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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>of the Neuromorphic Network Operation Taking into Account Stochastic Effects</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Alexander Yu. Morozov</string-name>
          <email>morozov@infway.ru</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Karine K. Abgaryan</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Dmitry L. Reviznikov</string-name>
          <email>reviznikov@mai.ru</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>125993</institution>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Moscow Aviation Institute (National Research University) (MAI)</institution>
          ,
          <addr-line>Volokolamskoe Highway, 4, Moscow</addr-line>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>RAS)</institution>
          ,
          <addr-line>st.Vavilova, 44, bld. 2, Moscow, 119333</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <fpage>84</fpage>
      <lpage>91</lpage>
      <abstract>
        <p>This paper simulates an analogue self-learning pulse neural network based on memristive elements, taking into account their stochastic properties. A variable-resistor model of a thinfilm memristor based on an exponential model for dopant drift is used as a memristor model. Stochastic properties are accounted for by a term in the memristor equation of state, which presents an additive (Gaussian) noise. Memristor switch from low-resistance to highresistance state in this case occurs differently from cycle to cycle, corresponding to the experimental data. The mathematical model previously developed by the authors is used; it describes the analogue implementation of a pulse self-learning neural network memristive elements as synaptic weights and a learning mechanism based on the STDP method. The operation of a network consisting of five neurons with 320 synapses for recognition of various black and white images is simulated. As a result of the simulation, the network was successfully learnt to recognize the given patterns VI International Conference Information Technologies and High-Performance Computing (ITHPC-2021),</p>
      </abstract>
      <kwd-group>
        <kwd>recognition</kwd>
        <kwd>titanium oxide</kwd>
        <kwd>TiO2</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        Artificial neural networks play a great role in modern life [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. With their development, it became
possible to study actual and practically significant tasks that often cannot be solved by classical
approaches. The recognition task belongs to such tasks. The scope of recognition applications is very
extensive: text recognition
(including
handwriting),
machine
vision, speech
or fingerprints
recognition, etc. Neural networks are actively used in such areas as: economics, medicine and
healthcare, avionics, the Internet, robotics, security, etc.
      </p>
      <p>
        One of the factors restraining the neural network development is the high computational
complexity of the corresponding neural network algorithms: a network training time can be measured
in weeks and months. Currently, to speed up their work, research is being conducted on creating
special processors [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ] based on the principles of the human brain activity. These processors are often
a hardware implementation of pulse neural networks.
      </p>
      <p>In conjunction</p>
      <p>
        with the development of specialized computing devices, the use of other
computational principles seems promising, namely analogue computations instead of digital ones,
since they are performed in orders of magnitude faster. Relatively new electrical elements
memristors [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ]-[
        <xref ref-type="bibr" rid="ref5">5</xref>
        ] - are actively used in the field of analogue computing. A memristor is a resistor,
which conductivity depends on the total electric charge flowing through it. In the absence of current,
      </p>
      <p>
        2021 Copyright for this paper by its authors.
it keeps its conductivity, which allows it to be used as an elementary memory cell, and it is possible to
dynamically change its resistance in the presence of current. This is a certain similarity of the
memristors’ properties with the properties of biological synapses, allowing them to be used to create
analogue neural networks [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ].
      </p>
      <p>
        Basically, the memristive effect occurs in various oxides due to the movement of ions (oxygen
vacancies) and the formation/destruction of conducting filaments. The ion movement is random and,
as a consequence, memristors have certain stochastic properties. A detailed experimental and
theoretical study of this effect was carried out in [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ]-[
        <xref ref-type="bibr" rid="ref9">9</xref>
        ].
      </p>
      <p>
        Mathematical models of memristors are traditionally formulated as dynamic systems with respect
to the parameter of memristor state, which characterizes the level of element’s conductivity [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ]-[
        <xref ref-type="bibr" rid="ref12">12</xref>
        ].
To account for random effects, a stochastic differential equation with additive noise for the state
variable can be used instead of the deterministic one [
        <xref ref-type="bibr" rid="ref13">13</xref>
        ].
      </p>
      <p>
        In this work we simulate a two-layer full-connected network with one layer of memristor elements
(synapses) [
        <xref ref-type="bibr" rid="ref14">14</xref>
        ]; the network consists of five neurons with 320 synapses. This number of neurons is
due to the number of images recognized (5 pieces); the number of synapses is determined by the total
number of pixels: 5x8x8 = 320. There is used the network architecture, in which each memristor
corresponds to a transistor (1T1R crossbar architecture). Due to this architecture, it is possible to train
the network at the hardware level using the STDP (Spike Timing Dependent Plasticity) method
[15][18]. According to this method, the change of neuron synaptic weights depends on the time difference
between input and output pulses.
      </p>
      <p>The main purpose of this scientific work is to simulate the functioning of the self-learning pulse
neural network with the hardware implementation based on memristive elements, taking into account
their stochastic properties in learning the recognition of five images.</p>
      <p>In the second section, a model of a variable-resistor thin-film memristor, based on an exponential
model of dopant drift, is presented. The third section provides a mathematical model of the neural
network. Next, the neural network operation is simulated and, finally, the main results of the work are
formulated.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Mathematical model of a memristor</title>
      <p>
        An approach based on representation of a memristor as a dynamic system with a generalized state
variable is widely used for simulating the memristor’s operation [
        <xref ref-type="bibr" rid="ref10 ref11 ref12">10-12</xref>
        ]. Variation of the state
variable determines the dynamics of the element's switching between different modes. Stochastic
effects can be accounted for by introducing a stochastic additive term into the dynamic system in the
form of additive white (Gaussian) noise [
        <xref ref-type="bibr" rid="ref13">13</xref>
        ]. The equation specifying the change in the state variable
of the memristor can be written in the following generalized form:
dx = F ( x)dt + dW ,
      </p>
      <p>Where F - rate of change of the state variable;  - coefficient characterizing noise intensity; W
Wiener process.</p>
      <p>Concretization of the functional dependence F ( x) and relation of the state variable with physical
parameters gives a memristor model. In the present paper, a variable-resistor thin-film memristor
model based on the exponential model for a doping impurity drift is used [19]:
 V 
 v Dp2 exp  RVopn I  dt , V  V p ,

dx =  dW +  v DVn2 exp  RVonn I  dt , V  Vn ,

 v RDo2n Idt , Vn  V  V p ,

R = Ron x + Roff (1 − x),</p>
      <p>V
R
I =
where
x  0, 1 — state variable;
Ron, Roff — minimum and maximum memristor resistance;
I , V , R — actual memristor’s current, voltage, and resistance values;
Vp , Vn — values of voltages at which state switching occurs;
 v —doping mobility coefficient;
D —semiconductor film thickness;
 — coefficient characterizing the noise intensity;
W — Wiener process.</p>
      <p>To obtain an approximate realization of the stochastic process x (t ) we use the Runge-Kutt method
of order 1.5. We determine an approximate solution using the grid t0  t1  t2  ...  tN −1  tN under the
initial condition x(t0 ) = x0
2</p>
      <p>1
xk +1 = xk + 4 3F ( x1k ) + F ( xk2 ) tk +1 +  Wk +1,
where tk +1 = tk +1 − tk, Wk +1 = W (tk +1 ) − W (tk ). Let N (0,1) is a normally distributed random variable
with zero mathematical expectation and unit variance. Then the random value Wk +1 is calculated as
Wk +1 = zk +1 tk +1 ,
where zk +1 is chosen from N (0,1).</p>
      <p>Note that we can use other methods of integrating stochastic ODEs, such as the Milstein method of
first order, which for this problem would be equivalent to the Euler-Maruyama method. In this case,
the solution on the (k + 1)-th time layer will be defined as
xk +1 = xk + F ( xk ) tk +1 + Wk +1.</p>
      <p>In this work, the memristor’s operation was simulated the following parameter values: Ron = 205
Ohm, Roff = 2128 Ohm,  v = 6  10 −10, V p = 0.65 V, Vn = −0.87 V, D = 621 nm, x(0) = 0, V (t ) - see at</p>
      <p>The presence of noise in the memristor model causes all parameters to take on the stochastic
properties. On the diagram with the volt-ampere characteristic, we can distinguish trajectories that
correspond to different switching cycles of the memristor. Here we observe the good correspondence
in the right part of the diagrams and satisfactory correspondence in their left parts.</p>
    </sec>
    <sec id="sec-3">
      <title>3. Mathematical model of a neuromorphic network</title>
      <p>We consider a two-layer fully connected self-learning analogue network with one layer of
memristor elements (synapses); it consists of 64 inputs and 5 neurons (Fig. 3).</p>
      <p>According to the STDP method, the learning mechanism is implemented through feedback (Vte). At
the moment of neuron activation, two pulses of opposite sign arrive via the feedback channel with
delays. If there is activity at the synapse and a positive feedback pulse arrives, then the resistance
value of the corresponding memristor decreases, and if a negative feedback pulse arrives, the
memristor resistance increases.</p>
      <p>The neuron model is a parallel RC circuit. As soon as the value of the potential across the capacitor
exceeds a certain threshold, its potential is reset, and signals Vte and Vout are generated. In addition, at
the moment of neuron activation, the potential of other neurons decreases in proportion to the
coefficient  .</p>
      <p>
        The mathematical model is set in accordance with [
        <xref ref-type="bibr" rid="ref14">14</xref>
        ]. The main difference of the model
presented below is the presence of a term  dW on the right-hand side of the state equations for
memristors, which correspond to synapses. As a result, the entire model of the neuromorphic network
becomes stochastic
      </p>
      <p> FX ( xi, j , Vtej − Vinjt ) dt + dWi, j , Vgi (t )  0,
dxi, j = 
0, Vgi (t ) = 0,
 V
 v Dp2 exp  RVopn RVi, j  dt, V  V p ,


FX ( xi, j ,V ) =  v Dn2 exp  RVonn RVi, j  dt, V  Vn ,
 V

</p>
      <p>dt, Vn  V  V p ,</p>
      <p>Ron V
 v D 2 Ri, j

Ri, j = Ron xi, j + Roff (1 − xi, j ),</p>
      <p>
dVinjt = 1  n
dt Cint Vgi (it=)1 0 Ri, j
d j = 1 −  (Vinjt − Vth ) j,
dt</p>
      <p>Vo+ut , j   out ,
Voujt = 
0, out   j ,
Vte+ , j   s ,
Vte− ,  r   j  r +  s ,</p>
      <p>
2 2
Vtej = Vte0 , r   j ,</p>
      <p>
Vˆtej − Vinjt − Vinjt  − max  (Vinit − Vth )ˆi, j   m (Vinit − Vth ) Vinjt ,</p>
      <p>Rint  i=1,m   i=1 </p>
      <p>
  
0, s   j  r  r +  s   j   r ,
 2 2
ˆi, j = 1 − (1 −  ij ), Vˆtej = max(0, min(Vtej , Vte0 )),
xi, j (0) = random 0,1, Vinjt (0) = 0, j (0)  max( r , out ), i = 1...64, j = 1...5,
where V gi is the actual voltage value at the i-th input of the neural network; Vtej - the actual voltage
value in the feedback of the j-th neuron; Voujt - the actual voltage value at the output of the j-th neuron;
 j - time elapsed since the last activation of the j-th neuron; Vinjt - voltage across the capacitor of the
jth neuron; Rint , Cint - the value of resistance and capacitance of neurons; Vte+, Vte−, Vte0 - the amplitude
values of the feedback pulses and the default voltage value; Vo+ut - the output pulse amplitude; Vth - the
neuron activation voltage level; Ri, j - the memristor’s resistance value of the i-th synapse of the j-th
neuron; xi, j - the memristor’s state of the i-th synapse of the j-th neuron;  r - the feedback signal
duration after neuron activation;  s - the duration of one pulse in the feedback signal, 2 s  r ;  out
the duration of one pulse at the network output; α - suppression coefficient;  ij - the Kronecker
symbol;  ( x) - delta function;  ( x)- Heaviside function;  - coefficient characterizing the noise
intensity; Wi, j- Wiener process corresponding to the i-th memristor of the j-th neuron.</p>
    </sec>
    <sec id="sec-4">
      <title>4. Simulation of the neuromorphic network operation. Results</title>
      <p>The recognition problem for five patterns is considered (Fig. 4) [21]. The process of training the
network is as follows: for each epoch (equal to  r 2 seconds), the input signals vector Vg (t )
corresponds either to one of the recognized patterns or is set randomly (the elements of the vector
0.27). Over time, the network adapts to pattern recognition. The Distribution of patterns among
neurons occurs in the course of training.</p>
      <p>The parameters of the mathematical model of the neural network are adjusted depending on the
memristor model. For the used model, which corresponds to a memristor based on titanium oxide
(TiO2), we have the following parameter values: Rint = 200 Ohms, Cint = 45 μF, Vte+ = 0.7 V, Vte− = −0.9
V, Vte0 = 10 mV, Vo+ut = 2 V, Vth = 9 mV, r = 3 ms, s = 50 μs,  out = 1.5 ms.</p>
      <p>Fig. 5 shows the process of synaptic weight adaptation to recognized patterns. The shade of grey
corresponds to the state variable value of the corresponding memristor: the darker, the greater the
conductivity; the lighter, the less. At the initial moment of time, all weights are initialized with
random values, and gradually change during the network operation. From about the 1200th era,
patterns began to be seen, the recognition of which was trained by the network: the information was
memorized by the neural network. The duration of one epoch is 1.5 ms.
The correspondence of the network weights to the patterns indicates that the network has successfully
trained to recognize the given images. Due to the stochastic component in the memristor model,
patterns can be distributed among neurons in different ways and the adaptation of weights can occur
at different rates.</p>
    </sec>
    <sec id="sec-5">
      <title>5. Conclusion</title>
      <p>The work is devoted to simulating the operation of an analogue self-learning pulse neural network
built on the basis of memristive elements in the image recognition mode. The simulation is carried out
taking into account the stochastic properties of memristors. A variable-resistor thin-film memristor
model based on an exponential dopant drift model, in which there is a term responsible for additive
(Gaussian) noise, is considered. The ampere-voltage characteristics of the model are compared with
experimental data on titanium oxide. The simulating of the operation for the network consisting of
five neurons with 320 synapses, designed to recognize five different black-and-white images of 8 by 8
pixels, is performed. As a result the network has successfully trained to recognize the given patterns.</p>
    </sec>
    <sec id="sec-6">
      <title>6. Acknowledgements</title>
      <p>The work was performed with the support of RFBR grant No. 19-29-03051mk.</p>
      <p>The studies were carried out using the resources of the Center for Shared Use of Scientific
Equipment "Center for Processing and Storage of Scientific Data of the Far Eastern Branch of the
Russian Academy of Sciences", funded by the Russian Federation represented by the Ministry of
Science and Higher Education of the Russian Federation under project No. 075-15-2021-663.</p>
    </sec>
    <sec id="sec-7">
      <title>7. References</title>
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