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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Spectral Model of the Encryption Key for a Symmetric Cryptosystem Based on Differential Transformations</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Olha Hryshchuk</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Korolyov Zhytomyr Military Institute</institution>
          ,
          <addr-line>22 Mira Avenue, Zhytomyr, 10004</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>In the transition and post-quantum periods, the problem of cybersecurity is significantly aggravated. The potential compromise of the best symmetric (AES-256) and asymmetric (RSA240) cryptosystems when an attacker uses quantum computers puts forward a number of security requirements for such systems. Today, a number of approaches are used to solve the problem of increasing cryptographic strength. Classic, which boils down to solving the problem of distributing encryption keys and new, the essence of which is to create promising cryptosystems based on new mathematical principles. The latter approach is based on cognitive cryptography, dynamic chaos theory, constructive, quantum and post-quantum cryptography, DNA algorithms, proxy models of cryptosystems, attribute-based cryptosystems, batch and non-commutative cryptography. The greatest interest from the point of view of security today is integrated cryptography. Thus, in previous works on this topic, it was proposed to create a symmetric cryptosystem based on differential transformations. The principle of functioning of this cryptosystem does not differ from the principles of functioning of classical symmetric cryptosystems. The only difference is that a symmetric cryptosystem based on differential transformations is based on the Fredholm integral equation of the first kind, the encryption key for which is its core. Special requirements for choosing an encryption key for a symmetric cryptosystem based on differential transformations are the requirements regarding its continuity, innate and symmetric. Following these requirements, the article offers a spectral model of the encryption key for the corresponding cryptosystem, which is built on the basis of differential transformations of Academician of the National Academy of Sciences of Ukraine G. E. Pukhov. It is shown that the spectral model of the encryption key for a symmetric cryptosystem on differential transformations is the sum of discret differential spectra for different values of the integer argument. Representation of the encryption key in the form of a spectral model makes it possible to implement encryption and decryption procedures by a symmetric cryptosystem using differential transformations in real time in the future.</p>
      </abstract>
      <kwd-group>
        <kwd>1 Encryption key</kwd>
        <kwd>spectral model</kwd>
        <kwd>symmetric cryptosystem</kwd>
        <kwd>differential transformations</kwd>
        <kwd>cybersecurity</kwd>
        <kwd>image</kwd>
        <kwd>T-spectrum</kwd>
        <kwd>discrete</kwd>
        <kwd>numeric argument</kwd>
        <kwd>Fredholm integral equation of the first kind</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>Cybersecurity has now become a cornerstone
on the agenda for many countries around the
world. The computerization of all spheres of state
and civil society activities, as well as the mass
access of citizens to information technologies,
threatens their use for illegal and terrorist
purposes. It is possible that the fact of carrying out
a cyberattack by one state against another can be
regarded as the beginning of aggression from
cyberspace. That is why in the world and Ukraine,
scientist’s eyes are increasingly focused on
cybersecurity issues.</p>
      <p>
        Based on the assessment of the current state of
Science and technology, it becomes obvious that
in the next 10 years there will be a breakthrough
in the use of quantum computers for solving
cybersecurity problems [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. The most pessimistic
predictions show that quantum cryptanalysis
based on Grover's algorithm will halve the
stability of all symmetric cryptographic
mechanisms [
        <xref ref-type="bibr" rid="ref2 ref3 ref4">2–4</xref>
        ]. Plans to create a 100-qubit
quantum computer by 2024 significantly
exacerbate this problem [
        <xref ref-type="bibr" rid="ref5 ref6">5, 6</xref>
        ].
      </p>
    </sec>
    <sec id="sec-2">
      <title>2. The Latest Studies and Printed</title>
    </sec>
    <sec id="sec-3">
      <title>Works Analysis</title>
      <p>
        Analysis of recent studies and publications
[
        <xref ref-type="bibr" rid="ref1 ref10 ref11 ref8 ref9">1, 8–11</xref>
        ] and others has shown that a number of
new approaches to ensuring the cryptographic
stability of symmetric cryptosystems are currently
known. In the transition and post-quantum period,
the approaches described in [
        <xref ref-type="bibr" rid="ref1 ref10 ref11 ref12 ref13 ref8 ref9">1, 8–13</xref>
        ] will also be
relevant.
      </p>
      <p>
        At the same time, there are other alternatives
to the established classical approaches. In
particular, general approaches to creating a new
class of cryptosystems are described in [
        <xref ref-type="bibr" rid="ref14 ref15">14, 15</xref>
        ],
but specific cryptographic mechanisms for their
implementation are not given.
      </p>
      <p>
        In [
        <xref ref-type="bibr" rid="ref16">16</xref>
        ], the idea of creating symmetric
cryptosystems based on the Fredholm integral
equation of the first kind was developed, and in
[
        <xref ref-type="bibr" rid="ref17">17</xref>
        ] the requirements for choosing an encryption
key were formalized. However, the key
generation mechanism and its spectral model are
not given.
      </p>
    </sec>
    <sec id="sec-4">
      <title>3. Purpose</title>
      <p>The purpose of this article is to develop a
mechanism for generating an encryption key for a
symmetric cryptosystem based on differential
transformations and obtain its spectral model.</p>
    </sec>
    <sec id="sec-5">
      <title>4. Concept presentation</title>
      <p>
        Based on [
        <xref ref-type="bibr" rid="ref18">18</xref>
        ], the encryption key K ( x, s ) is
the core of the Fredholm integral equation of the
first kind [
        <xref ref-type="bibr" rid="ref16 ref17">16, 17</xref>
        ]
b
 K ( x, s) z ( s ) ds = u ( x), a  x, s  b ,
a
where z ( s ) – plaintext;
u ( x ) – cipher.
      </p>
      <p>
        There are many special features for choosing
an encryption key for the Fredholm cryptosystem,
which can be applied to the function of the initial
wiggle [
        <xref ref-type="bibr" rid="ref19">19</xref>
        ]
      </p>
      <p>m
K ( x, s) =  gl ( x) ql ( s) . (1)</p>
      <p>l=1</p>
      <p>
        To obtain an analytical spectral model of the
encryption key (1), we will use differential
transformations of Academician of the National
Academy of Sciences of Ukraine G. E. Pukhov
[
        <xref ref-type="bibr" rid="ref20 ref21 ref22 ref23">20–23</xref>
        ], the use of which for solving
cybersecurity problems was first described in the
monograph [
        <xref ref-type="bibr" rid="ref24">24</xref>
        ].
      </p>
      <p>
        According to [
        <xref ref-type="bibr" rid="ref20 ref21 ref22 ref23">20–23</xref>
        ], differential
transformations are transformations of the form
X (k ) = x (k ) =
      </p>
      <p>H k  d k x (t ) </p>
      <p> 
k !  d t k
 t=0</p>
      <p>•
k=  t  k
• x (t ) =    X (k ) ,
k=0  H 
(2)
where x (t ) – the original, which is a continuous,
differentiable infinite number of times and
bounded together with all its derivatives, function
of a real argument t ;</p>
      <p>X (k ) and x (k ) equivalent notation of the
differential image of the original representing a
discrete (lattice) function of an integer argument
k =: 0, 1, 2,... ;</p>
      <p>H – a scale steel that has the dimension of an
argument t and is often chosen equal to the
segment 0  t  H on which the function is
• – a symbol of correspondence between the
considered x (t ) ;
X (k ) = x (k ) .</p>
      <p>x (t ) and
its
differential
image</p>
      <p>To the left of the symbol • is a direct
transformation that allows you to find the image
X (k ) behind the original x (t ) , and to the right
is a reverse transformation that allows you to get
the original behind the image in the form of a
(3)
ql ( s ) ,
m
K ( x,0) =  gl ( x) Hl2ъ(0 − 2) = 0;
l=1
m
K ( x,1) =  gl ( x) Hl2ъ(1 − 2) = 0;
l=1
for k =:1
for k =: 2
m
K ( x, 2) =  gl ( x) Hl2ъ(2 − 2) =
l=1</p>
      <p>m
=  gl ( x) Hl2 ;
l=1</p>
      <p>for k  3
m
K ( x, k  3) =  gl ( x) Hl2ъ(3 − 2) = 0.</p>
      <p>l=1</p>
      <p>Thus, the spectral model of the encryption key
K ( x, k ) for a symmetric cryptosystem
on
differential transformations in general form in the
image domain under the accepted conditions is the
sum of the discretits found (5)–(8), i.e.</p>
      <p>m
K ( x, k ) =  gl ( x) Hl2 .</p>
      <p>l=1</p>
      <p>
        We give examples of constructing a spectral
model of the encryption key for a symmetric
cryptosystem based on differential
transformations based on the initial data given in
[
        <xref ref-type="bibr" rid="ref25">25</xref>
        ]. So according to [
        <xref ref-type="bibr" rid="ref25">25</xref>
        ] the encryption key
K ( x, s) = xs . Then expression (4) is simplified
and takes the form
power series, which is nothing more than an
otherwise written Taylor series centered at a point
t = 0 .
      </p>
      <p>Differential images X (k ) are called
differential T-spectrum, and the values of the
T-function X (k ) for specific argument k values
are called samples.</p>
      <p>
        Using the direct transformation (2) and the
general property of the product of functions in the
image domain for differential transformations
[
        <xref ref-type="bibr" rid="ref20 ref21 ref22 ref23">20–23</xref>
        ] for expression (1), we obtain
      </p>
      <p>K ( x, s ) • K ( x, k )

m
  gl ( x) ql ( s ) •
l=1
m
 gl ( x)Ql (k ),
l=1
where gl ( x ) – constant;</p>
      <p>Ql (k )
Ql (k ) =</p>
      <p>H k  d k q ( s) 
l  
k !  d s k
 s=0</p>
      <p>.
–
original
image</p>
      <p>Let the function ql ( s ) belong to a class of
power functions, i.e. ql ( s) = sln .</p>
      <p>
        Then, according to [
        <xref ref-type="bibr" rid="ref20 ref21 ref22 ref23">20–23</xref>
        ], its image from the
general form Ql (k ) =
reduced to an expression
Hln , k = n,
Ql (k ) = Hlnъ(k − n) = 
0, k  n.
      </p>
      <p>Taking this into account, the right-hand side of
expression (3) will have the form</p>
      <p>H k  d k q ( s) 
l  
k !  d s k
 s=0
will be
(5)
(6)
(7)
(8)
(9)
(10)
(11)</p>
      <p>K ( x, k ) = xHъ( k −1) .
–
displaced
“teda”,
where
ъ( k − n)
1, k = n,
ъ(k − n) = </p>
      <p>0, k  n.</p>
      <p>We find in general the differential spectra for
model (4), substituting sequentially the values of
the integer argument k =: 0, 1, 2,3. If, for example
n = 2 , we have:
for k =: 0</p>
      <p>Changing the value of the integer argument
k =: 0, 1, 2,... by analogy with expressions (5)–
(8), we obtain the differential spectrum discretits
for the desired spectral model.</p>
      <p>For k =: 0
K ( x, 0) = 0 ;</p>
      <p>for k =:1
K ( x,1) = xH ;
K ( x, k  2) = 0 .
(13)</p>
      <p>
        So, for the example given in [
        <xref ref-type="bibr" rid="ref25">25</xref>
        ], taking into
account the discrete found (11)–(13), the desired
spectral model of the encryption key (4) is
determined by the expression
      </p>
      <p>K ( x, k ) = xH , m = l .</p>
      <p>We present a graph of the functions of the
encryption key (fig. 1 a) and its T-spectrum
(fig. 1 b) for the found model (10).
b)
Figure 1: Encryption key function-original (a) and
its differential T-spectrum (b) – image</p>
    </sec>
    <sec id="sec-6">
      <title>5. Conclusions</title>
      <p>
        In this paper, a mathematical model of the
encryption key for a symmetric cryptosystem
based on differential transformations is proposed
for the first time. The resulting spectral model in
the image domain is the sum of discretits for
specific argument k values. The model meets the
requirements put forward in [
        <xref ref-type="bibr" rid="ref19">19</xref>
        ], and its
convergence with the results of known studies
[
        <xref ref-type="bibr" rid="ref25">25</xref>
        ] confirms its adequacy.
      </p>
      <p>The direction of further research will be the
formation of a set of possible keys for a symmetric
cryptosystem based on differential
transformations and obtaining their Spectral
models. The main purpose of the resulting model
is its use in a symmetric cryptosystem on
differential transformations during encryption and
decryption in voice message transmission systems
(VoIP-traffic).</p>
    </sec>
    <sec id="sec-7">
      <title>6. Acknowledgements</title>
      <p>I would like to express my gratitude to the staff
of the research department of the scientific center
of the Korolyov Zhytomyr Military Institute for
their support and valuable comments, taking into
account which helped to improve the quality of
the presentation of the work.</p>
    </sec>
    <sec id="sec-8">
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    </sec>
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