Hindawi Publishing Corporation
Mathematical Problems in Engineering
Volume 2014, Article ID 894248, 5 pages
http://dx.doi.org/10.1155/2014/894248
Research Article
Stochastic Methods Based on VU-Decomposition Methods for
Stochastic Convex Minimax Problems
Yuan Lu,1 Wei Wang,2 Shuang Chen,3 and Ming Huang3
1
Normal College, Shenyang University, Shenyang 110044, China
School of Mathematics, Liaoning Normal University, Dalian 116029, China
3
School of Mathematical Sciences, Dalian University of Technology, Dalian 116024, China
2
Correspondence should be addressed to Wei Wang; wei 0713@sina.com
Received 6 August 2014; Revised 29 November 2014; Accepted 29 November 2014; Published 4 December 2014
Academic Editor: Hamid R. Karimi
Copyright © 2014 Yuan Lu et al. This is an open access article distributed under the Creative Commons Attribution License, which
permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
This paper applies sample average approximation (SAA) method based on VU-space decomposition theory to solve stochastic
convex minimax problems. Under some moderate conditions, the SAA solution converges to its true counterpart with probability
approaching one and convergence is exponentially fast with the increase of sample size. Based on the VU-theory, a superlinear
convergent VU-algorithm frame is designed to solve the SAA problem.
1. Introduction
In this paper, the following stochastic convex minimax problem (SCMP) is considered:
minπ π (π₯) ,
(1)
π (π₯) = max {πΈ [ππ (π₯, π)] : π = 0, . . . , π} ,
(2)
π₯βπ
where
and the functions ππ (π₯, π) : π
π β π
, π = 0, . . . , π, are convex
and πΆ2 , π : Ξ© β Ξ β π
π is a random vector defined
on probability space (Ξ©, Ξ₯, π); πΈ denotes the mathematical
expectation with respect to the distribution of π.
SCMP is a natural extension of deterministic convex
minimax problems (CMP for short). The CMP has a number
of important applications in operations research, engineering
problems, and economic problems. While many practical
problems only involve deterministic data, there are some
important instances where problems data contains some
uncertainties and consequently SCMP models are proposed
to reflect the uncertainties.
A blanket assumption is made that, for every π₯ β π
π ,
πΈ[ππ (π₯, π)], π = 0, . . . , π, are well defined. Let π1 , . . . , ππ be a
sampling of π. A well-known approach based on the sampling
is the so-called SAA method, that is, using sample average
value of ππ (π₯, π) to approximate its expected value because the
classical law of large number for random functions ensures
that the sample average value of ππ (π₯, π) converges with
probability 1 to πΈ[ππ (π₯, π)] when the sampling is independent
and identically distributed (idd for short). Specifically, we can
write down the SAA of our SCMP (1) as follows:
minπ πΜπ (π₯) ,
π₯βπ
(3)
where
πΜπ (π₯) = max {πΜππ (π₯) : π = 0, . . . , π} ,
1 π
πΜππ (π₯) := β ππ (π₯, ππ ) .
π π=1
(4)
The problem (3) is called the SAA problem and (1) the true
problem.
The SAA method has been a hot topic of research in
stochastic optimization. Pagnoncelli et al. [1] present the SAA
method for chance constrained programming. Shapiro et al.
[2] consider the stochastic generalized equation by using
the SAA method. Xu [3] raises the SAA method for a class
of stochastic variational inequality problems. Liu et al. [4]
2
Mathematical Problems in Engineering
give the penalized SAA methods for stochastic mathematical
programs with complementarity constraints. Chen et al. [5]
discuss the SAA methods based on Newton method to
the stochastic variational inequality problem with constraint
conditions. Since the objective functions of the SAA problems
in the references talking above are smooth, then they can be
solved by using Newton method.
More recently, new conceptual schemes have been developed, which are based on the VU-theory introduced in
[6]; see else [7β11]. The idea is to decompose π
π into two
orthogonal subspaces V and U at a point π₯, where the
nonsmoothness of π is concentrated essentially on V and the
smoothness of π appears on the U subspace. More precisely,
for a given π β ππ(π₯), where ππ(π₯) denotes the subdifferential
of π at π₯ in the sense of convex analysis, then π
π can be
decomposed into direct sum of two orthogonal subspaces,
that is, π
π = U β V, where V = lin(ππ(π₯) β π), and U = Vβ₯ .
As a result an algorithm frame can be designed for the SAA
problem that makes a step in the V space, followed by a UNewton step in order to obtain superlinear convergence. A
VU-space decomposition method for solving a constrained
nonsmooth convex program is presented in [12]. A decomposition algorithm based on proximal bundle-type method with
inexact data is presented for minimizing an unconstrained
nonsmooth convex function in [13].
In this paper, the objective function in (1) is nonsmooth,
but it has the structure which has the connection with VUspace decomposition. Based on the VU-theory, a superlinear
convergent VU-algorithm frame is designed to solve the
SAA problem. The rest of the paper is organized as follows. In
the next section, the SCMP is transformed to the nonsmooth
problem and the proof of the approximation solution set
converges to the true solution set in the sense that Hausdorff
distance is obtained. In Section 3, the VU-theory of the SAA
problem is given. In the final section, the VU-decomposition
algorithm frame of the SAA problem is designed.
(d) The moment-generating function ππ
(π‘) = πΈ[ππ‘π
(π) ] of
π
(π) is finite-valued for all π‘ in a neighborhood of zero, where
ππ (π‘) = πΈ[ππ‘(π(π ,π)βπΊ(π )) ] is the moment-generating function
of the random variable π(π , π) β πΊ(π ).
2. Convergence Analysis of SAA Problem
This shows that π(π₯Μπ, πβ ) < π, which implies π·(π₯Μπ, π β ) <
π.
In this section, we discuss the convergence of (3) to (1) as π
increases. Specifically, we investigate the fact that the solution
of the SAA problem (3) converges to its true counterpart as
π β β. Firstly, we make the basic assumptions for SAA
method. In the following, we give the basic assumptions for
SAA method.
Assumption 1. (a) Letting π be a set, for π = 1, . . . , π, the limits
ππΉπ (π‘) := lim ππΉππ (π‘)
πββ
(5)
exist for every π₯ β π.
(b) For every π β π, the moment-generating function
ππ (π‘) is finite-valued for all π‘ in a neighborhood of zero.
(c) There exists a measurable function π
: Ξ© β π
+ such
that
σ΅©
σ΅¨
σ΅©
σ΅¨σ΅¨
σ΅¨σ΅¨π (π σΈ , π) β π (π , π)σ΅¨σ΅¨σ΅¨ β€ π
(π) σ΅©σ΅©σ΅©π σΈ β π σ΅©σ΅©σ΅©
(6)
σ΅©
σ΅¨
σ΅©
σ΅¨
for all π β Ξ© and all π σΈ , π β π.
Theorem 2. Let πβ and ππ denote the solution sets of (1) and
(3). Assuming that both πβ and ππ are nonempty, then, for
any π > 0, one has π·(ππ, πβ ) < π, where π·(ππ, πβ ) =
supπ₯βππ π(π₯, πβ ).
Proof. For any points π₯Μ β ππ and π₯ β π
π , we have
Μ = max {πΜππ (π₯)
Μ , π = 0, . . . , π}
πΜπ (π₯)
}
{1 π
Μ ππ ) , π = 0, . . . , π}
= max { β ππ (π₯,
π
}
{ π=1
(7)
}
{1 π
β€ max { β ππ (π₯, ππ ) , π = 0, . . . , π} .
π
}
{ π=1
From Assumption 1, we know that, for any π > 0, there exist
π; if π > π, π = 0, . . . , π, then
σ΅¨σ΅¨
σ΅¨σ΅¨ π
σ΅¨
σ΅¨σ΅¨ 1
σ΅¨σ΅¨ βπ (π₯, ππ ) β πΈ [π (π₯, ππ )]σ΅¨σ΅¨σ΅¨ < π.
σ΅¨σ΅¨
σ΅¨σ΅¨
π
π
σ΅¨σ΅¨
σ΅¨σ΅¨ π π=1
σ΅¨
σ΅¨
(8)
By letting π > π, we obtain
}
{1 π
Μ β€ max { βππ (π₯, ππ ) , π = 0, . . . , π}
πΜπ (π₯)
π
}
{ π=1
β€ max {πΈ [ππ (π₯, ππ )] + π, π = 0, . . . , π}
(9)
= π (π₯) + π.
We now move on to discuss the exponential rate of
convergence of SAA problem (3) to the true problem (1) as
sample increases.
Theorem 3. Let π₯π be a solution to the SAA problem (3)
and πβ is the solution set of the true problem (1). Suppose
Assumption 1 holds. Then, for every π > 0, there exist positive
constants π(π) and π(π), such that
Prob {π (π₯π, πβ ) β₯ π} β€ π (π) expβππ(π)
(10)
for π sufficiently large.
Proof. Let π > 0 be any small positive number. By Theorem 2
and
σ΅¨σ΅¨σ΅¨ π
σ΅¨σ΅¨σ΅¨
σ΅¨σ΅¨ 1
σ΅¨
σ΅¨σ΅¨ βππ (π₯, ππ ) β πΈ [ππ (π₯, ππ )]σ΅¨σ΅¨σ΅¨ < π,
(11)
σ΅¨σ΅¨ π
σ΅¨σ΅¨
σ΅¨σ΅¨ π=1
σ΅¨σ΅¨
Mathematical Problems in Engineering
3
we have π(π₯π, π) < π. Therefore, by Assumption 1, we have
Prob {π (π₯π, πβ ) β₯ π}
σ΅¨σ΅¨
σ΅¨
σ΅¨
}
{σ΅¨σ΅¨σ΅¨σ΅¨ 1 π
π
π σ΅¨σ΅¨
β€ Prob {σ΅¨σ΅¨σ΅¨ β ππ (π₯, π ) β πΈ [ππ (π₯, π )]σ΅¨σ΅¨σ΅¨ β₯ πΏ}
σ΅¨σ΅¨
σ΅¨π
σ΅¨
}
{σ΅¨σ΅¨ π=1
Theorem 5. Suppose Assumption 4 holds. Then π
π can be
decomposition at π₯ : π
π = U β V, where
,
V = lin {βπΜππ (π₯) β βπΜ0π (π₯)}0=πβπΌ(π₯)
ΜΈ
(12)
β€ π (π) expβππ(π) .
The proof is complete.
3. The VU-Theory of the SAA Problem
In the following sections, we give the VU-theory, VUdecomposition algorithm frame, and convergence analysis of
the SAA problem.
The subdifferential of πΜπ at a point π₯ β π
π can be
computed in terms of the gradients of the function that are
active at π₯. More precisely,
ππΜπ (π₯)
β©} = 0.
U = {π β π
π | β¨π, {βπΜππ (π₯) β βπΜ0π (π₯)}0=πβπΌ(π₯)
ΜΈ
(19)
Proof. The proof can be directly obtained by using
Assumption 4 and the definition of the spaces V and
U.
Given a subgradient π β ππΜπ with V-component πV =
π
π π, the U-Lagrangian of πΜπ, depending on πV , is defined
by
π
dim U β π’ σ³¨σ³¨β πΏ π’ (π’; πV )
:= min {πΜπ (π₯ + ππ’ + πV) β β¨πV , Vβ©V } .
Vβπ
dim V
(20)
The associated set of V-space minimizers is defined by
{
πΌ π
= Conv {π β π
π | π = β π ββππ (π₯, ππ ) :
π π=1
πβπΌ(π₯)
{
π (π’; πV )
(13)
}
πΌ = (πΌπ )πβπΌ(π₯) β Ξ |πΌ(π₯)| } ,
}
(14)
is the set of active indices at π₯, and
π
(15)
π=1
Let π₯ β π
π be a solution of (3). By continuity of the structure
functions, there exists a ball π΅π (π₯) β π
π such that
βπ₯ β π΅π (π₯) ,
πΌ (π₯) β πΌ (π₯) .
(16)
For convenience, we assume that the cardinality of πΌ(π₯) is
π1 + 1 (π1 β€ π) and reorder the structure functions, so that
πΌ(π₯) = {0, . . . , π1 }. From now on, we consider that
βπ₯ β π΅π (π₯) ,
πΜπ (π₯) = πΜππ (π₯) ,
π β πΌ (π₯) .
(17)
The following assumption will be used in the rest of this paper.
Assumption 4. The set
{βπΜππ (π₯) β βπΜ0π (π₯)}0=πβπΌ(π₯)
ΜΈ
is linearly independent.
(i) the nonlinear system, with variable V and the parameter
π’,
πΜππ (π₯ + ππ’ + πV) β πΜ0π (π₯ + ππ’ + πV) = 0,
Ξ π = {πΌ β π
π | πΌπ β₯ 0, βπΌπ = 1} .
(21)
Theorem 6. Suppose Assumption 4 holds. Let π(π’) = π₯ + π’ β
V(π’) be a trajectory leading to π₯ and let π» := β2 πΏ π’ (0, 0). Then
for all π’ sufficiently small the following hold:
where
πΌ (π₯) = {π β πΌ | πΜπ (π₯) = πΜππ (π₯)}
:= {V : πΏ π’ (π’; πV ) = πΜπ (π₯ + ππ’ + πV) β β¨πV , Vβ©V } .
(18)
0 =ΜΈ π β πΌ (π₯)
(22)
has a unique solution V = V(π’) and V : π
dim U β
π
dim V is a πΆ2 function;
(ii) π(π’) is a πΆ2 -function with π½π(π’) = π + ππ½V(π’);
(iii) πΏ π’ (π’; 0) = πΜππ(π₯ + π’ β V(π’)) = πΜπ(π₯ + π’ β V(π’)) =
πΜπ(π₯) + (1/2)π’π π»π’ + π(|π’|2 );
π
(iv) βπΏ π’ (π’; 0) = π»π’ + π(|π’|);
(v) πΜπ(π(π’)) = πΜπ(π(π’)), π β πΌ(π₯).
π
Proof. Item (i) follows from the assumption that ππ are πΆ2
and applying a Second-Order Implicit Function Theorem
(see [14], Theorem 2.1). Since V(π’) is πΆ2 , π(π’) is πΆ2 and the
Jacobians π½V(π’) exist and are continuous. Differentiating the
primal track with respect to π’, we obtain the expression of
π½π(π’) and item (ii) follows.
(iii) By the definition of πΏ π’ (π’; πV ) and π(π’; πV ), we have
πΏ π’ (π’; 0) = πΜππ (π₯ + π’ β V (π’)) = πΜπ (π₯ + π’ β V (π’)) . (23)
4
Mathematical Problems in Engineering
According to the second-order expansion of πΏ π’ , we
obtain
πΏ π’ (π’; 0) = πΏ π’ (0; 0)
where
β πΌπ (π’) βπΜπ π (π₯(π) ) = πΜ(π) β ππΜπ (π₯(π) )
π
πβπΌ(π₯)
1
+ β¨βπΏ π’ (0; 0) , π’β© + π’πβ2 πΏ π’ (0; 0) π’ + π (|π’|) .
2
(24)
Since πΏ π’ (0; 0) = πΜππ(π₯), π β πΌ(π₯), βπΏ π’ (0; 0) = 0, and π» =
β πΏ π’ (0; 0),
2
1
πΏ π’ (π’; 0) = πΜππ (π₯) + π’π π»π’ + π (|π’|2 ) .
2
Similar to (iii), we get (iv):
(25)
βπΏ π’ (π’; 0) = βπΏ π’ (0; 0) + β¨π’π β2 πΏ π’ (0; 0) , π’β© + π (|π’|2 )
= π» + π (|π’|) .
(26)
The conclusion of (v) can be obtained in terms of (i) and the
definition of π(π’).
4. Algorithm and Convergence Analysis
Supposing 0 β ππΜπ(π₯), we give an algorithm frame which
can solve (3). This algorithm makes a step in the V-subspace,
followed by a U-Newton step in order to obtain superlinear
convergence rate.
π
(π)
β0 =
is such that π πΜ(π) = 0. Compute π₯(π+1) = π₯Μ(π) + πΏU
(π)
(π)
(π)
π₯ + πΏU β πΏV .
Step 6. Update: set π = π + 1 and return to Step 1.
Theorem 8. Suppose the starting point π₯(0) is close to π₯ enough
Μ
and 0 β riππ(π₯),
β2 πΏ π’ (0; 0) β» 0. Then the iteration points
(π) β
{π₯ }π=1 generated by Algorithm 7 converge and satisfy
σ΅©
σ΅©σ΅© (π+1)
σ΅©
σ΅©
σ΅©σ΅©π₯
β π₯σ΅©σ΅©σ΅©σ΅© = π (σ΅©σ΅©σ΅©σ΅©π₯(π) β π₯σ΅©σ΅©σ΅©σ΅©) .
σ΅©
Step 0. Initialization: given π > 0, choose a starting point π₯(0)
close to π₯ enough and a subgradient πΜ(0) β ππΜπ(π₯(0) ) and set
π = 0.
Step 1. Stop if
σ΅©σ΅© (π) σ΅©σ΅©
σ΅©σ΅©πΜ σ΅©σ΅© β€ π.
σ΅© σ΅©
(27)
σ΅© σ΅©
σ΅©
σ΅©σ΅© (π+1)
σ΅©σ΅©(π₯
β π₯)V σ΅©σ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©σ΅©(π₯(π) β π₯)V σ΅©σ΅©σ΅©σ΅©
σ΅©
σ΅©
σ΅©
σ΅©
σ΅©
= π σ΅©σ΅©σ΅©σ΅©(π₯(π) β π₯)U σ΅©σ΅©σ΅©σ΅© = π σ΅©σ΅©σ΅©σ΅©(π₯(π) β π₯)σ΅©σ΅©σ΅©σ΅© .
Step 3. Construct VU-decomposition at π₯; that is, π
π = V β
U. Compute
π
β2 πΏ π’ (0; 0) = π π (0) π,
(28)
π (0) = β πΌπ β2 πΜππ (π₯) .
(29)
(33)
Since β2 πΏ π’ (0; 0) exists and βπΏ π’ (0; 0) = 0, we have from the
definition of U-Hessian matrix that
π
βπΏ π’ (π’(π) ; 0) = π πΜ(π)
(34)
(π)
By virtue of (30), we have β2 πΏ π’ (0; 0)(π’(π) + πΏU
) = π(βπ’(π) βU ).
2
It follows from the hypothesis β πΏ π’ (0; 0) β» 0 that β2 πΏ π’ (0; 0)
(π)
is invertible and hence βπ’(π) + πΏU
β = π(βπ’(π) βU ). In
consequence, one has
(π₯(π+1) β π₯)U = (π₯(π+1) β π₯(π) )U
+ (π₯(π) β π₯(π) )U + (π₯(π) β π₯)U
Step 2. Find the active index set πΌ(π₯).
(32)
(π)
Proof. Let π’(π) = (π₯(π) β π₯)U and V(π) = (π₯(π) β π₯)V + πΏV
. It
follows from Theorem 6(i) that
σ΅© σ΅©
= 0 + β2 πΏ π’ (0; 0) π’(π) + π (σ΅©σ΅©σ΅©σ΅©π’(π) σ΅©σ΅©σ΅©σ΅©U ) .
Algorithm 7 (algorithm frame).
(31)
σ΅© σ΅©
(π)
= π’(π) + πΏU
= π (σ΅©σ΅©σ΅©σ΅©π’(π) σ΅©σ΅©σ΅©σ΅©U )
(35)
σ΅©
σ΅©
= π (σ΅©σ΅©σ΅©σ΅©π₯(π) β π₯σ΅©σ΅©σ΅©σ΅©) .
The proof is completed by combining (33) and (35).
where
πβπΌ(π₯)
Conflict of Interests
(π)
Step 4. Perform V-step. Compute πΏV
which denotes V(π’) in
(π)
(π)
(π)
(22) and set π₯ = π₯ + 0 β πΏV .
(π)
from the system
Step 5. Perform U-step. Compute πΏU
π
π
π π (0) ππΏU + π πΜ(π) = 0,
(30)
The authors declare that there is no conflict of interests
regarding the publication of this paper.
Acknowledgments
The research is supported by the National Natural Science
Foundation of China under Project nos. 11301347, 11171138,
and 11171049 and General Project of the Education Department of Liaoning Province no. L201242.
Mathematical Problems in Engineering
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Volume 2014
Volume 2014
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International Journal of
Advances in
Combinatorics
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Mathematical Physics
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Volume 2014
Journal of
Complex Analysis
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Volume 2014
International
Journal of
Mathematics and
Mathematical
Sciences
Mathematical Problems
in Engineering
Journal of
Mathematics
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Volume 2014
Hindawi Publishing Corporation
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Volume 2014
Volume 2014
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Volume 2014
Discrete Mathematics
Journal of
Volume 2014
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Discrete Dynamics in
Nature and Society
Journal of
Function Spaces
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Abstract and
Applied Analysis
Volume 2014
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Volume 2014
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Volume 2014
International Journal of
Journal of
Stochastic Analysis
Optimization
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Hindawi Publishing Corporation
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Volume 2014
Volume 2014
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