Sá R. Human biofield components explained: a tensegrity-based biophysical framework for energy medicine. Int J Complement Alt Med.
2025;18(2):77‒85. DOI: 10.15406/ijcam.2025.18.00731
In BTTM, these vibrational modes
disseminate signals throughout the component efficiently, without the
need for a linear flow of energy or matter (Figure 2)
Biofield-Tissue Tensegrity Matrix
(BTTM) is presented by combining concepts from physics, biology and medicine to serve
as a possible theoretical basis for energy therapies.
can act as non-local mediators
of cellular communication. Within the BTTM model, torsion fields
can be integrated as agents that enhance the bidirectional vibrational
coherence between phonons and solitons in the tissue tensegrity
matrix, connecting donor/therapist and recipient/patient.
https://pubs.acs.org/doi/10.1021/acscentsci.2c01114
microtubules are, unexpectedly, effective light harvesters.
exogenous photobiomodulation in the form of pulsed wave modulation of selected light wavelengths to direct endogenous biophotonic activity and molecular cellular dynamics. We highlight the relevance of this strategy to target and reprogram the developmental potential of tissue-resident stem cells in damaged tissues, affording precision regenerative medicine without the need for cell or tissue transplantation.
https://www.sciencedirect.com/science/article/pii/S0021925824023494
a memory state forms enabling the microtubule itself to behave as a memory-switching element whose hysteresis loss is nearly zero (12). These intriguing properties suggest that microtubules may play an essential role in high-speed informational processes, affecting cell biology at the level of both intra- and inter-cellular communication, (iii) Exploiting tryptophan autofluorescence lifetimes to probe energy hopping between aromatic residues in tubulin and microtubules, and investigating how the quencher concentration alters tryptophan autofluorescence lifetimes, showed that electronic energy can diffuse over 6.6 nm in microtubules (13). Such diffusion length is surprisingly high in microtubules, considering that they should be designed to play mechanical/structural roles intracellularly, and the equivalent value for chlorophyll a, which is known to be optimized for electronic energy transfer, is only in the 20 to 80 nm range (13)
https://phys.org/news/2025-03-experimental-nonlocal-energy-quantum-memories.html
"This insight led us to a bold conjecture: quantum correlations could enable the nonlocal alteration of energy distribution in space. This seemingly surreal phenomenon was alluded to in the de Broglie-Bohm theory, yet it has neither been formally named nor experimentally tested."
"The results imply that, in the framework of the de Broglie-Bohm theory, for two entangled particles, the energy carried by one of them can be changed from one place to another under the non-local influence of the other particle.
"This is exactly the 'nonlocal energy alteration' proposed in the study. It is important to emphasize that the term used here is 'alteration' rather than 'transfer,' meaning that this process does not involve superluminal energy transmission (i.e., it is a nonlocal energy modification induced by quantum correlations)."
Rick Sa responded to the below with some AI-cranked out generic spewed non-thinking response. Quite ironic since Eddie Oshins focused on what he called "Genuine Stupidity" instead of AI.
Additionally, I had hoped to draw attention among physicist to the plight of Yuri Orlov (eg. Oshins, 1983c). Orlov’s related approach, called “wave logic” (Orlov, 1975, 1981, 1982; Oshins 1983a), was initially a mathematical attempt to apply group theory to logic. Orlov insisted that “WAVE LOGIC IS NOT A LOGIC OF QUANTUM MECHANICS. Noncommuting operators of the wave logic relate to the same object and have a sense of equivalent propositions expressed in different languages. Noncommuting operators of quantum mechanics relate to different objects” (1975).
The corresponding “Lie algebra” (or local, mathematical group) is order dependent or noncommutative. This is the structure to the Lie algebra of observables in a quantum theory, although not in classical theory12.
The difference is that for classical waves that which does not commute is the position and the spatial frequency. For quantum particles that which does not commute is the position and the momentum which is related to spatial frequency through the all important Planck’s constant....
quantum, implicate holomovement which Pribram confuses with a hologram and classical sensory experience.
As I shall cite later, Bohm does not share this point of view. Indeed, he is quite clear both that holograms are classical entities and that according to quantum theory, any measurement requires a noninvertible, irreversible act of amplification, decoupling the observer from that which is observed.
The “laws of form” approach likened Epimenedes’ paradox (“This statement is false.”), and
self-referential paradox in general, to the arithmetic equation ( x = -1/x ). I took this arithmetic equation and converted it into a MATRIX eigenvalue equation [Xf = −I(X−1)f ], where X is a 2x2 matrix, f is a two spinor, -I is the additive inverse of the multiplicative identity, and X−1 represents the multiplicative matrix inverse to X.
Matrices have the property that their multiplication is order-dependent. Indeed, in describing Heisenberg’s creation of quantum mechanics, Max Born stated: “ ... And one morning ... I suddenly saw light: Heisenberg’s symbolic multiplication was nothing but the matrix calculus, well known to me since my student days.
... I recognized at once its formal significance. It meant that the two matrix products pq and qp are not
identical ... that matrix multiplication is not commutative ...” (Oshins and McGoveran, op.cit., ft.nt. 6). In quantum physics, there is a measure of the difference in such ordering, called the COMMUTATOR, which is precisely a measure of the INTERACTION between the measuring and the measured system ... the knower and the known.
What it did lead to was a confusion between Gabor’s holograms and Bohm’s notion of holomovement in his formulation of quantum physics, and, consequently, between classical wave models of coherent waves and quantum states which have projective, linear (and usually unitary) representations and thereby a (fundamentally different) principle of superposition.5
. Then again, this property of “noncommutivity” in itself might be valuable in some way....
In analogy to vectors, the sum of two turns is defined by addition head to tail modulo great circle transport . This addition is noncommutative, but associative. The turn of zero length T0(≡ T2kπ , k = 0, 1, 2...) realizes the identity operation (It has no length, nor direction ˆn, nor sense). The inverse to a turn T −1(T −1
AB ) = −T (+TBA), i.e. the turn with the same great circle and length,
but opposite sense. This group of Hamilton’s turns is isomorphic to SU(2,C) as 3-parameter objects giving a “finite size spinor” as “impenetrable object” in 3-space instead of a 2-parameter object such as Cartan’s “point spinor.” (Biedenharn and Louck, 1981; Sects. 2.3-2.4 & 2.7, note 2; and pp. 186 & 191)
I came up with the idea to construct matrix representations for them, similar
to what Heisenberg had done in quantum physics. I had been thinking about the suggestion by Watzlawick, Weakland and Fisch (1974) in Change: Principles of Problem Formulation and Problem Resolution to apply the mathematics of group theory to linguistic interaction because of their misdefinition (Ibid., pp. 4, 7) of mathematical “groups” as being “commutative” (order independent), since all quantum interactions take place through the property of not being commutative. I had come to MRI from New York to discuss this issue with Paul Watzlawick.
Although we shall be using the polarization of light in order to exhibit certain aspects of
interference, the reader is cautioned that the type of wave interference that is relevant to a quantum context has nothing to do with the interference of physical fields such as light (eg. as in holograms) (Oshins, 1989, 1991).]
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