanics. 1960, Engl. transl. McCormack T. J., Open Court, LaSalle, IL, USA Sciama D. W., 1953, On the origin of inertia. MNRAS 113, 34–42 Raine D. J., 1981, Mach's Principle and Space- Time Structure. Reports on Progress in Physics 44, 1151–1195 Nordtvedt K., 1988, Existence of the gravitomagnetic interaction. International Journal of Theoretical Physics, 27, 1395–1404 Heaviside O., 1893, A gravitational and electromagnetic analogy. Part I, The Electrician 31, 281–282 Ciufolini I., Wheeler J. A., 1995, Gravitation and Inertia. Princeton University Press, Princeton, NJ, USA Zeh H. D., 2007, The physical basis of the direction of time. 5th edn. Springer, Berlin, Germany Tuisku P., Pernu T. K., Annila A., 2009, In the light of time. Proc. R. Soc. A 465, 1173–1198 Scott D., Smoot G., 2004, Cosmic Background Radiation Mini-Review. arXiv:astro-ph/0406567 in The Review of Particle Physics. S. Eidelman, et al., Physics Letters, B592, 1 Assis A. K. T., Neves, M. C. D., 1995, History of the 2.7 K temperature prior to Penzias and Wilson. Apeiron 2, 79–84 Bielewicz P., Eriksen H. K., Banday A. J., Górski K. M., Lilje P. B., 2005, Multipole vector anomalies in the firstyear WMAP data: a cut-sky analysis. Astrophysical Journal 635, 750–760, arXiv:astro-ph/0507186, doi:10.1086/497263 Copi C. J., Huterer D., Schwarz D. J., Starkman G. D., On the large-angle anomalies of the microwave sky. Monthly Notices of the Royal Astronomical Society 367, 79–102, 2006, arXiv:astro-ph/0508047 de Oliveira-Costa A., Tegmark M., 2006, CMB multipole measurements in the presence of foregrounds. Physical Review D 74, 023005, arXiv:astro-ph/0603369 Mäkelä T., Annila A., 2010, Natural patterns of energy dispersal. Phys. Life Rev. 7, 477–498 Smolin L., 1997, The present moment in quantum cosmology: challenges to the arguments for the elimination of time. arXiv:gr-qc/0104097 Michelson A. A., Morley E. W., 1887, On the Relative Motion of the Earth and the Luminiferous Ether. American Journal of Science 34, 333–345 References 6 [34] Grahn P., Annila A., Kolehmainen E., 2016, On the exhaust of EM-drive. AIP Advances 6, 065205 [35] Schutz B. F., 2003, Gravity from the ground up. Cambridge University Press, Cambridge, UK, ISBN 0-52145506-5 [36] Abbott B. P., et al., 2016, Observation of Gravitational Waves from a Binary Black Hole Merger. Phys. Rev. Lett. 116, 061102 [37] Unruh W. G., 1976, Notes on black-hole evaporation. Physical Review D 14, 870–892 [38] Lense J., Thirring H., 1918, Uber den einfluss der eigenrotation der zentralkorper auf die bewegung der planeten und monde nach der einsteinschen gravitationstheorie. Phys Z. 19, 156–163 [39] Do Carmo M. P., 1976, Differential geometry of curves and surfaces; Prentice-Hall Inc. Englewood Cliffs, NJ, USA [40] Slobodyan Yu. S., Geodesic curvature. Encyclopedia of Mathematics, Hazewinkel M., Ed.; Springer, 2001; ISBN 978-1-55608-010-4. https://www.encyclopediaofmath.org/index.php/Geodesic_curvature [41] Annila A., 2010, All in action. Entropy 12, 2333–2358 [42] Annila A., 2012, The meaning of mass. Int. J. Theor. Math. Phys. 2, 67–78 [43] Einstein A., 1916, The Foundation of the General Theory of Relativity. Annalen der Physik 49, 769–822 [44] Zwicky F., 1933, Die Rotverschiebung von extragalaktischen Nebeln. Helvetica Physica Acta 6, 110–127 [45] Zwicky F., 1937, On the Masses of Nebulae and of Clusters of Nebulae. Astrophysical Journal 86, 217–246 [46] Annila A., 2011, Least-time paths of light. MNRAS 416, 2944–2948 [47] Koskela M., Annila A., 2011, Least-action perihelion precession. MNRAS 417, 1742–1746 [48] Casimir H. B. G., Polder D., 1948, The Influence of Retardation on the London-van der Waals Forces. Phys. Rev. 73, 360–372 [49] Wilson C. M., Johansson G., Pourkabirian A., Simoen M., Johansson J. R., Duty T., Nori F., Delsing P., 2011, Observation of the dynamical Casimir effect in a superconducting circuit. Nature 479, 376–379 [50] Lamb W. E., Retherford R. C., 1947, Fine Structure of the Hydrogen Atom by a Microwave Method. Physical Review 72, 241–243 [51] Bethe H. A., Salpeter E. E., 1957, Quantum Mechanics of One- and Two-Electron Atoms. Berlin: Springer-Verlag [52] Pohl R., et al, 2013, Laser spectroscopy of muonic hydrogen. Annalen der Physik 525, 647–651 [53] Carlson C. E., 2015, The proton radius puzzle. Progress in Particle and Nuclear Physics 82, 59–77 [54] Pohl R., et al, 2016, Laser spectroscopy of muonic deuterium. Science 353, 669–673 [55] Aharonov Y., Bohm D., 1959, Significance of Electromagnetic Potentials in the Quantum Theory. Phys. Rev. 115, 485–491 [56] Meissner W., Ochsenfeld R., 1933, Ein neuer Effekt bei Eintritt der Supraleitfähigkeit. Naturwissenschaften 21, 787–788 [57] Tajmar M., Plesescu F., Seifert B., Marhold K., 2007, Measurement of Gravitomagnetic and Acceleration Fields Around Rotating Superconductors. AIP Conf. Proc. 880, 1071–1082 [58] Lorenz L., 1867, On the identity of the vibrations of light with electrical currents. Philos. Mag. 34, 287–301 [59] Straumann N., 1984, General Relativity and Relativistic Astrophysics. Springer, New York [60] Annila A., 2012, Probing Mach’s principle. MNRAS 423, 1973–1977 [61] Poynting J. H., 1884, On the Transfer of Energy in the Electromagnetic Field. Philosophical Transactions of the Royal Society of London. 175, 343–361 [62] De Maupertuis P.-L. M., 1744, Accord de différentes lois de la nature qui avaient jusqu’ici paru incompatibles. Mémoires de l’Académie Royale des Sciences de Paris 417– 426 [63] De Maupertuis P.-L. M., 1746, Les loix du mouvement et du repos déduites d’un principe metaphysique. Hist. Acad. Roy. Sci. Belleslett. 267–294 [64] Kaptayn J. C., 1903, Skew frequency curves in biology and statistics. Noordhoff Astronomical Laboratory, Groningen, The Netherlands [65] Limpert E., Stahel W. A., Abbt M., 200, Log-normal distributions across the sciences: keys and clues. Bioscience 51, 341–352 [66] Kaila V. R. I., Annila A., 2008, Natural selection for least action. Proceeding of Royal Society A 464, 3055–3070 [67] Newton I., 1693, Third letter to Bentley, 25 Feb 1693. Quoted in The Works of Bentley R., D.D., 1838, 3, 212213 7