Some tight polynomial-exponential lower bounds for an exponential function

Size: px
Start display at page:

Download "Some tight polynomial-exponential lower bounds for an exponential function"

Transcription

1 Some tight polynomial-exponential lower bounds for an exponential function Christophe Chesneau To cite this version: Christophe Chesneau. Some tight polynomial-exponential lower bounds for an exponential function. 18. <hal-16864> HAL Id: hal Submitted on 1 Jan 18 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

2 Some tight polynomial-exponential lower bounds for an exponential function Christophe Chesneau a,1 a LMNO, University of Caen Normandie, France Abstract This note is devoted to new sharp lower bounds for exp(x. We first introduce and study a new lower bound defined with polynomial of degree and exponential (or hyperbolic functions. Then we propose two improvements of this lower bound by using two different approaches; the first approach consists in adding well-chosen polynomial term to it, whereas the second approach aims to transform it for large values of x. We show that they are better to well-known lower bounds. The analytic results are supported by some numerical studies and graphics. A part of the study is devoted to some integral methods having the ability to generate new lower bounds for exp(x. Keywords: Algebraic bounds, exponential function. MSC: 33B1, 6D7. 1. Introduction Inequalities involving exponential functions are useful in all the areas of mathematics. The most famous of them can be found in Mitrinović (1964, Bullen (1998 and Kuang (1993. See also Qi (1997, Bae (7, Kim (7 and Bae and Kim (9 for current developments on lower and upper bound for exp(x. The purpose of this note is to provide simple and tight lower bounds for exp(x. Such bounds are important tools to evaluate lower or upper bounds of mathematical terms involving exp(x. Basic examples include the functions cosh(x, sinh(x and tanh(x, the integral x exp(y dy, the sum exp( k, the cumulative distribution function of the Gaussian or Kolmogorov distributions. Well-known lower bounds for exp(x are cosh( x, sinh ( 6x /( 6x, exp(x x, 1 + x + x 4 / and ( 1 + x /a a with a >. The last one is sharp for x large only for large values of a, corresponding to a polynomial with a high degree and large coefficients when a is an integer. Recent sharp lower bounds can be found in Bagul (17 for x is a an interval of the form [, b] with a precise value for b. The motivation of this paper is to introduce new sharp lower bounds for exp(x defined with simple functions, at least uniformly better to the two benchmarks: cosh( x and 1 + x + x 4 /, for all x R. In a first part, a first lower bound is introduced. It is defined as an even function on R with simple polynomial of degree and exponential functions (without power of x. Comparison to cosh( x, exp(x x and 1 + x + x 4 / are made analytically and with the used of graphics. Then we propose two significant improvements of this lower bound via two different approaches. The first approach aims to add well chosen polynomial terms to the former lower bound. The second approach adopts the transformation suggested in Chesneau (17. It consists in weighting and translating the former lower bound when x is large enough. Only polynomial of degree and exponential functions are used. In each case, the theoretical results are supported by a short numerical study and some graphics, illustrating the tightness of the new lower bounds. k= 1 christophe.chesneau@unicaen.fr 1

3 Finally, we present new integration approaches to generate lower bounds for exp(x using existing lower bounds. The link existing with this approach and the main lower bound of the study is discussed. The rest of this note is structured as follows. Section presents our main lower bound. Section 3 is devoted to an improvement of this lower bound. Another improvement is developed in Section 4. Section 5 presents some integral approaches to determine lower bounds for exp(x. All the proofs of our results are postponed in Section 6.. Lower bound The main lower bound for exp(x is presented in the proposition below. Proposition 1. Let us define the function f(x by f(x = 1 [ ( exp x (7 4 ( x + x + exp x (7 + 4 ] x + x 1. (1 Then, for all x R, exp(x f(x 1. Let us observe that f(x is a continuous even function on R using simple polynomial-exponential functions. It is of the form f(x = (1/(G(x + G( x 1, where G(x = exp ( x (7 4 x + x. It can be also express in terms of hyperbolic cosh and sinh functions as: ( f(x = (7 + x cosh x 4 ( x sinh x 6. ( A visual comparison between exp(x and f(x is performed in Figure 1, for x [ 1, 1] for the first graphic and x [.5,.5] for the second graphic. We can see that the two curves are relatively close, specially for small value for x. This comment is also supported by Table 1 which indicates the numerical values of the error measure: R(b = b [ b f(x exp(x ] dx, for several values for b. The numerical studies are done with the software Mathematica (version 11, see Wolfram ( expx 6 expx fx 4 fx Figure 1: Superimposed curves of exp(x and f(x for x [ 1, 1] in the first graphic, and for x [.5,.5] in the second graphic. Table 1: Numerical evaluations of R(b for b {.5, 1, 1.5,,.5, 3}. b =.5 b = 1 b = 1.5 b = b =.5 b = 3 R(b The tightness of f(x is highlighted in Proposition below; we proves that f(x is uniformly greater to most well-known simple lower bounds for exp(x : cosh ( x, exp(x x, 1 + x + x 4 /.

4 Proposition. Let f(x be the function given by (1. We have, for all x R, [ ( ] f(x max cosh x, exp(x x, 1 + x + x4. Hence f(x can be viewed as the best lower bounds among cosh ( x, exp(x x and 1 + x + x 4 /. Figure illustrates this result by considering two intervals of values for x : [ 1, 1] and [ 3, 3], one for each graphics. It shows that f(x is closer to exp(x is comparison to cosh ( x, exp(x x and 1 + x + x 4 /..5 5 f(x 4 f(x. 1+x + x4 3 1+x + x4 cosh x cosh x 1.5 exp(x-x exp(x-x ( x Figure : Superimposed curves of f(x, 1 + x + x 4 /, cosh and exp(x x for x [ 1, 1] in the first graphic, and for x [ 3, 3] in the second graphic. Since cosh ( x 1 or exp(x x 1 or 1 + x + x 4 / 1, Proposition implies that f(x 1, which is the second inequality in Proposition 1. If we consider the polynomial of degree 6: 1 + x + x 4 / + x 6 /6, which is also a loser bound for exp(x, we have f(x 1 + x + x 4 / + x 6 /6 for some x, but their exists x such that the reverse holds. This motivates the study of some improvements of f(x, which concerns the rest of the study. Two modifications are proposed: adding a well-chosen polynomial term to f(x or transforming f(x for x large. Remark 1. Let us mention that some continuous even upper bounds for exp(x using hyperbolic cosh and sinh functions can be proved. An example with x bounded is the following: For any a > and x a, we have exp(x cosh (ax + (x/a sinh (ax ( exp(a x. 3. First improvement of the lower bound First of all, let us consider an intermediary result which can be viewed as an improvement of the wellknown inequality: for all x R, exp(x cosh ( x. Lemma 1. For all x R and n N, we define the polynomial P n (x by Then, for all x R and n N, we have P n (x = x 4 n k= exp(x cosh x k k!(k + 3(k + ( x + P n (x. Since P n (x for all x R and n N, it is clear that exp(x cosh ( x + P n (x cosh ( x. Let us observe that P n (x satisfies the recurrence relation: P n (x = P n 1 (x + x (n+ /(n!(n + 3(n +, with P (x = x 4 /3. Expressions of P n (x for several values of n are given in Table. Lemma 1 is a key tool to the proof of the following proposition in which we determine a tight lower bound of exp(x uniformly greater to f(x. 3

5 Table : Analytic expressions for P n(x with n {,..., 5}. n = n = 1 n = n = 3 P n (x 1 3 x4 1 3 x x6 1 3 x x x8 1 3 x x x x1 n = 4 n = x x x x x1 1 3 x x x x x x14 Proposition 3. For all x R and n N, we define the polynomial Q n (x by n Q n (x = 4x 6 x k ( k!(k + 3(k + k= 1 (k + 5(k x (k + 4(k + 7 Let f(x be the function given by (1. We define the function f (x; n by Then, for all x R and n N, we have f (x; n = f(x + Q n (x. exp(x f (x; n f(x. Thus f (x; n is a better lower to f(x for exp(x, for all x R. Remark that Q n (x satisfies the recurrence relation: Q n (x = Q n 1 (x+4x (n+3 /(n!(n+3(n+[1/((n+5(n+3+x /((n+4(n+7], with Q (x = x 6 /45 + x 8 /4. Expressions of Q n (x for several values of n are given in Table 3.. Table 3: Analytic expressions for Q n(x with n {,..., 5}. n = n = 1 n = Q n (x 1 45 x x x x x x x x x1 n = 3 n = x x x x x x x x x x x16 The result of Proposition 3 is illustrated in Figure 3. The two graphics consider the two intervals for x: [ 1, 1] and [.5,.5] expx f (x, f(x 6 4 expx f (x, f(x Figure 3: Superimposed curves of exp(x, f (x; n for n = and f(x for x [ 1, 1] in the first graphic, and for x [.5,.5] in the second graphic. Table 4 shows the numerical values of the error measure: R (b = b [ f (x; n exp(x ] b dx, for n = and several values for b. 4

6 Table 4: Numerical evaluations of R (b for b {.5, 1, 1.5,,.5, 3}. b =.5 b = 1 b = 1.5 b = b =.5 b = 3 R (b Second improvement of the lower bound We now investigate a transformation of f(x for large x, based on a multiplicative exponential weight and translation. It is an adaptation of the method developed by Chesneau (17 to f(x. Proposition 4. Let f(x be the function given by (1. For any a, we define the function f(x; a by f (x; a = f(x1 { x <a/} (x + f( x a exp(a x a 1 { x a/} (x, where 1 A (x denotes the indicator function over A, i.e. 1 A (x = 1 if x A and elsewhere. Then, for all a and x R, we have exp(x f (x; a f(x. Another look of the function f (x; a is given by f (x; a = max [ f(x, f( x a exp(a x a ]. Note that f (x; a is an even continuous function on R. It follows from Proposition 4 that f (x; a is a better lower to f(x for exp(x, for all a and x R. Figure 4 proposes a graphical illustration of Proposition 4. The two graphics consider the two intervals respectively: [ 1, 1] and [ 3, 3]. We see that exp(x and f (x, a with a = 1 are near confounded for the considered values for x, showing the sharpness of the lower bound. Owing to Proposition, we have f (x; a max [ ( cosh x, 1 + x + x4 [ ( + max cosh ( x a, ] 1 { x <a/} (x (1 + ( x a + ] ( x a4 exp(a x a 1 { x a/} (x. Therefore, defining with the same a, this lower bound is sharper to the lower bounds exhibited in Chesneau ( expx fox,1 fx 3 expx fox,1 fx Figure 4: Superimposed curves of exp(x, f (x; a for a = 1 and f(x for x [ 1, 1] in the first graphic, and for x [.5,.5] in the second graphic. Table 5 shows the numerical values of the error measure: R (b = b [ f (x; a exp(x ] b dx, for a = 1 and several values for b. The value a = 1 in the numerical study is arbitrary chosen; one can find a more optimal value for the problem for a given criteria of optimization. 5

7 Table 5: Numerical evaluations of R (b for b {.5, 1, 1.5,,.5, 3}. b =.5 b = 1 b = 1.5 b = b =.5 b = 3 R (b A comparison of the two lower bounds f (x; n and f (x; a is now discussed. When x is small, say x < a/ for a fixed a, we have f (x; n f(x = f (x; a, so f (x; n is better. When x is large, in view of Figure 4, and Tables 4 and 5, we claim that f (x; n is better for some a and n. As a direct applications of our results, let us mention that sharp polynomial-exponential lower bounds for exp(x give sharp polynomial-exponential lower bounds for cosh(x or sinh(x ; using the inequality exp(y 1 + y, for all y R, for any ψ(x {f(x, f (x; n, f (x; a}, for all x R, we have cosh(x = exp(x + exp( x 1 ( ψ(x + max(1 x,. On the other hand, using the inequality: exp( y 1 y + y /, for all y, for any x R, we have sinh(x = exp(x exp( x 1 These inequalities can be usefull in various mathematical settings. ( ψ(x max (1 x + x4, On some generators of lower bounds We now present and discuss some general approaches based on integration to generate new lower bounds for exp(x from existing lower bounds. When it is possible, conditions are mentioned to improved the tightness of the former lower bounds First integral approach The main result is described in the proposition below. Proposition 5. Let θ(x be a positive function on R and ω(x be the function defined by ω(x = (1 + t θ(tdt dy + 1. Suppose that exp(x θ(x for all x R. Then exp(x ω(x for all x R. Suppose that θ(x is even, two times differentiable with θ( = 1, θ ( = and (1+x θ(x θ (x for all x. Then, for all x R, we have ω(x θ(x. Under the assumptions of the two points above, we have So ω(x is a better lower bound to θ(x. exp(x ω(x θ(x. 6

8 Connections between Proposition 5 and 1 exist. Indeed, let us consider the well-known lower bound for exp(x : θ(x = cosh ( x. We have θ (x = sinh ( x and θ (x = cosh ( x. Therefore θ( = 1, θ ( = and (1 + x θ(x θ (x = 4x cosh ( x. It follows from Proposition 5 that a better lower bound of θ(x = cosh ( x is given by ω(x = = (1 + t θ(tdt dy + 1 ( ( 4y cosh y = (7 + x cosh + 3 ( sinh y ( x 4 ( x sinh x 6. + ( y sinh y dy + 1 We thus obtain the hyperbolic expression of the lower bound f(x given by (. Naturally, the first point of Proposition 5 can be used to generate new lower bounds for exp(x. For instance, using the inequality exp(y 1 + y for all y R, we have exp(x = exp(x x exp( x (1 + x x exp( x. Let us set θ(x = (1 + x x exp( x. Hence a new lower bound for exp(x is given by ω(x = (1 + t θ(tdt dy + 1 = [ exp(y ( y + 66y y 3 + 4y ] dy + 1 = exp( x ( x + 174x 36 x 3 + 4x x. However, note that this lower bound is not better to θ(x. In particular, the assumption (1 + x θ(x θ (x for all x R is not satisfied. This bound is tight but not shaper than f(x for all x R. Moreover, from a mathematical point of view, it is more difficult to manipulate to f(x. Let us mention that the well-known lower bounds: 1 + x + x 4 / and exp( x x, also satisfy θ( = 1, θ ( = and (1 + x θ(x θ (x for all x, yielding more sharp lower bounds ω(x for exp(x. However, one can show that they are not better to f(x for all x R (and the presented improvements. 5.. Generalization Proposition 6 below presents a generalization of Proposition 5. From two lower bounds θ 1 (x and θ (x of exp(x, one can construct a lower bound better to θ 1 (x or θ (x, under some assumptions. Proposition 6. Let θ 1 (x and θ (x be two positive functions on R and κ(x be the function defined by κ(x = (θ 1 (t + t θ (tdt dy + 1. Suppose that exp(x max [θ 1 (x, θ (x] for all x R. Then exp(x κ(x for all x R. Suppose that θ 1 (x and θ (x are even, two times differentiable with θ 1 ( = 1, θ 1( =, (θ 1 (x + x θ (x θ 1 (x for all x. Then, for all x R, we have κ(x θ 1 (x. This inequality holds with θ (x by inverting the role of θ 1 (x and θ (x in the definition of κ(x and the conditions. θ 1 ( = 1, θ ( = 1, θ 1( =, θ ( =, (θ 1 (x + x θ (x θ 1 (x and (θ 1 (x + x θ (x θ (x for all x. Then, for all x R, we have κ(x max [θ 1 (x, θ (x]. 7

9 Under the assumptions of the first point and the second item of the second point, we have exp(x κ(x max [θ 1 (x, θ (x]. So κ(x is a better lower bound to θ 1 (x for exp(x, or both of them. Taking θ 1 (x = θ (x in Proposition 6, we obtain Proposition 5 with θ(x = θ 1 (x. Note that, taking θ 1 (x = cosh ( x and θ (x = n k= x k /(k!, the first point and the first item of the second point of Proposition 6 are satisfied; we thus obtain Lemma 1. Another example is given by chosing θ 1 (x = f(x and θ (x = cosh ( x. After some calculus, we have ( ( ( κ(x = 7 cosh x x 3 cosh x 1 ( x sinh x 6. Also, one can show that the first point and the second item of the second point of Proposition 6 are satisfied; κ(x is a better lower bound to f(x. However, the comparison with the proposed improvements for f(x need further investigations Another integral approach We conclude this section by presenting another generator of lower bounds for exp(x. Proposition 7. Let θ(x be a positive function on R and γ(x be the function defined by γ(x = exp( x exp(t [(1 + tθ(t 1] dt + 1. If exp(x θ(x for all x R. Then exp(x ω(x for all x R. For instance, if θ(x = cosh ( x, we have ( γ(x = 8 exp( x (7 + x cosh x + ( (5 + x sinh x. However, one can show that γ(x is not better to f(x for all x R. 6. Proofs Proof of Proposition 1. Let us set g(x = exp(x f(x. We aim to study this function. It follows from several algebraic manipulations that g (x = x exp(x 1 [ ( exp x (3 4x + ( x exp x (3 + 4x + ] x. (3 In order to study the sign of g (x, let us investigate g (x. Algebraic manipulations and simplifications give [ ( ] g (x = (1 + x exp(x cosh x. (4 Owing to the elementary inequality: exp(x cosh ( x, we have g (x. Thus g (x is increasing. Since g ( =, the minimum of g(x is attained in x = : for all x R, we have g(x g( =, implying that exp(x f(x. The second inequality can be prove in a similar manner. Let us set h(x = f(x 1. It follows from several algebraic manipulations that h (x = 1 [ ( exp x (3 4x + ( x exp x (3 + 4x + ] x 8

10 and ( h (x = (1 + x cosh x. So h (x and h (x is increasing. Since h ( =, for all x R, we have h(x h( =. Hence f(x 1. This ends the proof of Proposition 1. Proof of Proposition. Let us prove that, for all x R, f(x cosh ( x, f(x exp(x x and f(x 1 + x + x 4 /, in turn. Proof for f(x cosh ( x. Let us set k(x = f(x cosh ( x. After calculus and simplifications, we obtain k (x = ( x + ( x exp x ( + x + ( x exp x and ( k (x = 4 cosh x x. Since k (x, k (x is increasing. Since k ( =, for all x R, we have k(x k( =, implying the desired inequality. Proof for f(x exp(x x. Let us set l(x = f(x exp(x + x. After calculus and simplifications, we obtain l (x = 1 [ ( exp x (3 4x + ( x exp x (3 + 4x + ] x exp(x + and ( l (x = (1 + x cosh x exp(x. We have l (x cosh ( x exp(x, so l (x is increasing. Since l ( =, for all x R, we have l(x l( =, implying the desired inequality. Proof for f(x 1 + x + x 4 /. Let us set m(x = f(x (1 + x + x 4 /. After calculus and simplifications, we obtain m (x = 1 [ ( exp x (3 4x + ( x exp x (3 + 4x + ] x 4x(1 + x and ( m (x = (1 + x cosh x 6x. Since cosh ( x = + ( k x /(k! > 1+x, we have m (x (1+x (1+x 6x = 4x 4. k= Thus m (x is increasing. Since m ( =, for all x R, we have m(x m( =, implying the desired inequality. The proof of Proposition is complete. On Remark 1. Let us set ρ(x = (1/[1 + (x/a]. Since x a, observe that ρ(x [, 1]. Also, we can write x = ρ(x(ax + (1 ρ(x( ax. Owing to the convexity of the function exp(y, we have This completes Remark 1. exp(x = exp [ρ(x(ax + (1 ρ(x( ax] ρ(x exp(ax + (1 ρ(x exp( ax = cosh (ax + x sinh (ax. a 9

11 Proof of Lemma 1. Let us set p(x = exp(x cosh ( x P n (x. Then we have and p (x = x exp(x ( sinh x 4 n k= x k+3 k!(k + 3 ( n p (x = exp(x + 4x exp(x cosh x 4x ( ( = exp(x cosh x + 4x (exp(x It follows from the well-know inequalities: exp(x cosh ( x and exp(x = + x k /k! > k= n k= x k k! x k k! k=. n k= x k /k! that p (x. So p (x is increasing and since p ( =, for all x R, we have p(x p( =. This concludes the proof of Lemma 1. Proof of Proposition 3. Set g(x = exp(x f(x and q(x = exp(x f (x; n = g(x Q n (x. Let us recall that g (x and g (x have been determined in (3 and (4 respectively. We have n q (x = g (x 4x 5 x k ( 1 k!(k + 3(k + k x k + 7 and, by (4, k= q (x = g (x 4(1 + x x 4 n k= x k k!(k + 3(k + [ ( n = (1 + x exp(x cosh x x 4 k= ] x k. k!(k + 3(k + It follows from Lemma 1 that q (x, implying that q (x is increasing and since q ( =, for all x R, we have q(x q( =. So exp(x f (x; n. Since Q n (x for all x R and n N, it is clear that f (x; n f(x. The proof of Proposition 3 is complete. Proof of Proposition 4. Using x = ( x a + a x a and Proposition 1, we have exp(x = exp(( x a exp(a x a f( x a exp(a x a. Let us set v(x; a = f( x a exp(a x a. Hence we have exp(x max [f(x, v(x; a]. We will now show that v(x; a can be a better lower bound to f(x for some x. Let us study it according to the variable a. After several algebraic calculus and simplifications, we obtain a v(x; a = exp ( a x a w( x a, where w(y is the function defined by w(y = 1 [ ( exp y (3 + 18y + 1 ( y + 4y 3 + exp y ( y 1 ] y + 4y 3 1y, Since exp ( a x a >, we need to determine the sign of w( x a. Let us show that w(y is increasing on R. After several algebraic calculus and simplifications, we have ( w (y = exp y (6 + y 4y ( y 3 + exp y (6 y 4y + y 3 1, 1

12 ( w (y = exp y ( 5 1y ( y + 4y 3 + exp y (5 1y + y + 4y 3 and [ ( w (y = y exp y (3 + 8y ( y + exp y ( 3 + 8y + ] y. Let us observe that this last function is even and of the form w (y = y (R(y R( y, with R(y = exp ( y ( 3 + 8y + y. So it is enough to study its sign on [,, which corresponds to the sign of R(y R( y on [,. We have, for all y, [ ( (R(y R( y = exp y (1 6 ( y + y + exp y (1 + 6 ] y + y ( = 4(1 + y cosh y + 4 ( y sinh y. So R(y R( y is increasing on [,, we have R(y R( y R( R( = for all y, and, a fortiori, w (y = y (R(y R( y for all y. Since w (y is even, we have w (y for all y R. This implies that w (y is increasing on R. Since w ( =, w (y is decreasing (, ] and increasing on (,. So w (y w ( = implying that w(y is increasing on R. It follows from this result that, if a < x, we have w( x a > w( =, implying that av(x; a >, so v(x; a is strictly increasing according to a. If a > x, we have w( x a < w( =, implying that av(x; a <, so v(x; a is strictly decreasing according to a. Clearly, we have av(x; a = if and only if a = x. Since f(x is an even function and v(x; = v(x; x = f(x, for all x a/, we have exp(x = v(x; x = For x < a/, we have Hence, for all x R, we have sup v(x; a v(x; a inf v(x; a = inf [v(x;, v(x; x ] = f(x. a [, x ] a [, x ] f(x = inf v(x; a sup v(x; a v(x; a. a [, x ] a> x exp(x max [f(x, v(x; a] = f(x1 { x <a/} (x + v(x; a1 { x a/} (x = f (x; a f(x. Proposition 1 is proved. Proof of Proposition 5. Let us prove the two points in turn. Let us remark that, by two successive integrations, we have so (1 + t exp(t dt dy = exp(x = Owing to exp(x θ(x, we have Hence exp(x ω(x. exp(x ω(x = y exp(y dy = exp(x 1, (1 + t exp(t dt dy + 1. (5 (1 + t [ exp(t θ(t ] dt dy. 11

13 Let us define the function β(x by Then we have β (x = x β(x = x (1 + t θ(tdt dy + 1 θ(x. (1 + t θ(tdt θ (x, β (x = (1 + x θ(x θ (x. Thanks to the assumption (1 + x θ(x θ (x, we have β (x, implying that β (x is increasing. Since θ ( =, we have β ( = and the minimum of β(x is attained in x =. Since θ( = 1, for all x, we have β(x β( =, implying that β( x for all x R. Since θ(x is even, we have ω(x = (1 + t θ(tdt dy + 1 θ(x. The proof of Proposition 5 is complete. Proof of Proposition 6. We proceed as the proof of Proposition 5. If follows from the equality (5, exp(x θ 1 (x and exp(x θ (x that exp(x κ(x = Hence exp(x κ(x. Let us define the function φ(x by x φ(x = Two differentiations give φ (x = x [ (exp(t θ 1 (t + t (exp(t θ (t ] dt dy. (θ 1 (t + t θ (tdt dy + 1 θ 1 (x. (θ 1 (t + t θ (tdt θ 1(x, φ (x = (θ 1 (x + x θ (x θ 1 (x. Since (θ 1 (x + x θ (x θ 1 (x, we have φ (x, implying that φ (x is increasing. Since θ 1( =, we have φ ( = and the minimum of φ(x is attained in x =. Since θ( = 1, for all x, we have φ(x φ( =, implying that φ( x for all x R. Since θ(x is even, we have κ(x = By exchanging the role of θ 1 (x and θ (x, we obtain κ(x = This ends the proof of Proposition 6. Proof of Proposition 7. We have (θ 1 (t + t θ (tdt dy + 1 θ 1 (x. (θ 1 (t + t θ (tdt dy + 1 θ (x. exp(t [ (1 + t exp(t 1 ] dt = [ exp(t + t exp(t ] x = exp( x ( exp(x 1, 1

14 so exp(x = 1 + exp( x If exp(x θ(x for all x R, we have exp(x 1 + exp( x Proposition 7 is proved. exp(t [ (1 + t exp(t 1 ] dt. exp(t [(1 + tθ(t 1] dt = γ(x. References Bae, J. (7. Optimal polynomial lower bounds for the exponential function, Honam Math. J. 9, 4, Bae, J. and Kim, S. (9. On a generalization of an upper bound for the exponential function, J. of Math. Anal. and Appl. 353, 1, 1 7. Bagul, Y.J. (17. Inequalities involving circular, hyperbolic and exponential functions. Journal of Mathematical inequalities, 11, 3, Brenner, J. L. and Alzer, H. (1991. Proc. R. Soc. Edinburgh, Bullen, P. S. (1998. A Dictionary of Inequalities. Pitman Monographs and Surveys in Pure and Applied Mathematics, Vol. 97, Longman, Harlow. Chesneau, C. (17. On two simple and sharp lower bounds for exp(x, preprint. Kim, S. (7. Densely algebraic bounds for the exponential function, Proc. Amer. Math. Soc. 135, Kuang, J. (1993. Applied Inequalities, nd edition. Hunan Education Press, Chang- sha, China. Mitrinović, D. S. (1964. Elementary Inequalities. P. Noordhoff Ltd., Groningen. Qi, F. (1997. A method of constructing inequalities about e x, Univ. Beograd. Publ. Elektrotehn. Fak. Ser. Mat., 8, 16 3, (1997. Wolfram, S. (1999. The Mathematica Book (4th edition, Cambridge Univ. Pr., Cambridge. Also see, 13

A new simple recursive algorithm for finding prime numbers using Rosser s theorem

A new simple recursive algorithm for finding prime numbers using Rosser s theorem A new simple recursive algorithm for finding prime numbers using Rosser s theorem Rédoane Daoudi To cite this version: Rédoane Daoudi. A new simple recursive algorithm for finding prime numbers using Rosser

More information

Cutwidth and degeneracy of graphs

Cutwidth and degeneracy of graphs Cutwidth and degeneracy of graphs Benoit Kloeckner To cite this version: Benoit Kloeckner. Cutwidth and degeneracy of graphs. IF_PREPUB. 2009. HAL Id: hal-00408210 https://hal.archives-ouvertes.fr/hal-00408210v1

More information

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space Chérif Amrouche, Huy Hoang Nguyen To cite this version: Chérif Amrouche, Huy Hoang Nguyen. New estimates

More information

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Matthieu Denoual, Gilles Allègre, Patrick Attia, Olivier De Sagazan To cite this version: Matthieu Denoual, Gilles Allègre, Patrick Attia,

More information

On size, radius and minimum degree

On size, radius and minimum degree On size, radius and minimum degree Simon Mukwembi To cite this version: Simon Mukwembi. On size, radius and minimum degree. Discrete Mathematics and Theoretical Computer Science, DMTCS, 2014, Vol. 16 no.

More information

DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS

DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS Issam Naghmouchi To cite this version: Issam Naghmouchi. DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS. 2010. HAL Id: hal-00593321 https://hal.archives-ouvertes.fr/hal-00593321v2

More information

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach Christophe Cruz, Helmi Ben Hmida, Frank Boochs, Christophe Nicolle To cite this version: Christophe Cruz, Helmi Ben Hmida,

More information

On the longest path in a recursively partitionable graph

On the longest path in a recursively partitionable graph On the longest path in a recursively partitionable graph Julien Bensmail To cite this version: Julien Bensmail. On the longest path in a recursively partitionable graph. 2012. HAL Id:

More information

Hook lengths and shifted parts of partitions

Hook lengths and shifted parts of partitions Hook lengths and shifted parts of partitions Guo-Niu Han To cite this version: Guo-Niu Han Hook lengths and shifted parts of partitions The Ramanujan Journal, 009, 9 p HAL Id: hal-00395690

More information

A remark on a theorem of A. E. Ingham.

A remark on a theorem of A. E. Ingham. A remark on a theorem of A. E. Ingham. K G Bhat, K Ramachandra To cite this version: K G Bhat, K Ramachandra. A remark on a theorem of A. E. Ingham.. Hardy-Ramanujan Journal, Hardy-Ramanujan Society, 2006,

More information

A Context free language associated with interval maps

A Context free language associated with interval maps A Context free language associated with interval maps M Archana, V Kannan To cite this version: M Archana, V Kannan. A Context free language associated with interval maps. Discrete Mathematics and Theoretical

More information

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122,

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, 244902 Juan Olives, Zoubida Hammadi, Roger Morin, Laurent Lapena To cite this version: Juan Olives,

More information

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma.

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Loïc De Pontual, Delphine Trochet, Franck Bourdeaut, Sophie Thomas, Heather Etchevers, Agnes Chompret, Véronique Minard,

More information

Lower bound of the covering radius of binary irreducible Goppa codes

Lower bound of the covering radius of binary irreducible Goppa codes Lower bound of the covering radius of binary irreducible Goppa codes Sergey Bezzateev, Natalia Shekhunova To cite this version: Sergey Bezzateev, Natalia Shekhunova. Lower bound of the covering radius

More information

The Mahler measure of trinomials of height 1

The Mahler measure of trinomials of height 1 The Mahler measure of trinomials of height 1 Valérie Flammang To cite this version: Valérie Flammang. The Mahler measure of trinomials of height 1. Journal of the Australian Mathematical Society 14 9 pp.1-4.

More information

A Simple Proof of P versus NP

A Simple Proof of P versus NP A Simple Proof of P versus NP Frank Vega To cite this version: Frank Vega. A Simple Proof of P versus NP. 2016. HAL Id: hal-01281254 https://hal.archives-ouvertes.fr/hal-01281254 Submitted

More information

Low frequency resolvent estimates for long range perturbations of the Euclidean Laplacian

Low frequency resolvent estimates for long range perturbations of the Euclidean Laplacian Low frequency resolvent estimates for long range perturbations of the Euclidean Laplacian Jean-Francois Bony, Dietrich Häfner To cite this version: Jean-Francois Bony, Dietrich Häfner. Low frequency resolvent

More information

A note on the computation of the fraction of smallest denominator in between two irreducible fractions

A note on the computation of the fraction of smallest denominator in between two irreducible fractions A note on the computation of the fraction of smallest denominator in between two irreducible fractions Isabelle Sivignon To cite this version: Isabelle Sivignon. A note on the computation of the fraction

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 016 HAL Id: hal-0131860

More information

Easter bracelets for years

Easter bracelets for years Easter bracelets for 5700000 years Denis Roegel To cite this version: Denis Roegel. Easter bracelets for 5700000 years. [Research Report] 2014. HAL Id: hal-01009457 https://hal.inria.fr/hal-01009457

More information

Completeness of the Tree System for Propositional Classical Logic

Completeness of the Tree System for Propositional Classical Logic Completeness of the Tree System for Propositional Classical Logic Shahid Rahman To cite this version: Shahid Rahman. Completeness of the Tree System for Propositional Classical Logic. Licence. France.

More information

Axiom of infinity and construction of N

Axiom of infinity and construction of N Axiom of infinity and construction of N F Portal To cite this version: F Portal. Axiom of infinity and construction of N. 2015. HAL Id: hal-01162075 https://hal.archives-ouvertes.fr/hal-01162075 Submitted

More information

approximation results for the Traveling Salesman and related Problems

approximation results for the Traveling Salesman and related Problems approximation results for the Traveling Salesman and related Problems Jérôme Monnot To cite this version: Jérôme Monnot. approximation results for the Traveling Salesman and related Problems. Information

More information

Exact Comparison of Quadratic Irrationals

Exact Comparison of Quadratic Irrationals Exact Comparison of Quadratic Irrationals Phuc Ngo To cite this version: Phuc Ngo. Exact Comparison of Quadratic Irrationals. [Research Report] LIGM. 20. HAL Id: hal-0069762 https://hal.archives-ouvertes.fr/hal-0069762

More information

A note on the acyclic 3-choosability of some planar graphs

A note on the acyclic 3-choosability of some planar graphs A note on the acyclic 3-choosability of some planar graphs Hervé Hocquard, Mickael Montassier, André Raspaud To cite this version: Hervé Hocquard, Mickael Montassier, André Raspaud. A note on the acyclic

More information

Can we reduce health inequalities? An analysis of the English strategy ( )

Can we reduce health inequalities? An analysis of the English strategy ( ) Can we reduce health inequalities? An analysis of the English strategy (1997-2010) Johan P Mackenbach To cite this version: Johan P Mackenbach. Can we reduce health inequalities? An analysis of the English

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 015 HAL Id: hal-0131860

More information

b-chromatic number of cacti

b-chromatic number of cacti b-chromatic number of cacti Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva To cite this version: Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva. b-chromatic number

More information

A new approach of the concept of prime number

A new approach of the concept of prime number A new approach of the concept of prime number Jamel Ghannouchi To cite this version: Jamel Ghannouchi. A new approach of the concept of prime number. 4 pages. 24. HAL Id: hal-3943 https://hal.archives-ouvertes.fr/hal-3943

More information

Some explanations about the IWLS algorithm to fit generalized linear models

Some explanations about the IWLS algorithm to fit generalized linear models Some explanations about the IWLS algorithm to fit generalized linear models Christophe Dutang To cite this version: Christophe Dutang. Some explanations about the IWLS algorithm to fit generalized linear

More information

Vibro-acoustic simulation of a car window

Vibro-acoustic simulation of a car window Vibro-acoustic simulation of a car window Christophe Barras To cite this version: Christophe Barras. Vibro-acoustic simulation of a car window. Société Française d Acoustique. Acoustics 12, Apr 12, Nantes,

More information

The Windy Postman Problem on Series-Parallel Graphs

The Windy Postman Problem on Series-Parallel Graphs The Windy Postman Problem on Series-Parallel Graphs Francisco Javier Zaragoza Martínez To cite this version: Francisco Javier Zaragoza Martínez. The Windy Postman Problem on Series-Parallel Graphs. Stefan

More information

A proximal approach to the inversion of ill-conditioned matrices

A proximal approach to the inversion of ill-conditioned matrices A proximal approach to the inversion of ill-conditioned matrices Pierre Maréchal, Aude Rondepierre To cite this version: Pierre Maréchal, Aude Rondepierre. A proximal approach to the inversion of ill-conditioned

More information

On a series of Ramanujan

On a series of Ramanujan On a series of Ramanujan Olivier Oloa To cite this version: Olivier Oloa. On a series of Ramanujan. Gems in Experimental Mathematics, pp.35-3,, . HAL Id: hal-55866 https://hal.archives-ouvertes.fr/hal-55866

More information

On path partitions of the divisor graph

On path partitions of the divisor graph On path partitions of the divisor graph Paul Melotti, Eric Saias To cite this version: Paul Melotti, Eric Saias On path partitions of the divisor graph 018 HAL Id: hal-0184801 https://halarchives-ouvertesfr/hal-0184801

More information

On infinite permutations

On infinite permutations On infinite permutations Dmitri G. Fon-Der-Flaass, Anna E. Frid To cite this version: Dmitri G. Fon-Der-Flaass, Anna E. Frid. On infinite permutations. Stefan Felsner. 2005 European Conference on Combinatorics,

More information

On the link between finite differences and derivatives of polynomials

On the link between finite differences and derivatives of polynomials On the lin between finite differences and derivatives of polynomials Kolosov Petro To cite this version: Kolosov Petro. On the lin between finite differences and derivatives of polynomials. 13 pages, 1

More information

Thomas Lugand. To cite this version: HAL Id: tel

Thomas Lugand. To cite this version: HAL Id: tel Contribution à la Modélisation et à l Optimisation de la Machine Asynchrone Double Alimentation pour des Applications Hydrauliques de Pompage Turbinage Thomas Lugand To cite this version: Thomas Lugand.

More information

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 Sibiri Christian Bandre To cite this version: Sibiri Christian Bandre. There are infinitely many twin primes

More information

A generalization of Cramér large deviations for martingales

A generalization of Cramér large deviations for martingales A generalization of Cramér large deviations for martingales Xiequan Fan, Ion Grama, Quansheng Liu To cite this version: Xiequan Fan, Ion Grama, Quansheng Liu. A generalization of Cramér large deviations

More information

Comments on the method of harmonic balance

Comments on the method of harmonic balance Comments on the method of harmonic balance Ronald Mickens To cite this version: Ronald Mickens. Comments on the method of harmonic balance. Journal of Sound and Vibration, Elsevier, 1984, 94 (3), pp.456-460.

More information

Self-dual skew codes and factorization of skew polynomials

Self-dual skew codes and factorization of skew polynomials Self-dual skew codes and factorization of skew polynomials Delphine Boucher, Félix Ulmer To cite this version: Delphine Boucher, Félix Ulmer. Self-dual skew codes and factorization of skew polynomials.

More information

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Shahid Rahman To cite this version: Shahid Rahman. Soundness of the System of Semantic Trees for Classical Logic

More information

ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS

ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS Abdelhafid Younsi To cite this version: Abdelhafid Younsi. ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS. 4 pages. 212. HAL Id:

More information

Solving a quartic equation and certain equations with degree n

Solving a quartic equation and certain equations with degree n Solving a quartic equation and certain equations with degree n Abdeljalil Saghe To cite this version: Abdeljalil Saghe. Solving a quartic equation and certain equations with degree n. EUROPEAN JOURNAL

More information

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications Alexandre Sedoglavic To cite this version: Alexandre Sedoglavic. A non-commutative algorithm for multiplying (7 7) matrices

More information

Unfolding the Skorohod reflection of a semimartingale

Unfolding the Skorohod reflection of a semimartingale Unfolding the Skorohod reflection of a semimartingale Vilmos Prokaj To cite this version: Vilmos Prokaj. Unfolding the Skorohod reflection of a semimartingale. Statistics and Probability Letters, Elsevier,

More information

Periodic solutions of differential equations with three variable in vector-valued space

Periodic solutions of differential equations with three variable in vector-valued space Periodic solutions of differential equations with three variable in vector-valued space Bahloul Rachid, Bahaj Mohamed, Sidki Omar To cite this version: Bahloul Rachid, Bahaj Mohamed, Sidki Omar. Periodic

More information

Analysis of Boyer and Moore s MJRTY algorithm

Analysis of Boyer and Moore s MJRTY algorithm Analysis of Boyer and Moore s MJRTY algorithm Laurent Alonso, Edward M. Reingold To cite this version: Laurent Alonso, Edward M. Reingold. Analysis of Boyer and Moore s MJRTY algorithm. Information Processing

More information

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle Nathalie Olivi-Tran, Paul M Gauthier To cite this version:

More information

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation On Poincare-Wirtinger inequalities in spaces of functions of bounded variation Maïtine Bergounioux To cite this version: Maïtine Bergounioux. On Poincare-Wirtinger inequalities in spaces of functions of

More information

Some diophantine problems concerning equal sums of integers and their cubes

Some diophantine problems concerning equal sums of integers and their cubes Some diophantine problems concerning equal sums of integers and their cubes Ajai Choudhry To cite this version: Ajai Choudhry. Some diophantine problems concerning equal sums of integers and their cubes.

More information

On Newton-Raphson iteration for multiplicative inverses modulo prime powers

On Newton-Raphson iteration for multiplicative inverses modulo prime powers On Newton-Raphson iteration for multiplicative inverses modulo prime powers Jean-Guillaume Dumas To cite this version: Jean-Guillaume Dumas. On Newton-Raphson iteration for multiplicative inverses modulo

More information

Norm Inequalities of Positive Semi-Definite Matrices

Norm Inequalities of Positive Semi-Definite Matrices Norm Inequalities of Positive Semi-Definite Matrices Antoine Mhanna To cite this version: Antoine Mhanna Norm Inequalities of Positive Semi-Definite Matrices 15 HAL Id: hal-11844 https://halinriafr/hal-11844v1

More information

Full-order observers for linear systems with unknown inputs

Full-order observers for linear systems with unknown inputs Full-order observers for linear systems with unknown inputs Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu To cite this version: Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu. Full-order observers

More information

Passerelle entre les arts : la sculpture sonore

Passerelle entre les arts : la sculpture sonore Passerelle entre les arts : la sculpture sonore Anaïs Rolez To cite this version: Anaïs Rolez. Passerelle entre les arts : la sculpture sonore. Article destiné à l origine à la Revue de l Institut National

More information

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Marie Duhamel To cite this version: Marie Duhamel. Evolution of the cooperation and consequences

More information

Nel s category theory based differential and integral Calculus, or Did Newton know category theory?

Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Elemer Elad Rosinger To cite this version: Elemer Elad Rosinger. Nel s category theory based differential

More information

Entropies and fractal dimensions

Entropies and fractal dimensions Entropies and fractal dimensions Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. Entropies and fractal dimensions. Philica, Philica, 2016. HAL Id: hal-01377975

More information

Confluence Algebras and Acyclicity of the Koszul Complex

Confluence Algebras and Acyclicity of the Koszul Complex Confluence Algebras and Acyclicity of the Koszul Complex Cyrille Chenavier To cite this version: Cyrille Chenavier. Confluence Algebras and Acyclicity of the Koszul Complex. Algebras and Representation

More information

The Accelerated Euclidean Algorithm

The Accelerated Euclidean Algorithm The Accelerated Euclidean Algorithm Sidi Mohamed Sedjelmaci To cite this version: Sidi Mohamed Sedjelmaci The Accelerated Euclidean Algorithm Laureano Gonzales-Vega and Thomas Recio Eds 2004, University

More information

A Study of the Regular Pentagon with a Classic Geometric Approach

A Study of the Regular Pentagon with a Classic Geometric Approach A Study of the Regular Pentagon with a Classic Geometric Approach Amelia Carolina Sparavigna, Mauro Maria Baldi To cite this version: Amelia Carolina Sparavigna, Mauro Maria Baldi. A Study of the Regular

More information

Dispersion relation results for VCS at JLab

Dispersion relation results for VCS at JLab Dispersion relation results for VCS at JLab G. Laveissiere To cite this version: G. Laveissiere. Dispersion relation results for VCS at JLab. Compton Scattering from Low to High Momentum Transfer, Mar

More information

On one class of permutation polynomials over finite fields of characteristic two *

On one class of permutation polynomials over finite fields of characteristic two * On one class of permutation polynomials over finite fields of characteristic two * Leonid Bassalygo, Victor A. Zinoviev To cite this version: Leonid Bassalygo, Victor A. Zinoviev. On one class of permutation

More information

L institution sportive : rêve et illusion

L institution sportive : rêve et illusion L institution sportive : rêve et illusion Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar To cite this version: Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar. L institution sportive : rêve et illusion. Revue

More information

Differential approximation results for the Steiner tree problem

Differential approximation results for the Steiner tree problem Differential approximation results for the Steiner tree problem Marc Demange, Jérôme Monnot, Vangelis Paschos To cite this version: Marc Demange, Jérôme Monnot, Vangelis Paschos. Differential approximation

More information

Numerical Exploration of the Compacted Associated Stirling Numbers

Numerical Exploration of the Compacted Associated Stirling Numbers Numerical Exploration of the Compacted Associated Stirling Numbers Khaled Ben Letaïef To cite this version: Khaled Ben Letaïef. Numerical Exploration of the Compacted Associated Stirling Numbers. 2017.

More information

On the Griesmer bound for nonlinear codes

On the Griesmer bound for nonlinear codes On the Griesmer bound for nonlinear codes Emanuele Bellini, Alessio Meneghetti To cite this version: Emanuele Bellini, Alessio Meneghetti. On the Griesmer bound for nonlinear codes. Pascale Charpin, Nicolas

More information

RENORMALISATION ON THE PENROSE LATTICE

RENORMALISATION ON THE PENROSE LATTICE RENORMALISATION ON THE PENROSE LATTICE C. Godreche, Henri Orland To cite this version: C. Godreche, Henri Orland. RENORMALISATION ON THE PENROSE LATTICE. Journal de Physique Colloques, 1986, 47 (C3), pp.c3-197-c3-203.

More information

Cramér large deviation expansions for martingales under Bernstein s condition

Cramér large deviation expansions for martingales under Bernstein s condition Cramér large deviation expansions for martingales under Bernstein s condition Xiequan Fan, Ion Grama, Quansheng Liu To cite this version: Xiequan Fan, Ion Grama, Quansheng Liu. Cramér large deviation expansions

More information

Linear Quadratic Zero-Sum Two-Person Differential Games

Linear Quadratic Zero-Sum Two-Person Differential Games Linear Quadratic Zero-Sum Two-Person Differential Games Pierre Bernhard To cite this version: Pierre Bernhard. Linear Quadratic Zero-Sum Two-Person Differential Games. Encyclopaedia of Systems and Control,

More information

All Associated Stirling Numbers are Arithmetical Triangles

All Associated Stirling Numbers are Arithmetical Triangles All Associated Stirling Numbers are Arithmetical Triangles Khaled Ben Letaïef To cite this version: Khaled Ben Letaïef. All Associated Stirling Numbers are Arithmetical Triangles. 2017.

More information

Multiple sensor fault detection in heat exchanger system

Multiple sensor fault detection in heat exchanger system Multiple sensor fault detection in heat exchanger system Abdel Aïtouche, Didier Maquin, Frédéric Busson To cite this version: Abdel Aïtouche, Didier Maquin, Frédéric Busson. Multiple sensor fault detection

More information

Tropical Graph Signal Processing

Tropical Graph Signal Processing Tropical Graph Signal Processing Vincent Gripon To cite this version: Vincent Gripon. Tropical Graph Signal Processing. 2017. HAL Id: hal-01527695 https://hal.archives-ouvertes.fr/hal-01527695v2

More information

Finite Volume for Fusion Simulations

Finite Volume for Fusion Simulations Finite Volume for Fusion Simulations Elise Estibals, Hervé Guillard, Afeintou Sangam To cite this version: Elise Estibals, Hervé Guillard, Afeintou Sangam. Finite Volume for Fusion Simulations. Jorek Meeting

More information

Unbiased minimum variance estimation for systems with unknown exogenous inputs

Unbiased minimum variance estimation for systems with unknown exogenous inputs Unbiased minimum variance estimation for systems with unknown exogenous inputs Mohamed Darouach, Michel Zasadzinski To cite this version: Mohamed Darouach, Michel Zasadzinski. Unbiased minimum variance

More information

Sparse multivariate factorization by mean of a few bivariate factorizations

Sparse multivariate factorization by mean of a few bivariate factorizations Sparse multivariate factorization by mean of a few bivariate factorizations Bernard Parisse To cite this version: Bernard Parisse. Sparse multivariate factorization by mean of a few bivariate factorizations.

More information

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Bernard Brogliato To cite this version: Bernard Brogliato. Dissipative Systems Analysis and Control, Theory and Applications:

More information

On The Exact Solution of Newell-Whitehead-Segel Equation Using the Homotopy Perturbation Method

On The Exact Solution of Newell-Whitehead-Segel Equation Using the Homotopy Perturbation Method On The Exact Solution of Newell-Whitehead-Segel Equation Using the Homotopy Perturbation Method S. Salman Nourazar, Mohsen Soori, Akbar Nazari-Golshan To cite this version: S. Salman Nourazar, Mohsen Soori,

More information

Replicator Dynamics and Correlated Equilibrium

Replicator Dynamics and Correlated Equilibrium Replicator Dynamics and Correlated Equilibrium Yannick Viossat To cite this version: Yannick Viossat. Replicator Dynamics and Correlated Equilibrium. CECO-208. 2004. HAL Id: hal-00242953

More information

Trajectory Optimization for Differential Flat Systems

Trajectory Optimization for Differential Flat Systems Trajectory Optimization for Differential Flat Systems Kahina Louadj, Benjamas Panomruttanarug, Alexre Carlos Brao-Ramos, Felix Antonio Claudio Mora-Camino To cite this version: Kahina Louadj, Benjamas

More information

Towards an active anechoic room

Towards an active anechoic room Towards an active anechoic room Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède To cite this version: Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède. Towards an active

More information

A Slice Based 3-D Schur-Cohn Stability Criterion

A Slice Based 3-D Schur-Cohn Stability Criterion A Slice Based 3-D Schur-Cohn Stability Criterion Ioana Serban, Mohamed Najim To cite this version: Ioana Serban, Mohamed Najim. A Slice Based 3-D Schur-Cohn Stability Criterion. ICASSP 007, Apr 007, Honolulu,

More information

IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE

IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE V. Szekely, S. Torok, E. Kollar To cite this version: V. Szekely, S. Torok, E. Kollar. IMPROVEMENTS OF THE VARIABLE THERMAL RESIS- TANCE. THERMINIC 2007,

More information

Solving the neutron slowing down equation

Solving the neutron slowing down equation Solving the neutron slowing down equation Bertrand Mercier, Jinghan Peng To cite this version: Bertrand Mercier, Jinghan Peng. Solving the neutron slowing down equation. 2014. HAL Id: hal-01081772

More information

Symmetric Norm Inequalities And Positive Semi-Definite Block-Matrices

Symmetric Norm Inequalities And Positive Semi-Definite Block-Matrices Symmetric Norm Inequalities And Positive Semi-Definite lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna Symmetric Norm Inequalities And Positive Semi-Definite lock-matrices 15

More information

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Susumu Kato, Eisuke Miura, Mitsumori Tanimoto, Masahiro Adachi, Kazuyoshi Koyama To cite this

More information

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES Antonin Pottier, Rabia Nessah To cite this version: Antonin Pottier, Rabia Nessah. BERGE VAISMAN AND NASH EQUILIBRIA: TRANS- FORMATION OF GAMES.

More information

Stickelberger s congruences for absolute norms of relative discriminants

Stickelberger s congruences for absolute norms of relative discriminants Stickelberger s congruences for absolute norms of relative discriminants Georges Gras To cite this version: Georges Gras. Stickelberger s congruences for absolute norms of relative discriminants. Journal

More information

The core of voting games: a partition approach

The core of voting games: a partition approach The core of voting games: a partition approach Aymeric Lardon To cite this version: Aymeric Lardon. The core of voting games: a partition approach. International Game Theory Review, World Scientific Publishing,

More information

Quasi-Lovász Extensions and Their Symmetric Counterparts

Quasi-Lovász Extensions and Their Symmetric Counterparts Quasi-Lovász Extensions and Their Symmetric Counterparts Miguel Couceiro, Jean-Luc Marichal To cite this version: Miguel Couceiro, Jean-Luc Marichal. Quasi-Lovász Extensions and Their Symmetric Counterparts.

More information

Computer Visualization of the Riemann Zeta Function

Computer Visualization of the Riemann Zeta Function Computer Visualization of the Riemann Zeta Function Kamal Goudjil To cite this version: Kamal Goudjil. Computer Visualization of the Riemann Zeta Function. 2017. HAL Id: hal-01441140 https://hal.archives-ouvertes.fr/hal-01441140

More information

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart To cite this version: Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart.

More information

Thermodynamic form of the equation of motion for perfect fluids of grade n

Thermodynamic form of the equation of motion for perfect fluids of grade n Thermodynamic form of the equation of motion for perfect fluids of grade n Henri Gouin To cite this version: Henri Gouin. Thermodynamic form of the equation of motion for perfect fluids of grade n. Comptes

More information

Positive mass theorem for the Paneitz-Branson operator

Positive mass theorem for the Paneitz-Branson operator Positive mass theorem for the Paneitz-Branson operator Emmanuel Humbert, Simon Raulot To cite this version: Emmanuel Humbert, Simon Raulot. Positive mass theorem for the Paneitz-Branson operator. Calculus

More information

Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle

Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle Roland Bacher To cite this version: Roland Bacher. Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle.

More information

Sharp inequalities and complete monotonicity for the Wallis ratio

Sharp inequalities and complete monotonicity for the Wallis ratio Sharp inequalities and complete monotonicity for the Wallis ratio Cristinel Mortici Abstract The aim of this paper is to prove the complete monotonicity of a class of functions arising from Kazarinoff

More information

On constraint qualifications with generalized convexity and optimality conditions

On constraint qualifications with generalized convexity and optimality conditions On constraint qualifications with generalized convexity and optimality conditions Manh-Hung Nguyen, Do Van Luu To cite this version: Manh-Hung Nguyen, Do Van Luu. On constraint qualifications with generalized

More information

Theoretical calculation of the power of wind turbine or tidal turbine

Theoretical calculation of the power of wind turbine or tidal turbine Theoretical calculation of the power of wind turbine or tidal turbine Pierre Lecanu, Joel Breard, Dominique Mouazé To cite this version: Pierre Lecanu, Joel Breard, Dominique Mouazé. Theoretical calculation

More information

Hardware Operator for Simultaneous Sine and Cosine Evaluation

Hardware Operator for Simultaneous Sine and Cosine Evaluation Hardware Operator for Simultaneous Sine and Cosine Evaluation Arnaud Tisserand To cite this version: Arnaud Tisserand. Hardware Operator for Simultaneous Sine and Cosine Evaluation. ICASSP 6: International

More information