Abstract
The recent wave of interest to modeling the process of decision making with the aid of the quantum formalism gives rise to the following question: ‘How can neurons generate quantumlike statistical data?’ (There is a plenty of such data in cognitive psychology and social science). Our model is based on quantumlike representation of uncertainty in generation of action potentials. This uncertainty is a consequence of complexity of electrochemical processes in the brain; in particular, uncertainty of triggering an action potential by the membrane potential. Quantum information state spaces can be considered as extensions of classical information spaces corresponding to neural codes; e.g., 0/1, quiescent/firing neural code. The key point is that processing of information by the brain involves superpositions of such states. Another key point is that a neuronal group performing some psychological function F is an open quantum system. It interacts with the surrounding electrochemical environment. The process of decision making is described as decoherence in the basis of eigenstates of F. A decision state is a steady state. This is a linear representation of complex nonlinear dynamics of electrochemical states. Linearity guarantees exponentially fast convergence to the decision state.
Introduction
The recent revolution in quantum information has a strong foundational impact, in particular, development of the quantum information interpretation (Zeilinger and Brukner^{1}, Plotnitsky^{2}, D’ Ariano^{3}, Fuchs and Schack^{4}). According to this interpretation, the quantum formalism is about information and probability which can be gained through observations (cf. Bohr^{5}). In principle, the quantum formalism endowed with the information interpretation can be applied to other areas of research^{6}, e.g., modeling the process of decision making by humans and, more generally, human cognition. We remark that the same conclusion can be derived on the basis of consistent consideration of the principles of quantum logic: violation of the laws of Boolean logic needs not be rigidly coupled to observation on quantum physical systems (see especially Svozil^{7} and Ozawa^{8,9}).
We now turn to theory of decision making and recall that Tversky and Kahenman^{10} and other researchers in psychology and economics (starting with the seminal paradoxes of Allais^{11} and Ellsberg^{12}) demonstrated cases where classical probability (CP) prescription and actual human thinking persistently diverge, at least relative to baseline classical intuitions. There is a plenty of probabilistic data that do not match the laws of CP. These data was typically related to probability fallacies and irrational behavior.
Do people follow the CPrules? Are there any other laws that can be applied to formalize human judgments?
After demonstrating first evidence on deviation from the postulates of CPbased decision models, Tversky, Kahenman started to advertise the heuristic approach as an alternative to probabilistic modeling of decision making.
However, as was shown during the last ten years, some of the main problems of the CPbased decision making, expected utility theory and its later modifications such as subjective expected utility and prospect theories, can be resolved on the basis of quantum probability (QP) calculus. The QPapproach to modeling of decision making is a purely operational approach describing probability distributions of observations’ outputs. The description is formal and it is based on the calculus of Hermitian operators in complex Hilbert space.
Researchers use the quantum formalism to describe aforementioned nonclassical data, to resolve paradoxes and to model various psychological effects such as conjunction, disjunction, and order effects, see, e.g., monographs^{6,13,14,15} and some representative papers^{16,17,18,19,20,21}. The main tool is the machinery of quantum interference for incompatible observables^{6,14}; see also^{22,23} for tests of contextuality in decision making based on the Belltype^{24,25} inequalities. In many cases, models based on quantum theory can be seen as providing a formalization of relevant heuristic principles (e.g., the quantum model for the conjunction fallacy^{18}, can be thought of as a formalization of Tversky and Kahneman’s representativeness heuristic^{26}).
As is often the case with cognitive models^{27}, in this approach the brain is considered as a black box that processes information in accordance with the laws of quantum information theory and generates QPdata. To distinguish this operational approach from the approaches based on quantum physical processes in the brain (e.g.^{28,29}), we call it the ‘quantumlike’. The quantumlike community is multidisciplinary: around two hundred experts in cognitive, social, and political sciences, psychology, quantum physics, economics, finances, genetics, and molecular biology. For the expression ‘quantumlike’, Google scholar gives 5260 links. However, the absence of connection with neurophysiological processes makes the grounds of the quantumlike modeling rather shaky. There is a deep gap between neurophysiology and the quantumlike approach or cognitive informatics in general. The aim of this paper is to make this gap less deep, cf.^{30,31}.
From the philosophical viewpoint, we handle the problem of reduction of mental processes to electrochemical processes at the neuron level. This reduction is not straightforward and it is based on the methodology of the onticepistemic approach, see Atmanspacher^{32}, see also^{33}.
Results
Modeling information processing by neurons with theory of open quantum systems
The main idea behind our model connecting functioning of neuronal structures to quantumlike statistics of decision making by humans is that neuron’s state space must have the Hilbert space structure, i.e., a single neuron has to ‘work’ with probabilistic superpositions of states caring cognitive information. At the same time a neuron is treated as an open system, which state of superposition is affected by information flows from the electrochemical environment composed of signals (electrical currents, electromagnetic field, neurotransmitters) generated by other neurons.
Authors developing the genuine quantum physical models of the brain functioning pointed to impossibility of considering neurons in a state of superposition^{28,29}. As a consequence, neurons were not considered as the basic units of information processing. This viewpoint on neurons’ role in information processing diminished the interest of neurophysiologists to such models. In our model, we present a natural electrochemical basis for superposition states of a neuron or a group of neurons (in the latter case, states are generally nonseparable  entangled).
The classical information approach to modeling of the brain functioning uses discrete states of a neuron corresponding to various neural codes^{34}; e.g., 0/1, quiescent/firing neural code. We stress the role of states of uncertainty, e.g., neither quiescent nor firing, in information processing. Such states can be represented as superpositions. Our aim is to lift processing of such states to the quantumlike statistics of outputs of a psychological function F.
Here we make a short remark about terminology. The standard neural code is based on nonfiring/firing states. We make the nonfiring state more detailed. The quiescent state is still encoded by 0 and understood as the state of inactivity, i.e., the refractory state. However, besides of firing and quiescent states, a neuron can be in a state of uncertainty characterized by the range of values of the membrane potential, \(V\in [\,\,70,\,55]\) (see Fig. 1 for illustration). In this state a neuron can generate an action potential with some probability. Uncertainty in generation of action potentials is a consequence of stochastic operation of ion channels. We also point to random failure of generation, conduction, and acceptance of action potentials (by other neurons)^{35,36}.
Another distinguishing feature of our model is that a neuronal group, say G, performing some psychological function F is an open quantum information system. It interacts with the surrounding electrochemical environment E, which also can be modeled with the operational quantum information approach. Interaction of a neuronal group G performing the Ftask with E is modeled at the information level by using the quantum master equation.
The process of decision making is described as decoherence of the quantum(like) information state of G in the basis of eigenstates of F. A decision state \(\bar{\rho }\) is a steady state of the dynamics ρ(t) of the Gstate; \(\bar{\rho }\) is diagonal in the Fbasis. The existence of steady states is a consequence of interaction with E. In short, by our model a group of neurons G is ‘working’ on a function F, but then convergence for G is driven by the broader electrochemical environment treated as an information reservoir.
The steady state \(\bar{\rho }\) represents the weights of possible outputs of F. In our model a concrete Foutput is selected by a classical random generator with probabilities encoded in the decision state. This is the simplest way to reproduce statistics given by the Born rule. However, there is a plenty of other possibilities to model completion of the process of decision making. We recall that a decision state can be treated as a classical state (for F) and a variety of rules of the CPdecision theory can be explored.
In our model even a single neuron can be in a state of superposition representing uncertainty generated by the membrane potential V. The main source of this uncertainty is interactions with surrounding neural network (cf.^{30}), which may be of huge complexity. Roughly speaking, an isolated neuron is a classical system, cf.^{28,29,38} (but, of course, an isolated biosystem is dead, cf. Schrödinger^{37}). Thus the basis of the quantumlike representation for a single neuron is its openness as an electrochemical system.
The crucial feature of the quantumlike representation of information is its linearity. The complex nonlinear dynamics of electrical and chemical flows is lifted to the linear dynamics described, e.g., by GoriniKossakowskiSudarshanLindblad equation^{39}. Here convergence to a steady state is exponentially rapid: state fluctuations are damped by the factors of the form e^{−λt}, where λ = a + ib, a > 0. This makes it possible to approach the decision state very quickly. In some sense, the brain transforms the disadvantage of complex fluctuations in information processing (in the form of electrochemical uncertainty) into advantage given by the linear representation. We emphasize that the latter is probabilistic.
We point to another important implication of the use of the quantumlike representation. By coupling some psychological functions to different orthonormal bases the brain is able to realize these functions in the state space of the same group of neurons. Generally, two functions are incompatible (complementary): it is impossible to approach the decision state that is diagonal with respect to both bases. The statistical patterns of such incompatibility in neuronal performance can be found at the behavioral level^{6,14,15,16,17,18,20,21,22,40}.
Quantumlike superposition from generation of action potentials
We propose to describe uncertainty in generation of an action potential by a neuron, say N, by using states’ superposition. Consider two dimensional complex Hilbert space \( {\mathcal H} \) (qubit space). At a concrete instant of time neuron’s state can be mathematically described by a superposition of two states, quiescent and firing, labeled by 0〉,1〉:
It is assumed that these states are orthogonal and normalized, i.e., 〈01〉 = 0 and 〈αα〉 = 1, α = 0, 1. Here the coordinates c_{0} and c_{1} with respect to the quiescentfiring basis are complex amplitudes representing potentialities for a neuron to be quiescent or firing. Probabilistically these potentialities are expressed by the Born rule of quantum theory:
These probabilities can be interpreted statistically. Let ψ be a steady state (with respect to the dynamics performing a psychological function). Consider a single neuron N and a sufficiently long time interval T = MΔ, \(M\gg 1\), and find the frequency ν_{1} = n_{1}/M, where n_{1} is the number of Δintervals such that N produces a spike. Then p_{1} ≈ ν_{1}. We repeat that steady states play the exceptional role in our model as decision states.
This is a good place to mention that the frequentist interpretation of QM was used by von Neumann in book^{41} where he referred to von Mises’ frequency approach to probability, probability as the limit of frequencies in a long series of trials, in a collective^{42}. The frequencist interpretation of QM was actively used by one of coauthors^{43}, in particular, for demystification of quantum probability. Recently this interpretation was explored in article^{44} in connection with the known law of combining density matrices for subensembles.
This is the ‘observational definition’ of probability. An observer can count spikes. But who is the observer? In our model the brain (more concretely, each psychological function) is a system that is able to perform selfobservations, detection of information states of neurons and neuronal groups (but not electrochemical states).
General quantumlike representation of neurons’ states
Neuron’s state space is a complex Hilbert space \( {\mathcal H} \) of dimension m. In this space we consider the fixed orthonormal basis \(\alpha \rangle ,\alpha =0,\ldots ,m1\), consisting of states which can be identified by selfobservations of some psychological function F. Thus each state of a neuron can be represented by superposition
where complex probability amplitudes c_{α} represent potentiality of observation of this neuron in the state α〉.
Now consider a group G of neurons. The state space of this group is the tensor product \({ {\mathcal H} }_{G}\) of single neuron’s state spaces. Since neurons in G interact with each other and with the surrounding electrochemical environment, generally the Gstate is entangled. (The meaning of entanglement here is simply a statement that we cannot decompose the state for two neurons into a product state from each neuron individually).
Consider two neurons and firing/quiescent coding. Generally the state of the compound system G has the form
where the complex probability amplitudes \({c}_{00},\ldots ,{c}_{11}\) represent the potentiality of the compound system G to occupy one of the states \(00\rangle ,\ldots ,11\rangle \). This potentiality is interpreted probabilistically, e.g., p_{11} = c_{11}^{2} is the probability of both neurons firing. Superposition (4) represents correlated behavior of two neurons in G. Consider, for example, the state of the form:
(this is one of the Bell states, see (6). A couple of neurons in these state fire and relax simultaneously (up to the time window Δ).
Example of incompatible representations: distinguishable versus indistinguishable neurons
In the same Hilbert state space, there can be selected a variety of orthonormal bases which can be used by various psychological functions. Hence, the same neuronal group can perform a variety of generally incompatible psychological functions. We illustrate this possibility with a simple example.
Consider two neurons, \(G=\{{{\mathscr{N}}}_{1},{{\mathscr{N}}}_{2}\}\) in the state (5). In this state the neurons in G are indistinguishable. We stress that this is information indistinguishability. Physically, \({{\mathscr{N}}}_{1}\) and \({{\mathscr{N}}}_{2}\) are distingushable: they are located in different places, they have different geometry of connections and so on. Thereby such quantum states match perfectly the ensemble neural coding with indistinguishable neurons. To model quantumlike information processing by indistinguishable neurons, we represent the state space \({ {\mathcal H} }_{G}\) as the direct sum of the symmetric and antisymmetric tensor product spaces: \({ {\mathcal H} }_{G}={ {\mathcal H} }_{G}^{s}\oplus { {\mathcal H} }_{G}^{as}\). Permutation in any pair of neurons does not change vectors belonging to \({ {\mathcal H} }_{G}^{s},\) but it changes the sign for vectors beloning to \({ {\mathcal H} }_{G}^{as}\mathrm{.}\) We illustrate this decomposition in the fourdimensional case \({ {\mathcal H} }_{G}= {\mathcal H} \otimes {\mathcal H} \). Consider the orthonormal basis known in quantum information theory as the Bell basis:
It is clear that the states ψ_{1}, ψ_{2}, ψ_{3} are invariant with respect to permutations of the neurons. This is the basis in \({ {\mathcal H} }_{G}^{s}\mathrm{.}\) Thus any state of the ensemble of two (informationally) indistinguishable neurons can be represented as superposition of these states. We remark that ψ_{4} is the only antisymmetric state, so here \({ {\mathcal H} }_{G}^{as}\) is onedimensional.
It is convenient to work in the Fock representation. For 0/1 coding (quiescent/firing), this is a representation based on counting the number of firing neurons. The basis of the Fock space consists of the states \(n\rangle \), n = 0, 1, 2. (big brackets are used to distinguish Fock states from neurons’ states αβ〉, α, β = 0, 1). Here
So, working in the Fock representation we are concerned only with the number of firing neurons. Each state \(\psi \in { {\mathcal H} }_{G}^{s}\) can be represented in the form of superposition:
where \({\sum }_{n}\,{d}_{n}{}^{2}=1.\) Thus if the configuration of two indistinguishable neurons is prepared in the state ψ sufficiently many times, then relative frequency of finding n = 0, 1, 2, firing neurons approximately equals to P_{n} = d_{n}^{2}, (This is again the (self)observation interpretation of probability.)
Quantumlike representation of psychological functions
Consider the space of quantumlike states of the group of neurones G involved in realization of some psychological function F. We proceed with modelling both possibilities: distinguishable and indistinguishable neurons.
Mathematically a psychological F is coupled to some fixed orthonormal basis {α〉} in the space of quantumlike states. This basis may be considered as a quantum information representation of the concrete neural code. Suppose that F has values \({f}_{1},\ldots ,{f}_{s}\) (e.g., just two values ± 1). It is assumed that each value f_{j} is coupled to the corresponding set of basis vectors (neuronal states) \({A}_{f},f={f}_{1},\ldots ,{f}_{s}\). Thus F is mathematically represented by decomposition of the basis in disjoint blocks A_{f}. Formally F can be written as the Hermitian operator of the form:
We remark that the expression
has the mathematical meaning of orthogonal projector on the subspace L_{f} generated by basis vectors from the block A_{f}. Therefore formally the psychological function can be written in the form: \(F={\sum }_{f}\,{f}_{j}{\pi }_{f}.\) However, in our model the process of information processing by neurons is based on the concrete states of the neuronal group G performing F. Thus the concrete decomposition of π_{f}, see (11), plays an important role in modeling of the functioning of F. We remark that in quantum theory selection of the concrete basis can be interpreted as selection of the context of measurement. Thus a psychological function is represented not simply by a Hermitian operator, but by an orthonormal basis (or more precisely, by its decomposition into disjoint blocks corresponding to the values of F).
In the simplest case F is represented by the Hermitian operator with nondegenerate spectrum, i.e., there is onetoone correspondence between the Fvalues and basis vectors, \(f\to {\alpha }_{f}\rangle .\) In this case, \(F={\sum }_{f}\,f{\alpha }_{f}\rangle \langle {\alpha }_{f}.\) However, generally the Foperator is degenerate. Take say 100 neurons and 0/1 neural code. Then the corresponding space of quantumlike states has the dimension D = 2^{100}.
Discussion
We presented a quantumlike model of processing of information by a group of neurons interacting with the surrounding electrochemical environment. The crucial element of the model is encoding uncertainty in generation of action potentials by superpositions of discrete states representing clusters of electrochemical states (classical or genuine quantum). Such superposition representation of uncertainty can be lifted to generation of QPfeatures of outputs of a psychological function F that are reflected in statistical data collected in cognitive psychology, game theory, social and political sciences, e.g.^{6,13,14,15,16,17,18,19,20,21}. A psychological function is coupled to the fixed basis in the neuronal state space and in principle the latter can be coupled to some classical neural code. From this viewpoint, the complex problem of the neural code is resolved by recognizing that the brain can work with a variety of ‘quantumlike neural codes’ corresponding to orthonormal bases in the state spaces of groups of neurons working on psychological functions.
The basic feature of the presented model is that even the state of a single neuron can be described as a quantumlike state. In the real situation of neuronal network, such network interacts with the neuron by neurotransmitters, which modify the membrane potential of the neuron’s cell body. In other words, the neuron’s potential is influenced by the inputs from other neurons. The modified potential changes the probability of firing of this neuron. This effect can be called ‘uncertainty’. Then we can treat one neuron as a quantumlike machine. The further analysis of information processing of a neuron or neuronal network becomes simple (and, in particular, linear).
In future we plan to generalize the present quantumlike model of brain’s functioning by taking into account the structure of the electrochemical environment, especially the role of neurotransmitters in creation of the superposition representation of information states processed by neurons. At the same time our model can be treated more abstractly, namely, as a quantumlike model of artificial intelligence, cf. Briegel^{45}.
Methods
Density operators as signatures of environments
The theory of open quantum systems requires us to consider not only pure states of G, but also states given by density operators. (A density operator ρ is a Hermitian positively semidefinite operator with unit trace.) Each pure state (given by a normalized vector ψ of the state space, i.e., 〈ψψ〉 = 1) can be represented by the density operator, the orthogonal projector on ψ. Typically the ρstate is interpreted as a mixed state, i.e., a state representing a statistical mixture of pure states. This interpretation is quite ambiguous, because the same density operator can be represented as a mixture of different ensembles of states. We use the interpretation related to the Naimark’s dilation theorem by which each density operator ρ (describing the state of some system S) can be obtained as a partial trace of a pure state of a larger system, composed of S and its environment. The trace is taken with respect to the degrees of freedom of the environment. Then, following D’Ariano^{3} we interpret a pure state as an informationally complete state. Generally, a state given by a density operator is informationally incomplete, since it contains the impact of some environment and a variety of environments may generate the same ρstate.
Information dynamics of open neuronal systems
In quantum information theory the dynamics of the state of an open system is typically described by the GoriniKossakowskiSudarshanLindblad (GKSL) equation^{39}. It can be written in the form
where H is a Hermitian operator (Hamiltonian) acting in the state space of a system (in our case a group of neurons G ‘working’ for a psychological function F) and L is a linear operator acting in the space of linear operators (such maps are often called superoperators). In quantum physics, typically the operator H represents the state dynamics in the absence of outer environment. (It is assumed that H is positively defined.) Generally, Hamiltonian H can also contain effects of the environment. The superoperator L has to map density operators into density operators, i.e., it has to preserve ‘Hermitianity’, positive definiteness, and the trace. For the present paper, its concrete form is not important, see, e.g., work^{39}. The real parameter γ > 0 is the coupling constant; it represents strength of (information) interaction with environment \( {\mathcal E} \). Generally both H and L depend on the initial state of the environment and its interaction with neurons (described in the information framework).
In quantum physics the dynamics of an isolated system is described by the Schrödinger equation. For a biological system, it seems to be meaningless to use the notion of an isolated system, even in the approximate setting. Therefore the operator H in equation (12) has to be treated on the equal grounds with the superoperator L, i.e., as representing (information) interaction with the environment.
The GKSLequation is a linear ordinary differential equation with constant coefficients. For such an equation, one can quite easily understand whether its solutions ‘stabilize’ to a steady state (by writing it in the vector form and finding the corresponding eigenvalues). Stabilization of ρ(t) is understood as damping of fluctuations around the final (stable) state. In the mathematical model this is the limiting process \(\bar{\rho }={\mathrm{lim}}_{t\to \infty }\,\rho (t).\) However, in reality fluctuations may become negligibly small quite fast. Suppose that function F operates with fluctuations’ threshold ε > 0. Then the exponentially decreasing factors in a solution very quickly approach ε.
Probabilistic functioning of psychological functions
Consider some psychological function F and its representation (10) with the basis {α〉}. Let \(\bar{\rho }\) be a steady state for the neuronal information dynamics (modeled mathematically with, e.g., equation (12)) and let it be diagonal in the αbasis. Thus \(\bar{\rho }\) can be considered a classical state (for the psychological function F), cf. Zurek^{46}. Now we can present the frequentist interpretation of the probabilities encoded in diagonal representation of \(\bar{\rho }\) (its Schatten decomposition),
where p_{α} ≥ 0, and \({\sum }_{\alpha }\,{p}_{\alpha }=1.\)
The state \(\bar{\rho }\) represents statistics of realization of the basis states {α〉} in the time series of selfobservations on the neuronal group G involved in realization of the psychological function F.
Thereby, we reserve the statistical mixture interpretation only for the Schatten decomposition, see^{47} for the motivation based on entropic considerations.
The psychological function F is modeled as an observer for the neuronal group G. Since, for this psychological function, the steady state \(\bar{\rho }\) is classical, observations performed by F can be modeled as classical monitoring of the state of G.
Consider again some time window Δ. This is the ‘interval of state determination’: by monitoring G during the time window Δ the psychological function F reports (to itself) that the Gstate is α〉. Consider now some period of time \(T=M{\rm{\Delta }},\,M\gg 1.\) The F monitors the Gstates during this period. Suppose that the αstate was observed n_{α} times. Define the relative frequency: \({\nu }_{\alpha }=\frac{{n}_{\alpha }}{{\sum }_{\beta }\,{n}_{\beta }}.\) Then by the frequentist interpretation p_{α} ≈ ν_{α}. We remark that this probabilistic representation is used in statistical signal processing in neuroscience.
Thus F approaches the steady state with the Schatten decomposition corresponding to the basis Feigenstates. Then F determines the frequency probability distribution p = {p_{α}} encoded in this steady state. This probability distribution is easily transformed into the probability distribution of the possible outcomes of F: \({p}_{F}(f)={\sum }_{\alpha \in {A}_{f}}\,{p}_{\alpha },\) see decomposition (10) of F. Formally
where π_{f} is the projector corresponding to the value f. But the latter is only a formal mathematical representation. The Fneural code is represented by the basis {α〉} and F monitors appearance of these basis states.
Finally, F should select one concrete outcome f. Since the probability distribution p_{F} is classical, we are now in the framework of classical theory of decision making. In principle any decision rule of this theory can be used. The quantum statistics, given by Born rule (14), is preserved if finalization of Ffunctioning is based on the use of classical random generator with the probability distribution p_{F}. Such random generator can be easily realized through some electrochemical process in the brain.
One can relate this final step with the free will. Even if, for some value f, probability \({p}_{F}(f)\ll 1,\) there is still a chance that F may select this alternative. (On the other hand, if F were working, e.g., with odds, it would never select this output.)
Quantum information versus physical states of neurons
After presenting our quantumlike model of decision making by brain’s modules called psychological functions, we come back to the deep foundational question of the interrelation between quantum informational and physical states. Most quantum information theorists mentioned by the article take the viewpoint that “quantum states” are not the physical states of the quantum objects, but are part of the mathematical machinery (based on Born’s rule) for predicting the probabilities or statistics (when the experiment is repeated many times) of the outcomes of possible quantum measurements, in which, once the measurement is performed, a given outcome is observed. The physical state of say a photon is not so different from a classical state. (There are additional complexities, but they are not important for the moment.) We can say that quantum states are epiphenomenal to the physical reality of the relevant objects. Physical processes of interaction of microsystems with measurement devices or (by expressing the viewpoint of theory of open quantum systems) with surrounding environment organize themselves exactly so that the quantum theory provides the adequate description in some nonphysical information space.
In some information interpretations, especially QBism, the role of observer is highlighted. QBism’s emphasis of this role matches well with the QP approach to decision making^{48}: humans are considered as observers performing selfmeasurements by answering questions and solving problems. Humans assign subjective probabilities to possible outcomes of selfmeasurements. However, by closing the gap between electrochemical processes in the brain and the QPstructure of humans’ decision making, we do not imply the presence of a subjective entity, such as Ghost in the machine^{49}. And here it is important to note that not all quantum information interpretations are so strongly based on the subjective component, that is, corresponding to a picture of an agent simulating quantum probabilities. In the quantum information approach probabilities can be interpreted objectively; in particular, by using the decoherence viewpoint on generation of steady states and their interpretation as presenting classical frequency probabilities.
In our quantumlike model a psychological function F expresses the subjective side of brain’s functioning  it generates probabilities p_{f}. They can be treated in the same way as those subjective probabilities which are considered in subjective expected utility theory or prospect theory. However, the form of the functioning of F is based on the electrochemical processes in the brain. And in the previous sections we described the mechanism of transition from electrochemical states to the quantuminformation states. Each such state represents a cluster of electrochemical states of a neuron and surrounding electrochemical environment E. To describe this transition mathematically is difficult if possible at all. Electrochemical processes in the brain organize themselves to guarantee stable dynamical processing in some nonphysical quantum information space, so to say the mental space. This dynamics matches the abstract mathematical QP model, which has received plenty of confirmation from experimental data collected in cognitive psychology and decision making, see introduction. We use the decoherence model of generation of steady states representing subjective probabilities. The absence of the explicit mathematical description of the mapping of clusters of electrochemical states into quantumlike superpositions does not diminish the significance of outlining (using function F) a physical basis for how quantumlike mental representations and corresponding uncertainty relations can emerge, from the action potentials by neurons (cf. Marr^{50}).
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Acknowledgements
I.B. was supported by a Marie SklodowskaCurie Individual Fellowship, Grant Agreement 696331, E.M.P. was supported by Leverhulme Trust grant RPG2015311, and A.K. was partially supported by the EUproject “Quantum Information Access and Retrieval Theory” (QUARTZ), Grant No. 721321.
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All authors carried out the research and contributed to design and development of the model. All authors reviewed the manuscript. A.K. and I.B. wrote the manuscript; E.M.P. contributed as an expert in cognitive psychology and decision making and quantum probabilistic modeling; I.Y. contributed as an expert in molecular biology and quantumlike modeling of biological processes. The idea to encode uncertainty in generation of action potential by using the quantum information representation was proposed by A.K. who also prepared paper’s revision based on reviewers’ comments.
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Khrennikov, A., Basieva, I., Pothos, E.M. et al. Quantum probability in decision making from quantum information representation of neuronal states. Sci Rep 8, 16225 (2018). https://doi.org/10.1038/s41598018345313
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DOI: https://doi.org/10.1038/s41598018345313
Keywords
 Neuron State
 Quantumlike Representation
 Neuronal Groups
 Open Quantum Systems
 Electrochemical Environment
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