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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>A Finite Field of Square Matrices of Order 2</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Emil Faure</string-name>
          <email>e.faure@chdtu.edu.ua</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Anatoly Shcherba</string-name>
          <email>a.shcherba@chdtu.edu.ua</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Artem Skutskyi</string-name>
          <email>a.b.skutskyi.asp21@chdtu.edu.ua</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Artem Lavdanskyi</string-name>
          <email>a.lavdanskyi@chdtu.edu.ua</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Cherkasy State Technological University</institution>
          ,
          <addr-line>460 Shevchenko blvd., Cherkasy, 18006</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>State Scientific and Research Institute of Cybersecurity Technologies and Information Protection</institution>
          ,
          <addr-line>3 M. Zaliznyak str., Kyiv, 03142</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <fpage>306</fpage>
      <lpage>312</lpage>
      <abstract>
        <p>This paper focuses on constructing a Galois field of square matrices of order 2 and substantiates a theoretical basis for developing schemes of cryptographic transformation of information, key exchange, and digital signature. This research goal has been achieved by investigating a family of square matrices of order 2 with the commutative operation of matrix multiplication from the general linear group over the prime field of integers modulo. It has been proved that this commutative family of matrices is simultaneously diagonalized. The matrix that performs diagonalization has been calculated. This matrix is common to all matrices of the commutative family. The research has defined the family of matrices forming a Galois field of order with common operations of matrix multiplication and addition. The multiplicative cyclic group of this field has been shown.</p>
      </abstract>
      <kwd-group>
        <kwd>1 Finite field</kwd>
        <kwd>square matrices</kwd>
        <kwd>commutative family of matrices</kwd>
        <kwd>diagonalization</kwd>
        <kwd>key agreement</kwd>
        <kwd>cryptography</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        The theory of finite fields plays one of the key
roles in cryptography. Thus, the operations of
addition, multiplication, and finding inverse
values in symmetric encryption algorithms [1–
2] are implemented over an extended finite
field GF (2n ) . Algorithms testing simplicity
and factorization of integers rely on the theory
of finite fields [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ], which is the foundation of
asymmetric cryptography [
        <xref ref-type="bibr" rid="ref4 ref5 ref6 ref7">4–7</xref>
        ]. Finite fields
are an integral tool for creating electronic
digital signatures, including those based on
elliptic curves [
        <xref ref-type="bibr" rid="ref10 ref11 ref12 ref13 ref8 ref9">8–14</xref>
        ].
      </p>
      <sec id="sec-1-1">
        <title>The recent trends in cryptography indicate</title>
        <p>that applications of matrix theory in
information representation and transformation
are expanding. In particular, this approach has
already proven its effectiveness in the AES
encryption standard [2].</p>
        <p>Previous research findings into matrix
theory [15] developed a public-key
cryptosystem based on commutative
semirings of tropical cyclic matrices, where
multiplication is the usual addition of numbers,
while the usual multiplication of numbers in
the tropical semiring is absent.</p>
      </sec>
      <sec id="sec-1-2">
        <title>The study [16] investigated chaotic image</title>
        <p>encryption technology and the application of
matrix semi-tensor product theory.</p>
        <p>In the study [17], the authors propose a
homomorphic encryption technique based on
matrix transformations with shifts, rotations,
and transpositions. A recent study [18]
proposes a code-based digital signature. The
proposed scheme uses the McEliece
cryptosystem [19] based on random inverse
matrices.</p>
        <p>Another major study describes Shamir’s
three-pass random matrix ciphering
mechanism [20] that deploys a three-pass
protocol with encryption operators that are
random matrices. However, this research was
limited by operations on commutative matrices,
and uses inverse, circular, and permutation
matrices, leaving the matrix fields beyond the
scope of the study.</p>
        <p>As we have indicated above, finite matrix
fields have potential applications in
cryptographic schemes used in information
transformation, key exchange, and digital
signature. In addition, the authors of this
research have described potentially effective
applications of finite matrix fields in
permutation-based data transmission systems
[21–24].</p>
      </sec>
      <sec id="sec-1-3">
        <title>The study [25] identifies and investigates</title>
        <p>families of square matrices of order 2 with the
commutative operation of multiplication for
solving cryptographic information
transformation problems.</p>
      </sec>
      <sec id="sec-1-4">
        <title>Six families of matrices from the general</title>
        <p>linear group GL (n, Z p ) [26–27] of the order n
are defined over the prime field of integers
modulo p , for which the multiplication
operation is commutative.</p>
        <p>In [25], the authors show that one of the
families of square matrices of order 2 with the
commutative operation of matrix
multiplication is the family
 t, a,b, k  Z p , 
  a 1  
6 = t   , t  0,b  0,  .</p>
        <p>  b a + k  
 a (a + k ) − b  0
with b and k fixed and supplemented with an
identity matrix. We denote this family as
  a 1   1 0  
t   , s   ,
  b a + k   0 1  
 
CGLb,k (2, Z p ) =  t, s, a,b, k  Z p ,  .
 t, s  0, 
a (a + k ) − b  0 </p>
      </sec>
      <sec id="sec-1-5">
        <title>The study [25] has proved that the matrix family</title>
        <p>CGLb,k ( 2, Z p )
is
a
commutative
(abelian) group by multiplication. In addition,
the study has shown that the order of the group
D = k 2 + 4b  u2  Z p
is
CGLb,k ( 2, Z p ) for
p2 − 1.</p>
        <sec id="sec-1-5-1">
          <title>Obviously, a (a + k ) − b  0 if and only if</title>
          <p>D = k 2 + 4b  u2  Z p .</p>
        </sec>
      </sec>
      <sec id="sec-1-6">
        <title>Further, we shall accept that</title>
        <p>  a 1   1 0  
t   , s   ,
  b a + k   0 1  
 
CGLb,k (2, Z p ) = t, s, a,b, k  Z p ,  .
t, s  0, 
 
D = k 2 + 4b  u2  Z p </p>
        <p>This paper aims to build a Galois field of
square matrices of order 2 based on the group
of matrices CGLb,k ( 2, Z p ) , thus substantiating
a theoretical basis for developing schemes for
the cryptographic transformation of
information.
2. Diagonalization of Matrices</p>
        <p>From CGLb,k ( 2, Z p )
Note that, according to the study [28],
permutable matrices of simple structure can
be brought into diagonal form simultaneously,
that is, by a similarity transformation.</p>
        <p>By matrices of simple structure, we mean
matrices of order n , which have linearly
independent eigenvectors [28]. Since the
eigenvectors corresponding to pairwise
different characteristic numbers are always
linearly independent, a sufficient condition for
the matrix to have a simple structure is that all
the roots of the characteristic equation are
different [28–29].</p>
      </sec>
      <sec id="sec-1-7">
        <title>The characteristic polynomial of the matrix</title>
        <p> a 1 
A =   CGLb,k (2, Z p ) is
 b a + k </p>
        <p>A −  E =
a − 
b</p>
        <p>1
a + k − 
=
where E is an identity matrix of size n = 2 .</p>
      </sec>
      <sec id="sec-1-8">
        <title>The discriminant of the characteristic equation is</title>
        <p>D = (2a + k )2 − 4(a2 + ak − b) = k 2 + 4b .</p>
        <p>If D value is a quadratic nonresidue in the
prime field of integers Z p
( D = k 2 + 4b  u2  Z p ) ,
the
characteristic
polynomial has no roots in Z p . Since the power
of the equation is n = 2 , the polynomial is
irreducible over the Z p field.</p>
      </sec>
      <sec id="sec-1-9">
        <title>Consider an irreducible</title>
        <p>f ( x) = x2 − D  Z p  x .
polynomial</p>
      </sec>
      <sec id="sec-1-10">
        <title>The simple algebraic extension of degree 2</title>
        <p>over Z p is defined as a quadratic field
Fp2 = Z p  D  [30], where D = k 2 + 4b  u2  Z p .</p>
        <sec id="sec-1-10-1">
          <title>Galois field Fp2 has the characteristic p</title>
          <p>
            and degree 2 [
            <xref ref-type="bibr" rid="ref3">3</xref>
            ].
          </p>
        </sec>
        <sec id="sec-1-10-2">
          <title>Remark 1. Fp2 is a field of decomposition</title>
          <p>of characteristic polynomials for matrices from
the group CGLb,k ( 2, Z p ) . Eigenvalues of the
That is, there is a matrix C =  c11 c12  with
 c21 c22 
elements from Fp2 so that for each matrix
A CGLb,k (2, Z p ) the product C −1  A  C is a
diagonal
C−1  A  C = 1 (a,t ) 0  .</p>
          <p> 0 2 (a,t ) </p>
        </sec>
      </sec>
      <sec id="sec-1-11">
        <title>Here, we find such a matrix C .</title>
        <p>matrix:
Since C−1  A  C = 1 (a,t )
 0
0 </p>
        <p> , then
2 (a,t ) 
matrix
 a 1 
tA = t   
 b a + k 
Fp2 = Z p  D  are
t
1,2 (a,t ) = (2a + k </p>
        <p>2</p>
      </sec>
      <sec id="sec-1-12">
        <title>Thus, for the</title>
        <p>characteristic
tA −  E = t 2 A − 
t</p>
        <p>E = 0 ,</p>
        <p>over the field
D ) , t  0 .</p>
        <p>(1)
matrix tA , t  0 , the
equation is
whence
1,2 ( a,t ) = t 1,2 (a ) , where 1,2 ( a ) are the
 a 1 
eigenvalues of the matrix A =   over
 b a + k 
the field Fp2 = Z p  D  .</p>
        <p>
          
t
If  (a,t ) = (2a + k  D ) is one of the
2
roots of the characteristic polynomial
irreducible over Z p , where   Fp2 , then, by
Theorem 2.14 from [
          <xref ref-type="bibr" rid="ref3">3</xref>
          ], the other root of the
equation is  p (a,t ) = t (2a + k D ) .
        </p>
        <p>2</p>
      </sec>
      <sec id="sec-1-13">
        <title>The eigenvalues for the matrix sE are</title>
        <p>1,2 ( s ) = s  0 .</p>
      </sec>
      <sec id="sec-1-14">
        <title>Lemma 1.3.19 from [29] proves that the</title>
        <p>family of diagonalizable matrices is a
commutative family if and only if it is
simultaneously diagonalizable. Based on this
lemma, we formulate our next remark.</p>
      </sec>
      <sec id="sec-1-15">
        <title>Remark 2. The commutative family of</title>
        <p>matrices CGLb,k ( 2, Z p ) over the field
is
simultaneously
Fp2 = Z p  D </p>
        <p>
diagonalizable.
 a 1   c11
t    
 b a + k   c21
c12  =
c22 
 c11
= 
 c21
c12 1 (a,t )</p>
        <p>0
c22 </p>
        <p>After multiplying the
comparing them, we arrive at
0 </p>
        <p>.</p>
        <p>2 (a,t ) 
t (ac11 + c21 ) = c111 (a,t ),

t (bc11 + (a + k ) c21 ) = c211 (a,t ),

t (ac12 + c22 ) = c122 (a,t ),
t (bc12 + (a + k ) c22 ) = c222 (a,t ).</p>
        <p>Considering that 1,2 ( a,t ) = t 1,2 (a ) , we
rewrite the equation system as:
matrices
and
ac11 + c21 = c111 (a),

bc11 + (a + k )c21 = c211 (a),

ac12 + c22 = c122 (a),
bc12 + (a + k )c22 = c222 (a).
(a − 1 ( a)) c11 + c21 = 0,

bc11 + (a + k − 1 (a)) c21 = 0,

(a − 2 ( a)) c12 + c22 = 0,

bc12 + (a + k − 2 ( a)) c22 = 0.</p>
      </sec>
      <sec id="sec-1-16">
        <title>The last equation system transformed into the next one: can be</title>
      </sec>
      <sec id="sec-1-17">
        <title>We take the first eigenvalue of the matrix</title>
        <p> a 1  2a + k + D
tA = t   b a + k  as 1 (a) = 2 .
Then the second eigenvalue of the matrix tA is
2a + k − D
2 (a) = .</p>
        <p>2</p>
        <p>From the first two equations of the system,
we have:</p>
        <p>We shall accept c11 = 1. Then c21 = k + D
2
and the first eigenvector of the matrix C is
 1 
 
e1 =  k + D  .</p>
        <p> 2 </p>
        <p>The second eigenvector of the matrix C can
be found similarly from the other two
 1 
 
equations of the system: e2 =  k − D  .
 2 
 1 1 
Then the matrix C =  k + D k − D  .</p>
        <p> 2 2 </p>
      </sec>
      <sec id="sec-1-18">
        <title>Note that the matrix C is independent of a</title>
        <p>and t values and is common for CGLb,k (2, Z p )
.</p>
      </sec>
      <sec id="sec-1-19">
        <title>Here, we perform a verification to complete the presentation.</title>
        <p> k − D 
C−1  A  C = C1  k +2 D −1t  ba a +1 k  
 − 2 1 
1 </p>
        <p>
k − D  =</p>
        <p>2 
 1

 k + D</p>
        <p> 2
= t  2a + k2+ D 0  =</p>
        <p> 0 2a + k2+ D 
= 1 (0a,t ) 2 (0a,t ) .</p>
      </sec>
      <sec id="sec-1-20">
        <title>Consider the set of nondegenerate diagonal</title>
        <p>matrices D over the field Fp2 = Z p  D  :

 0  
D =  0  p ,  Fp2  . (2)
</p>
        <p>Remark 3. The mapping g ( A) = C−1  A  C
defines a one-to-one correspondence
(bijection) between matrices from
CGLb,k (2, Z p ) and diagonal matrices from D .

Hence, g : CGLb,k (2, Z p )  D .

Proof.</p>
        <p>Let A1, A2 CGLb,k (2, Z p ) , A  A2 , 1,1p
1
and 2 ,2p are eigenvalues of matrices A1 and
A2 correspondently.</p>
      </sec>
      <sec id="sec-1-21">
        <title>Then</title>
        <p>C−1  01 01p   C  C−1  02 02p   C 
 1  2.</p>
      </sec>
      <sec id="sec-1-22">
        <title>The number of different matrices of the set</title>
        <p>D is equal to p2 −1, which corresponds to the
order of the multiplicative abelian group
CGLb,k (2, Z p ) .</p>
        <p>This implies that the mapping g = g ( A)
establishes a one-to-one correspondence
between CGLb,k (2, Z p ) and D .
3. Galois Field of Square 2×2</p>
        <p>Matrices</p>
      </sec>
      <sec id="sec-1-23">
        <title>We shall use the notation</title>
        <p>  a 1   1 0 
t   b a + k , s   ,</p>
        <p> 0 1  
Fb,k =  t, s, a,b, k  Z p , </p>
        <p>D = k 2 + 4b  u2  Z p 
for the matrix family, where p is a prime
number and b , k are fixed in Z p .</p>
        <p>Theorem 1. The matrix family Fb,k is a
Galois field of order p2 with usual ordinary
operations of matrix multiplication and
addition.</p>
        <p>Proof.</p>
        <p>It is obvious that Fb,k = CGLb,k (2, Z p )  ,
where  =  0 0 .</p>
        <p> 0 0</p>
      </sec>
      <sec id="sec-1-24">
        <title>Here, we show that the addition operation</title>
        <p>is closed in the set Fb,k .</p>
        <p>According to Remarks 2 and 3, there is the
same matrix C for random matrices A1 and A2
from Fb,k that
0 
2p   C−1;</p>
        <p>
1 + 2
 A1 + A2 = C  
 0</p>
        <p>The Galois field Fp2 = Z p  D  has a

characteristic p . Therefore, due to Proposition
7.1.4 from [30], an equation
1p + 2p = (1 + 2 ) p is satisfied.</p>
      </sec>
      <sec id="sec-1-25">
        <title>Consequently, for</title>
        <p>A + A2 = C  3
1  0
0 
3p   C−1
3 = 1 + 2 :
C−1  ( A1 + A2 )  C = 3 0 
 0 3p   D . Obviously,
C−1    C = .</p>
      </sec>
      <sec id="sec-1-26">
        <title>According to Remark 3, there is a single</title>
        <p>matrix A3 CGLb,k (2, Z p ) , where
A + A2 = A3  Fb,k .</p>
        <p>1
0 
3p  , 3  Fp2 . Therefore,</p>
        <p>Thus, we can present the matrix family Fb,k
in the form of a fixed matrix C :
  0  </p>
        <p> 0  p   C−1,  Fp2 = Z p  D  .</p>
        <p>Fb,k = C   </p>
        <p>Therefore, Fb,k is an algebraic field for
ordinary operations on matrices, and its order
is p2 .
*</p>
        <p>Corollary 1. The multiplicative group Fb,k
of the finite field Fb,k is cyclic, i.e. the group
CGLb,k (2, Z p ) is cyclic.</p>
      </sec>
      <sec id="sec-1-27">
        <title>Corollary 2. The number of primitive</title>
        <p>elements in the field Fb,k is  ( p2 −1) , where
 (m) is the Euler function of m .</p>
      </sec>
    </sec>
    <sec id="sec-2">
      <title>4. Conclusion</title>
      <p>Thus, this study has shown that the
commutative family of matrices
  a 1   1 0  
t   , s   ,
  b a + k   0 1  
CGLb,k (2, Z p ) =  t, s, a,b, k  Z p , 
 t, s  0, 
a (a + k ) − b  0 
is simultaneously diagonalizable over the field
Fp2 = Z p  D  .</p>
      <p></p>
      <sec id="sec-2-1">
        <title>The matrix performing diagonalization is</title>
        <p> 1 1 
C =  k + D k − D  . The matrix C does

 2 2 
not depend on the values of a or t and is</p>
      </sec>
      <sec id="sec-2-2">
        <title>It was also shown that the matrix family</title>
        <p> 0 0
Fb,k = CGLb,k (2, Z p )  , where  =   ,
 0 0
forms a Galois field of order p2 with usual
matrix multiplication and addition operations.
Consequently, CGLb,k (2, Z p ) is a multiplicative
cyclic group.</p>
        <p>The finite field of square 2 2 matrices
investigated in this study can be applied to
construct new schemes of cryptographic
matrix transformations. In addition, the
approach used to find the finite field of
matrices of order 2 allows extending this
approach to the study of square matrices of
higher orders. Further research might explore
a 3 3 matrix set and attempt to construct the</p>
      </sec>
      <sec id="sec-2-3">
        <title>Galois field in it.</title>
        <p>5. Acknowledgments
This research was funded by the Ministry of
Education and Science of Ukraine under grant
0123U100270.
or
common for CGLb,k (2, Z p ) .
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