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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Modelling of the derivatives pricing with multifactor volatility</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Burtnyak Ivan</string-name>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Malytska Anna</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Gvozdytskyi Vitalii</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Simon Kuznets Kharkiv National University of Economics</institution>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Vasyl Stefanyk Precarpathian National University</institution>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <fpage>92</fpage>
      <lpage>108</lpage>
      <abstract>
        <p>The pricing of options generated by diffusion processes, where diffusion depends on two groups of variables, was carried out. An algorithm for calculating the approximate price of derivatives and the accuracy of valuations has been developed, which allows to perform the analysis and to make precautionary to minimize the risk of derivatives pricing arising on the stock market. The method of finding the indicative price for a wide class of derivatives has been expanded. Using the spectral theory of self-adjoint operators in Hilbert space and the wave theory of singular and regular perturbations, an analytical formula of the approximate asset price was set, which was described by models with stochastic volatility dependent on l-fast variable and n-slow variable factors, and on local variable.</p>
      </abstract>
      <kwd-group>
        <kwd>derivative pricing</kwd>
        <kwd>diffusion processes</kwd>
        <kwd>Ornstein-Uhlenbeck process</kwd>
        <kwd>spectral theory</kwd>
        <kwd>singular and regular perturbation theory</kwd>
        <kwd>stochastic volatility</kwd>
        <kwd>SturmLiouville theory</kwd>
        <kwd>Vasicek model</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>
        been used by many scientists, namely to forecast options prices [
        <xref ref-type="bibr" rid="ref10">9</xref>
        ], to find interest rate on
securities [
        <xref ref-type="bibr" rid="ref15">14</xref>
        ], to simulate volatility of financial assets [
        <xref ref-type="bibr" rid="ref14">13</xref>
        ]. Both spectral theory and
stochastic volatility models have become an indispensable tool in financial mathematics,
due to the fact that derivative prices are subject to Brownian motion and correlate with
volatility [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. Study of stochastic volatility, in particular the volatility of an asset
controlled by non-local diffusion [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ].
      </p>
      <p>
        Short-term interest rate dynamics models were considered in Vasicek's work [
        <xref ref-type="bibr" rid="ref12">11</xref>
        ] for
derivatives pricing. Significant contribution to the theory of interest rates was made in
[810], namely: finding the credit spread of credit market instruments, determining the price
of interest rate options, determining the risk and return on derivatives of the stock market.
The models developed by these scientists have their advantages and disadvantages, but
each is used to increase the liquidity of the financial markets. The use of more complex
models, despite their theoretical validity, causes complex multi-parameter functions of the
profitability curve to be obtained, and this causes significant errors in the calculations.
      </p>
      <p>
        Using spectral analysis, Linetsky [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ] applied the spectral theory of self-adjoint
operators to different models, and in particular to the Vasicek model. Lorig [
        <xref ref-type="bibr" rid="ref12">11</xref>
        ]
considered short-term interest rates described by Vasicek's model with stochastic
volatility dependent on two factors, one of which is fast and the other is slowly changing.
The spectral theory and the theory of singular and regular perturbations is applied to
selfadjoint operators in Hilbert spaces, which describe processes with multidimensional
stochastic volatility having l-fast variable, n-slow variable factors,
      </p>
      <p>. In particular, this theory applies to the short-term interest rates described by Vasicek's
model. The approximate price of the bonds and their profitabilty are calculated. Applying
the Sturm-Liouville theory, Fredholm alternatives, and analyzing singular and regular
perturbations at different time scales, we obtained explicit formulas for the approximation
of bond prices and profitability.</p>
      <p>The goal of the article is to develop an algorithm for finding the approximate price of
derivatives and to find explicit formulas for finding their value based on the development
of eigen functions and eigenvalues of self-adjoint operators using boundary tasks for
singular and regular perturbations. To set the theorem of estimating the accuracy of option
prices approximation.</p>
      <p>The main advantage over other developed methods is that finding the price of
derivatives is reduced to solving the problem of finding the eigenvalues and
eigenfunctions of a particular equation that fits this model.</p>
      <p>II Methodology and Data</p>
      <p>Let represent short interest rates. One of the most widely known models of short
interest rates is the Vasicek model, in which is modeled as an Ornstein-Uhlenbeck
process with multidimensional stochastic volatility.
i.e.</p>
      <p>The Ornstein – Uhlenbeck process is described by a second-order differential equation
ща parabolic type</p>
      <p>Let’s calculate the density of distribution of this process. To do this, consider the
Cauchy problem for (1). With the initial condition
( ) ( )
( )
where</p>
      <p>( )– smooth finite function.</p>
      <p>Let’s apply the Fourier transform. In particular,
[</p>
      <p>|
√
( ∫
(
)
∫
(
)
)]</p>
    </sec>
    <sec id="sec-2">
      <title>The initial condition has the form</title>
      <p>The Cauchy problem (3), (4) for a linear non-uniform differential equation in partial
first-order derivatives is solved by the method of characteristics
( )
)
})
)
)}</p>
      <p>)}
(
)
)
(</p>
      <p>√
(
( )
))</p>
      <p>}
(
(
{
)} (</p>
      <p>)
(
(
∫ (
)
)
√ ∫ ( ) ∫ {
( ( ) )}}
{ ( )
Let’s distinguish the complete square by
( ) (</p>
      <p>( (</p>
      <p>Indeed ∮( ) – closed contour,
integral theorem, the integral is zero.
√</p>
      <p>(
{(
(</p>
      <p>(
(
(
)
)
(
(
∫
(
)) (
√
√
)) (
)
(</p>
      <p>(
)
)
∫
)) (
)) (
)) (
)
)
)
)
)
)}
√
)
√
√
)
)
√</p>
      <p>( )
)) ( )
– analytical function, so, by Cauchy's</p>
      <p>( )
, the contour is arranged symmetrically
will transform into ∫
, and ∫</p>
      <p>∫
(
)
|
||
|
with (
(</p>
      <p>))
along the axis
with
if
∫
∫
with therefore equality (7) holds.</p>
    </sec>
    <sec id="sec-3">
      <title>Let's check that goes to zero at</title>
      <p>| |
With fixed
|∫
|</p>
      <p>| ∫
|</p>
      <p>|
( )) as ( ), where
( (
(</p>
      <p>))√
)
∫
|
then because
Similarly, ∫</p>
      <p>. Will get
so fundamental solution or the Green's function has the form</p>
      <p>On the other hand, on the probabilistic side, the Green's function is the density of
distribution.</p>
      <p>
        Using the methods of spectral theory and the theory of singular and regular
perturbations, we can find the approximate price of Ornstein-Uhlenbeck two-barrier
options with multivariate volatility, as a self-function decomposition using infinitesimal
generators of (l + n + 1)-dimensioned diffusions, that is,
diffusion depends on one local variable, the l-dimensional fast-variable factor and the
ndimensional slow-variable factor. This work is an extension of [
        <xref ref-type="bibr" rid="ref12 ref14 ref6">6, 11, 13</xref>
        ], in [
        <xref ref-type="bibr" rid="ref12">11</xref>
        ] l = 1
and n = 1.
      </p>
      <p>Process can represent many economic phenomena and processes. For example,
inventory value, index price, reliable short interest, etc. More broadly, is an external
factor that characterizes the cost of any of the above processes. By physical measure of
process , we understand process , which has an instant drift ( ) and stochastic
volatility ( ) ( ) , which contains both components: local
( )and non-local ( ). It should be noted, that infinitesimal
generators for and have a form
(
( )
( )
)
(
( )
( )
)
are characterized by the values
and
respectively. Thus,
and
an internal timeline
and</p>
      <p>Let’s consider
and
, to make the
inner time scale
small and the inner time scale
– large. Therefore,
fast variables, and
are slowly variable factors. Note that
and
the form of the Ornstein-Uhlenbeck process [20]
have</p>
      <p>are
have
̅
the right part of which has a form</p>
      <p>̅ (9)
Let’s reduce (9) to the equation , where , so that there is no
first derivative in the obtained equation, that is, we look for a solution in the form
( ) ( )
where ( ) new unknown function, and let’s choose ( )in such way to have
( ) . (10)</p>
      <p>Having reduced into (10), we will have ̅ , herefrom
will have</p>
    </sec>
    <sec id="sec-4">
      <title>Thus, In our case</title>
      <p>( )
( )
(
̅
{ ∫</p>
      <p>̅
) (
̅
)
}
̅
̅
)
For reasons of solution, let's make a substitution
we will have
therefrom</p>
    </sec>
    <sec id="sec-5">
      <title>From the point that We have</title>
      <p>̅
√
̅
)
(√̅
√
∫
) (
(
̅
√ ̅
̅
)
( (</p>
      <p>̅
̅
( (
̅
(
̅</p>
      <p>)
√
̅
̅
√</p>
      <p>)
̅
)</p>
      <p>)
)</p>
      <p>̅
)
√
̅
( )
(
√ ̅
̅
√</p>
      <p>)
√
(</p>
      <p>̅
√
̅</p>
      <p>)
then
√
̅
(</p>
      <p>̅
need solution to be equal 0 at points
picture, so we will replace the variables
̅
and</p>
      <p>, and
, we’ll have
̅
)
)
√ (
̅
)
̅
and
do not give such a
(
̅
or
then
on eigen values and eigen functions we will explore
̅ ̅</p>
      <p>)</p>
    </sec>
    <sec id="sec-6">
      <title>The general solution has the form</title>
      <p>√
(
̅
Let’s check the fulfilling of boundary conditions, if
, with
( )
(
̅</p>
      <p>) (</p>
    </sec>
    <sec id="sec-7">
      <title>Let’s find the scalar product</title>
      <p>(
( )
( ))
∫</p>
    </sec>
    <sec id="sec-8">
      <title>With Thus,</title>
      <p>̅
∫
∫
{
̅</p>
      <p>}
(
(
)
)</p>
      <p>|
∫(
√
√
(</p>
      <p>̅
̅</p>
      <p>̅
̅
)
{
∫
̅
(
∫[
(
̅
√
)
) √
√</p>
      <p>√
(
)
}</p>
      <p>(
)
)
|
{
̅
)
(
(
|
}
(
√
)
( )
( ))
{
III Results and analysis</p>
      <p>
        Let be the securities without paying dividends on an asset (for example, stock,
index, etc.). Often, is modelled as a geometric Brownian motion with constant volatility
(e.g. Black-Scholes formula) [
        <xref ref-type="bibr" rid="ref7 ref8">7</xref>
        ]. Consider as a model of geometric Brownian motion
with multidimensional stochastic volatility. In particular, ̃dynamics in are given by:
( ) ̃ , ( )
Let’s calculate the approximate price of the double barrier of the option defined on .
Let us write down the operator 〈 〉 and its associated densities at speed ( )
〈
〉
      </p>
      <p>̅
For a double barrier option with
and
( ) ( )</p>
      <p>̅ ̅
barrier values, the payout is:
( )</p>
      <p>( ) { } ( ) { }, ( ), ,</p>
      <p>To calculate the value of this parameter, at first, it is needed to find the eigenvalues of
the operator 〈 〉 with boundary conditions</p>
      <p>( ) , ( ) .</p>
      <p>It should be noted that a regular killing of boundary conditions at the ends and are
entered. Equation</p>
      <p>
        〈 〉 (〈 〉)
with the above boundary conditions can be found in [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ]
( )
      </p>
      <p>
        ̅√
,
and
On the basis [
        <xref ref-type="bibr" rid="ref13">12</xref>
        ] let’s calculate
(
( )
      </p>
      <p>)
(
( )</p>
      <p>) (
(
̃
̅ (
)</p>
      <p>̅ (
( ( )</p>
      <p>( )
(
)
̅</p>
      <p>( )
(
( )
)
((
)(
(
̅ )
( ))
And for
let’s find
(
̅</p>
      <p>(
(
̅
(
( )
)
̅
(</p>
      <p>)
( )
( )
̅
)
)
(
( ))
̅
)
̅
))
̅ (
̅
(
( )
̅
( )
( ))
)
( )
( )
̃
Calculation
(</p>
      <p>( )
̅ (
̅
(
)( ( ) ( )
( ) ( ))
( ) ( )
( )
̅
( ̅
( )
(
) ( )
( ))</p>
      <p>( )
( )
(√
{ (
̅</p>
      <p>) }
(</p>
      <p>)
̅
(</p>
      <p>{ (
) )
̅̅̅̅
{
̅
̅
)
̅
) }
(</p>
      <p>̅
(
̅</p>
      <p>) }
̅
)
̅ )
)
(
)
(√̅ (
̅
)
√ √
̅ )</p>
      <p>̅ ) ̅
{ (̅ (
(
̅
)
̅(
̅
)
(̅ (
̅ ) }
̅ )
̅) )
After replacing the variable √ (</p>
      <p>̅
(
( )</p>
      <p>( ))</p>
      <p>Because
therefrom it follows that</p>
      <p>( )
)
( )
∫ (</p>
      <p>)
( )
)
√
{
∫
( )
and
:</p>
      <p>By integrating by the parts, given that such an integral contains pair degrees
decreases and reduces to ∫ and integral which contains – not pair equals
zero, times, taking by parts we will get ( ( ) ( ))</p>
      <p>
        To find the price of the bond with payments ( ) { } , it’s needed to solve
the equation (15) on finding the eigenvalues at the segment ( ) with 〈 〉,
according to (15). As both ends and are natural boundaries, then the solution has a
form [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ]
̅
)
̅
)
( )
(
      </p>
      <p>̅
̅̅̅̅ {(
)
)
(
(
̅̅̅̅ {(
)
̅
)</p>
    </sec>
    <sec id="sec-9">
      <title>Calculation of can be found in [1-3] 106</title>
    </sec>
    <sec id="sec-10">
      <title>Operators</title>
      <p>̃
are written on the basis of recurrence ratios:</p>
      <p>̅</p>
      <p>For zero coupon bonds, the profitability curve is considered more often rather than the
price of the bond itself. Return in zero-coupon bonds, for which one dollar is paid at
time is determined by the ratio:</p>
      <p>Let’s get an approximation for a zero coupon bond, sorting it out both bond prices
and return by degrees √ and √ :
(
(
√
̅
√
̅
)
)
√
̅
)</p>
      <p>(
)</p>
      <p>(
)(
̅</p>
      <p>̅
√
̅
̅
(
(
)
)
̅
)]
̅ (
(
̅√
)</p>
      <p>(
)
√
(
)
)
)
)
)]
̅</p>
      <p>)
)</p>
      <p>}
(</p>
      <p>)
̅ (
( )
̅ (</p>
      <p>}
}
̅
)
)
}
}
}
}
}
∑ √</p>
      <p>∑ √
{ (
∑ √
∑ √
) }
Grouped by degrees√
and √</p>
      <p>we will get:
(
)
∑ √
∑ √</p>
      <p>
        Note: the drawings are built by component in each corresponding timeline, similarly
for the two components as in [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ].
      </p>
      <p>IV Conclusions</p>
      <p>Thus, the studies conducted in the work allow us to draw the following conclusions.</p>
      <p>An algorithm for finding the approximate price of derivatives has been developed and
explicit formulas have been found for finding their value based on the decomposition of
eigen functions and eigenvalues of self-adjoint operators using boundary tasks for singular
and regular perturbations. The theorem of estimating the accuracy of derivatives prices
approximation is established, on the scales of systems of slow and fast variable factors on
which volatility of derivative financial instruments depends.</p>
      <p>The general method of finding the approximate price for a wide range of derivatives
has been obtained. It has been established that derivative payments can be
pathdependent, and the underlying process may exhibit a jump whose intensity depends on
multidimensional volatility. The price of options depends on the stochastic
multidimensional volatility, which is described by a path-dependent process. Finding the
price of derivatives comes down to the task of finding the eigenvalues and eigenfunctions
of a particular equation that fits this model.</p>
      <p>The approximate price of bonds and their profitability are determined by the methods
of spectral theory and wave perturbation theory. The spectral theory and the theory of
singular and regular perturbations have been applied to short-term interest rates described
by the Vasicek model. The approximate price of the bonds and their profitability are
calculated.</p>
      <p>The main advantage of the reviewed pricing methodology is that, by combining
methods with spectral theory, regular perturbation theory and singular perturbation theory,
it reduces to solving equations on finding eigenfunctions and eigenvalues.</p>
    </sec>
  </body>
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