<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2024.122031</article-id><article-id pub-id-type="publisher-id">JAMP-131261</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Mechanism of Universal Quantum Computation in the Brain
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Aman</surname><given-names>Chawla</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Salvatore</surname><given-names>Domenic Morgera</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Computer Science and Engineering, Indian Institute of Technology, Delhi, India</addr-line></aff><aff id="aff2"><addr-line>Department of Electrical Engineering, University of South Florida, Tampa, USA</addr-line></aff><pub-date pub-type="epub"><day>07</day><month>02</month><year>2024</year></pub-date><volume>12</volume><issue>02</issue><fpage>468</fpage><lpage>474</lpage><history><date date-type="received"><day>25,</day>	<month>December</month>	<year>2023</year></date><date date-type="rev-recd"><day>19</day>	<month>February</month>	<year>2024</year>	</date><date date-type="accepted"><day>22,</day>	<month>February</month>	<year>2024</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, the authors extend 
  [1] and provide more details of how the brain may act like a quantum computer. In particular, positing the difference between voltages on two axons as the environment for ions undergoing spatial superposition, we argue that evolution in the presence of metric perturbations will differ from that in the absence of these waves. This differential state evolution will then encode the information being processed by the tract due to the interaction of the quantum state of the ions at the nodes with the “controlling’ potential. Upon decoherence, which is equal to a measurement, the final spatial state of the ions is decided and it also gets reset by the next impulse initiation time. Under synchronization, several tracts undergo such processes in synchrony and therefore the picture of a quantum computing circuit is complete. Under this model, based on the number of axons in the corpus callosum alone, we estimate that upwards of 50 million quantum states might be prepared and evolved every second in this white matter tract, far greater processing than any present quantum computer can accomplish.
 
</p></abstract><kwd-group><kwd>Axons</kwd><kwd> Quantum computation</kwd><kwd> Metric perturbation</kwd><kwd> Decoherence</kwd><kwd> Time-coded information</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>As per Tegmark [<xref ref-type="bibr" rid="scirp.131261-ref2">2</xref>] , the smallest neuron imaginable, with only a single ion traversing the cell, would have a decoherence time of 10e−14 seconds. As per [<xref ref-type="bibr" rid="scirp.131261-ref3">3</xref>] , gravitational waves with strains of the order of h = 1e−16 will have an impact on axon tract information processing at the time order of 10e−14 seconds to 10e−18 seconds. Multiply each of the above three time periods by 1e17 to get 1000 seconds, 1000 seconds and 1 second. Thus, if I start my clock now and a neuron can stay coherent for 1000 seconds, then in parallel I can consider the other two numbers. That is, I will send along (in the past) a gravitational wave in the direction of my neuron tract. Say at t = 0 it interacts with the axon tract. As a result, if in its absence there was zero time difference between action potential initiation times on the two axons, in its presence this increases to say 100 seconds. As information is time-coded in the brain, the organism can sense the fact that there is some timing differential in progress. But can it do something with this information? Well, suppose the wave is switched on and off 3 times, then about 300 seconds of time differential is accumulated by the tract input-output. But each of the neurons in the tract was in a quantum state during this time. This implies that the tract itself was in a joint quantum state. Now in the absence of these 3 switches, the quantum state would be preserved, but due to the 3 switches, it would get perturbed to a different state. This transformation can then be measured quantum mechanically, in order to detect the passage of 3 switches of a gravitational wave. If no measurement is performed, then because the coherence time is an additional 700 seconds, the perturbed quantum state would in principle be held for another 700 seconds. In contrast, if the coherence time was say 0.1 second, then there would be no initial quantum state which could be perturbed 3 times gently to another quantum state and we would strictly be in the classical domain.</p><p>The perturbed quantum state is held for 700 seconds. This quantum information can, if it is part of a larger tract quantum state, be considered as a new state of the larger tract. In other words, the gravity wave induced a “quantum operation’’ on part of the brain. Several such different gravity waves can impinge sequentially or in parallel in different brain regions, carrying out a quantum computation in the brain. The moment the computation is over, say, the coherence time elapses and a decohering mechanism such as a measurement is carried out on the brain. This measurement thus reads out the result of this quantum computation. In other words, the brain can act like a quantum computer [<xref ref-type="bibr" rid="scirp.131261-ref1">1</xref>] .</p><p>The paper is structured as follows. In Section 2 we provide a review of Tegmark’s paper and its implications and differences as compared to the present work, along with a survey of relevant papers. In Section 3 we look in detail at the action potential level, going further down to the quantum level. Finally, we conclude in Section 4.</p></sec><sec id="s2"><title>2. Literature Review</title><p>In a series of papers [<xref ref-type="bibr" rid="scirp.131261-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref6">6</xref>] , V. S. Markin studied the propagation of action potentials in nerve bundles. Markin’s method differs from that of Hodgkin and Huxley in that he assumes a solvable model. In other words, by assuming a simple form for the ionic currents, he is able to get a solution to the propagation equations. He extends his single-axon model to several interacting axons as well.</p><p>In Jonathan Bell’s work on the coupled propagation of action potentials [<xref ref-type="bibr" rid="scirp.131261-ref7">7</xref>] , he looks at the ephaptic coupling. In this context, he studies “waves” propagating on coupled axons using perturbation theory. Bell’s paper is seminal and adds rigor to Arvanitaki’s experimental work on ephaptic transmission. Bell is able to give an exact theorem governing the rise of the coupled pulse.</p><p>In Wojtiech Zurek’s works on decoherence [<xref ref-type="bibr" rid="scirp.131261-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref10">10</xref>] , he starts with simple model systems and studies decoherence under coupling between two systems. This work is related to his work on the classical-quantum border since decoherence is effectively how one transitions from the quantum to the classical domain. Zurek’s work is important and he may be one of the “fathers” of decoherence theory.</p><p>Tegmark’s paper [<xref ref-type="bibr" rid="scirp.131261-ref2">2</xref>] contains decoherence computations. He divides the problem into ion-ion, ion-water and other decoherence mechanisms. For each such mechanism, he considers a superposition of ions between the inside and the outside of the cell. Within say the ion-ion collision-mediated decoherence section, he computes how long the spatial superposition state will stay quantum mechanical. His estimates yield the conclusion that decoherence precludes a significant role for quantum features because the characteristic time of a neuron is the action potential duration of 2 ms. He also considers microtubules and the associated decoherence times.</p><p>This absence of quantum effects can be used to argue that the brain and conscious processes can be entirely explained in terms of classical physics. In the present paper however, we show that the entire universe in a sense has a say in the quantum computation being performed in each part of the brain and the action potential is a very “summed up” or “gross” indication of what is happening at the deeper physical layers of the brain<sup>1</sup>.</p><p>Einstein and Rosen, in a joint paper, explore the consequences of general relativity in a specific direction, that of the generation and propagation of cylindrical gravitational waves [<xref ref-type="bibr" rid="scirp.131261-ref12">12</xref>] . Thorne’s work on gravitational radiation provides detailed analysis and a modern survey of the then-current status of the field of gravitational wave research [<xref ref-type="bibr" rid="scirp.131261-ref13">13</xref>] . Other relevant literature includes the paper of Penrose and Hameroff wherein they propose microtubule-based quantum computation in the brain [<xref ref-type="bibr" rid="scirp.131261-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.131261-ref16">16</xref>] . In the next section, we delve deeper into our specific proposal as it pertains to the theme of this paper.</p></sec><sec id="s3"><title>3. Mechanism</title><p>In this section, we delve into the mechanism by which a metric perturbation ends up influencing the quantum computation performed in an axon tract. Consider two slightly temporally displaced action potentials, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>Due to the gravitational wave, the temporal gap between the two action potentials, a, takes the value a<sub>1</sub> seconds during its presence and a<sub>2</sub> seconds during its absence. Suppose that V<sub>2</sub> - V<sub>1</sub> induces the quantum environment of an ion in the node of Ranvier (please see <xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>Thus the potential V(x) that enters into the Schrodinger evolution equation will be different during the presence and the absence of the gravitational wave. That is, the evolution will be different in the two cases. Again, if a different gravitational wave-tract interaction takes place, the evolution will be of yet another type. Post evolution and subsequent decoherence, and following further classical evolution (see <xref ref-type="fig" rid="fig3">Figure 3</xref>), the action potential initiation process of the cell starts up again and this re-prepares a quantum state of the tract.</p><p>Suppose there are a few tracts, each with synchronized impulses, where the synchronization has taken place using a combination of electric fields (between tracts) and currents (intra-tract) [<xref ref-type="bibr" rid="scirp.131261-ref17">17</xref>] . At a particular instant say t<sub>a</sub>, all the axons are synchronized, and a joint quantum state is prepared on each of the axons. If there is a way for us to show that this joint state is actually entangled, then it results in more interesting processes taking place in the tract. But regardless, the joint quantum state of the ions will evolve under the influence of slightly different gravitational impact on each axon. And because there is this parallel evolution, we have the process of a quantum circuit evolution taking place [<xref ref-type="bibr" rid="scirp.131261-ref18">18</xref>] . This is illustrated in <xref ref-type="fig" rid="fig4">Figure 4</xref>. Where square blocks are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, unitary gates are normally placed in the usual quantum circuit paradigm [<xref ref-type="bibr" rid="scirp.131261-ref19">19</xref>] , and triangular blocks are where measurements (POVMs, say) are normally performed.</p></sec><sec id="s4"><title>4. Limitations and Future Work</title><p>We have presented a model for brain quantum computation in this paper. The key insight of this model was obtained once progress was made in understanding how metric perturbations influence the timing of action potentials in a tract that has current-mediated coupling [<xref ref-type="bibr" rid="scirp.131261-ref3">3</xref>] . From there we connected the modified action potential waveforms to the modified environment that an ion in the axon’s node of Ranvier would experience. This allowed us to visualize the entire intertwined cycle of a single computation starting with quantum evolution, decoherence, and classical evolution and finally followed by the classical reset phase wherein a new action potential is initiated. This four-step cycle can potentially be used to develop novel classical-quantum machine-learning algorithms as well.</p><p>Furthermore, we could have set up a mathematical framework for the entire process of quantum computation, but did not do so. We felt that there are adequate presentations of quantum computation in the literature. Our main goal was to present the novel aspect, namely that these computations can take place in the coherence window and the external “control” or “direction” is provided by impinging metric perturbations. In future work we need to investigate and demonstrate a mechanism for entanglement between the various tracts.</p><p>To conclude, this paper has pushed forward our understanding of how man and his universe are integrated as one inseparable whole, even at the level that at least some aspects of what man thinks and does are enabled and directed by fundamental phenomena in the universe. Thus without the need for positing any external entity, the universe is seen to be a guiding force in the life of each being.</p><p>This paper’s view is not without its limitations. For example, different brain-like entities, all and each governed by the whole universe, do interact in space and time. The present paper says nothing about the interaction’s back-action on each entity and its quantum computation. The picture shown by Tegmark [<xref ref-type="bibr" rid="scirp.131261-ref2">2</xref>] with a pie-chart-like partitioning into the observer, observation and the observed acquires added relevance in the light of this remark and will need to be further explored in future work. Further, John Wheeler’s view of the universe as a self-excited quantum circuit [<xref ref-type="bibr" rid="scirp.131261-ref20">20</xref>] can be re-imagined as a medusa-headed serpent looking at its own origin, instead of a single-headed serpent doing so. Which of the two possibilities is more realistic, is left for future research.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Chawla, A. and Morgera, S.D. (2024) Mechanism of Universal Quantum Computation in the Brain. Journal of Applied Mathematics and Physics, 12, 468-474. https://doi.org/10.4236/jamp.2024.122031</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.131261-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chawla, A. (2022) A Gedanken Experiment on the Brain as a Quantum Computer. Research Gate Preprint.</mixed-citation></ref><ref id="scirp.131261-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Tegmark, M. (2000) Importance of Quantum Decoherence in Brain Processes. Physical Review E, 61, Article 4194. https://doi.org/10.1103/PhysRevE.61.4194</mixed-citation></ref><ref id="scirp.131261-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Chawla, A. and Morgera, S.D. (2023) Computer Study of Metric Perturbations Impinging on Coupled Axon Tracts. 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