Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Quantum Coherence in Ion Channels: An Alternating Electric Field Could Put the Idea to the Test

inquantio

Published Jul 21, 2026• 0 citations
Publisher

Abstract

The selectivity filter of a potassium channel passes about 100 million ions per second while still turning sodium away at a ratio of at least 10,000 to 1. The researchers proposed quantum coherence as a hypothesis, pointing out that the matter wavelength of a potassium ion (about 0.05 nm) is within a factor of five of the spacing of the potential inside the filter (about 0.24-0.25 nm), and that a calculated tunneling probability multiplied by the ion's trapping frequency gives a throughput approaching the measured conduction rate. As the key test of that hypothesis they proposed a resonance effect: when the channel is driven by an alternating electric field, the current should fall sharply at particular driving conditions, a phenomenon called dynamic localization that classical rate equation models cannot produce. [Quantum Biology Society] Every process in a living organism, from nerve signaling to muscle contraction, passes at some point through a protein tunnel called an ion channel. Potassium channels are among the most impressive of them. In the bacterial KcsA channel, an open gate lets through about 100 million potassium ions (K⁺) per second, close to the physical limit set by diffusion. At the same time it turns away sodium ions (Na⁺), which are similar in size, at a ratio of better than 10,000 to 1. The classical account explains this selectivity through the attraction between the ion and the filter, the repulsion between ions, and the fact that potassium pays a smaller energy penalty than sodium for shedding its hydration shell. But there is a physical tension in that picture: the thermal fluctuations of the backbone atoms that form the filter are large compared with the small difference in size between potassium and sodium, which has prompted calls to re-examine the traditional explanation. Alipasha Vaziri of the Howard Hughes Medical Institute's Janelia Farm Research Campus in the United States and Martin B. Plenio of the Institute of Theoretical Physics at Ulm University in Germany brought a quantum mechanical yardstick to this dilemma in a 2010 paper in New Journal of Physics (vol. 12, article 085001). The significance of the work lies not in asserting that quantum coherence definitely exists inside an ion channel, but in raising its possible existence as a hypothesis and designing a concrete way to test it experimentally. The authors were explicit that they are not arguing for macroscopic quantum states across the brain: any coherence they expect is a protein level phenomenon confined to subnanometer distances and picosecond times. ■ A Filter That Passes 100 Million Ions a Second and Sorts Them 10,000 to 1 The selectivity filter of the KcsA channel is a narrow tube about 0.3 nm across and about 1.2 nm long. Amino acid chains reaching in from four subunits form its walls, with the oxygen atoms of carbonyl groups lined up pointing into the pore. Sets of these oxygens lie in a plane and form binding sites where an ion can briefly rest. The passage is so narrow that a potassium ion, normally surrounded by eight water molecules, has to shed that entire hydration shell before it can enter. Inside the tube, potassium ions and water molecules move in single file, alternating with one another. Numerical calculations of the free energy of ion conduction find two configuration paths that are nearly degenerate in energy, separated by only about 2 kcal/mol, and x-ray diffraction data support this picture, revealing two equally represented arrangements of water and potassium in the filter, known as the 1,3 and 2,4 states. The binding sites are spaced about 0.24 nm apart, and the height of the barrier an ion must cross rises and falls between about 1.7 and 8 kBT (roughly 1-5 kcal/mol) depending on whether a given site is occupied and on the thermal vibrations of the protein. ■ Can an Ion Behave Like a Wave? At this point the authors offer two quantum mechanical estimates. The first turns on the idea of a matter wave. At room temperature the de Broglie wavelength of a potassium ion works out to about 0.05 nm, within a factor of five of the periodic spacing of the potential inside the filter (0.24-0.25 nm). That leaves room, they suggest, for the ion to behave like a wave striking a kind of diffraction grating as it crosses the periodic energy barriers. The second is quantum tunneling. The probability that a potassium ion passes through a barrier rather than over it comes out at about 7×10⁻⁵. Assuming the ion rattles against the barrier inside its binding site roughly 10¹² times per second, the product of the two gives a transmission rate approaching the observed figure of about 100 million ions per second. The system interacts strongly with its surroundings, however, so coherence cannot survive indefinitely. The authors' rough estimate puts the decoherence time, the interval over which the quantum state is destroyed, at 10⁻⁹-10⁻⁸ seconds, comparable to the expected tunneling times, and they identify the stretching vibration of the carbonyl groups as the main culprit. The protein structure that guides the ion is, paradoxically, also the source of the noise that scrambles its quantum state. ■ The Fingerprint of Coherence: A Sharp Drop in Current Under an Alternating Field The paper's central contribution is its proposal for measuring that coherence directly. The authors focus on what happens when an external alternating (ac) electric field is applied to shake the energy levels of the channel periodically. If the strength of the applied field is scanned while the driving frequency is held fixed, the ion current falls off sharply at particular values, a resonance effect known as dynamic localization, with the positions of the dips set jointly by the frequency and the strength of the drive. The principle is that when the shaking is mistimed, the probability waves describing the ion's possible routes interfere destructively, so the ion fails to advance and is trapped where it is. What matters is that this resonance can never appear in a classical rate equation model, in which the process is described purely in terms of probabilities: a classical model has no phase to interfere with in the first place, and the current would be essentially independent of the strength of the driving field. Conversely, as noise grows and quantum dephasing deepens, the resonances become shallower. Measuring the depth of the valley into which the current falls therefore offers a quantitative gauge of how much quantum coherence survives inside the channel. ■ Experimental Feasibility The tool the authors propose for the test is a modification of patch clamping, the electrophysiology technique long in routine use in biophysics. Using an excised patch, a steady ionic current is established by the difference in potassium concentration across the membrane (90 mM against 3 mM); an ac field at around 100 MHz is then superimposed and the resulting change in current is observed. The largest obstacle is the capacitive current induced by the fast ac field. At around 3 μA it is a million times larger than the picoampere (pA) ionic current the experiment is trying to measure. The authors set out practical ways around this: lock-in detection that exploits the difference in timing between the two currents, circuits that introduce negative capacitance as compensation, chambers built around artificial lipid bilayers, and nitrogen vacancy (NV) centers in diamond, nanoscale sensors recently developed for recording picoampere currents in biological systems. ■ Significance and Outlook The lasting value of this paper is that it takes quantum coherence in ion channels, until then an abstract speculation, and brings it into the realm of a physical prediction that can actually be verified or falsified with a current measurement. The authors themselves acknowledge that the model behind their calculations simplifies the formidable complexity of a real channel, and that ion conduction is a many body phenomenon, so more rigorous simulations and experiments must follow. Indeed, in the years since the 2010 proposal, more skeptical calculations of how long coherence can be maintained have appeared, and the debate, along with the experimental challenge, remains open. Whichever way the answer falls, the paper stands as an important marker in biophysics for supplying an experimental blueprint for judging how far the machinery of life is classical and where it begins to be quantum. #QuantumBiology #IonChannel #PotassiumChannel #SelectivityFilter #QuantumCoherence #Decoherence #KcsA #QuantumTunneling #MatterWave #Electrophysiology https://arxiv.org/abs/1006.3892

DOI
10.5281/zenodo.21468082

Related papers

Quantum Dynamics and Non-Local Effects Behind Ion Transition States during Permeation in Membrane Channel Proteins

Johann Summhammer, Georg Sulyok, Gustav Bernroider

ions in the highly conserved KcsA selectivity filter motive of voltage gated ion channels. We first show that the de Broglie wavelength of thermal ions is not much smaller than the periodic structure of Coulomb potentials in the nano-pore model of the selectivity filter. This implies that an ion may no longer be viewed to be at one exact position at a given time but can better be described by a quantum mechanical wave function. Based on first principle methods, we demonstrate solutions of a non-linear Schrödinger model that provide insight into the role of short-lived (~1 ps) coherent ion transition states and attribute an important role to subsequent decoherence and the associated quantum to classical transition for permeating ions. It is found that short coherences are not just beneficial but also necessary to explain the fast-directed permeation of ions through the potential barriers of the filter. Certain aspects of quantum dynamics and non-local effects appear to be indispensable to resolve the discrepancy between potential barrier height, as reported from classical thermodynamics, and experimentally observed transition rates of ions through channel proteins.

Entropy•Jul 27, 2018•24 citations

Quantum Rogue Waves Determine the Opening and Closing of Ion Channels... Demonstration of a Correlated Disorder Quantum Model

inquantio

A study published in Frontiers in Quantum Science and Technology elucidates that correlated disorder acts as a tunable quantum switch regulating the conduction and trapping of ions, by modeling biological ion channels as a linear quantum chain. As analyzed through a tight-binding Hamiltonian and Lindblad operators, the average traversal time of ions increases logarithmically according to the correlation parameter of the disorder, and it was confirmed that this mirrors the growth of quantum rogue wave probability. It mathematically proves that living organisms can precisely control the opening and closing of channels by adjusting microscopic disorder to quantum mechanically express transient trapped states inside the ion passageway. [Quantum Biology Society] Ion channels, which regulate the flow of ions across the cell membrane, serve as nanoscale gatekeepers essential for sustaining life. Until now, the opening and closing mechanism of ion channels has been explained by classical protein structural changes, but recently, the introduction of quantum mechanical transport models is opening a new perspective on observing life phenomena. The paper titled "Correlated disorder as a tunable switch between trapping and conduction in quantum ion channels," published in the international journal Frontiers in Quantum Science and Technology, mathematically proved the possibility that ion channels are sophisticated quantum switches utilizing quantum rogue waves (anomalous waves that become abnormally massive, amplifying like ocean waves). A joint research team including Iara Patrícia Da Silva Ramos, Rafael Gandolfi Lanzini, Leonardo Brunnet, and Sandra D. Prado from the Institute of Physics at the Federal University of Rio Grande do Sul in Brazil spearheaded this innovative study. ■ Quantum Chains and Rogue Waves in Ion Channels The research team modeled a biological ion channel (the selectivity filter of the KcsA potassium channel) as a one-dimensional linear quantum chain and precisely investigated the impact of correlated disorder—microscopic structural fluctuations within the protein—on the system through a tight-binding Hamiltonian and the Lindblad master equation. The analysis confirmed that as the balance between localization and mobility within the channel is regulated by disorder, anomalous wave phenomena such as quantum rogue waves, which coagulate abnormally massive energy, occur. ■ The Quantum Switch of Trapped States Controlled by Disorder According to the results of 10,000 independent ensemble simulations performed by the research team, the average traversal time of ions crossing the channel increased sharply in a logarithmic form in proportion to the correlation parameter (A) of the disorder. Surprisingly, this delay in traversal time perfectly matched the increased probability of quantum rogue waves occurring. This means that as the correlation of disorder becomes stronger, transient trapped states that delay the movement of particles are quantum mechanically expressed inside the ion channel. Ultimately, this suggests that living organisms possess highly evolved systems that actively adjust microscopic disorder within cells, precisely controlling them like a quantum switch alternating between conduction and trapping in ion passageways. https://www.frontiersin.org/journals/quantum-science-and-technology/articles/10.3389/frqst.2025.1725290/full

•Jul 13, 2026•0 citations

Quantum coherence on selectivity and transport of ion channels

Mina Seifi, Ali Soltanmanesh, Afshin Shafiee

Abstract Recently, it has been suggested that ion channel selectivity filter may exhibit quantum coherence, which may be appropriate to explain ion selection and conduction processes. Potassium channels play a vital role in many physiological processes. One of their main physiological functions is the efficient and highly selective transfer of K + ions through the membranes into the cells. To do this, ion channels must be highly selective, allowing only certain ions to pass through the membrane, while preventing the others. The present research is an attempt to investigate the relationship between hopping rate and maintaining coherence in ion channels. Using the Lindblad equation to describe a three-level system, the results in different quantum regimes are examined. We studied the distillable coherence and the second order coherence function of the system. The oscillation of distillable coherence from zero, after the decoherence time, and also the behavior of the coherence function clearly show the point that the system is coherent in ion channels with high throughput rates.

arXiv:2205.14389•Scientific Reports•Jun 2, 2022•20 citations

Coulomb interaction rules timescales in potassium ion channel tunneling

N De March, S D Prado, L G Brunnet

Assuming the selectivity filter of KcsA potassium ion channel may exhibit quantum coherence, we extend a previous model by Vaziri and Plenio (2010 New J. Phys. 12 085001) to take into account Coulomb repulsion between potassium ions. We show that typical ion transit timescales are determined by this interaction, which imposes optimal input/output parameter ranges. Also, as observed in other examples of quantum tunneling in biological systems, the addition of moderate noise helps coherent ion transport.

arXiv:1803.04480•Journal of Physics Condensed Matter•May 11, 2018•7 citations

Active quantum memory: Exploring the quantum dynamical process of voltage-gated ion channel

Yu-Juan Sun, Wei-Min Zhang

It is known that the opening or closing mechanism of a voltage-gated ion channel is triggered by the potential difference across the cell membrane in the nervous system. Based on this picture, we model the ion channel as a nanoscale two-terminal ionic tunneling junction. We apply an external time-varying voltage on the junction to mimic the membrane potential difference in the stimulation of neurons. We derive the non-Markovian quantum Langevin equation from the first principle of quantum mechanics for the ion transport in ion channels, and obtain the ion transport current in terms of quantum tunnelings of ions controlled by the time-varying voltage. We find that the time-varying voltage induces an effective magnetic flux, which causes quantum coherence in ion tunnelings. This effective magnetic flux induces further an oscillatory component to the spectral structure of the ion system, forming a time-dependent quantum memory. Such voltage-induced memory is defined as the active quantum memory, which manifests in the system with a regular oscillatory sideband structure in the ion transport current. The sideband structure demonstrates a multicrossing hysteresis in the current-voltage ( I − V ) curve, responding to the variation of the time-varying voltage (membrane potential difference). We also find that the strength of active quantum memory can be described by the ratio of amplitude and frequency of the time-varying voltage, and can be quantitatively measured through the number of nonzero cross points in the I − V hysteresis and conductance-voltage diagram. Additionally, we explore the temperature dependence of the active quantum memory in such a system. Further, we apply this model to the ion channel system on the biological energy scale. The description of these active quantum memory characteristics provides a quantum mechanical understanding to the underlying mechanism of ion channel dynamics.

arXiv:2411.12362•Physical Review Research•Jul 10, 2026•0 citations

Quantum coherence in ion channels: resonances, transport and verification

Alipasha Vaziri, Martin Bodo Plenio

Recently it was demonstrated that long-lived quantum coherence exists during excitation energy transport in photosynthesis. It is a valid question up to which length, time and mass scales quantum coherence may extend, how one may detect this coherence and what, if any, role it plays in the dynamics of the system. Here we suggest that the selectivity filter of ion channels may exhibit quantum coherence, which might be relevant for the process of ion selectivity and conduction. We show that quantum resonances could provide an alternative approach to ultrafast two-dimensional (2D) spectroscopy to probe these quantum coherences. We demonstrate that the emergence of resonances in the conduction of ion channels that are modulated periodically by time-dependent external electric fields can serve as signatures of quantum coherence in such a system. Assessments of experimental feasibility and specific paths towards the experimental realization of such experiments are presented.

arXiv:1006.3892•New Journal of Physics•Aug 2, 2010•88 citations
The selectivity filter of a potassium channel passes about 100 million ions per second while still turning sodium away at a ratio of at least 10,000 to 1. The researchers proposed quantum coherence as a hypothesis, pointing out that the matter wavelength of a potassium ion (about 0.05 nm) is within a factor of five of the spacing of the potential inside the filter (about 0.24-0.25 nm), and that a calculated tunneling probability multiplied by the ion's trapping frequency gives a throughput approaching the measured conduction rate. As the key test of that hypothesis they proposed a resonance effect: when the channel is driven by an alternating electric field, the current should fall sharply at particular driving conditions, a phenomenon called dynamic localization that classical rate equation models cannot produce. [Quantum Biology Society] Every process in a living organism, from nerve signaling to muscle contraction, passes at some point through a protein tunnel called an ion channel. Potassium channels are among the most impressive of them. In the bacterial KcsA channel, an open gate lets through about 100 million potassium ions (K⁺) per second, close to the physical limit set by diffusion. At the same time it turns away sodium ions (Na⁺), which are similar in size, at a ratio of better than 10,000 to 1. The classical account explains this selectivity through the attraction between the ion and the filter, the repulsion between ions, and the fact that potassium pays a smaller energy penalty than sodium for shedding its hydration shell. But there is a physical tension in that picture: the thermal fluctuations of the backbone atoms that form the filter are large compared with the small difference in size between potassium and sodium, which has prompted calls to re-examine the traditional explanation. Alipasha Vaziri of the Howard Hughes Medical Institute's Janelia Farm Research Campus in the United States and Martin B. Plenio of the Institute of Theoretical Physics at Ulm University in Germany brought a quantum mechanical yardstick to this dilemma in a 2010 paper in New Journal of Physics (vol. 12, article 085001). The significance of the work lies not in asserting that quantum coherence definitely exists inside an ion channel, but in raising its possible existence as a hypothesis and designing a concrete way to test it experimentally. The authors were explicit that they are not arguing for macroscopic quantum states across the brain: any coherence they expect is a protein level phenomenon confined to subnanometer distances and picosecond times. ■ A Filter That Passes 100 Million Ions a Second and Sorts Them 10,000 to 1 The selectivity filter of the KcsA channel is a narrow tube about 0.3 nm across and about 1.2 nm long. Amino acid chains reaching in from four subunits form its walls, with the oxygen atoms of carbonyl groups lined up pointing into the pore. Sets of these oxygens lie in a plane and form binding sites where an ion can briefly rest. The passage is so narrow that a potassium ion, normally surrounded by eight water molecules, has to shed that entire hydration shell before it can enter. Inside the tube, potassium ions and water molecules move in single file, alternating with one another. Numerical calculations of the free energy of ion conduction find two configuration paths that are nearly degenerate in energy, separated by only about 2 kcal/mol, and x-ray diffraction data support this picture, revealing two equally represented arrangements of water and potassium in the filter, known as the 1,3 and 2,4 states. The binding sites are spaced about 0.24 nm apart, and the height of the barrier an ion must cross rises and falls between about 1.7 and 8 kBT (roughly 1-5 kcal/mol) depending on whether a given site is occupied and on the thermal vibrations of the protein. ■ Can an Ion Behave Like a Wave? At this point the authors offer two quantum mechanical estimates. The first turns on the idea of a matter wave. At room temperature the de Broglie wavelength of a potassium ion works out to about 0.05 nm, within a factor of five of the periodic spacing of the potential inside the filter (0.24-0.25 nm). That leaves room, they suggest, for the ion to behave like a wave striking a kind of diffraction grating as it crosses the periodic energy barriers. The second is quantum tunneling. The probability that a potassium ion passes through a barrier rather than over it comes out at about 7×10⁻⁵. Assuming the ion rattles against the barrier inside its binding site roughly 10¹² times per second, the product of the two gives a transmission rate approaching the observed figure of about 100 million ions per second. The system interacts strongly with its surroundings, however, so coherence cannot survive indefinitely. The authors' rough estimate puts the decoherence time, the interval over which the quantum state is destroyed, at 10⁻⁹-10⁻⁸ seconds, comparable to the expected tunneling times, and they identify the stretching vibration of the carbonyl groups as the main culprit. The protein structure that guides the ion is, paradoxically, also the source of the noise that scrambles its quantum state. ■ The Fingerprint of Coherence: A Sharp Drop in Current Under an Alternating Field The paper's central contribution is its proposal for measuring that coherence directly. The authors focus on what happens when an external alternating (ac) electric field is applied to shake the energy levels of the channel periodically. If the strength of the applied field is scanned while the driving frequency is held fixed, the ion current falls off sharply at particular values, a resonance effect known as dynamic localization, with the positions of the dips set jointly by the frequency and the strength of the drive. The principle is that when the shaking is mistimed, the probability waves describing the ion's possible routes interfere destructively, so the ion fails to advance and is trapped where it is. What matters is that this resonance can never appear in a classical rate equation model, in which the process is described purely in terms of probabilities: a classical model has no phase to interfere with in the first place, and the current would be essentially independent of the strength of the driving field. Conversely, as noise grows and quantum dephasing deepens, the resonances become shallower. Measuring the depth of the valley into which the current falls therefore offers a quantitative gauge of how much quantum coherence survives inside the channel. ■ Experimental Feasibility The tool the authors propose for the test is a modification of patch clamping, the electrophysiology technique long in routine use in biophysics. Using an excised patch, a steady ionic current is established by the difference in potassium concentration across the membrane (90 mM against 3 mM); an ac field at around 100 MHz is then superimposed and the resulting change in current is observed. The largest obstacle is the capacitive current induced by the fast ac field. At around 3 μA it is a million times larger than the picoampere (pA) ionic current the experiment is trying to measure. The authors set out practical ways around this: lock-in detection that exploits the difference in timing between the two currents, circuits that introduce negative capacitance as compensation, chambers built around artificial lipid bilayers, and nitrogen vacancy (NV) centers in diamond, nanoscale sensors recently developed for recording picoampere currents in biological systems. ■ Significance and Outlook The lasting value of this paper is that it takes quantum coherence in ion channels, until then an abstract speculation, and brings it into the realm of a physical prediction that can actually be verified or falsified with a current measurement. The authors themselves acknowledge that the model behind their calculations simplifies the formidable complexity of a real channel, and that ion conduction is a many body phenomenon, so more rigorous simulations and experiments must follow. Indeed, in the years since the 2010 proposal, more skeptical calculations of how long coherence can be maintained have appeared, and the debate, along with the experimental challenge, remains open. Whichever way the answer falls, the paper stands as an important marker in biophysics for supplying an experimental blueprint for judging how far the machinery of life is classical and where it begins to be quantum. #QuantumBiology #IonChannel #PotassiumChannel #SelectivityFilter #QuantumCoherence #Decoherence #KcsA #QuantumTunneling #MatterWave #Electrophysiology https://arxiv.org/abs/1006.3892
ions in the highly conserved KcsA selectivity filter motive of voltage gated ion channels. We first show that the de Broglie wavelength of thermal ions is not much smaller than the periodic structure of Coulomb potentials in the nano-pore model of the selectivity filter. This implies that an ion may no longer be viewed to be at one exact position at a given time but can better be described by a quantum mechanical wave function. Based on first principle methods, we demonstrate solutions of a non-linear Schrödinger model that provide insight into the role of short-lived (~1 ps) coherent ion transition states and attribute an important role to subsequent decoherence and the associated quantum to classical transition for permeating ions. It is found that short coherences are not just beneficial but also necessary to explain the fast-directed permeation of ions through the potential barriers of the filter. Certain aspects of quantum dynamics and non-local effects appear to be indispensable to resolve the discrepancy between potential barrier height, as reported from classical thermodynamics, and experimentally observed transition rates of ions through channel proteins.
A study published in Frontiers in Quantum Science and Technology elucidates that correlated disorder acts as a tunable quantum switch regulating the conduction and trapping of ions, by modeling biological ion channels as a linear quantum chain. As analyzed through a tight-binding Hamiltonian and Lindblad operators, the average traversal time of ions increases logarithmically according to the correlation parameter of the disorder, and it was confirmed that this mirrors the growth of quantum rogue wave probability. It mathematically proves that living organisms can precisely control the opening and closing of channels by adjusting microscopic disorder to quantum mechanically express transient trapped states inside the ion passageway. [Quantum Biology Society] Ion channels, which regulate the flow of ions across the cell membrane, serve as nanoscale gatekeepers essential for sustaining life. Until now, the opening and closing mechanism of ion channels has been explained by classical protein structural changes, but recently, the introduction of quantum mechanical transport models is opening a new perspective on observing life phenomena. The paper titled "Correlated disorder as a tunable switch between trapping and conduction in quantum ion channels," published in the international journal Frontiers in Quantum Science and Technology, mathematically proved the possibility that ion channels are sophisticated quantum switches utilizing quantum rogue waves (anomalous waves that become abnormally massive, amplifying like ocean waves). A joint research team including Iara Patrícia Da Silva Ramos, Rafael Gandolfi Lanzini, Leonardo Brunnet, and Sandra D. Prado from the Institute of Physics at the Federal University of Rio Grande do Sul in Brazil spearheaded this innovative study. ■ Quantum Chains and Rogue Waves in Ion Channels The research team modeled a biological ion channel (the selectivity filter of the KcsA potassium channel) as a one-dimensional linear quantum chain and precisely investigated the impact of correlated disorder—microscopic structural fluctuations within the protein—on the system through a tight-binding Hamiltonian and the Lindblad master equation. The analysis confirmed that as the balance between localization and mobility within the channel is regulated by disorder, anomalous wave phenomena such as quantum rogue waves, which coagulate abnormally massive energy, occur. ■ The Quantum Switch of Trapped States Controlled by Disorder According to the results of 10,000 independent ensemble simulations performed by the research team, the average traversal time of ions crossing the channel increased sharply in a logarithmic form in proportion to the correlation parameter (A) of the disorder. Surprisingly, this delay in traversal time perfectly matched the increased probability of quantum rogue waves occurring. This means that as the correlation of disorder becomes stronger, transient trapped states that delay the movement of particles are quantum mechanically expressed inside the ion channel. Ultimately, this suggests that living organisms possess highly evolved systems that actively adjust microscopic disorder within cells, precisely controlling them like a quantum switch alternating between conduction and trapping in ion passageways. https://www.frontiersin.org/journals/quantum-science-and-technology/articles/10.3389/frqst.2025.1725290/full
Abstract Recently, it has been suggested that ion channel selectivity filter may exhibit quantum coherence, which may be appropriate to explain ion selection and conduction processes. Potassium channels play a vital role in many physiological processes. One of their main physiological functions is the efficient and highly selective transfer of K + ions through the membranes into the cells. To do this, ion channels must be highly selective, allowing only certain ions to pass through the membrane, while preventing the others. The present research is an attempt to investigate the relationship between hopping rate and maintaining coherence in ion channels. Using the Lindblad equation to describe a three-level system, the results in different quantum regimes are examined. We studied the distillable coherence and the second order coherence function of the system. The oscillation of distillable coherence from zero, after the decoherence time, and also the behavior of the coherence function clearly show the point that the system is coherent in ion channels with high throughput rates.
Assuming the selectivity filter of KcsA potassium ion channel may exhibit quantum coherence, we extend a previous model by Vaziri and Plenio (2010 New J. Phys. 12 085001) to take into account Coulomb repulsion between potassium ions. We show that typical ion transit timescales are determined by this interaction, which imposes optimal input/output parameter ranges. Also, as observed in other examples of quantum tunneling in biological systems, the addition of moderate noise helps coherent ion transport.
It is known that the opening or closing mechanism of a voltage-gated ion channel is triggered by the potential difference across the cell membrane in the nervous system. Based on this picture, we model the ion channel as a nanoscale two-terminal ionic tunneling junction. We apply an external time-varying voltage on the junction to mimic the membrane potential difference in the stimulation of neurons. We derive the non-Markovian quantum Langevin equation from the first principle of quantum mechanics for the ion transport in ion channels, and obtain the ion transport current in terms of quantum tunnelings of ions controlled by the time-varying voltage. We find that the time-varying voltage induces an effective magnetic flux, which causes quantum coherence in ion tunnelings. This effective magnetic flux induces further an oscillatory component to the spectral structure of the ion system, forming a time-dependent quantum memory. Such voltage-induced memory is defined as the active quantum memory, which manifests in the system with a regular oscillatory sideband structure in the ion transport current. The sideband structure demonstrates a multicrossing hysteresis in the current-voltage ( I − V ) curve, responding to the variation of the time-varying voltage (membrane potential difference). We also find that the strength of active quantum memory can be described by the ratio of amplitude and frequency of the time-varying voltage, and can be quantitatively measured through the number of nonzero cross points in the I − V hysteresis and conductance-voltage diagram. Additionally, we explore the temperature dependence of the active quantum memory in such a system. Further, we apply this model to the ion channel system on the biological energy scale. The description of these active quantum memory characteristics provides a quantum mechanical understanding to the underlying mechanism of ion channel dynamics.
Recently it was demonstrated that long-lived quantum coherence exists during excitation energy transport in photosynthesis. It is a valid question up to which length, time and mass scales quantum coherence may extend, how one may detect this coherence and what, if any, role it plays in the dynamics of the system. Here we suggest that the selectivity filter of ion channels may exhibit quantum coherence, which might be relevant for the process of ion selectivity and conduction. We show that quantum resonances could provide an alternative approach to ultrafast two-dimensional (2D) spectroscopy to probe these quantum coherences. We demonstrate that the emergence of resonances in the conduction of ion channels that are modulated periodically by time-dependent external electric fields can serve as signatures of quantum coherence in such a system. Assessments of experimental feasibility and specific paths towards the experimental realization of such experiments are presented.