<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <journal-title-group>
        <journal-title>Global Optimality Conditions in Nonconvex Optimization. Journal
of Optimization Theory and Applications</journal-title>
      </journal-title-group>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.1007/s10957-016-0998-7</article-id>
      <title-group>
        <article-title>Global Optimality Conditions for Optimization Problem with D.C. Inequality and Equality Constraints</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>Alexander S. Strekalovsky Matrosov Institute for System Dynamics and Control Theory SB RAS Lermontov st.</institution>
          ,
          <addr-line>134, 664033 Irkutsk</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2017</year>
      </pub-date>
      <volume>173</volume>
      <issue>3</issue>
      <fpage>539</fpage>
      <lpage>546</lpage>
      <abstract>
        <p>This paper addresses the nonconvex optimization problem with the cost function and constraints given by d.c. functions. The original problem is reduced to a problem without inequality and equality constraints by means of the exact penalization techniques. Furthermore, the penalized problem is presented as a d.c. minimization problem. For the latter problem we develop the global optimality conditions (GOCs) which reduce the nonconvex optimization problem to a family of convex problems. In the paper the properties of the GOCs are investigated. The effectiveness of the GOCs is demonstrated by examples.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>Consider the following problem:
(P) :</p>
      <p>f0(x) := g0(x) − h0(x) ↓ mxin; x ∈ S; 
fi(x) := gi(x) − hi(x) ≤ 0; i ∈ I = {1; : : : ; m};
fi(x) := gi(x) − hi(x) = 0; i ∈ E = {m + 1; : : : ; l}; </p>
      <p>V(P) := inf(f0; F ) := inxf{f0(x) | x ∈ F )} &gt; −∞:</p>
      <p>Exact Penalty
Introduce the penalty function W (·) for Problem (P) as follows</p>
      <p>W (x) := max{0; f1(x); : : : ; fm(x)} + ∑ |fj(x)| :</p>
      <p>Further, along with Problem (P), consider the penalized problem without the inequality and equality
constraints:
(P ) :
(x) , f0(x) +</p>
      <p>W (x) ↓ mxin; x ∈ S;
where ≥ 0 is a penalty parameter.</p>
      <p>As well-known, if z ∈ Sol(P ), and z is feasible in (P), i.e. z ∈ F , then z turns out to be a global solution
to (P): z ∈ Sol(P) [Nocedal et al., 2006, Bonnans et al., 2006, Izmailov et al., 2014, Hiriart-Urruty et al., 1993,
Clarke, 1983, Burke, 1991]. On the other hand, the inverse implementation does not, in general, hold.</p>
      <p>
        Hence, the crucial moment of the exact penalization (EP) theory is the existence of a threshold value ∗ ≥ 0
of the penalty parameter ≥ 0 for which Sol(P ) ⊂ Sol(P) ∀ ≥ ∗: In other words, for ≥ ∗ Problems
(P) and (P ) turn out to be equivalent in the sense that Sol(P) = Sol(P )
        <xref ref-type="bibr" rid="ref12 ref13">(see Chapt. VII, Lemma 1.2.1
in [Hiriart-Urruty et al., 1993])</xref>
        .
      </p>
      <p>On the other hand, the existence of the threshold exact penalty parameter ∗ ≥ 0 allows us to solve a
single unconstrained problem instead of a sequence of unconstrained problems with k → ∞ [Byrd et al., 2012,
Di Pillo et al., 2012, Di Pillo et al., 2015].</p>
      <p>
        Recall that under various constraint qualification (CQ) conditions
        <xref ref-type="bibr" rid="ref14 ref15 ref16 ref18 ref2 ref7">(MFCQ, etc. [Robinson, 1976, Burke, 1991,
Zaslavski, 2013, Kruger, 2015, Kruger et al., 2014])</xref>
        , the error bound properties [Nocedal et al., 2006,
Bonnans et al., 2006, Izmailov et al., 2014, Robinson, 1976, Burke, 1991, Han et al., 1979, Kruger, 2015,
Kruger et al., 2014], the metric sub-regularity conditions, calmness of constraints systems can help to prove
the existence of the exact penalty threshold ∗ ≥ 0 even for a global solution [Clarke, 1983, Burke, 1991,
Cococcioni et al., 2017, Zaslavski, 2013, Di Pillo et al., 2012, Di Pillo et al., 2015].
      </p>
      <p>Assume that some regularity condition is fulfilled that ensures the existence of such threshold value ∗ ≥ 0 of
penalty parameter.
3</p>
      <p>Global Optimality Conditions (GOC)
Before all, we will prove that the cost function
as a difference of convex functions. Indeed, since</p>
      <p>(·) of Problem (P ) is a d.c. function, i.e. it can be represented
|fi(x)| = max{gi(x) − hi(x); hi(x) − gi(x)} ± [gi(x) + hi(x)] = 2 max{gi(x); hi(x)} − [gi(x) + hi(x)];
it can be readily seen that
where
(x) =△ f0(x) +
max{0; fi(x); i ∈ I} +
∑ |fi(x)| = G (x) − H (x);
i∈E
H (x) := h0(x) +
[∑ hi(x) + ∑(gj(x) + hj(x))];
i∈I
j∈E
G (x) :=
(x) + H (x) = g0(x) +
max{∑ hj(x); [gj(x) + ∑j̸=i hj(x)]; i ∈ I}+
j∈I
j∈I
(1)
(2)
(3)
(4)
∑ max{gi(x); hi(x)}: (5)
i∈E
Obviously, G (·) and H (·) are both convex functions [Hiriart-Urruty et al., 1993, Rockafellar et al., 1998,
Rockafellar, 1970], so that the function (·) is a d.c. function, as claimed. Besides, it is clear, that for a
feasible (in (P)) point z ∈ S we have</p>
      <p>W (z) =△ max{0; f1(z); : : : ; fm(z)} + ∑ |fi(z)| = 0;</p>
      <p>i∈E
and therefore, for := f0(z), we obtain
Theorem 3.1. Let a point z ∈ F be a solution to Problem (P) and
value of penalty parameter.</p>
      <p>Then, for every pair (y; ) ∈ IRn × IR such that
the following inequality holds
0 &gt; G (u) −</p>
      <p>− ⟨∇H (y); u − y⟩;
Then, using the equation (7) and the convexity of the function H (·), we derive
0 &gt; G (u) −
− H (u) + H (y) =
(u) −
=
(u) −
(z);
or, (z) &gt; (u); z ∈ F ; u ∈ S: Hence, the point z can not be a solution to (P ).</p>
      <p>Moreover, if z and u are feasible in (P), z; u ∈ F , and since W (u) = 0, we obtain f0(z) = (z) &gt; (u) =
f0(u): It means that z ∈= Sol(P) and u ∈ F is a vector better than z ∈ F .</p>
      <p>Hence, the conditions (7)–(8) of Theorem 3.1 possess the classical constructive (algorithmic) property (once
the conditions are violated, one can find a feasible vector which is better than the point under investigation).</p>
      <p>Let us demonstrate the effectiveness of this property by an example.</p>
      <p>
        Example 3.1. Consider the problem
        <xref ref-type="bibr" rid="ref1 ref17">([Nocedal et al., 2006, Example 12.20])</xref>
        f0(x) = 4x1x2 ↓ min;
      </p>
      <p>x
f1(x) = x21 + x2 − 1 = 0:
2
x ∈ IR2; }
Remark 3.1. It is not difficult to note that Theorem 3.1 reduces the solution of the nonconvex Problem (P )
to an investigation of the family of the convex (linearized) problems
(P L(y)) :
Φ y(x) := G (x) − ⟨∇H (y); x⟩ ↓ min;
x
x ∈ S;
depending on the pairs (y; ) ∈ IRn+1 which fulfill the equation (7) (or, what is the same),
(P L(y)) :
Φ y(x) := G (x) − ⟨∇h0(y) +</p>
      <p>∇hi(y) +
[∑
i∈I
j∈E
∑(∇gj (y) + ∇hj (y))]; x⟩ ↓ min;
x
x ∈ S:
(9′)</p>
      <p>It is worth noting that the linearization is carried out with respect to the “unified” nonconvexity of Problem
(P) accumulated by the function H (·) (see (P)–(1) and (4)) that includes all the functions hi(·); i ∈ {0} ∪
I ∪ E ; gj (·); j ∈ E , which generate all nonconvexity in Problems (P) and (P ) (according to the representations
(3)–(5)).</p>
      <p>Hence, the verification of the principal inequality (8) can be performed by solving the linearized problems
(P L(y)) and varying the parameters (y; ) satisfying (7). Besides, we have to verify (8), which can be rewritten
as follows</p>
      <p>V(P L(y)) ≥</p>
      <p>− ⟨∇H (y); y⟩ =: N (y; );
where V(P L(y)) is the optimal value of the linearized problem (P L(y))
Remark 3.2. Suppose, we found a triple (y; ; u), (y; ) ∈ IRn × IR;
principal inequality (8) is violated, i.e.</p>
      <p>H (y) =
− , u ∈ S, such that the
(6)
(7)
(8)
(9)
(8′)
(10)
It is easy to see that the point z = (√22 ; √22 )⊤,
equation ∇f0(z) + 1∇f1(z) = 0 ∈ IR2 with 1 = −2. However, it is not clear whether the point z is a global
solution. In order to decide on it, let us apply Theorem 3.1.</p>
      <p>:= f0(z) = 2, is feasible: f1(z) = 0 and satisfies the
KKTg0(x) = (x1 + x2)2;
h0(x) = (x1 − x2)2;
g1(x) = x22 + x22;
h1(x) ≡ 1:</p>
    </sec>
    <sec id="sec-2">
      <title>Besides, let set</title>
      <p>:= 3 &gt; | 1| = 2. Then, according to (4) and (5), we have</p>
      <p>H (x) = h0(x) + [g1(x) + h1(x)] = (x1 − x2)2 + 3(x21 + x22 + 1);
G (x) = g0(x) + 2 max{g1(x); h1(x)} = (x1 + x2)2 + 6 max{x12 + x22; 1}:
}
Let choose, now, y = (−1; 0:5)⊤ which is unfeasible in the problem (10). Then we have</p>
      <p>H (y) = (y1 − y2)2 + 3(y12 + y22 + 1) = 9
and, as a consequence, we derive = H (y) + = 9 + 2 = 11. Furthermore, let choose a feasible point
u = (−0:6; 0:8)⊤, u21 + u22 = 1, and compute G (u) (see (12))</p>
      <p>G (u) = (u1 + u2)2 + 6 max{u12 + u22; 1} = (0:2)2 + 6 = 6:04:
Besides, it is not difficult to compute that u − y = (−0:6; 0:8)⊤ − (−1; 0:5)⊤ = (0:4; 0:3)⊤,
∇H (y) = 2(y1 − y2; y2 − y1)⊤ + 6(y1; y2)⊤ = 2(4y1 − y2; 4y2 − y1)⊤ = (−9; 6)⊤:</p>
    </sec>
    <sec id="sec-3">
      <title>Whence we immediately derive that</title>
      <p>⟨∇H (y); u − y⟩ = ⟨(−9; 6)⊤; (0:4; 0:3)⊤⟩ = −3:6 + 1:8 = −1:8;</p>
      <p>+ ⟨∇H (y); u − y⟩ = 11 − 1:8 = 9:2 &gt; 6:04 = G (u):
The latter inequality means that in Problem (10) the principal inequality (8) of Theorem 3.1 is violated.</p>
      <p>Hence, the point z = (√22 ; √22 )⊤ is not a global solution to the problem (10) in virtue of Theorem 3.1.
Indeed, it is confirmed by the inequality f0(u) = −0:48 &lt;
= f0(z) = 2.</p>
      <p>Let consider now possible relations between the conditions (7)–(8) of Theorem 3.1 and the classical optimality
conditions, in particular, the KKT theorem for Problem (P). For this purpose, suppose that a feasible (in
Problem (P)) point z satisfies the conditions (7)–(8) of Theorem 3.1.</p>
      <p>First, let set in (7)–(8) y = z. Then we immediately derive that := H (z) + = G (z).
Therefore, from (8) it follows the validity of the inequality</p>
      <p>G (x) − G (z) ≥ ⟨∇H (z); x − z⟩ ∀x ∈ S:
It implies that the point z (satisfying (7)–(8)) is a solution to the linearized convex problem as follows
(P L(z)) :</p>
      <p>G (x) − ⟨∇H (z); x⟩ ↓ min;
x
Since (P L(z)) is a convex problem, then the following inclusion is, as well-known, the necessary and sufficient
optimality condition for z being a solution to (P L(z)):
When S = IRn, the inclusion (13) implies
which is the necessary optimality condition for Problem (P ) with S = IRn [Hiriart-Urruty, 1985,
Strekalovsky, 2003]. Thus, the conditions (7)–(8) of Theorem 3.1 entail the well-known optimality
conditions (13) and (13′) [Nocedal et al., 2006, Bonnans et al., 2006, Izmailov et al., 2014, Floudas et al., 2004,
Strekalovsky, 2013, Strekalovsky, 2014, Strekalovsky, 2017, Strekalovskiy, 2003] for Problem (P ).</p>
      <p>Nevertheless, the natural question arises on whether it is possible to find a triple (y; ; u) ∈ IR2n+1, satisfying
(7) and which violates the inequality (8).
(11)
(12)
(13)
(13′)
Theorem 3.2. Assume, that a feasible in Problem (P) point z is not an "-solution to (P), i.e.
In addition, let a vector v ∈ IRn satisfy the following inequality
Then, for any penalty parameter
conditions take place
&gt; 0 one can nd a tuple (y; ; u), (y; ) ∈ IRn+1, u ∈ F , the following
inf(f0; F ) + " = V(P) + " &lt; := f0(z):
(H) :
f0(v) &gt;</p>
      <p>− ":
(a) H (y) =
(b) G (y) ≤ ;
(c) G (u) −
− + ";
&lt; ⟨∇H (y); u − y⟩: 


(14)
(15)
(16)
(17)
(18)
(19)
(20′)</p>
      <p>Now let us demonstrate the effectiveness of the GOCs of Theorems 3.1 and 3.2 on another example.</p>
    </sec>
    <sec id="sec-4">
      <title>Example 3.2. Consider the problem</title>
      <p>f0(x) = x21 − 2x22 + x23 ↓ min; x ∈ IR3;</p>
      <p>2 x
f1(x) = x23 − x1 − x22 = 0; f2(x) = 4x1x3 = 0;
It can be readily seen that the point z = (0; 0; 0)⊤; := f0(z) = 0 is a degenerate KKT point in the problem
(17), since f1(z) = f2(z) = 0; ∇f0(z) = ∇f1(z) = ∇f2(z) = (0; 0; 0)⊤. However, it is not clear whether the
KKT vector z is a global solution to (17) or not. Therefore, let us apply Theorems 3.1 and 3.2 to clarify the
situation.</p>
      <p>It is easy to see that in the problem (17) we have g0(x) = x21 + x2; h0(x) = 2x22; g1(x) = x2; h1(x) =
gx221(x+) x=22.(x1In+axd3d)2it;iohn,2(uxs)in=g(xth1e−dx.c3.)2:representation f2(x) = 4x1x3 3= (x1 + x3)2 − (x1 − x3)2; 3we obtain</p>
      <p>For simplicity of presentation, we will apply the denotation S = [−2; 1] for bounding the variable x2 ∈ IR, but
in the investigation of the linearized problems we use two inequality constraints x2 ≤ 1; x2 + 2 ≥ 0:
Hence, according to (3)–(5) we have
Let us set := 1; y = ( 16 ; 1; 76 )⊤ ∈= F . Then we obtain</p>
      <p>H (x) = h0(x) + ∑[gj(x) + hj(x)] =</p>
      <p>j∈E
= 2x22 + [(x23 + x21 + x22) + (x1 + x3)2 + (x1 − x3)2] = 2x22 + [3x21 + 3x23 + x22];</p>
      <p>G (x) = g0(x) + 2 ∑max{gj(x); hj(x)} =</p>
      <p>j∈E
= x21 + x23 + 2 [max{x23; x21 + x22} + max{(x1 + x3)2; (x1 − x3)2}]:</p>
      <p>∇H (x) = (0; 4x2; 0)⊤ + (6x1; 2x2; 6x3)⊤ = 6(x1; x2; x3)⊤;
besides, ∇H (y) = (1; 6; 7)⊤:</p>
      <p>In order to find a suitable point in u ∈ F , consider the linearized problem as follows
(P L(y)) :</p>
      <p>G (x) − ⟨∇H (y); x⟩ = x12 + x32 + 2 max{x32; x12 + x22}+
+ 2 max{(x1 + x3)2; (x1 − x3)2} − ⟨(1; 6; 7)⊤; x⟩ ↓ mxin; x ∈ IR3;
−2 ≤ x2 ≤ 1: (20)
It is not difficult to see that the problem (20) amounts to the following one [Hiriart-Urruty, 1998]
x21 + x23 + 2 1 + 2 2 − x1 − 6x2 − 7x3 ↓ (mx;in);
x32 ≤ 1; x21 + x22 ≤ 1;</p>
      <p>= ( 1; 2) ∈ IR2; (x1 + x3)2 ≤ 2; (x1 − x3)2 ≤ 2;
x2 ≤ 1; x2 + 2 ≥ 0; x ∈ IR3:




</p>
      <p>Besides, as above, it can be readily seen that the Slater condition holds in (20′). Furthermore, the solution
vector (u; ∗) ∈ IR5 satisfies the complementarity conditions as follows
1(x32 − 1) = 0 = 2(x12 + x22 − 1); 3[(x1 + x3)2 − 2] = 0 = 4[(x1 − x3)2 − 2]; }</p>
      <p>1(x2 − 1) = 0 = 2(x2 + 2):
and, besides, we have for ∗ = ( ∗1; ∗2)⊤
∗1 = max{ u32; u12 + u22 };</p>
      <p>∗2 = max{ (u1 + u3)2; (u1 − u3)2 }:
In addition, since the Lagrange function for the problem (20′) has thee following form
(21)
(22)
(24)
(25)
(25′)</p>
      <p>L(x; ; 1; 2; 3; 4; 1; 2) = x21 + x23 + 2 1 + 2 2 − x1 − 6x2 − 7x3+
+ 1(x32 − 1) + 2(x12 + x2 − 1) + 3[(x1 + x3)2 − 2] + 4[(x1 − x3)2 − 2] + 1(x2 − 1) − 2(x2 + 2); (23)
2
(an, besides, ( 1; 2; 3; 4; 1; 2)
tions [Rockafellar, 1993]
∈</p>
      <p>IR+6), then the</p>
      <p>KKT system</p>
      <p>contains the following
equa</p>
      <p>It can be readily seen that the point u = (0; 1; 1)⊤ satisfies the KKT conditions (21),(24),(25) with
∗ = ( ∗1; ∗2)⊤ = (1; 1)⊤ (see (22)). Indeed, the equation (25) with u = (0; 1; 1)⊤ take the form
(a)
(b)
(c)
2 3 − 1 − 2 4 = 0; or
2 2 − 6 + 1 − 2 = 0;
2 − 7 + 2 1 + 2 3 + 2 4 = 0:
3 − 4 = 21 ; 


Then, from (25′) (a) we derive 3 = 54 , 4 = 34 . Further, from (25′) (c) with the help of (24) it follows that
2 1 = 5 − 2( 3 + 4) = 1, i.e. 1 = 12 , 2 = 23 .</p>
      <p>On the other hand, thanks to (21) we see that 2 = 2(u) = 0.Then (25′) (b) provides that 1 = 3. Hence,
the point u = (0; 0; 1)T really is a KKT point in (20′), and, due to convexity of problem (20′), u is also a solution
to (20) ((u; ∗)T is a solution to (20′)).</p>
      <p>Now let us verify whether the principal inequality (8) of Theorem 3.1 holds with (y; ; u) where
( 1 7 ) 1
= H (y) + ; = f0(z) = 0. First compute H (y) with y = ; 1; : H (y) = 3(y12 + y22 + y32) = 7 .
6 6 6
1</p>
      <p>Thus, = H (y) = 7 6 . Furthermore, + ⟨∇H(y); (u − y)⟩ = 5 56 . On the other hand, it can be readily
computed, that G (u) = u21 + u23 + 2 ∗1 + 2 ∗2 = 5.</p>
      <p>5
Therefore, we have G (u) = 5 &lt; 5 6 = + ⟨∇H(y); u − y⟩.</p>
      <p>Hence, the principal inequality (8) of Theorem 3.1 is violated, and, as a consequence, the degenerate KKT
point z = (0; 0; 0)T is not a global solution to the problem (17).
( 1 7 )T
Moreover, by solving the linearized problem (PL(y)) with y = ; 1; , we constructed the feasible in (17)
6 6
point u = (0; 1; 1)T , which is better than z, since f0(u) = −1 &lt; 0 = f0(z) = 0.</p>
      <p>Furthermore, it can be readily seen, as above, that the point u = (0; 1; 1)T is also a KKT point in the original
problem (17), but not a global solution to (17). Moreover we can show this fact, by repeating the same procedure
of finding another pair (y1; 1), such that H (y1) = 1 − 1, where 1 := f0(u) = f0(z1); z1 := u; and by solving
the linearized problem (PL1) := (PL(y1)), which provides the point u1 such that</p>
      <p>So, by the procedure described above we give a hint how may be constructed one of the simplest global search
procedures which is able to escape stationary points and local solutions in non-convex Problem (P).
4</p>
      <p>Sufficient Optimality Conditions
Now we turn to the question on when the conditions (7)–(8) of Theorem 3.1 become sufficient for a feasible point
being a global solution to nonconvex Problem (P).</p>
      <p>Theorem 4.1. Suppose that for a feasible in Problem (P) point z, := f0(z), the condition (H){(15) is ful lled.
In addition, let some penalty parameter &gt; 0 be given. Finally, assume that for every pair (y; ) ∈ IRn × IR,
satisfying the relation
(a)
Acknowledgements
Then, the point z ∈ F turns out to be an "-global solution to Problem (P ) as well as to Problem (P).
This work was supported by the Russian Science Foundation (Project No. 15-11-20015).</p>
    </sec>
  </body>
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