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D I D A C T I C S O F M A T H E M A T I C S

No. 13(17) 2016

Wiktor Ejsmont

Department of Mathematics and Cybernetics, Wrocław University of Economics wiktor.ejsmont@ue.wroc.pl

FREE MEIXNER DISTRIBUTIONS

Wiktor Ejsmont

Abstract. In this paper the most important distributions in free probability (and maybe in

the universe) will be presented. It is worth emphasizing that these distributions are not known among economists.

Keywords: Meixner distributions. Jel Classification: C40, C46.

DOI: 10.15611/dm.2016.13.02.

1. Introduction

In this paper we will focus on the presentation of free distributions of a Meixner type. By ‘type’ we understand measures defined up to offset and dilation. Below we describe the probabilistic measures for normalized measures, i.e. with zero mean and variance equal to one, which depend on two parameters. In general, free Meixner distributions depend on four parameters. Classical Meixner distributions were introduced in terms of orthogonal polynomials in [Meixner 1934]. Meixner’s system of orthogonal polynomials in free probability was established by Anshelevich [Anshelevich 2003], Saitoh and Yoshida [Saitoh, Yoshida 2001], and Bożejko and Wysoczański [Bożejko, Wysoczanski 2001]. Meixner free distributions can be classified as the following six types: Wigner’s distribution, free Poisson distribution, free Pascal distribution (free negative binomial distribution), free gamma distri-bution, free binomial distridistri-bution, and pure free Meixner distribution. This classification was presented by Bożejko and Bryc [Bożejko, Bryc 2006], and was inspired by the fact that classical Meixner distributions, with similar pa-rameters, satisfy the so-called Laha–Lukacs properties. The current paper is a review and does not present free probability theory to readers. The readers of this paper are assumed to be familiar with the basic ideas of free harmonic analysis.

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14 Wiktor Ejsmont

2. Meixner distributions

In this section we present the most important facts related to free Meixner distributions. A distribution which can be given by the Cauchy–Stieltjes transform of the form

𝐺𝐺𝜇𝜇𝑎𝑎,𝑏𝑏(𝑧𝑧) = � 1 𝑧𝑧 − 𝑦𝑦 𝑹𝑹 𝑑𝑑𝜇𝜇𝑎𝑎,𝑏𝑏(𝑑𝑑𝑦𝑦) = (1) (1+2𝑏𝑏)𝑧𝑧+𝑎𝑎−�(𝑧𝑧−𝑎𝑎)2−4(1+𝑏𝑏) 2(𝑏𝑏𝑧𝑧2+𝑎𝑎𝑧𝑧+1) = 1 𝑧𝑧− 1 𝑧𝑧−𝑎𝑎− 𝑏𝑏+1 𝑧𝑧−𝑎𝑎−𝑏𝑏+1 ,

where the branch of the square root should satisfy ℑ(𝐺𝐺𝜇𝜇(𝑧𝑧)) ≤ 0 for ℑ(𝑧𝑧) > 0 (see [Saitoh, Yoshida 2001]), is called a normalized free Meixner distribution { 𝜇𝜇𝑎𝑎,𝑏𝑏: 𝑎𝑎 ∈ ℝ, 𝑏𝑏 ≥ − 1}.

Equation (1) describes the distribution with zero mean and variance equal to one. Absolutely continuous part of 𝜇𝜇𝑎𝑎,𝑏𝑏 equals

�4(1+𝑏𝑏)−(𝑥𝑥−𝑎𝑎)2

2𝜋𝜋(𝑏𝑏𝑥𝑥2+𝑎𝑎𝑥𝑥+1) 𝑑𝑑𝑑𝑑, (2)

where 𝑎𝑎 − 2�(1 + 𝑏𝑏) ≤ 𝑑𝑑 ≤ 𝑎𝑎 + 2�(1 + 𝑏𝑏). This measure has one atom if 0 ≤ 4𝑏𝑏 < 𝑎𝑎2, and two atoms if −1 ≤ 𝑏𝑏 < 0. For a given parameterization,

monic polynomials that are orthogonal with respect to the measure 𝜇𝜇𝑎𝑎,𝑏𝑏, satisfy the relations

(𝑑𝑑 − 𝑎𝑎)𝑝𝑝𝑛𝑛(𝑑𝑑) = 𝑝𝑝𝑛𝑛+1(𝑑𝑑) + (𝑏𝑏 + 1)𝑝𝑝𝑛𝑛−1(𝑑𝑑), 𝑛𝑛 = 2,3, …, (3)

where

𝑝𝑝0(𝑑𝑑) = 1, 𝑝𝑝1(𝑑𝑑) = 𝑑𝑑, (4)

or equivalently, Jacobi parameters are of the form

𝐽𝐽(𝜇𝜇𝑎𝑎,𝑏𝑏) = �0,1, 𝑏𝑏 + 1, 𝑏𝑏 + 1, 𝑏𝑏 + 1, …�.𝑎𝑎, 𝑎𝑎, 𝑎𝑎, … (5)

Assuming that 𝑚𝑚𝑖𝑖(𝜇𝜇) is the ith moment of the measure µ, then the generating function of the moments corresponding to equation (1) is of the form

𝑀𝑀𝜇𝜇𝑎𝑎,𝑏𝑏(𝑧𝑧) = ∑∞𝑖𝑖=0𝑚𝑚𝑖𝑖(𝜇𝜇𝑎𝑎,𝑏𝑏) = 1 𝑧𝑧𝐺𝐺𝜇𝜇𝑎𝑎,𝑏𝑏� 1 𝑧𝑧� = 1+2𝑏𝑏+𝑎𝑎𝑧𝑧−�(1−𝑧𝑧𝑎𝑎)2−4𝑧𝑧2(1+𝑏𝑏) 2(𝑧𝑧2+𝑎𝑎𝑧𝑧+𝑏𝑏) , (6)

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Free Meixner distributions

15

for sufficiently small |𝑧𝑧|. The R-transform corresponding to 𝑀𝑀(𝑧𝑧) is given by

ℛ𝜇𝜇𝑎𝑎,𝑏𝑏(𝑧𝑧) = ∑∞𝑖𝑖=0𝑅𝑅𝑖𝑖+1(X)𝑧𝑧𝑖𝑖 = 𝐺𝐺𝜇𝜇−1𝑎𝑎,𝑏𝑏(𝑧𝑧) − 1/𝑧𝑧 =

2𝑧𝑧

1−𝑧𝑧𝑎𝑎+�(1−𝑧𝑧𝑎𝑎)2−4𝑧𝑧2𝑏𝑏, (7)

where the square root should be chosen as lim

𝑧𝑧→0ℛ𝜇𝜇(𝑧𝑧) = 0 (see [Saitoh,

Yoshida 2001]). The numbers 𝑅𝑅𝑖𝑖 are called free cumulants of the probability measure 𝜇𝜇𝑎𝑎,𝑏𝑏.

Depending on the values of a and b, the distribution 𝜇𝜇𝑎𝑎,𝑏𝑏 can become one of the following six types:

• Wigner’s distribution, if 𝑎𝑎 = 𝑏𝑏 = 0;

• free Poisson distribution, if 𝑏𝑏 = 0 and 𝑎𝑎 ≠ 0;

• free Pascal distribution (free negative binomial distribution), if 𝑏𝑏 > 0 and 𝑎𝑎2 > 4𝑏𝑏;

• free gamma distribution, if 𝑏𝑏 > 0 and 𝑎𝑎2 = 4𝑏𝑏;

• pure free Meixner distribution, if 𝑏𝑏 > 0 and 𝑎𝑎2 < 4𝑏𝑏;

• free binomial distribution, if −1 ≤ 𝑏𝑏 < 0.

There are so-called Kesten’s measures in this classification (see [Kesten 1959]) obtained with 𝑏𝑏 ≠ 0 and 𝑎𝑎 = 0, i.e. their density is given by

�4(1+𝑏𝑏)−𝑥𝑥2

2𝜋𝜋(𝑏𝑏𝑥𝑥2+1)

.

(8)

Saitoh and Yoshida in [Saitoh, Yoshida 2001] proved that Meixner dis-tributions are free infinitely divisible if and only if 𝑏𝑏 ≥ 0 (for a given param-eterization). The Lévy–Khinchin representation in this case takes the beauti-ful form

ℛ𝜇𝜇𝑎𝑎,𝑏𝑏(𝑧𝑧) = ∫

𝑧𝑧 1−𝑥𝑥𝑧𝑧

ℝ 𝑤𝑤𝑎𝑎,𝑏𝑏(𝑑𝑑𝑑𝑑), (9)

where 𝑤𝑤𝑎𝑎,𝑏𝑏 is Wigner’s measure with mean a and variance b. In particular, we obtain from (9) and (7)

𝑅𝑅𝑛𝑛+2(𝜇𝜇𝑎𝑎,𝑏𝑏) = ∫ 𝑑𝑑 𝑛𝑛𝑤𝑤𝑎𝑎,𝑏𝑏(𝑑𝑑𝑑𝑑). (10)

Another interesting formula for the cumulants of the free Meixner distribu-tions is the following equation (from [Bożejko, Bryc 2006]):

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16 Wiktor Ejsmont

where 𝑠𝑠(𝜈𝜈) are blocks of size 1 with partitions, whereas 𝑁𝑁𝐶𝐶1,2(𝑛𝑛) is a set of all non-crossing partitions of the set {1, … , 𝑛𝑛}, such that each block of parti-tions is of size either 1 or 2, i.e. |𝐵𝐵𝑖𝑖| = 1 or |𝐵𝐵𝑖𝑖| = 2.

We proceed now to the main result of Bożejko and Bryc in [Bożejko, Bryc 2006] that supports the premise from the abstract. They proved that ran-dom variables with linear conditional first moment and quadratic conditional variance have free Meixner distributions.

Theorem 1. Let us assume that X, Y are freely independent, self-adjoint,

non-degenerate elements of a non-commutative probabilistic space, and that there are constants 𝛼𝛼, 𝛼𝛼0, 𝑎𝑎, 𝑏𝑏, 𝐶𝐶 ∈ ℝ such that

𝐸𝐸(X|X + Y) = 𝛼𝛼(X + Y) + 𝛼𝛼0 (12)

and

𝑉𝑉𝑎𝑎𝑎𝑎(X|X + Y) = 𝐶𝐶[1 + 𝑎𝑎(X + Y) + 𝑏𝑏(X + Y)2]. (13)

Then random variables X and Y have free Meixner distributions. In par-ticular, when 𝐸𝐸(X) = 𝐸𝐸(Y) = 0 and 𝐸𝐸(X2+ Y2) = 1, then the distribution of X is one of the six types presented above.

Bibliography

Anshelevich M. (2003). Free martingale polynomials. J. Funct. Anal. 201(1). Pp. 228-261. Bożejko M., Bryc W. (2006). On a class of free Lévy laws related to a regression problem.

J. Funct. Anal. 236(1). Pp. 59-77.

Bożejko M., Wysoczański J. (2001). Remarks on t-transformations of measures and

convo-lutions. Ann. Inst. H. Poincaré Probab. Statist. 37(6). Pp. 737-776.

Kesten H. (1959). Symmetric random walks on groups. Trans. Amer. Math. Soc. 92. Pp. 336-354.

Laha R.G., Lukacs E. (1960). On a problem connected with quadratic regression. Biometrika 47. Pp. 335-343.

Meixner J. (1934). Orthogonale Polynomsysteme mit einer besonderen Gestalt der

erzeugenden Funktion. J. London Math. Soc. 9. Pp. 6-13.

Saitoh N., Yoshida H. (2001). The infinite divisibility and orthogonal polynomials with

a constant recursion formula in free probability theory. Probab. Math. Statist. 21(1).

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D I D A C T I C S O F M A T H E M A T I C S

No. 13(17) 2016

Tadeusz Janaszak

Department of Mathematics and Cybernetics, Wrocław University of Economics tadeusz.janaszak@ue.wroc.pl

SOME REMARKS ABOUT SERIES

Tadeusz Janaszak

Abstract. This paper presents a proof of the classical theorem of the theory of series. This

proof would be used in lectures on the series theory.

Keywords: series, convergent, divergent series, harmonic series. Jel Classification: C00.

DOI: 10.15611/dm.2016.13.03.

1. Introduction

In the lectures of calculus the direct proof of the theorem that the series

=1

1

n n

α is convergent for 1<α is rarely introduced. The knowledge about

the convergence of this series is used in exercises but the proof of the con-vergence of this series is presented on the whole by the integral criterion. In standard textbooks of calculus it is difficult to find a direct proof of conver-gence of the series. This paper presents a direct proof of converconver-gence of the series. This text is a supplement for numerous books of calculus.

Theorem. The series

=1

1

n n

α

is divergence where 0<α ≤1 and convergence where 1<α.

For the proof of the theorem it is necessary to show a lot of lemmata.

Lemma 1. The harmonic series

∞ =1

1

n n

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18 Tadeusz Janaszak

Proof. The harmonic series is equal such that:

... 2 1 ... 1 2 1 ... 8 1 ... 5 1 4 1 3 1 2 1 1 1 1 1 1 + + + + + + + + + + + + = + ∞ =

n n n n . It is possible to group the terms of harmonic series:

2 3 2 1 1 1 0 = + = a , 4 1 3 1 2 1 1 2 1 2 1 1 + = + + = a , = + + + + + + = 2 2 2 3 2 2 1 3 2 1 2 2 1 1 2 1 a 8 1 7 1 6 1 5 1+ + + , …, 1 2 1 ... 1 2 1 + + + + = n n n a .

The harmonic series is equal

∞ = ∞ = = 0 1 1 n n n a n . It is obvious that 2 1 2 1 1+ > , and 2 1 4 1 4 1 4 1 3 1+ > + = , and 2 1 8 1 ... 8 1 8 1 ... 5 1 = + + > + + , and 2 1 2 1 2 2 2 1 ... 1 2 1 1 = ⋅ > + + + + n+ n n n n . From

here the result below is true:

∞ = + + > 1 ... 2 1 2 1 1 n n , i.e. the harmonic series

∞ =1

1

n n

is divergent.

Proof of the theorem: the series

∞ =1

1

n n

α is divergence for 0<α ≤1.

If α is a number such that 0<α <1 then for natural numbers the ine-quality nα <n holds, hence the unequal α

n n

1

1 < holds too, i.e. the harmo-nic series

∞ =1 1 n n is a minorant of series

∞ =1 1 n nα

for 0<α <1. Hence the minorant is a divergence series the series (1) is divergence for 0<α <1.

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Some remarks about series 19

Lemma 2. For each natural number n the expression is true:

(

1

)

1 1 ... 3 2 1 2 1 1 + = + ⋅ + + ⋅ + ⋅ n n n n . Proof by induction.

For n=1 the left side is equal 2 1

and the right side is equal 2 1

too. Suppose that for some n the expression above holds. It is necessary to prove that

(

) (

)(

)

2 1 2 1 1 1 1 ... 3 2 1 2 1 1 + + = + + + + ⋅ + + ⋅ + ⋅ n n n n n n .

The left side of the equality above by the induction assumption is equal

(

1

)(

2

)

1 1+ + + + n n n n

(

)

(

1

)(

2

)

1 2 + + + + ⋅ = n n n n

(

1

)(

2

)

1 2 2 + + + + = n n n n

(

)

(

1

)(

2

)

12 + + + = n n n , it is obvious that

(

)

(

1

)(

2

)

12 + + + n n n 2 1 + + = n n , so the proof of the lemma is complete.

Corollary. The series

(

)

=1 ⋅ +1

1

n n n

is convergent, the sum is equal to 1.

Proof. Because

(

)

∞ =1 ⋅ +1 1 n n n

(

)

1 1 lim 1 1 lim 1 = + =       + ⋅ = ∞ → = ∞ →

n n n n n n k n , the

thesis of the corollary is true.

Lemma 3. The series

∞ =1 2

1

n n

is convergent and the sum of this is less than or equal to 2. ... 4 3 1 3 2 1 2 1 1 1 ... 4 4 1 3 3 1 2 2 1 1 1 1 2 = + ⋅ + ⋅ + ⋅ + ≤ + ⋅ + ⋅ + ⋅ +

∞ = n n

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20 Tadeusz Janaszak

Proof. By this expression the conclusion below holds:

+ ≤

∞ = 1 1 1 2 n n

(

)

2 1 1 1 = + ⋅

∞ = n n n . The lemma is true.

Lemma 4. The series

∞ =1 1 n n α is convergent for 2 1 1+ = α .

Proof. It is necessary to see the expressions:

= ⋅

∞ =1 1 n n n + + + ⋅ + ⋅ + ⋅ + ⋅ + ⋅ 8 8 1 ... 5 5 1 2 4 1 3 3 1 2 2 1 1 1 1 + ⋅ + + ⋅ + ⋅ + 15 15 1 ... 10 10 1 3 9 1 + + ⋅ + + ⋅ + ⋅ 24 24 ... 1 ... 17 17 1 4 16 1

(

)

(

)

... 2 2 1 ... 1 1 1 1 2 2 2 2 2 + + ⋅ + + + + ⋅ + + ⋅ + k k k k k k k k i.e.

(

)

∑ ∑

∞ = = ∞ =         + ⋅ + = ⋅ 1 2 0 2 2 1 1 1 k k j n n n k j k j . It is possible to write some obvious inequalities

3 1 1 1 2 1 1 1 1 1 1 3 3 1 2 2 1 1 1 1 3 = + ⋅ = + + ≤ ⋅ + ⋅ + , and 8 5 2 1 2 2 2 4 1 ... 2 4 1 2 4 1 8 8 1 ... 5 5 1 2 4 1 3 = + ⋅ = ⋅ + + ⋅ + ⋅ ≤ ⋅ + + ⋅ + ⋅ , and 27 7 3 1 3 2 3 9 1 ... 3 9 1 3 9 1 15 15 1 ... 10 10 1 3 9 1 3 = + ⋅ = ⋅ + + ⋅ + ⋅ ≤ ⋅ + + ⋅ + ⋅ , and 64 9 4 1 4 2 4 16 1 ... 4 16 1 4 16 1 24 24 1 ... 17 17 1 4 16 1 3 = + ⋅ = ⋅ + + ⋅ + ⋅ ≤ ⋅ + + ⋅ + ⋅ ,

(9)

Some remarks about series 21 and generally

(

)

(

)

. 1 2 1 ... 1 1 2 2 1 ... 1 1 1 1 3 2 2 2 2 2 2 2 2 k k k k k k k k k k k k k k k k + = ⋅ + + ⋅ + ⋅ ≤ + ⋅ + + + + ⋅ + + ⋅

By this the inequality

(

)

∑ ∑

∞ = =         + ⋅ + 1 2 0 2 2 1 k k j k j k j

∞ = + ≤ 1 3 1 2 k k k holds i.e. the evaluation

∞ =1 ⋅ 1 n n n

∞ = + ≤ 1 3 1 2 k k k is true. For every natural number k the expression

2 3 3 3 3 1 2 k k k k k = ≤ +

holds, so the series

∞ = ∞ = ⋅ = 1 2 1 2 1 3 4 n n n n

is a majorant of the series

∞ =1 ⋅ 1 n n n i.e.

∞ =1 ⋅ 1 n n n

∞ = ⋅ ≤ 1 2 1 3 n n .

Because the series

∞ =1 2

1

n n

is convergent, by lemma 3, so the series

=1 ⋅

1

n n n

is convergent too. The sum of the series is less than or equal to 6.

Lemma 5. If the series

∞ =1 1 n nα is convergent for s 2 1 1+ = α where s is

some natural number, then it is convergent for 1 2

1 1+ +

= s

(10)

22 Tadeusz Janaszak

Proof. Let for sN to be

( )

s s

2 1 =

β . It is necessary to show that the series

( ) ∞ =1 ⋅ + 1 1 n s n

n β is convergent if the series

( )

∞ =1 ⋅ 1 n s n n β is convergent. The series

( ) ∞ =1 ⋅ + 1 1 n s n n β is equal to

( ) ∞ =1 ⋅ 1 n n nβ s i.e. ( )

∞ =1 ⋅ + 1 1 n s n n β ( ) ( ) 3 3 ( ) ... 1 2 2 1 1 1 1 + ⋅ + ⋅ + ⋅ = s s s β β β .

The inequalities below obviously hold: ( ) + ( ) + ( ) ≤ ⋅ β s βs β s 3 3 1 2 2 1 1 1 1 1 1 1 1 1 1+ + 3 1 1 1 2⋅ + = = and ( ) ( ) ( ) ≤ ⋅ + + ⋅ + ⋅ β s β s β s 8 8 1 ... 5 5 1 2 4 1 ( )s β 2 4 5 ⋅ and ( ) ( ) ( ) ≤ ⋅ + + ⋅ + ⋅ βs β s βs 15 15 1 ... 10 10 1 3 9 1 [ ]s β 3 8 7 ⋅ and ( ) ( ) ( ) ≤ ⋅ + + ⋅ + ⋅ β s β s β s 24 24 1 ... 17 17 1 4 16 1 ( )s β 4 16 9 ⋅ and generally ( )

(

) (

)

( )

(

) (

)

( ) ≤ + ⋅ + + + + ⋅ + + ⋅ s s s k k k k k k k k β β 2 2 β 1 ... 1 1 1 1 2 2 2 2 2 ( )s k k k β ⋅ + 2 1 2 .

The equality below is certain:

( )s ( )s ( )s k k k k k k k k β β β ≤ = ⋅ +1 3 3 2 2 2 ,

by this it is obvious that

( ) ≤ ⋅

∞ =1 + 1 1 n s n n β

( ) ∞ = ⋅ ⋅ 1 1 3 n s n n β ,

(11)

Some remarks about series 23

by the comparison test for convergence of infinite series the series ( )

∞ =1 ⋅ + 1 1 n s n

n β is convergent if the series

( )

∞ =1 ⋅ 1 n s n

n β is convergent. The sum

of the series

( ) ∞ =1 ⋅ + 1 1 n s n

n β is less than or equal to 1

3

2⋅ s+ . By mathematical induction there is the finish of lemma 5.

Proof of the theorem: the series

∞ =1

1

n n

α is convergence where 1<α.

If 1<α that there is a natural number s such that + s <α 2 1 1 i.e.

[ ]

α β < + s

1 so for each natural n it is n1+β( )s <nα

and consequently ( )s n nα < 1+β 1 1 , by this the series

( )

∞ =1 ⋅ 1 n s n

n β is a majorant of the series

∞ =1

1

n n

α and

conse-quently the series

∞ =1

1

n n

α is convergent. The proof of the theorem is finished.

Usually the proof of the theorem is shown by the integral test for

convergence:

On the interval

[

m, ∞

)

where mN the function f

( )

x is positive and decreasing then the series

( )

=m

n n

f and the integral

( )

m

dx x

f are both at the same time convergent or divergent.

Proof of the theorem with use the integral test for convergence. The integral dx x

∞ 1 1 is divergence because

( )

=∞ ∞ → f t t

lim . For α ≠1 the indefinite integral is equal:

⋅ −

− = α α α 1 1 1 1 x

x . The value of the

antideriva-tive at the point x=1 is equal 1 1 − α , the limit α − ∞ → 1 lim x

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24 Tadeusz Janaszak

α <

1 and it is infinity for 0<α <1. So dx x

∞ 1 1 α equals 1 1 − α for 1<α and infinity for 0<α <1. This conclusion finishes the proof of the theorem.

The direct proof of the convergence of the series

∞ =1

1

n n

α for 1<α in

another way is presented in [Fihtenholz 1978, vol. 2, p. 227], the proof of the divergence is presented in the same way as in this paper.

Bibliography

Antoniewicz R., Misztal A. (2000). Matematyka dla studentów ekonomii. PWN. Warszawa. Fichtenholz G.M. (1978). Rachunek różniczkowy i całkowy. PWN. Warszawa.

Gewert M., Skoczylas Z. (2005). Analiza matematyczna 2. Oficyna Wydawnicza GIS. Wrocław.

Smoluk A. (2007). Podstawy analizy matematycznej. Wydawnictwo Akademii Ekonomicz-nej we Wrocławiu.

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z dnia 07 września 2010 roku w sprawie wymagań, jakim powinna odpowiadać ochro- na wartości pieniężnych przechowywanych i transportowanych przez przedsiębiorców i inne

The free-free conditions were simulated suspending the beam with springs introducing an extra natural frequency, reasonably lower than the first resonance in bending

In this paper we consider the global motion of a drop of a viscous barotropic fluid in the general case, i.e.. Then the mo- tion of the drop is described by the following system