Startseite Nonlinear Sherman-type inequalities
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Nonlinear Sherman-type inequalities

  • Marek Niezgoda EMAIL logo
Veröffentlicht/Copyright: 21. September 2018

Abstract

An important class of Schur-convex functions is generated by convex functions via the well-known Hardy–Littlewood–Pólya–Karamata inequality. Sherman’s inequality is a natural generalization of the HLPK inequality. It can be viewed as a comparison of two special inner product expressions induced by a convex function of one variable. In the present note, we extend the Sherman inequality from the (bilinear) inner product to a (nonlinear) map of two vectorial variables satisfying the Leon–Proschan condition. Some applications are shown for directional derivatives and gradients of Schur-convex functions.

MSC 2010: 26B25; 26D15; 26D10

1 Introduction

We say that an n-tuple 𝐲 = ( y 1 , , y n ) T n is majorized by an n-tuple 𝐱 = ( x 1 , , x n ) T n , and write 𝐲 𝐱 , if

i = 1 l y [ i ] i = 1 l x [ i ] for  l = 1 , , n ,    and    i = 1 n y i = i = 1 n x i .

Here x [ 1 ] x [ n ] and y [ 1 ] y [ n ] are the entries of 𝐱 and 𝐲 , respectively, arranged in decreasing order [13, p. 8].

It is known that for 𝐱 , 𝐲 n ,

(1.1) 𝐲 𝐱 if and only if 𝐲 conv n 𝐱 ,

where the symbol conv means “the convex hull of”, and n denotes the group of n × n permutation matrices (see [5, p. 16], [6, p. 12] and [7]).

An n × m real matrix 𝐒 = ( s i j ) is called column stochastic (resp. row stochastic) if s i j 0 for i = 1 , , n , j = 1 , , m , and all column sums (resp. row sums) of 𝐒 are equal to 1, i.e., i = 1 n s i j = 1 for j = 1 , , m (resp. j = 1 m s i j = 1 for i = 1 , , n ).

An n × n real matrix 𝐒 = ( s i j ) is said to be doubly stochastic if it is column stochastic and row stochastic [13, pp. 29–30]. The set of all n × n doubly stochastic matrices is denoted by 𝔻 n .

A doubly stochastic matrix is a convex combination of some permutation matrices, and vice versa [13, Theorem A.2.]. That is, 𝔻 n = conv n . Therefore, (1.1) takes the following form: for 𝐱 , 𝐲 n ,

𝐲 𝐱 if and only if 𝐲 = 𝐒𝐱

for some doubly stochastic n × n matrix 𝐒 (see [13, p. 33]).

A function F : J n with an interval J is said to be Schur-convex on J n if for 𝐱 , 𝐲 J n ,

𝐲 𝐱 implies F ( 𝐲 ) F ( 𝐱 ) .

See [13, pp. 79–154] for applications of Schur-convex functions.

Some important examples of Schur-convex functions are included in the following theorem.

Theorem A ([8, 11]).

Let f : J R be a real convex function defined on an interval J R .

Then, for x = ( x 1 , x 2 , , x n ) T J n and y = ( y 1 , y 2 , , y n ) T J n ,

𝐲 𝐱 𝑖𝑚𝑝𝑙𝑖𝑒𝑠 i = 1 n f ( y i ) i = 1 n f ( x i ) .

Throughout, the symbol ( ) T denotes the operation of taking the transpose of a matrix. So, 𝐒 is a column stochastic matrix if and only if 𝐒 T is a row stochastic matrix.

A generalization of Theorem A is the following result (see [17], cf. also [4]).

Theorem B ([17]).

Let f be a real convex function defined on an interval J R . Let a = ( a 1 , , a n ) T R + n , b = ( b 1 , , b m ) T R + m , x = ( x 1 , , x n ) T J n and y = ( y 1 , , y m ) T J m .

If

(1.2) 𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some n × m row stochastic matrix S = ( s i j ) , then

(1.3) j = 1 m b j f ( y j ) i = 1 n a i f ( x i ) .

If f is concave, then inequality (1.3) is reversed.

Statements (1.2) and (1.3) are referred to as Sherman’s condition and Sherman’s inequality, respectively. Consult [1, 2, 3, 4, 9, 10, 14, 15, 16] for generalizations and applications of Theorem B.

Observe that, when m = n , inequality (1.3) can be rewritten as

(1.4) 𝐛 , f ( 𝐲 ) 𝐚 , f ( 𝐱 ) ,

where , is the standard inner product on n , and f ( 𝐱 ) = ( f ( x 1 ) , , f ( x n ) ) T and f ( 𝐲 ) = ( f ( y 1 ) , , f ( y n ) ) T . Further, (1.4) can be restated as

(1.5) Ψ ( 𝐛 , f ( 𝐲 ) ) Ψ ( 𝐚 , f ( 𝐱 ) ) ,

where Ψ is the inner product map on n , i.e.,

Ψ ( 𝐜 , 𝐳 ) = 𝐜 , 𝐳 for  𝐜 , 𝐳 n .

In the next section, we study inequalities of the form (1.5) for an arbitrary (nonlinear) map Ψ of two variables in n .

2 Sherman-type inequality for nonlinear maps

In [12], Leon and Proschan gave some interesting inequalities for the Hadamard product map Ψ ( 𝐱 , 𝐲 ) = 𝐱 𝐲 , where 𝐱 𝐲 = ( x 1 y 1 , , x n y n ) T for 𝐱 = ( x 1 , , x n ) T n and 𝐲 = ( y 1 , , y n ) T n . They applied a finite reflection group G acting on n with the property that for each g G there exist h , k G such that

(2.1) 𝐱 g 𝐲 = k ( ( h 𝐱 ) 𝐲 ) for  𝐱 , 𝐲 n .

Example 2.1.

Let Ψ : n × n n be defined by Ψ ( 𝐱 , 𝐲 ) = 𝐱 𝐲 , the Hadamarad product on n .

If G = n (the permutation group acting on n ), then

𝐱 p 𝐲 = p ( p - 1 𝐱 𝐲 )  for  𝐱 , 𝐲 n  and  p n .

So, (2.1) is met with g = p , h = p - 1 = p T and k = p .

If G = n (the sign changes group acting on n ), then

𝐱 c 𝐲 = ( c 𝐱 ) 𝐲  for  𝐱 , 𝐲 n  and  c n .

Therefore, (2.1) holds with g = c , h = c and k = id .

In what follows, we adapt this idea for any map Ψ of two vectorial variables and for the group G = n of n × n permutation matrices acting on n .

We say that a map Ψ : n × n l admits the Leon–Proschan property for the permutation group n if for each g n there exist h n and k l such that

(2.2) Ψ ( 𝐱 , g 𝐲 ) = k Ψ ( h 𝐱 , 𝐲 ) for  𝐱 , 𝐲 n .

With k = id , statement (2.2) is called the simplified Leon–Proschan property.

Example 2.2.

Take Ψ : n × n l to be given by Ψ ( 𝐱 , 𝐲 ) = Φ ( 𝐱 + 𝐲 ) , where Φ : n l is a permutation-invariant function.

We have

Ψ ( 𝐱 , p 𝐲 ) = Ψ ( p - 1 𝐱 , 𝐲 )  for  𝐱 , 𝐲 n  and  p n .

Therefore, (2.2) holds with g = p , h = p - 1 = p T and k = id .

More generally, let Ψ : n × n l be a permutation-invariant function in the sense

Ψ ( p 𝐱 , p 𝐲 ) = Ψ ( 𝐱 , 𝐲 ) for all  𝐱 , 𝐲 n  and  p n .

Then it follows that

Ψ ( 𝐱 , p 𝐲 ) = Ψ ( p - 1 𝐱 , 𝐲 ) for all  𝐱 , 𝐲 n  and  p n ,

which is the simplified Leon–Proschan property with g = p and h = p - 1 = p T .

Throughout, stands for the componentwise order on l with l .

For a given function f : , we extend f to n by

(2.3) f ( ( x 1 , , x n ) T ) = ( f ( x 1 ) , , f ( x n ) ) T for  x 1 , , x n

In the sequel, for a map Ψ : n × n l , we consider the set

𝒜 Ψ = { 𝐱 n :  for  𝐲 , 𝐳 n  inequality  𝐲 𝐳  implies  Ψ ( 𝐱 , 𝐲 ) Ψ ( 𝐱 , 𝐳 ) } .

In other words,

(2.4) 𝒜 Ψ = { 𝐱 n :  the one-variable map  Ψ ( 𝐱 , )  is nondecreasing on  n } .

For example, if Ψ is the inner product map, then

𝒜 Ψ = { 𝐱 n :  for  𝐲 , 𝐳 n  inequality  𝐲 𝐳  implies  𝐱 , 𝐲 𝐱 , 𝐳 } = + n .

Theorem 2.3.

Let Ψ : R n × R n R l be a map. Let f : R R be a convex function. Assume the following conditions:

  1. The map Ψ admits the simplified Leon–Proschan property, that is, for each g n there exists h n such that

    Ψ ( 𝐱 , g 𝐲 ) = Ψ ( h 𝐱 , 𝐲 ) for  𝐱 , 𝐲 n .

  2. For each 𝐱 n the one-variable map Ψ ( 𝐱 , ) is convex (with respect to ) on n , i.e., for 𝐲 1 , , 𝐲 m n , t 1 , , t m 0 , i = 1 m t i = 1 ,

    Ψ ( 𝐱 , i = 1 m t i 𝐲 i ) i = 1 m t i Ψ ( 𝐱 , 𝐲 i ) .

  3. For each 𝐲 n the one-variable map Ψ ( , 𝐲 ) is concave (with respect to ) on n , i.e., for 𝐱 1 , , 𝐱 m n , t 1 , , t m 0 , i = 1 m t i = 1 ,

    Ψ ( i = 1 m t i 𝐱 i , 𝐲 ) i = 1 m t i Ψ ( 𝐱 i , 𝐲 ) .

Fix any x , y R n and a , b R n with b A Ψ . If

(2.5) 𝐲 = i = 1 m t i g i 𝐱 𝑎𝑛𝑑 𝐚 = i = 1 m t i h i 𝐛

for some g i P n and h i P n such that Ψ ( h i x , y ) = Ψ ( x , g i y ) , i = 1 , , m , then the following Sherman-type inequality holds:

(2.6) Ψ ( 𝐛 , f ( 𝐲 ) ) Ψ ( 𝐚 , f ( 𝐱 ) ) .

Proof.

For any 𝐳 n we get

(2.7) Ψ ( 𝐛 , i = 1 m t i g i 𝐳 ) i = 1 m t i Ψ ( 𝐛 , g i 𝐳 ) = i = 1 m t i Ψ ( h i 𝐛 , 𝐳 ) Ψ ( i = 1 m t i h i 𝐛 , 𝐳 ) = Ψ ( 𝐚 , 𝐳 ) .

In fact, the first inequality is due to (ii). The first equality follows from (i). The second inequality is a consequence of (iii). And the last equality is valid by (2.5).

By setting 𝐳 = f ( 𝐱 ) , from (2.7) we have

(2.8) Ψ ( 𝐛 , i = 1 m t i g i f ( 𝐱 ) ) Ψ ( 𝐚 , f ( 𝐱 ) ) .

Because the extension (2.3) of f is convex on n (with respect to ), we find that

f ( i = 1 m t i g i 𝐱 ) i = 1 m t i f ( g i 𝐱 ) .

Hence, by the monotonicity of Ψ ( 𝐛 , ) on n (with respect to ) (see (2.4)), we obtain

Ψ ( 𝐛 , f ( i = 1 m t i g i 𝐱 ) ) Ψ ( 𝐛 , i = 1 m t i f ( g i 𝐱 ) ) .

It is not hard to check that

f ( g i 𝐱 ) = g i f ( 𝐱 ) , i = 1 , , m .

Therefore, the last inequality becomes

(2.9) Ψ ( 𝐛 , f ( i = 1 m t i g i 𝐱 ) ) Ψ ( 𝐛 , i = 1 m t i g i f ( 𝐱 ) ) .

Finally, by combining (2.5), (2.8) and (2.9) we derive a Sherman-type inequality as follows:

Ψ ( 𝐛 , f ( 𝐲 ) ) = Ψ ( 𝐛 , f ( i = 1 m t i g i 𝐱 ) ) Ψ ( 𝐛 , i = 1 m t i g i f ( 𝐱 ) ) Ψ ( 𝐚 , f ( 𝐱 ) ) .

This completes the proof. ∎

By 𝕄 n we denote the space of all n × n real matrices. Clearly, n 𝔻 n 𝕄 n .

Corollary 2.4.

Let f : R R be a convex function and let Ψ : R n × R n R l be a map satisfying assumptions (ii) and (iii) of Theorem 2.3. Additionally, let θ : M n M n be a linear map such that

  1. for each g n ,

    (2.10) Ψ ( 𝐱 , g 𝐲 ) = Ψ ( θ ( g ) 𝐱 , 𝐲 ) for  𝐱 , 𝐲 n .

Fix any x , y R n and a , b R n with b A Ψ . If

(2.11) 𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = θ ( 𝐒 ) 𝐛

for some S D n , then inequality (2.6) holds.

Proof.

Since 𝐒 conv n , we obtain that 𝐒 = i = 1 m t i g i for some g 1 , , g m n and t 1 , , t m 0 with t 1 + + t m = 1 . Then (2.11) implies (2.5). So, it is enough to apply Theorem 2.3. ∎

Corollary 2.5.

Let f : R R be a convex function and let Ψ : R n × R n R l be a map satisfying assumptions (ii) and (iii) of Theorem 2.3. Additionally, assume that

  1. a map Ψ is permutation-invariant in the sense that for each g n

    Ψ ( g 𝐱 , g 𝐲 ) = Ψ ( 𝐱 , 𝐲 ) for  𝐱 , 𝐲 n .

Fix any x , y R n and a , b R n with b A Ψ . If

(2.12) 𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some S D n , then inequality (2.6) holds.

Proof.

It follows from (i’) that

Ψ ( 𝐱 , g 𝐲 ) = Ψ ( g - 1 𝐱 , 𝐲 ) for  𝐱 , 𝐲 n  and  g n .

However, for g n one has g - 1 = g T . So, (2.10) is met with θ ( g ) = g - 1 = g T for g n . Therefore, the usage of Corollary 2.4 with θ = ( ) T leads us to (2.6) via (2.11) and (2.12), as desired. ∎

3 Sherman-type inequalities induced by directional derivative of a Schur-convex function

We remind that for a function ψ : n the directional derivative 𝐲 ψ ( 𝐱 ) of ψ at the point 𝐱 in the direction 𝐲 is given by

𝐲 ψ ( 𝐱 ) = lim t 0 ψ ( 𝐱 + t 𝐲 ) - ψ ( 𝐱 ) t

(provided the limit there exists).

It is readily seen that if ψ is permutation-invariant, i.e., ψ ( p 𝐱 ) = ψ ( 𝐱 ) for 𝐱 n and p n , then

(3.1) p 𝐲 ψ ( p 𝐱 ) = 𝐲 ψ ( 𝐱 ) for  𝐱 , 𝐲 n  and  p n .

Thus the directional derivative of ψ is a permutation-invariant map.

By taking Ψ ( 𝐱 , 𝐲 ) = 𝐲 ψ ( 𝐱 ) with 𝐱 , 𝐲 n , we find that

𝒜 Ψ = { 𝐱 n :  the one-variable map  Ψ ( 𝐱 , ) = ψ ( 𝐱 )  is nondecreasing on  n } .

Theorem 3.1.

Let ψ : R n R be a Schur-convex function. Assume that for any x , y R n there exists the directional derivative y ψ ( x ) of ψ at the point x in the direction y . Let f : R R be convex. Assume that assumptions (ii) and (iii) of Theorem 2.3 are satisfied for Ψ ( x , y ) = y ψ ( x ) with x , y R n .

Fix any x , y R n and a , b R n with b A Ψ . If

(3.2) 𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some S D n , then the following Sherman-type inequality holds:

(3.3) f ( 𝐲 ) ψ ( 𝐛 ) f ( 𝐱 ) ψ ( 𝐚 ) .

Proof.

Since ψ is Schur-convex, it is permutation-invariant. By virtue of (3.1), the directional derivative of ψ is permutation-invariant. That is, Corollary 2.5 (i’) is fulfilled with Ψ ( 𝐱 , 𝐲 ) = 𝐲 ψ ( 𝐱 ) for 𝐱 , 𝐲 n . Simultaneously, (3.2) gives (2.12) which implies (2.6). Thus we get (3.3), completing the proof. ∎

We now consider Theorem 3.1 in the context of ψ with Gâteaux differentiability. That is, we assume that the directional derivative 𝐲 ψ ( 𝐱 ) , viewed as a function of a direction 𝐲 , is linear and continuous on n . Then there exists the gradient ψ ( 𝐱 ) of ψ at the point 𝐱 such that

𝐲 ψ ( 𝐱 ) = ψ ( 𝐱 ) , 𝐲 for  𝐱 , 𝐲 n ,

where , is the standard inner product on n .

For the map Ψ ( 𝐱 , 𝐲 ) = ψ ( 𝐱 ) , 𝐲 with 𝐱 , 𝐲 n , we find that

𝒜 Ψ = { 𝐱 n :  the one-variable map  ψ ( 𝐱 ) ,  is nonnegative on  n }
= { 𝐱 n : ψ ( 𝐱 ) + n } .

Thus the condition 𝐛 𝒜 Ψ means that ψ ( 𝐛 ) + n .

Corollary 3.2.

Let ψ : R n R be a Gâteaux differentiable Schur-convex function. Let f : R R be convex. Assume that the assumption (iii) of Theorem 2.3 is satisfied for Ψ ( x , y ) = ψ ( x ) , y with x , y R n .

Fix any x , y R n and a , b R n with ψ ( b ) R + n . If

𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some S D n , then the following Sherman-type inequality holds:

(3.4) ψ ( 𝐛 ) , f ( 𝐲 ) ψ ( 𝐚 ) , f ( 𝐱 ) .

Proof.

Condition (ii) of Theorem 2.3 holds by the linearity of Ψ ( 𝐱 , 𝐲 ) = ψ ( 𝐱 ) , 𝐲 with respect to 𝐲 . Therefore, it is sufficient to apply Theorem 3.1. ∎

By putting

(3.5) ψ ( 𝐱 ) = 𝐱 2 = 𝐱 , 𝐱 for  𝐱 n ,

which is a Schur-convex function by virtue of its convexity and permutation-invariance, we have

(3.6) ψ ( 𝐱 ) = 2 𝐱 for  𝐱 n .

In this case, condition ψ ( 𝐛 ) + n means that 𝐛 + n .

It is interesting that under (3.5) and (3.6) inequality (3.4) in Corollary 3.2 holds in the form

𝐛 , f ( 𝐲 ) 𝐚 , f ( 𝐱 ) ,

which is the classical Sherman’s inequality (see Theorem B). Thus Corollary 3.2 is a generalization of Theorem B (whenever m = n ). Moreover, by setting 𝐚 = ( 1 , , 1 ) n with a doubly stochastic 𝐒 , we can get Theorem A.

It is not hard to verify for the map Ψ ( 𝐱 , 𝐲 ) = 𝐱 ψ ( 𝐲 ) with 𝐱 , 𝐲 n that

𝒜 Ψ = { 𝐱 n :  the one-variable map  Ψ ( 𝐱 , ) = 𝐱 ψ ( )  is nondecreasing on  n } .

Theorem 3.3.

Let ψ : R n R be a Schur-convex function. Assume that for any x , y R n there exists the directional derivative x ψ ( y ) of ψ at the point x in the direction y . Let f : R R be convex. Assume that assumptions (ii) and (iii) of Theorem 2.3 are satisfied for Ψ ( x , y ) = x ψ ( y ) with x , y R n .

Fix any x , y R n and a , b R n with b A Ψ . If

(3.7) 𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some S D n , then the following Sherman-type inequality holds:

(3.8) 𝐛 ψ ( f ( 𝐲 ) ) 𝐚 ψ ( f ( 𝐱 ) ) .

Proof.

Because ψ is Schur-convex, its directional derivative is permutation-invariant (see (3.1)). For this reason, Corollary 2.5 (i’) is satisfied for the map Ψ ( 𝐱 , 𝐲 ) = 𝐱 ψ ( 𝐲 ) , 𝐱 , 𝐲 n . Furthermore, (3.7) gives (2.12), which implies (2.6). Finally, we get (3.8), as claimed. ∎

For the map Ψ ( 𝐱 , 𝐲 ) = ψ ( 𝐲 ) , 𝐱 with 𝐱 , 𝐲 n we have

𝒜 Ψ = { 𝐱 n :  the one-variable map  Ψ ( 𝐱 , ) = ψ ( ) , 𝐱  is nondecreasing on  n } .

Condition 𝐛 𝒜 Ψ means that the one-variable map Ψ ( 𝐛 , ) = ψ ( ) , 𝐛 is nondecreasing on n , that is, for 𝐲 , 𝐳 n ,

(3.9) 𝐲 𝐳 implies ψ ( 𝐲 ) , 𝐛 ψ ( 𝐳 ) , 𝐛 .

Corollary 3.4.

Let ψ : R n R be a Gâteaux differentiable Schur-convex function. Let f : R R be convex. Assume that assumptions (ii) and (iii) of Theorem 2.3 are satisfied for Ψ ( x , y ) = ψ ( y ) , x with x , y R n .

Fix any x , y R n and a , b R n with b A Ψ . If

𝐲 = 𝐒𝐱 𝑎𝑛𝑑 𝐚 = 𝐒 T 𝐛

for some S D n , then the following Sherman-type inequality holds:

(3.10) ψ ( f ( 𝐲 ) ) , 𝐛 ψ ( f ( 𝐱 ) ) , 𝐚 .

Proof.

It is sufficient to apply Theorem 3.3. ∎

To illustrate the last result, choose

(3.11) ψ ( 𝐱 ) = exp 𝐱 , 𝐞 for  𝐱 n ,

where 𝐞 = ( 1 , , 1 ) n . This is a Schur-convex function.

It is readily seen that

(3.12) ψ ( 𝐱 ) = ( exp 𝐱 , 𝐞 ) 𝐞 for  𝐱 n .

Here

Ψ ( 𝐱 , 𝐲 ) = ψ ( 𝐲 ) , 𝐱 = ( exp 𝐲 , 𝐞 ) 𝐞 , 𝐱 = 𝐞 , 𝐱 exp 𝐲 , 𝐞 .

Evidently, this map is convex with respect to 𝐲 and concave with respect to 𝐱 , which proves the validity of conditions (ii) and (iii) in Theorem 2.3.

In this case, condition 𝐛 𝒜 Ψ means that (3.9) holds in the form

𝐲 𝐳 implies 𝐞 , 𝐛 exp 𝐲 , 𝐞 𝐞 , 𝐛 exp 𝐳 , 𝐞 ,

which is true whenever 𝐞 , 𝐛 0 .

It follows from (3.11) and (3.12) that inequality (3.10) in Corollary 3.4 holds in the form

𝐞 , 𝐛 exp f ( 𝐲 ) , 𝐞 𝐞 , 𝐚 exp f ( 𝐱 ) , 𝐞 .

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Received: 2018-04-23
Revised: 2018-06-28
Accepted: 2018-07-09
Published Online: 2018-09-21

© 2020 Walter de Gruyter GmbH, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 Public License.

Artikel in diesem Heft

  1. Frontmatter
  2. On the moving plane method for boundary blow-up solutions to semilinear elliptic equations
  3. Regularity of solutions of the parabolic normalized p-Laplace equation
  4. Cahn–Hilliard equation on the boundary with bulk condition of Allen–Cahn type
  5. Blow-up solutions for fully nonlinear equations: Existence, asymptotic estimates and uniqueness
  6. Radon measure-valued solutions of first order scalar conservation laws
  7. Ground state solutions for a semilinear elliptic problem with critical-subcritical growth
  8. Generalized solutions of variational problems and applications
  9. Existence and non-existence results for Kirchhoff-type problems with convolution nonlinearity
  10. Nonlinear Sherman-type inequalities
  11. Global regularity for systems with p-structure depending on the symmetric gradient
  12. Homogenization of a net of periodic critically scaled boundary obstacles related to reverse osmosis “nano-composite” membranes
  13. Noncoercive resonant (p,2)-equations with concave terms
  14. Evolutionary quasi-variational and variational inequalities with constraints on the derivatives
  15. Sharp estimates on the first Dirichlet eigenvalue of nonlinear elliptic operators via maximum principle
  16. Localization and multiplicity in the homogenization of nonlinear problems
  17. Remarks on a nonlinear nonlocal operator in Orlicz spaces
  18. A Picone identity for variable exponent operators and applications
  19. On the weakly degenerate Allen-Cahn equation
  20. Continuity results for parametric nonlinear singular Dirichlet problems
  21. Construction of type I blowup solutions for a higher order semilinear parabolic equation
  22. Singularly perturbed Choquard equations with nonlinearity satisfying Berestycki-Lions assumptions
  23. Comparison results for nonlinear divergence structure elliptic PDE’s
  24. Constant sign and nodal solutions for parametric (p, 2)-equations
  25. Monotonicity formulas for coupled elliptic gradient systems with applications
  26. Berestycki-Lions conditions on ground state solutions for a Nonlinear Schrödinger equation with variable potentials
  27. A class of semipositone p-Laplacian problems with a critical growth reaction term
  28. The role of superlinear damping in the construction of solutions to drift-diffusion problems with initial data in L1
  29. Reconstruction of Tesla micro-valve using topological sensitivity analysis
  30. Lewy-Stampacchia’s inequality for a pseudomonotone parabolic problem
  31. Global well-posedness of nonlinear wave equation with weak and strong damping terms and logarithmic source term
  32. Regularity Criteria for Navier-Stokes Equations with Slip Boundary Conditions on Non-flat Boundaries via Two Velocity Components
  33. Homoclinics for singular strong force Lagrangian systems
  34. A constructive method for convex solutions of a class of nonlinear Black-Scholes equations
  35. On a class of nonlocal nonlinear Schrödinger equations with potential well
  36. Superlinear Schrödinger–Kirchhoff type problems involving the fractional p–Laplacian and critical exponent
  37. Regularity for minimizers for functionals of double phase with variable exponents
  38. Boundary blow-up solutions to the Monge-Ampère equation: Sharp conditions and asymptotic behavior
  39. Homogenisation with error estimates of attractors for damped semi-linear anisotropic wave equations
  40. A-priori bounds for quasilinear problems in critical dimension
  41. Critical growth elliptic problems involving Hardy-Littlewood-Sobolev critical exponent in non-contractible domains
  42. On the Sobolev space of functions with derivative of logarithmic order
  43. On a logarithmic Hartree equation
  44. Critical elliptic systems involving multiple strongly–coupled Hardy–type terms
  45. Sharp conditions of global existence for nonlinear Schrödinger equation with a harmonic potential
  46. Existence for (p, q) critical systems in the Heisenberg group
  47. Periodic traveling fronts for partially degenerate reaction-diffusion systems with bistable and time-periodic nonlinearity
  48. Some hemivariational inequalities in the Euclidean space
  49. Existence of standing waves for quasi-linear Schrödinger equations on Tn
  50. Periodic solutions for second order differential equations with indefinite singularities
  51. On the Hölder continuity for a class of vectorial problems
  52. Bifurcations of nontrivial solutions of a cubic Helmholtz system
  53. On the exact multiplicity of stable ground states of non-Lipschitz semilinear elliptic equations for some classes of starshaped sets
  54. Sign-changing multi-bump solutions for the Chern-Simons-Schrödinger equations in ℝ2
  55. Positive solutions for diffusive Logistic equation with refuge
  56. Null controllability for a degenerate population model in divergence form via Carleman estimates
  57. Eigenvalues for a class of singular problems involving p(x)-Biharmonic operator and q(x)-Hardy potential
  58. On the convergence analysis of a time dependent elliptic equation with discontinuous coefficients
  59. Multiplicity and concentration results for magnetic relativistic Schrödinger equations
  60. Solvability of an infinite system of nonlinear integral equations of Volterra-Hammerstein type
  61. The superposition operator in the space of functions continuous and converging at infinity on the real half-axis
  62. Estimates by gap potentials of free homotopy decompositions of critical Sobolev maps
  63. Pseudo almost periodic solutions for a class of differential equation with delays depending on state
  64. Normalized multi-bump solutions for saturable Schrödinger equations
  65. Some inequalities and superposition operator in the space of regulated functions
  66. Area Integral Characterization of Hardy space H1L related to Degenerate Schrödinger Operators
  67. Bifurcation of time-periodic solutions for the incompressible flow of nematic liquid crystals in three dimension
  68. Morrey estimates for a class of elliptic equations with drift term
  69. A singularity as a break point for the multiplicity of solutions to quasilinear elliptic problems
  70. Global and non global solutions for a class of coupled parabolic systems
  71. On the analysis of a geometrically selective turbulence model
  72. Multiplicity of positive solutions for quasilinear elliptic equations involving critical nonlinearity
  73. Lack of smoothing for bounded solutions of a semilinear parabolic equation
  74. Gradient estimates for the fundamental solution of Lévy type operator
  75. π/4-tangentiality of solutions for one-dimensional Minkowski-curvature problems
  76. On the existence and multiplicity of solutions to fractional Lane-Emden elliptic systems involving measures
  77. Anisotropic problems with unbalanced growth
  78. On a fractional thin film equation
  79. Minimum action solutions of nonhomogeneous Schrödinger equations
  80. Global existence and blow-up of weak solutions for a class of fractional p-Laplacian evolution equations
  81. Optimal rearrangement problem and normalized obstacle problem in the fractional setting
  82. A few problems connected with invariant measures of Markov maps - verification of some claims and opinions that circulate in the literature
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