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CRC Press eBooks

Quantum Mechanics of Ion Channels

Mohammad Ashrafuzzaman

Published Jul 30, 2021• 0 citations
Publisher

Abstract

Ion channels are stable over a wide range of time scales in the order of millisecond to microsecond or even smaller time range. This time scale is based on measurements using available experimental techniques. The same time scale is indeed followed by channel-carried charges while getting transported across the host membrane. This concept of gross time-dependent motion is valid when one consider ion channels to be classical mechanical systems following related formalism regarding their construction, transport, and other localized static and dynamic phenomena. Three decades ago, Conti and Stuhmer recorded the asymmetric displacement currents associated with the gating of nerve sodium channels in cell-attached macropatches of Xenopus laevis oocytes injected with exogenous mRNA coding for rat-brain-II sodium channels. Theoretically, tunneling is possible whenever quantum states are separated by a potential energy barrier, where the potential energy is a function of some state variable(s) of the system.

DOI
10.1201/9781003010654-10

Related papers

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

Relevance of Quantum Mechanics in Circuit Implementation of Ion channels in Brain Dynamics

Mitra, Indranil, Sisir Roy

With an increasing amount of experimental evidence pouring in from neurobiological investigations, it is quite appropriate to study viable reductionist models which may explain some of the features of brain activities. It is now quite well known that the Hodgkin-Huxley (HH) Model has been quite successful in explaining the neural phenomena. The idea of circuit equivalents and the membrane voltages corresponding to neurons have been remarkable which is essentially a classical result. In view of some recent results which show that quantum mechanics may be important at suitable length scales inside the brain, the question which becomes quite important is to find out a proper quantum analogue of the HH scheme which will reduce to the well known HH model in a suitable limit. From the ideas of neuro-manifold and the relevance of quantum mechanics at some length scales in the ion channels, we investigate this situation in this paper by taking into consideration the Schrödinger equation in an arbitrary manifold with a metric, which is in some sense a special case of the heat kernel equation. The next important approach we have taken in order to bring about it's relevance in brain studies and to make connection with HH models is to find out a plausible circuit equivalents of it. What we do realize is that for a proper quantum mechanical description and it's circuit implementation of the same we need to incorporate the non commutativity inside the circuit model. It has been realized here that the metric is a dynamical entity governing space time and for considering equivalent circuits it plays a very distinct role. We have used the methods of stochastic quantization and have constructed a specific case here and see that HH model inductances gets renormalized in the quantum limit.

arXiv:q-bio/0606008•Jun 8, 2006•3 citations

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

inquantio

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

•Jul 21, 2026•0 citations

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 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

Quantum mechanics and its interpretation

Peter Holland

The nature of the problem The quantum world is inexplicable in classical terms. The predictions pertaining to the interaction of matter and light embodied in Newton's laws for the motion of particles and Maxwell's equations governing the propagation of electromagnetic fields are in flat contradiction with the experimental facts at the microscopic scale. A key feature of quantum effects is their apparent indeterminism, that individual atomic events are unpredictable, uncontrollable and literally seem to have no cause. Regularities emerge only when one considers a large ensemble of such events. This indeed is generally considered to constitute the heart of the conceptual problem posed by quantum phenomena, necessitating a fundamental revision of the deterministic classical world view. Some of the principal phenomena, among those discussed in this book, are as follows: ( a ) Self-interference: a beam of electrons sent one at a time through a barrier containing two apertures builds up through a series of localized detection events on a screen an interference pattern characteristic of waves (cf. the frontispiece and §5.1). ( b ) Tunnelling: an α-particle trapped in a nucleus can pass through a potential barrier in a manner forbidden to a classical particle (§5.3). ( c ) The stability of matter: atoms and molecules are found to exist only in certain discrete, or ‘stationary’, energy states. For this reason they do not ‘collapse’, the result predicted by classical electrodynamics. During transitions between stationary states (quantum jumps) an atom exchanges a discrete quantity of energy with the electromagnetic field (§§4.5, 7.6). […]

Cambridge University Press eBooks•May 13, 1993•3 citations
Ion channels are stable over a wide range of time scales in the order of millisecond to microsecond or even smaller time range. This time scale is based on measurements using available experimental techniques. The same time scale is indeed followed by channel-carried charges while getting transported across the host membrane. This concept of gross time-dependent motion is valid when one consider ion channels to be classical mechanical systems following related formalism regarding their construction, transport, and other localized static and dynamic phenomena. Three decades ago, Conti and Stuhmer recorded the asymmetric displacement currents associated with the gating of nerve sodium channels in cell-attached macropatches of Xenopus laevis oocytes injected with exogenous mRNA coding for rat-brain-II sodium channels. Theoretically, tunneling is possible whenever quantum states are separated by a potential energy barrier, where the potential energy is a function of some state variable(s) of the system.
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.
With an increasing amount of experimental evidence pouring in from neurobiological investigations, it is quite appropriate to study viable reductionist models which may explain some of the features of brain activities. It is now quite well known that the Hodgkin-Huxley (HH) Model has been quite successful in explaining the neural phenomena. The idea of circuit equivalents and the membrane voltages corresponding to neurons have been remarkable which is essentially a classical result. In view of some recent results which show that quantum mechanics may be important at suitable length scales inside the brain, the question which becomes quite important is to find out a proper quantum analogue of the HH scheme which will reduce to the well known HH model in a suitable limit. From the ideas of neuro-manifold and the relevance of quantum mechanics at some length scales in the ion channels, we investigate this situation in this paper by taking into consideration the Schrödinger equation in an arbitrary manifold with a metric, which is in some sense a special case of the heat kernel equation. The next important approach we have taken in order to bring about it's relevance in brain studies and to make connection with HH models is to find out a plausible circuit equivalents of it. What we do realize is that for a proper quantum mechanical description and it's circuit implementation of the same we need to incorporate the non commutativity inside the circuit model. It has been realized here that the metric is a dynamical entity governing space time and for considering equivalent circuits it plays a very distinct role. We have used the methods of stochastic quantization and have constructed a specific case here and see that HH model inductances gets renormalized in the quantum limit.
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.
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.
The nature of the problem The quantum world is inexplicable in classical terms. The predictions pertaining to the interaction of matter and light embodied in Newton's laws for the motion of particles and Maxwell's equations governing the propagation of electromagnetic fields are in flat contradiction with the experimental facts at the microscopic scale. A key feature of quantum effects is their apparent indeterminism, that individual atomic events are unpredictable, uncontrollable and literally seem to have no cause. Regularities emerge only when one considers a large ensemble of such events. This indeed is generally considered to constitute the heart of the conceptual problem posed by quantum phenomena, necessitating a fundamental revision of the deterministic classical world view. Some of the principal phenomena, among those discussed in this book, are as follows: ( a ) Self-interference: a beam of electrons sent one at a time through a barrier containing two apertures builds up through a series of localized detection events on a screen an interference pattern characteristic of waves (cf. the frontispiece and §5.1). ( b ) Tunnelling: an α-particle trapped in a nucleus can pass through a potential barrier in a manner forbidden to a classical particle (§5.3). ( c ) The stability of matter: atoms and molecules are found to exist only in certain discrete, or ‘stationary’, energy states. For this reason they do not ‘collapse’, the result predicted by classical electrodynamics. During transitions between stationary states (quantum jumps) an atom exchanges a discrete quantity of energy with the electromagnetic field (§§4.5, 7.6). […]