The simplicity of the remainder in certain quadrature formulas

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T. Popoviciu
Institutul de Calcul

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T. Popoviciu, La simplicité du reste dans certaines formules de quadrature, Mathematica (Cluj), 6(29) (1964), pp. 157-184 (in French)

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Mathematica Cluj

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Published by the Romanian Academy  Publishing House

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1222-9016

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2601-744X

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THE SIMPLICITY OF THE REMAINDER IN CERTAIN QUADRATURE FORMULAS

by
TIBERIU POPOVICIU
in Cluj
§ 1.

  1. 1.

    Let us consider the quadrature formula

11f(x)dx=i=1pj=0ki1ci,jf(j)(zi)+R[f]\int_{-1}^{1}f(x)dx=\sum_{i=1}^{p}\sum_{j=0}^{k_{i}-1}c_{i,j}f^{(j)}\left(z_{i}\right)+R[f] (1)

Orz1,z2,,zpz_{1},z_{2},\ldots,z_{p}arep(1)p(\geqq 1)distinct points on the real axis; these are the nodes of the formula.k1,k2,,kpk_{1},k_{2},\ldots,k_{p}areppnatural numbers andci,jc_{i,j}independent coefficients of the functionff.

The functionffis defined, continuous and has a continuous derivative of order equal tomax(k11,k21,,kp1)\max\left(k_{1}-1,k_{2}-1,\ldots,k_{p}-1\right)over an intervalEEcontaining the points1.1-1.1and the knotszi,i=1.2,,pz_{i},i=1,2,\ldots,pThe derivative of order 0 is the function itself.

We will refer to\mathscr{F}all of these functions.\mathscr{F}is a linear set and contains, in particular, all polynomials.

The accents in the second part of (1) denote successive derivations.

In what follows, unless expressly stated otherwise, we will assume thatEEreduces to the smallest closed interval containing the nodes and points1.1-1.1.

The integral of the left-hand side of (1) could be taken between any two finite limits, but we do not restrict the generality by taking these limits to be equal to -1 and 1 respectively. The passage through the interval[1.1][-1,1]at any finite integration interval[HAS,B][A,B]is done using the
linear transformation formulax=2yHASBBHASx = 2y - AB / BASuch a transformation preserves the continuity, differentiability of all orders, and also any convexity of the functions.
2. The second termR[f]R[f]The second term of formula (1) is the remainder of that formula. It is a linear (additive and homogeneous) functional defined on the set\mathscr{F}.

Formula (1) and the remainderR[f]R[f]corresponding values ​​have a degree of accuracy. It is the integern1n\geqq-1completely determined by the condition thatR[f]R[f]let zero on any polynomial of degreennand thatR[xn+1]0R[x^{n+1}] ≠ 0It is also said that formula (1) or the remainderR[f]R[f]the degree of accuracy of this formulannIn the following, we can always assumen0n\geqq 0the casen==1n==-1, not intervening. The conditionn0n\geqq 0is, moreover, equivalent to2=i=1pci,02=\sum_{i=1}^{p}c_{i,0}.

The restR[f]R[f]is said to be of simple form if there exists an integern(0)n(\geqq 0)independent of functionff, such as one might have

R[f]=M[ξ1,ξ2,,ξn+2;f],R[f]=M\left[\xi_{1},\xi_{2},\ldots,\xi_{n+2};f\right], (2)

OrMMEast0\neq 0and independent of the functionff\in\mathscr{F}, the pointsξ1,ξ2,,ξn+2\xi_{1},\xi_{2},\ldots,\xi_{n+2}being distinct, within the intervalEEand dependent, in general, on the functionffIn this case, the numbernnis completely determined (is unique) and is precisely the degree of accuracy ofR[f]R[f].

The rating[ξ1,ξ2,,ξn+2;f]\left[\xi_{1},\xi_{2},\ldots,\xi_{n+2};f\right]denotes the difference divided (of ordern+1)n+1)of the functionffon the points, or the nodes,ξ1,ξ2,,ξn+2\xi_{1},\xi_{2},\ldots,\xi_{n+2}We assume that the definition and main properties of differences divided over distinct or non-distinct nodes are known.

It is easy to see that, under the previous assumptions, the numberMMis equal toR[xn+1]=R[xn+1+P]R\left[x^{n+1}\right]=R\left[x^{n+1}+P\right], OrPPis an arbitrary polynomial of degreenn.

If we agree to designate byDk[f]D_{k}[f]a difference divided by orderkkof the functionffonk+1k+1distinct, unspecified nodes within the intervalEE, formula (2) can be written

R[f]=R[xn+1]Dn+1[f].R[f]=R\left[x^{n+1}\right]D_{n+1}[f]. (3)

We introduced the notion of simplicity of a linear functional, of the nature of remainderR[f]R[f](initially under another name) in other works [5, 6]. We have supplemented and clarified this research in a more detailed paper [9]. We ask the reader to refer to this paper for our earlier results, which will often be implicitly used in the following.

This work is devoted to the study of the simplicity of the remainder in certain quadrature formulas of the form (1) (§§ 1-3). These are, in short, applications of our previous results. In the last § (§ 4) we will make some remarks on the simplicity of the remainder in certain quadrature formulas relating to integrals extended over an infinite interval.
3. The numbersk1,k2,,kpk_{1},k_{2},\ldots,k_{p}are the multiplicity orders of the nodesz1,z2,,zpz_{1},z_{2},\ldots,z_{p}respective. We askk1+k2++kp=mk_{1}+k_{2}+\ldots+k_{p}=mand then we havemp1m\geqq p\geqq 1We can assume thatkik_{i}nodes are confused at the pointziz_{i}Therefore, thatziz_{i}is a node of orderkik_{i}of multiplicity (simple ifki=1k_{i}=1, double ifki=2k_{i}=2etc). The total number of nodes, distinct or not, is therefore equal tommand we can designate these nodes byx1,x2,,xmx_{1},x_{2},\ldots,x_{m}, by choosing the notations, for example, in such a way that we havexk1+k2+ki1+j=zi,j=1.2,,ki,i=1.2,,px_{k_{1}+k_{2}+\ldots k_{i-1}+j}=z_{i},j=1,2,\ldots,k_{i},i=1,2,\ldots,p(the sumk1+k2+,+ki1k_{1}+k_{2}+,\ldots+k_{i-1}being replaced by 0 fori=1i=14.
In what follows we will always assume that the degree of accuracy of formula (1) is at least equal tom1m-1With the previous data, this condition completely determines formula (1), the right-hand side of which is then obtained by approximating the functionffby its Lagrange-Hermite polynomial on the nodesxi,i=1.2,,mx_{i},i=1,2,\ldots,m[7]. If, therefore, we designate bynnthe degree of accuracy of formula (1) and ifnm1n\geqq m-1the coefficientsci,jc_{i,j}are completely determined. Whatever the given nodesx1,x2,,xmx_{1},x_{2},\ldots,x_{m}Therefore, there always exists one and only one formula (1) with a degree of accuracym1\geqq m-1.

Moreover, for given nodes with given multiplicity orders, the calculation of the coefficientsci,jc_{i,j}is, in general, quite complicated. Formula (11), which will be given later (no. 7), gives us

ci,ki1=1(ki1)!j=1jip(zizj)kj1L(x)xzidx,i=1.2,,pc_{i,k_{i}-1}=\frac{1}{\left(k_{i}-1\right)!\prod_{\begin{subarray}{c}j=1\\ j\neq i\end{subarray}}^{p}\left(z_{i}-z_{j}\right)^{k_{j}}}\int_{-1}\frac{l(x)}{x-z_{i}}dx,i=1,2,\ldots,p (4)

Or
L(x)l(x)is the polynomial (6) furthest away.
Forp=1p=1this formula becomes

c1,k11=1(k11)!11(xz1)k11dx=(1z1)k1(1)k1(1+z1)k1k1!c_{1,k_{1}-1}=\frac{1}{\left(k_{1}-1\right)!}\int_{-1}^{1}\left(x-z_{1}\right)^{k_{1}-1 }dx=\frac{\left(1-z_{1}\right)^{k_{1}}-(-1)^{k_{1}}\left(1+z_{1}\right)^{k_{1}}}{k_{1}!} (5)

Calculating the other coefficientsci,jc_{i,j}is more complicated. We will only give it here in certain very specific cases.
5. The degree of accuracy can easily be delimited at a higher level.nnof formula (1) (degree of accuracynm1n\geqq m-1Let's assumen=m++q1n=m++q-1, then the hypothesisnm1n\geqq m-1comes down toq0q\geqq 0Consider the polynomial
(6)

L(x)=i=1m(xxi)=i=1p(xzi)kil(x)=\prod_{i=1}^{m}\left(x-x_{i}\right)=\prod_{i=1}^{p}\left(x-z_{i}\right)^{k_{i}}

The polynomialQ(x)=L(x)i=1p(xzi)1(1)ki2Q(x)=l(x)\prod_{i=1}^{p}\left(x-z_{i}\right)^{\frac{1-(-1)^{k_{i}}}{2}}is of degreem+pm+p, is non-negative (onE)E)and we haveR[Q]=11Q(x)dx>0R[Q]=\int_{-1}^{1}Q(x)dx>0Therefore, we necessarily haveqpq\leqq p.

This delimitation can be refined by taking into account, to some extent, the distribution of the nodes. If we denote byp1p_{1}the number(p)(\leqq p)knotsziz_{i}belonging to the open interval(1.1)(-1.1)we haveqp1q\leqq p_{1}This property can be demonstrated in the same way by taking, instead ofQ(x)Q(x)the polynomialL(x)zi(1.1)(xzi)1(1)ki2l(x)\prod_{z_{i}\in(-1,1)}\left(x-z_{i}\right)^{\frac{1-(-1)^{k_{i}}}{2}}where the product is extended only to those nodes.

6. We have 1st

THEOREM 1. For the formula (1) (of degree of accuracym1\geqq m-1) or of a degree of accuracy equal ton=m+q1n=m+q-1it is necessary and sufficient that the polynomialL(x)l(x)either orthogonal to any polynomial of degreeq1q-1on the interval[1.1][-1,1]and that one has

R[xn+1]=11xqL(x)dx=11Q(x)L(x)dx0R\left[x^{n+1}\right]=\int_{-1}^{1}x^{q}l(x)dx=\int_{-1}^{1}Q(x)l(x)dx\neq 0 (7)

OrQ(x)=xq+P(x),P(x)Q(x) = x^{q} + P(x), P(x)being any polynomial of degreeq1q-1The
condition is necessary. This property results from the formula

R[QL]=11Q(x)L(x)dxR[Ql]=\int_{-1}^{1}Q(x)l(x)dx

ifQ(x)Q(x)is any polynomial.

The condition is sufficient. This property follows from the fact that ifQ,SQ,Sare respectively the quotient and remainder of the division of any polynomialPPby polynomial (6), we haveR[P]=R[QL]+R[S]==R[QL]R[P]=R\left[Q_{l}\right]+R[S]==R[Ql].

We can put the property expressed by Theorem 1 in another form. Let

Pi(x)=1xPi1(x)dx,i=1.2,,P0(x)=L(x)P_{i}(x)=\int_{-1}^{x}P_{i-1}(x)dx,i=1,2,\ldots,P_{0}(x)=l(x) (8)

We then have

Pi(x)=1(i1)!1x(xt)i1L(t)dt,i=1.2,P_{i}(x)=\frac{1}{(i-1)!}\int_{-1}^{x}(x-t)^{i-1}l(t)dt,i=1,2,\ldots

And

Pi(1)=0,Pi(i)(x)=L(x),i=1.2,P_{i}(-1)=0,P_{i}^{(i)}(x)=l(x),i=1,2,\ldots (9)

And it is easy to see that the property expressed by Theorem 1 can be stated in the following equivalent form:

THEOREM 2. For the formula (1) (of degree of accuracym1\geqq m-1) or of a degree of accuracy equal ton=m+q1n=m+q-1It is necessary and sufficient that:

  1. 1.

    P1(1)0P_{1}(1)\neq 0Forq=0q=0.

  2. 2.

    P1(1)=P2(1)==Pq(1)=0,Pq+1(1)0P_{1}(1)=P_{2}(1)=\ldots=P_{q}(1)=0,\quad P_{q+1}(1)\neq 0, Forq>0q>0.

The numberR[xn+1]R\left[x^{n+1}\right]is then also given by the formula

R[xn+1]=(1)qq!Pq+1(1)=(1)qq!11Pq(x)dxR\left[x^{n+1}\right]=(-1)^{q}q!P_{q+1}(1)=(-1)^{q}q!\int_{-1}^{1}P_{q}(x)dx (10)
  1. 7.

    The remainder of formula (1) (degree of accuracym1\geqq m-1) is given by

R[f]=11L(x)[x1,x2,,xm,x;f]dxR[f]=\int_{-1}^{1}l(x)\left[x_{1},x_{2},\ldots,x_{m},x;f\right]dx (11)

If we ask

ω(x)=[x1,x2,,xm,x;f]\omega(x)=\left[x_{1},x_{2},\ldots,x_{m},x;f\right] (12)

and if we use the integration by parts formula, we deduce (q>0q>0)

R[f]=i=1q(1)i1Pi(1)ω(i1)(1)+(1)q11Pq(x)ω(q)(x)dxR[f]=\sum_{i=1}^{q}(-1)^{i-1}P_{i}(1)\omega^{(i-1)}(1)+(-1)^{q}\int_{-1}^{1}P_{q}(x)\omega^{(q)}(x)dx (13)

We can then deduce
THEOREM 3. If there exists a non-negative integerqqsuch as :

  1. 1.

    P0(x)=L(x)P_{0}(x)=l(x)does not change sign on[1.1][-1,1], Forq=0q=0

  2. 2.

    Pi(1)=0,i=1.2,,qP_{i}(1)=0,i=1,2,\ldots,qAndPq(x)P_{q}(x)does not change sign on[1.1][-1,1], powq>0q>0,
    then the restR[f]R[f]of formula (1) (assumed to have a degree of accuracym1)\geqq m-1)is of a degree of accuracy equal ton=m+q1n=m+q-1and is of the simple form.

Taking into account the well-known formula

ω(q)(x)=q![x1,x2,,xm,x,x,,xq+1;f],\omega^{(q)}(x)=q![x_{1},x_{2},\ldots,x_{m},\underbrace{x,x,\ldots,x}_{q+1};f], (14)

the theorem results from the formula

R[f]=(1)qq!11Pq(x)[x1,x2,,xm,x,x,,xq+1;f]dxR[f]=(-1)^{q}q!\int_{-1}^{1}P_{q}(x)[x_{1},x_{2},\ldots,x_{m},\underbrace{x,x,\ldots,x}_{q+1};f]dx (15)

which is verified under the accepted assumptions, and because of the fact thatR[f]R[f]is of the simple form if (and only if)R[f]0R[f]\neq 0for any functionff\in\mathscr{F}. convex of ordernnonEE.

A function is said to be convex of ordernnonEEif all its differences divided (of ordern+1n+1) onn+2n+2points, not all of them combined, ofEEare positive. The property expressed by Theorem 3 is what we can call Steffensen's simplicity criterion, by virtue of the important theorem of J. I. Steffensen [12] relating to the remainder of Cotes' quadrature formula. J. I. Steffensen assumes that the functionffhas a derivative of ordern+1n+1continues, but we will see that the remainder in Cotes' formula is of the simple form under the set hypothesis of the continuity of the functionff8.
The conditions under which the Steffensen criterion is applicable must be specified. We will demonstrate in this work that the Steffensen criterion applies only under the assumption thatfWf\in\mathbb{F}This property is expressed by Theorem 5 further on.

Let us note, in passing, that the numberqqof theorem 3 may not exist. For example, the remainder of the quadrature formula

11f(x)dx=\displaystyle\int_{-1}^{1}f(x)dx= 23[f(12)+f(0)+f(12)]+0f(0)+R[f]=\displaystyle\frac{2}{3}\left[f\left(-\frac{1}{\sqrt{2}}\right)+f(0)+f\left(\frac{1}{\sqrt{2}}\right)\right]+0\cdot f^{\prime}(0)+R[f]= (16)
=23[f(12)+f(0)+f(12)]+R[f]\displaystyle=\frac{2}{3}\left[f\left(-\frac{1}{\sqrt{2}}\right)+f(0)+f\left(\frac{1}{\sqrt{2}}\right)\right]+R[f]

can exclaim

R[f]=11x2(x212)[0.0,12,12,x;f]dxR[f]=\int_{-1}^{1}x^{2}\left(x^{2}-\frac{1}{2}\right)\left[0,0,-\frac{1}{\sqrt{2}},\frac{1}{\sqrt{2}},x;f\right]dx (17)

In this caseR[x4]=1150R\left[x^{4}\right]=\frac{1}{15}\neq 0The numberqqTheorem 3 does not exist, since otherwise it should be equal to 0. But the polynomialL(x)=P0(x)=x2(x212)l(x)=P_{0}(x)=x^{2}\left(x^{2}-\frac{1}{2}\right)changes sign over the interval[1.1][-1,1]We will see later (no. 15) that the remainder of formula (16) is of simple form. This result is obtained by interpreting formula (16) with the value 3 ofmminstead of the value 4.9.
If we refer to how we obtained formula (15), we see that for Steffensen's criterion to be applicable, it suffices that the function (14) be continuous on the interval[1.1][-1,1]. Ifq=0q=0This additional assumption is even unnecessary since the productL(x)l(x)'[x1,x2,,xm,x;f]\left[x_{1},x_{2},\ldots,x_{m},x;f\right]is equal to the difference between the functionffand its Lagrange-Hermite polynomial on the knotsx1,x2,,xmx_{1},x_{2},\ldots,x_{m}The result is

THEOREM 4. If we haveL(x)0l(x)\geqq 0on the interval[1.1][-1,1], the remainder of formula (1) (assumed to have a degree of accuracym1\geqq m-1) is the degree of accuracym1m-1and is of the simple form.

This is particularly true if the nodesz1,z2,,zpz_{1},z_{2},\ldots,z_{p}are all outside the open interval (1.1-1,1), or if all the nodes that belong to(1.1)(-1,1), are of even order of multiplicity.
10. Let

ki={ki, if zi[1.1]0 if zi[1.1],i=1.2,,pk_{i}^{\prime}=\left\{\begin{array}[]{ll}k_{i},&\text{ si }z_{i}\in[-1.1]\\ 0&\text{ si }z_{i}\notin[-1.1]\end{array},i=1,2,\ldots,p\right.

For 1a continuity on[1.1][-1,1]of the function (14) i1 it suffices that the functionf(ϵ)f(\epsilon\mathscr{F})has a derivative, continuous of orderq+max(k1,k2,,kp)q+\max\left(k_{1}^{\prime},k_{2}^{\prime},\ldots,k_{p}^{\prime}\right)onEEThis obviously happens if

q+max(k1,k2,,kp)max(k11,k21,,kp1)q+\max\left(k_{1}^{\prime},k_{2}^{\prime},\ldots,k_{p}^{\prime}\right)\leqq\max\left(k_{1}-1,k_{2}-1,\ldots,k_{p}-1\right)

according to the definition of the set\mathscr{F}In this case, Steffensen's criterion is therefore applicable. But we will demonstrate that this criterion is always applicable, regardless of condition (19).

Let us consider the functionsφn+1,λ(x)=(xλ+|xλ|2)n(n1)\varphi_{n+1,\lambda}(x)=\left(\frac{x-\lambda+|x-\lambda|}{2}\right)^{n}(n\geqq 1)which, for any real value of the parameterλ\lambdaadmit a continuous derivative of ordern1n-1on the real axis.

By virtue of Theorem 15 of our cited work [9], the Steffensen criterion is certainly applicable if

m+q11,m2max(k1,k2,,kp)m+q-1\geqq 1,\quad m-2\geqq\max\left(k_{1}^{\prime},k_{2}^{\prime},\ldots,k_{p}^{\prime}\right) (20)

The first condition is always met forp2p\geqq 2and, sincemp+1max(k1,k2,,kp)m-p+1\geqq\max\left(k_{1}^{\prime},k_{2}^{\prime},\ldots,k_{p}^{\prime}\right), the second condition is also always verified forp3p\geqq 3. Ifp=2p=2, this second condition (20) is satisfied, unless one of the nodesz1,z2z_{1},z_{2}is simple and the other (simple or not) belongs to the closed interval[1.1][-1,1].

We can now state
THEOREM 5. Steffensen's simplicity criterion (Theorem 3) is still applicable to formula (1) (assumed to have a degree of accuracym1\geqq m-1).

From the foregoing, the theorem is proven, except in the noted exceptions, that is, unless inequalities (20) are not simultaneously satisfied and if, by virtue of Theorem 4, we also haveq>0q>011.
We could eliminate the noted exceptions by using, instead of Theorem 15 of our work cited [9], a more powerful simplicity criterion, but we will not address this issue here. We will continue with the analysis of the noted exceptions. In this way, we will have the opportunity to establish the existence and uniqueness of certain formulas of the type (1). The proof of Theorem 5 in these exceptions will be indirect and will consist of showing that if the hypotheses of Theorem 3 are verified, the rest is indeed of the simple form.

Taking into account the symmetry of the problem with respect to the interval[1.1][-1,1]It suffices to examine the following two exceptional cases:

Case 1.p=1,1z1<1p=1,-1\leqq z_{1}<1
Case 2.p=2,k2=1,1z11,z1<z2p=2,k_{2}=1,-1\leqq z_{1}\leqq 1,z_{1}<z_{2}

It is also sufficient to eliminate from this the direct examination of cases whereq=0q=012.
Case1(p=1)1(p=1)To simplify the notation a bit, let's

z1=α,k1=kz_{1}=\alpha,\quad k_{1}=k (21)

and we can assume1α<1-1\leqq\alpha<1.

We have

L(x)=P0(x)=(xα)k,P1(x)=(xα)k+1+(1)k(1+α)k+1k+1l(x)=P_{0}(x)=(x-\alpha)^{k},P_{1}(x)=\frac{(x-\alpha)^{k+1}+(-1)^{k}(1+\alpha)^{k+1}}{k+1}

The polynomialP0(x)P_{0}(x)does not change sign on[1.1][-1,1]yes, orα=1\alpha=-1orkkis even. Ifkkis odd and1<α<1-1<\alpha<1the polynomialP0(x)P_{0}(x)changes sign on[1.1][-1,1]and the conditionP1(1)=0P_{1}(1)=0gives usα=0\alpha=0We then haveP1(x)=xk+11k+10P_{1}(x)=\frac{x^{k+1}-1}{k+1}\leqq 0on[1.1][-1,1].

It is therefore sufficient to demonstrate the simplicity of the rest of the formula of type (1):

(F1)p=1,k= odd, α=0,q=1,n=k\left(F_{1}\right)\quad p=1,\quad k=\text{ impair, }\alpha=0,\quad q=1,\quad n=k

In the following paragraph, we will give the explicit form of this formula (formula (40)) and, in general, of formulas (1) for whichp=1p=113.
Case2(p=2,k2=1)2\left(p=2,k_{2}=1\right)To simplify the notation, we set in this case

z1=α,z2=β,1α=u,1+α=v,k1=kz_{1}=\alpha,\quad z_{2}=\beta,\quad 1-\alpha=u,\quad 1+\alpha=v,k_{1}=k (22)

We have

L(x)=P0(x)=(xα)k(xβ)l(x)=P_{0}(x)=(x-\alpha)^{k}(x-\beta)
P1(x)=(xα)k+2(1)k+2vk+2k+2(βα)(xα)k+1+(1)kvk+1k+1P_{1}(x)=\frac{(x-\alpha)^{k+2}-(-1)^{k+2}v^{k+2}}{k+2}-(\beta-\alpha)\frac{(x-\alpha)^{k+1}+(-1)^{k}v^{k+1}}{k+1}

and the polynomialP0(x)P_{0}(x)does not change sign on[1.1][-1,1]in the casesα=1,β1;k=\alpha=-1,\beta\geqq 1;k=peer,1<α<1β-1<\alpha<1\leqq\betaAndα=1<β\alpha=1<\beta.

It remains to demonstrate the simplicity of the remainder in the following formulas of type (1):
(F2\mathrm{F}_{2})p=2,1=α<β<1,P1(1)=0,q=1,n=k+1\quad p=2,-1=\alpha<\beta<1,P_{1}(1)=0,q=1,n=k+1
(F3\mathrm{F}_{3})p=2,k=\quad p=2,k=peer,1<α<β<1,P1(1)=0,q=1,n=k+1-1<\alpha<\beta<1,P_{1}(1)=0,q=1,n=k+1
(F4\mathrm{F}_{4})p=2,k=\quad p=2,k=odd,1<α<β=1,P1(1)=0,q=1,n=k+1-1<\alpha<\beta=1,P_{1}(1)=0,q=1,n=k+1
(F5\mathrm{F}_{5})p=2,k=\quad p=2,k=odd,1<α<1<β,P1(1)=0,q=1,n=k+1-1<\alpha<1<\beta,P_{1}(1)=0,q=1,n=k+1
(F6\mathrm{F}_{6})p=2,k=\quad p=2,k=odd,1<α<β<1,P1(1)=P2(1)=0,q=2,n==k+2-1<\alpha<\beta<1,P_{1}(1)=P_{2}(1)=0,q=2,n==k+2

In the formulas(F2)(F5)\left(\mathrm{F}_{2}\right)-\left(\mathrm{F}_{5}\right)the functionP1(x)P_{1}(x)changes the direction of monotony on[1.1][-1,1]only once (to the pointβ\betaFor(F2)\left(\mathrm{F}_{2}\right),(F3)\left(\mathrm{F}_{3}\right)and to the pointα\alphaFor(F4),(F5)\left(\mathrm{F}_{4}\right),\left(\mathrm{F}_{5}\right)). OfP1(1)=0P_{1}(1)=0It therefore follows thatP1(x)P_{1}(x)does not change sign on[1.1][-1,1].

LegalityP1(1)=0P_{1}(1)=0, in the case of the formula(F2)\left(\mathrm{F}_{2}\right)gives usβ=kk+2\beta=\frac{k}{k+2}which is well understood in(1.1)(-1,1)This demonstrates the existence of a unique such formula.

For the formula(F3)\left(\mathrm{F}_{3}\right)1'equationP1(1)=0P_{1}(1)=0becomes
(23)

βα=k+1k+2uk+2vk+2uk+1+vk+1\beta-\alpha=\frac{k+1}{k+2}\cdot\frac{u^{k+2}-v^{k+2}}{u^{k+1}+v^{k+1}}

from which we deduce
(24)

1β=uk+2+(2k+3α)vk+1(k+2)(uk+1+vk+1)1-\beta=\frac{u^{k+2}+(2k+3-\alpha)v^{k+1}}{(k+2)\left(u^{k+1}+v^{k+1}\right)}

From (23) it follows, taking into account1<α<1-1<\alpha<1that we haveβα>0\beta-\alpha>0respectivelyβα<0\beta-\alpha<0depending onα<0\alpha<0respectivelyα>0\alpha>0From (23) it follows that1β>01-\beta>0The result is that there is a unique formula.(F3)\left(F_{3}\right)for everythingα(1.0)\alpha\in(-1,0).

In the case of formulas(F4),(F5)\left(\mathrm{F}_{4}\right),\left(\mathrm{F}_{5}\right)equalityP1(1)=0P_{1}(1)=0becomes
(25)

βα=k+1k+2uk+2+vk+2uk+1vk+1\beta-\alpha=\frac{k+1}{k+2}\cdot\frac{u^{k+2}+v^{k+2}}{u^{k+1}-v^{k+1}}

who determinesβ\betadepending onα\alphaFormula (25) shows us that in order to haveα<β(1<α<1)\alpha<\beta(-1<\alpha<1)it is necessary and sufficient thatα\alphais negative. The derivative ofβ\betacompared toα\alpha,

dβdα=u2k+2+v2k+2+2(uv)k(2k2+4k+1+α2)(k+2)(uk+1vk+1)2\frac{d\beta}{d\alpha}=\frac{u^{2k+2}+v^{2k+2}+2(uv)^{k}\left(2^{k^{2}}+4k+1+\alpha^{2}\right)}{(k+2)\left(u^{k+1}-v^{k+1}\right)^{2}}

shows us thatβ\betais an increasing function ofα\alphaon[1.0)[-1,0)It is easy to see that ifα\alphavaries from -1 to0(1α<0),β0(-1\leqq\alpha<0),\betagrows fromhh+2\frac{h}{h+2}has++\inftyTherefore, there exists a formula and a set of the form (F4\mathrm{F}_{4}) and for this formulaα\alphais equal to a numberhasabetween -1 and0(1<has<0)0(-1<a<0), very determined. For everythingα(has,0)\alpha\in(a,0)There is a formula and a single form (F5\mathrm{F}_{5}).

It remains to be demonstrated that there exists a formula of the form (F6\mathrm{F}_{6}AssumingP1(1)=0P_{1}(1)=0the polynomialP1(x)P_{1}(x)changes sign over the interval[1.1][-1,1]In this case, only once. So if we haveP2(1)=0P_{2}(1)=0the polynomialP2(x)P_{2}(x)does not change sign on[1.1][-1,1]Taking into account (25),P2(1)P_{2}(1)is given by the formula

P2(1)=u2k+4v2k+4+2(uv)k+1(2k2+8k+7+α2)(k+2)2(k+3)(uk+1vk+1)P_{2}(1)=\frac{-u^{2k+4}-v^{2k+4}+2(uv)^{k+1}\left(2k^{2}+8k+7+\alpha^{2}\right)}{(k+2)^{2}(k+3)\left(u^{k+1}-v^{k+1}\right)}

and is a function ofα\alphaThe derivative of this function is given by the formula

(k+2)2(k+3)(uk+1vk+1)2dP2(1)dα==(k+3)(u3k+4+v3k+4)4α[2k3+10k2+3k+3+(k+3)α2](uk+1vk+1)++(4k3+20k2+27k+9+(k+3)α2]uv(uk+vk)\begin{gathered}(k+2)^{2}(k+3)\left(u^{k+1}-v^{k+1}\right)^{2}\frac{dP_{2}(1)}{d\alpha}=\\ =(k+3)\left(u^{3k+4}+v^{3k+4}\right)-\\ -4\alpha\left[2k^{3}+10k^{2}+3k+3+(k+3)\alpha^{2}\right]\left(u^{k+1}-v^{k+1}\right)+\\ +\left(4k^{3}+20k^{2}+27k+9+(k+3)\alpha^{2}\right]uv\left(u^{k}+v^{k}\right)\end{gathered}

The functionP2(1)P_{2}(1)ofα\alphais therefore increasing on the interval[1.0)[-1,0)It has a negative value.2k+3(k+2)2(k+3)-\frac{2^{k+3}}{(k+2)^{2}(k+3)}Forα=1\alpha=-1and is certainly positive forhasα<0a\leq\alpha<0(since thenP1(x)P_{1}(x)does not change sign on[1.1][-1,1]). It follows that there is one and only one pointα=has*\alpha=a^{*}in the meantime(1,has)(-1,a)for whichP2(1)=0P_{2}(1)=0. Ifb*b^{*}is the value ofβ\betataken from (25) forα=has*\alpha=a^{*}, the only formula of the form (F0F_{0}) is obtained forα=has*,β=b*\alpha=a^{*},\beta=b^{*}.

We have therefore demonstrated the existence of the formulas(F2)(F6)\left(\mathrm{F}_{2}\right)-\left(\mathrm{F}_{6}\right)and even the uniqueness of the formulas(F2),(F4),(F6).I\left(F_{2}\right),\left(F_{4}\right),\left(F_{6}\right).I^{\prime}'existence of the formula(F6)\left(F_{6}\right)also results, in a different way, from another of our works [8].

In the following paragraph, we will give the explicit form of some of these formulas (formula (45)) and, in general, formulas for whichp==2,k2=1p==2,k_{2}=1(formula (40)).

For the formulas(F1)(F6)\left(F_{1}\right)-\left(F_{6}\right)(nos. 12, 13) we have also indicated the corresponding value ofqqand their degree of accuracynn.

Demonstrating the simplicity of the remainders of the formulas(F1)(F6)\left(F_{1}\right)-\left(F_{6}\right)will be given in the following paragraph. In this way, Theorem 5 will be proven.

To conclude this section, we will look at some applications.
14. First application. Cotes' formulas are quadrature formulas of the form (1) with all nodes simple and equidistant (and of degree of accuracy).m1\geqq m-1).

More generally, let us consider, with JE STEFFENSEN, the formula of the type (1)

hasbf(x)dx=i=1mcif(zi)+R[f]\int_{a}^{b}f(x)dx=\sum_{i=1}^{m}c_{i}f\left(z_{i}\right)+R[f] (26)

Orm=s2r+1m=s-2r+1, s being a natural number,rran integer12s\leqq\frac{1}{2}sand the (simple) knots being given by the formulas

zi=has+(r+i1)bhass,i=1.2,,mz_{i}=a+(r+i-1)\frac{b-a}{s},\quad i=1,2,\ldots,m (27)

The coefficientsci,i=1.2,,mc_{i},i=1,2,\ldots,mare completely determined by the condition that formula (26) has its degree of accuracym1\geqq m-1.

We then have the

THEOREM 6. The remainder of Cotes' formula (26) is of degree of exactness2[m12]+12\left[\frac{m-1}{2}\right]+1and is of the simple form.

To demonstrate this theorem, it suffices to modify very slightly the proof given by Steffensen [12], assuming that the functionffhas a continuous derivative of order2[m12]+12\left[\frac{m-1}{2}\right]+1

For demonstration 1a, we distinguish two cases depending on the parity of the numbermm(or ofss)

  1. 1.

    Ifmmis odd, thereforessis even, we havehasbL(x)dx=0\int_{a}^{b}l(x)dx=0And

(1)min(r,1)hasxL(x)dx0, For x[has,b](-1)^{\min(r,1)}\int_{a}^{x}l(x)dx\geqq 0,\text{ pour }x\in[a,b] (28)

It is precisely this inequality that was demonstrated in a very elegant way by JE STEFFENSEN.

The Steffensen criterion is applicable (we consider the interval[has,b][a,b]instead of[1.1][-1,1]). The restR[f]R[f]of formula (26) is of degree of accuracymmand is of the simple form.

Note, moreover, that in this case we have
(29)

(1)min(r1.0)R[f]>0(-1)^{\min(r-1,0)}R[f]>0

for any (continuous) functionffconvex of ordermm2.
Ifmmis even, thereforessis odd, still according to JE STEFFENSEN we decompose the remainder

R[f]=hasbL(x)[z1,z2,,zm;x;f]dxR[f]=\int_{a}^{b}l(x)\left[z_{1},z_{2},\ldots,z_{m};x;f\right]dx (30)

in short

R[f]=R1[f]+R2[f]R[f]=R_{1}[f]+R_{2}[f] (31)

corresponding to the decomposition[has,bbhass][bbhass,b|\left[a,b-\frac{b-a}{s}\right]\cup\left[b-\frac{b-a}{s},b\mid\right.of the integration interval[has,b][a,b]of the second member of (30). We have [12],

R1[f]=hasbbhassL(x)xzm[z1,z2,,zm1,x;f]dxR_{1}[f]=\int_{a}^{b-\frac{b-a}{s}}\frac{l(x)}{x-z_{m}}\left[z_{1},z_{2},\ldots,z_{m-1},x;f\right]dx

which is the remainder of a formula of the form (26) corresponding tom1m-1, therefore to an odd number of nodes, but with the same value ofrrAs a result, we have

(1)min(r1.0)R1[f]>0(-1)^{\min(r-1,0)}R_{1}[f]>0 (32)

for any (continuous) functionffconvex of orderm1m-1We
also have

R2[f]=bbhassbL(x)[z1,z2,,zm,x;f]dxR_{2}[f]=\int_{b-\frac{b-a}{s}}^{b}l(x)\left[z_{1},z_{2},\ldots,z_{m},x;f\right]dx

Here we have(1)min(r1.0)L(x)0(-1)^{\min(r-1,0)}l(x)\geqq 0on the interval[bbhass,b]\left[b-\frac{b-a}{s},b\right]and, by virtue of the theorem3,R2[f]3,R_{2}[f]is the degree of accuracym1m-1and of the simple form. Furthermore, we have

(1)min(r1.0)R2[f]>0(-1)^{\min(r-1,0)}R_{2}[f]>0 (33)

for any (continuous) functionff, convex of orderm1m-1From
(31) - (33) it follows that inequality (29) is still verified for any (continuous) functionff, convex of orderm1m-1.

We can see that this result is valid even ifs=1s=1We then haveR[f]=R2[f]R[f]=R_{2}[f].

Theorem 6 is therefore proven. We also see that in formula (2) or (3), in this case, we havesgM=sgR[xn+1]=sg(1)min(r1.0)\mathrm{sg}M=\mathrm{sg}R\left[x^{n+1}\right]=\mathrm{sg}(-1)^{\mathrm{min}(r-1,0)}.LeL_{e}sign of the numerical coefficientMMdepends solely on the numberrr15.
Second application. A formula of type (1), with simple nodes and coefficientsci,0,i=1.2,,p(=m)c_{i,0},i=1,2,\ldots,p(=m)all equal and of the same degree of accuracym\geq mThis is called a Chebyshev quadrature formula. Such a formula is therefore of the form

11f(x)dx=2mi=1mf(zi)+R[f]\int_{-1}^{1}f(x)dx=\frac{2}{m}\sum_{i=1}^{m}f\left(z_{i}\right)+R[f] (34)

where the nodesz1,z2,,znz_{1},z_{2},\ldots,z_{n}are determined (apart from a permutation) by the condition that the formula in question has the degree of accuracym\geqq m.

We know that such a formula exists only for the values ​​1, 2,3, 4, 5, 6, 7, 93,4,5,6,7,9ofmmThe nodes are then inside the interval[1.1][-1,1]and we can takeE=[1.1]E=[-1,1].

We have 1st
theorem 7. The remainder of Chebyshev's formula (34) (for the possible values ​​ofmm) is of a degree of accuracy equal to2[m2]+12\left[\frac{m}{2}\right]+1and is of the simple form.

The property results from applying Theorem 3.
The polynomialL(x)=P0(x)l(x)=P_{0}(x)is found to be calculated, for example, in the book by VI Krilov [2]. This polynomial is given by the table

m=1,x;m=2,x213;m=3,x3x2;m=4,x423x2+115\displaystyle m=1,x;m=2,x^{2}-\frac{1}{3};m=3,x^{3}-\frac{x}{2};m=4,x^{4}-\frac{2}{3}x^{2}+\frac{1}{15}
m=5,x556x3+7x72;m=6,x6x4+15x21105;\displaystyle m=5,x^{5}-\frac{5}{6}x^{3}+\frac{7x}{72};m=6,x^{6}-x^{4}+\frac{1}{5}x^{2}-\frac{1}{105};
m=7,x776x5+119360x3149x6480;\displaystyle m=7,x^{7}-\frac{7}{6}x^{5}+\frac{119}{360}x^{3}-\frac{149x}{6480};
m=9,x932x7+2740x557560x3+53x22400.\displaystyle m=9,x^{9}-\frac{3}{2}x^{7}+\frac{27}{40}x^{5}-\frac{57}{560}x^{3}+\frac{53x}{22400}.

From this, we can deduce the polynomials.P1(x)P_{1}(x)correspondents,

m=1,12(x21);m=2,x(x21)3;m=3,x2(x21)4;\displaystyle m=1,\frac{1}{2}\left(x^{2}-1\right);\quad m=2,\frac{x\left(x^{2}-1\right)}{3};m=3,\frac{x^{2}\left(x^{2}-1\right)}{4};
m=4,145x(x21)(9x21);m=5,x21144[24(x218)2+58];\displaystyle m=4,\frac{1}{45}x\left(x^{2}-1\right)\left(9x^{2}-1\right);\quad m=5,\frac{x^{2}-1}{144}\left[24\left(x^{2}-\frac{1}{8}\right)^{2}+\frac{5}{8}\right];
m=6,x(x21)(15x46x2+1)105;\displaystyle m=6,\frac{x\left(x^{2}-1\right)\left(15x^{4}-6x^{2}+1\right)}{105};
m=7,x2112960[1620x2(x2518)2+46x2+22];\displaystyle m=7,\frac{x^{2}-1}{12960}\left[1620x^{2}\left(x^{2}-\frac{5}{18}\right)^{2}+46x^{2}+22\right];
m=9,x2144800[4480(x4716x2+15512)2+303532x2+597092048].\displaystyle m=9,\frac{x^{2}-1}{44800}\left[4480\left(x^{4}-\frac{7}{16}x^{2}+\frac{15}{512}\right)^{2}+\frac{3035}{32}x^{2}+\frac{59709}{2048}\right].

We can see that formmoddP1(x)P_{1}(x)does not change sign on[1.1][-1,1]Theorem 7 therefore follows for these values ​​ofmm. Formmeven the polynomialP1(x)P_{1}(x)changes sign on[1.1][-1,1], we deduce, for these values ​​ofmm, polynomialsP2(x)P_{2}(x)correspondents,

m=2,(x21)212;m=4,190(x21)2(3x2+1)\displaystyle m=2,\frac{\left(x^{2}-1\right)^{2}}{12};m=4,\frac{1}{90}\left(x^{2}-1\right)^{2}\left(3x^{2}+1\right)
m=6,1840(x21)2(15x4+2x2+3)\displaystyle m=6,\frac{1}{840}\left(x^{2}-1\right)^{2}\left(15x^{4}+2x^{2}+3\right)

which do not change sign on[1.1][-1,1]Theorem 7 therefore also follows for these values ​​ofmm.

We also give the value of the degree in the following table.nnaccuracy and coefficientR[xn+1]R\left[x^{n+1}\right]Chebyshev's formulas,

mm 1 2 3 4 5 6 7 9
nn 1 3 3 5 5 7 7 9
R[xn+1]R\left[x^{n+1}\right] 23\frac{2}{3} 845\frac{8}{45} 115\frac{1}{15} 32945\frac{32}{945} 13756\frac{13}{756} 161575\frac{16}{1575} 28148600\frac{281}{48600} 16373920\frac{163}{73920}

For the calculation ofR[xn+1]R\left[x^{n+1}\right]We can use formula (7) and we can check the results obtained using the formula

R[xn+1]=11xn+1dx2mi=1mzin+1=2n+22mi=1mzin+1,n=2[m2]+1R\left[x^{n+1}\right]=\int_{-1}^{1}x^{n+1}dx-\frac{2}{m}\sum_{i=1}^{m}z_{i}^{n+1}=\frac{2}{n+2}-\frac{2}{m}\sum_{i=1}^{m}z_{i}^{n+1},n=2\left[\frac{m}{2}\right]+1

and taking into account

1(1)v+1v+1=2mi=1mziv,v=1.2,,2[m2]+1\frac{1-(-1)^{v+1}}{v+1}=\frac{2}{m}\sum_{i=1}^{m}z_{i}^{v},v=1,2,\ldots,2\left[\frac{m}{2}\right]+1

Form=3m=3T'chebycheff's formula (34) is none other than formula (16), the remainder of which is therefore given by the formulaR[f]=115D4[f]R[f]=\frac{1}{15}D_{4}[f], whatever the functionffcontinues over the interval[1.1][-1,1], the nodes of the divided differenceD4[f]D_{4}[f]which appears in this formula being within this interval (and generally depending on the functionff).
16. Third application. Theorem 3 also allows us to construct formulas (1) having a remainder of a given degree of accuracym+q1(q0)m+q-1(q\geqq 0)and of the simple form. It suffices to take as nodes the roots (assumed all to be real) of a polynomial of the formL(x)=[(x21)qQ(x)](q)l(x)=\left[\left(x^{2}-1\right)^{q}Q(x)\right]^{(q)}, OrQQis a polynomial of degreemqm-qwhose sign does not change on[1.1][-1,1]This polynomial can always be chosen such thatL(x)l(x)has all its real roots. If, in particular, we takem=qm=q, done ifQQis a constant (0\neq 0), the polynomialLlis given by the formula

L(x)=m!(2m)![(x21)m](m)l(x)=\frac{m!}{(2m)!}\left[\left(x^{2}-1\right)^{m}\right]^{(m)}

THEOREM 8. The remainder in Gauss's quadrature formula withmmnodes, is of degree of accuracy2m12m-1and is of the simple form, regardless of the functionff, continues over the integration interval.

The coefficientR[x2m]R\left[x^{2m}\right]results, by applying formula (15),

R[x2m]=m!(2m)!11xm[(x21)m](m)dx=m!m!(2m)!11(1x2)mdx==22m+1(m!)4(2m)!(2m1)!\begin{gathered}R\left[x^{2m}\right]=\frac{m!}{(2m)!}\int_{-1}^{1}x^{m}\left[\left(x^{2}-1\right)^{m}\right]^{(m)}dx=-\frac{m!m!}{(2m)!}\int_{-1}^{1}\left(1-x^{2}\right)^{m}dx=\\ =\frac{2^{2m+1}(m!)^{4}}{(2m)!(2m-1)!}\end{gathered}

§ 2

  1. 17.

    Let's return to formula (1). If we setR*[f]=R[f]R^{*}[f]=R\left[f^{\prime}\right], the linear functionalR*[f]R^{*}[f]is, defined on the differentiable functionsffwhose derivative belongs to\mathscr{F}.

According to a previous result (see Theorem 13 of our cited work [9]), so that the restR[f]R[f]either degree of accuracynnand in simple form, it is necessary and sufficient thatR*[f]R^{*}[f]either degree of accuracyn+1n+1and of the simple form.

If we assume thatR*[f]R^{*}[f]has the degree of accuracym+qm+qOrq0q\geqq 0, We have

R*[f]=i=1pq1μi[yi,yi+1,,yi+m+q+1;f]R^{*}[f]=\sum_{i=1}^{p^{\prime}-q-1}\mu_{i}\left[y_{i},y_{i+1},\ldots,y_{i+m+q+1};f\right] (35)

Or :

  1. 1.

    p=p+2,p+1p^{\prime}=p+2,p+1respectivelyppdepending on the points1.1-1,1are both distinct from the nodesziz_{i}, one and only one of the points1.1-1,1coincides with one of the nodesziz_{i}, respectively each of the points1.1-1,1coincides with one of theppknotsziz_{i}.

  2. 2.

    Inequalitypq11p^{\prime}-q-1\geqq 1is verified. It results from the inequalityqp2q\leq p^{\prime}-2which is a consequence of the boundaries given toqqin the preceding paragraph (no. 5).

  3. 3.

    y1y2ym+py_{1}\leqq y_{2}\leqq\ldots\leqq y_{m+p^{\prime}}These points includeki+1k_{i}+1times 1st knotziz_{i}, Fori=1.2,,pi=1,2,\ldots,pand each of the points1.1-1,1distinct nodesziz_{i}.

  4. 4.

    The coefficientsμi,i=1.2,,pq1\mu_{i},i=1,2,\ldots,p^{\prime}-q-1are independent of function 1aff.

The coefficientR*[xm+q+1]R^{*}\left[x^{m+q+1}\right]is given by the formula

R*[xm+q+1]=i=1pq1μiR^{*}\left[x^{m+q+1}\right]=\sum_{i=1}^{p^{\prime}-q-1}\mu_{i} (36)

Moreover, formulas (35) and (36) are valid only under the assumption thatR*[f]R^{*}[f]vanishes on any polynomial of degreem+qm+q.

We deduce from this
theorem 9. Under the hypotheses and with the previous notation, if all the coefficientsμi,i=1.2,,pq1\mu_{i},i=1,2,\ldots,p^{\prime}-q-1are of the same sign (all0\geqq 0or all0\leqq 0), the restR[f]R[f]of formula (1) is of degree of accuracyn=m++q1n=m++q-1and is of the simple form.

It follows from the problem data that theμi,i=1.2,,pq1\mu_{i},i=1,2,\ldots,p^{\prime}-q-1are never all zero. Formula (36) also shows us that we have

R[xn+1]=1m+q+1i=1pq1μiR\left[x^{n+1}\right]=\frac{1}{m+q+1}\sum_{i=1}^{p^{\prime}-q-1}\mu_{i} (37)
  1. 18.

    First application. In the casepq1=1p^{\prime}-q-1=1, Orq=p2q=p^{\prime}-2, the second member of (35) contains only one term and the restR[f]R[f]is necessarily of the simple form. The coefficientμ1\mu_{1}(who is0\neq 0) can be calculated by identifying the two sides of equation (35). We thus find

μ1=ki!ci,kiPij(zizj)kj+1\mu_{1}=-k_{i}!c_{i,k_{i}}\Pi_{j}^{\prime}\left(z_{i}-z_{j}\right)^{k_{j}+1} (38)

where it was placedz0=1,zp+1=1,k0=kp+1=0,c0.0=1,cp+1.0=1z_{0}=-1,z_{p+1}=1,k_{0}=k_{p+1}=0,c_{0,0}=1,c_{p+1,0}=-1, in the productPi\Pi^{\prime}the valueiiofjjis an exception and where the indicesi,ji,jscan the values:

  1. 1.

    0.1,,p+10,1,\ldots,p+1if the points1.1-1,1are both distinct from the nodes (p=p+2p^{\prime}=p+2).

  2. 2.

    1.2,,p+1,z1=11,2,\cdots,p+1,z_{1}=-1and point 1 is different from the nodes (p=p+1p^{\prime}=p+1)

  3. 3.

    0.1,,p,zp=10,1,\ldots,p,z_{p}=1and point -1 is different from the nodes (p==p+1p^{\prime}==p+1).

  4. 4.

    1.2,,p1,2,\ldots,pAndz1=1,zp=1z_{1}=-1,z_{p}=1.
    (37) it is easy to compare the value ofR[xn+1]R\left[x^{n+1}\right]deduced from formulas (37), (38) with that which is obtained from (10).

  5. 5.

    An important special case is obtained for

L(x)=(ρ+σ+m)!(ρ+σ+2m)![(x+1)ρ+m(x1)σ+m](m),l(x)=\frac{(\rho+\sigma+m)!}{(\rho+\sigma+2m)!}\left[(x+1)^{\rho+m}(x-1)^{\sigma+m}\right]^{(m)},

Orm,ρ,σm,\rho,\sigmaare non-negative integers, not all of which are zero. In this case, we havep=m+2,q=mp^{\prime}=m+2,q=mAndm=0m=0The corresponding formula (1) is Obrechkoff's formula [3]. Gauss's formula is also a special case (ρ=σ=0,m>0\rho=\sigma=0,m>0).

We therefore have the following generalization of Theorem 8,
Theorem 10. The remainder in the quadrature formula considered withρ+σ+m\rho+\sigma+mnodes (includingρ\rhocoincide with -1 andσ\sigmawith 1) is the degree of accuracyn=ρ+σ+2m1n=\rho+\sigma+2m-1and is of the simple form, regardless of the functionffhaving on[1.1][-1,1]a continuous derivative of maximum order(ρ,σ)(\rho,\sigma).

The coefficientR[xn+1]R\left[x^{n+1}\right]is calculated as in the specific case of Gauss's formula and we obtain

R[xρ+σ+2m]=(1)σ2ρ+σ+2m+1m!(ρ+m)!(σ+m)!(ρ+σ+m)!(ρ+σ+2m)!(ρ+σ+2m+1).R\left[x^{\rho+\sigma+2m}\right]=\frac{(-1)^{\sigma}2^{\rho+\sigma+2m+1}m!(\rho+m)!(\sigma+m)!(\rho+\sigma+m)!}{(\rho+\sigma+2m)!(\rho+\sigma+2m+1)}.
  1. 20.

    The formulas(F1),(F2),F4),(F6)\left.\left(\mathrm{F}_{1}\right),\left(\mathrm{F}_{2}\right),\mathrm{F}_{4}\right),\left(\mathrm{F}_{6}\right)are of the previous form (pq1=1p^{\prime}-q-1=1) and therefore have remainders of the simple form.

Whenp=1p=1Using notation (21), formula (1) becomes

11f(x)dx=i=0k1uki(v)ki(ki)!f(k1i)(α)+R[f]\int_{-1}^{1}f(x)dx=\sum_{i=0}^{k-1}\frac{u^{k-i}-(-v)^{k-i}}{(k-i)!}f^{(k-1-i)}(\alpha)+R[f] (39)

The degree of accuracy is equal tok1k-1, unlesskkis odd andα=0\alpha=0, when it is equal tokkIn the latter case, we find the formula (F1F_{1}) which can therefore be written
(40)

11f(x)dx=2i=0k121(k2i)!f(k12i)(0)+2k+2Dk+1[f](k= odd )\int_{-1}^{1}f(x)dx=2\sum_{i=0}^{\frac{k-1}{2}}\frac{1}{(k-2i)!}f^{(k-1-2i)}(0)+\frac{2}{k+2}D_{k+1}[f](k=\text{ impair })

When, orkkis even orkkis arbitrary andα(1.1)\alpha\in(-1,1)The remainder of the formula, by virtue of Theorem 3, is of the simple form and is given by the formula

R[f]=uk+1(v)k+1k+1Dk[f].R[f]=\frac{u^{k+1}-(-v)^{k+1}}{k+1}D_{k}[f].

Whenkkis odd andα(1.0)(0.1)\alpha\in(-1,0)\cup(0,1)The rest is a matter of degree of accuracy.k1k-1but is not of the simple form. This property results from the study of formula (62) of our work cited [9], a formula which we presented as a generalization of Obrechkoff's formula [3]. We will return to this formula later (no. 23).
21. Whenp=2p=2Andk2=1k_{2}=1Using notation (22), formula (1) becomes

11f(x)dx=\displaystyle\int_{-1}^{1}f(x)dx= (41)
=i=0k11(k1i)![uki(v)kiki1(βα)i+1uk+1vk+1k+1]f(k1i)(α)+\displaystyle=\sum_{i=0}^{k-1}\frac{1}{(k-1-i)!}\left[\frac{u^{k-i}-(-v)^{k-i}}{k-i}-\frac{1}{(\beta-\alpha)^{i+1}}\cdot\frac{u^{k+1}-v^{k+1}}{k+1}\right]f^{(k-1-i)}(\alpha)+
+uk+1(v)k+1k+1f(β)(βα)k+R[f].\displaystyle+\frac{u^{k+1}-(-v)^{k+1}}{k+1}\cdot\frac{f(\beta)}{(\beta-\alpha)^{k}}+R[f].

The degree of accuracy of this formula is equal tok,k+1k,k+1Ork+2k+2(qqis respectively equal to 0, 1 or 2). We have

R[xk+1]=uk+2(v)k+2k+2+(αβ)uk+1(v)k+1k+1R\left[x^{k+1}\right]=\frac{u^{k+2}-(-v)^{k+2}}{k+2}+(\alpha-\beta)\frac{u^{k+1}-(-v)^{k+1}}{k+1} (42)

If the degree of accuracy is>k>kthe differenceαβ\alpha-\betais given by the formula

αβ=k+1k+2uk+2(v)k+2uk+1(v)k+1\alpha-\beta=-\frac{k+1}{k+2}\cdot\frac{u^{k+2}-(-v)^{k+2}}{u^{k+1}-(-v)^{k+1}}

which amounts to (23) respectively to (25) depending on thatkkis even respectively odd and in these cases we have

R[xh+2]=u2k+4+v2k+42(uv)k+1(2k2+8k+7+α2)(k+2)2(k+3)[uk+1(v)k+1]\displaystyle R\left[x^{h+2}\right]=\frac{u^{2k+4}+v^{2k+4}-2(-uv)^{k+1}\left(2k^{2}+8k+7+\alpha^{2}\right)}{(k+2)^{2}(k+3)\left[u^{k+1}-(-v)^{k+1}\right]} (43)
R[xk+3]=2u2k+5v2k+5+2α(uv)k+1(2k2+10k+11+α2)(k+2)(k+3)(k+4)[uk+1(v)k+1]\displaystyle R\left[x^{k+3}\right]=2\frac{u^{2k+5}-v^{2k+5}+2\alpha(-uv)^{k+1}\left(2k^{2}+10k+11+\alpha^{2}\right)}{(k+2)(k+3)(k+4)\left[u^{k+1}-(-v)^{k+1}\right]}

Forα=1,β=kk+2\alpha=-1,\beta=\frac{k}{k+2}taking into account (41), (43), we find the formula(F2)\left(\mathrm{F}_{2}\right)which is therefore written

11f(x)dx=i=0k12ki(k1i)![1k1(k+2)i+1(k+1)i+2]f(k1i)(α)+\displaystyle\int_{-1}^{1}f(x)dx=\sum_{i=0}^{k-1}\frac{2^{k-i}}{(k-1-i)!}\left[\frac{1}{k-1}-\frac{(k+2)^{i+1}}{(k+1)^{i+2}}\right]f^{(k-1-i)}(\alpha)+ (45)
+2(k+2)k(k+1)k+1f(kk+2)+2k+3(k+2)2(k+3)Dk+2[f]\displaystyle+\frac{2(k+2)^{k}}{(k+1)^{k+1}}f\left(\frac{k}{k+2}\right)+\frac{2^{k+3}}{(k+2)^{2}(k+3)}D_{k+2}[f]

The formula(F4)\left(\mathrm{F}_{4}\right)is obtained from (41), assumingkkodd,α\alphaequal to the numberhasadefined in no. 13 andβ=1\beta=1The remainder of this formula is equal to

R[xk+2]Dk+2[f]R\left[x^{k+2}\right]D_{k+2}[f] (46)

where the coefficientR[xk+2]R\left[x^{k+2}\right]is given by formula (43), withkkodd andα=has\alpha=a.

Similarly, the formula(F6)\left(\mathrm{F}_{6}\right)is obtained from (41) assumingkkodd andα=has*,β=b*\alpha=a^{*},\beta=b^{*}, Orhas*,b*a^{*},b^{*}are the numbers defined in no. 13. The remainder of this formula is equal toR[xk+3]Dk+3[f]R\left[x^{k+3}\right]D_{k+3}[f]where the coefficientR[xk+3]R\left[x^{k+3}\right]is given by formula (44) forkkodd andα=has*\alpha=a^{*}22.
Second application. Let us now suppose thatpq1=2p^{\prime}-q-1=2The second member of (35) then contains two terms and the remainderR[f]R[f]is of the simple form if and only ifμ1μ20\mu_{1}\mu_{2}\geqq 0(therefore, if and only if the two coefficientsμ1,μ2\mu_{1},\mu_{2}are of the same sign). In accordance with the definition of the numberqqwe must also haveμ1+μ2=R*[xm+q+1]0\mu_{1}+\mu_{2}=R^{*}\left[x^{m+q+1}\right]\neq 0Soμ1μ2<0\mu_{1}\mu_{2}<0, the restR[f]R[f]is the degree of accuracym+q1m+q-1and is not of simple form. Formula (35) is valid, of course, only under the assumption thatR[f]R[f]vanishes for any polynomial of degreem++q1m++q-1, but whenμ1μ2=0\mu_{1}\mu_{2}=0Orμ1+μ2=0\mu_{1}+\mu_{2}=0We return, by a simple modification of the notations, to the first application (when there is only one term in the second member of (35)).

We have

R*[f]=f(1)f(1)i=1pj=0ki1ci,jf(j+1)(zi)R^{*}[f]=f(1)-f(-1)-\sum_{i=1}^{p}\sum_{j=0}^{k_{i}-1}c_{i,j}f^{(j+1)}\left(z_{i}\right) (47)

So ifq=p1q=p-1, therefore if the degree of accuracy ofR[f]R[f]Eastm++p2m++p-2and if the nodeszi,i=1.2,,pz_{i},i=1,2,\ldots,pare all within the open interval(1.1)(-1,1), formula (35) can be written (y1=1,ym+p+2=1y_{1}=-1,y_{m+p+2}=1)
(48)R*[f]=μ1[y1,y2,,ym+p+1;f]+μ2[y2,y3,,ym+p+2;f]=\quad R^{*}[f]=\mu_{1}\left[y_{1},y_{2},\ldots,y_{m+p+1};f\right]+\mu_{2}\left[y_{2},y_{3},\ldots,y_{m+p+2};f\right]=

=μ1\displaystyle=\mu_{1} [1,z1,z1,,z1k1+1,z2,z2,,z2k2+1,zp,zp,,zpkp+1;f]+\displaystyle{[-1,\underbrace{z_{1},z_{1},\ldots,z_{1}}_{k_{1}+1},\underbrace{z_{2},z_{2},\ldots,z_{2}}_{k_{2}+1}\cdots,\underbrace{z_{p},z_{p},\ldots,z_{p}}_{k_{p+1}};f]+}
+μ2[z1,z1,,z1k1+1,z2,z2,,z2k2+1,,zp,zp,,zpkp+1,1;f]\displaystyle+\mu_{2}[\underbrace{z_{1},z_{1},\ldots,z_{1}}_{k_{1}+1},\underbrace{z_{2},z_{2},\ldots,z_{2}}_{k_{2}+1},\ldots,\underbrace{z_{p},z_{p},\ldots,z_{p}}_{k_{p}+1}1;f]

where the coefficientsμ1,μ2\mu_{1},\mu_{2}are given by the formulas

μ1=(1)m+p1i=1p(1+zi)ki+1,μ2=i=1p(1zi)ki+1\mu_{1}=(-1)^{m+p-1}\prod_{i=1}^{p}\left(1+z_{i}\right)^{k_{i}+1},\quad\mu_{2}=\prod_{i=1}^{p}\left(1-z_{i}\right)^{k_{i}+1} (49)

and we can state
THEOREM 11. The remainder of formula (1) where the nodeszi,i=1.2,pz_{i},i=1,2,\ldots pare all within the interval(1.1)(-1,1)and whose degree of accuracy is equal tom+p2m+p-2, is of the simple form respectivelynn'is not of the simple form depending on thatm+pm+pis an odd number or an even number.
23. Let's take formula (39) again forkkodd andα(1.0)(0.1)\alpha\in(-1,0)\cup(0,1)The hypotheses of Theorem 11 are verified and we havem=k,p==1m=k,p==1SOm+pm+pis even. It follows that the formula has a degree of accuracyk1k-1, but the rest of it is not of simple form.

The hypotheses of Theorem 11 are also verified for the formula (F3\mathrm{F}_{3}). In this casem=k+1,p=2m=k+1,p=2and the summ+pm+pis odd. It follows that the remainder of this formula, of degree of accuracyk+1k+1, is of simple form. This remainder is given by (46) whereR[xk+2]R\left[x^{k+2}\right]is given by formula (43) wherekkis even.

An example of a formula of the type(F3)\left(\mathrm{F}_{3}\right)is given by(k=2)(k=2)

11f(x)dx=225[9f(13)5f(13)+16f(12]+34135D4[f]\int_{-1}^{1}f(x)dx=\frac{2}{25}\left[9f\left(-\frac{1}{3}\right)-5f^{\prime}\left(-\frac{1}{3}\right)+16f\left(\frac{1}{2}\right]+\frac{34}{135}D_{4}[f]\right.
  1. 24.

    To complete the proof of Theorem 5, we still need to study the formula (F5\mathrm{F}_{5}). In this case we can write

R*[f]=μ1[1,α,α,,αk+1,1,β;f]+μ2[α,α,,αk+1,1,β,β;f].R^{*}[f]=\mu_{1}[-1,\underbrace{\alpha,\alpha,\ldots,\alpha}_{k+1},1,\beta;f]+\mu_{2}[\underbrace{\alpha,\alpha,\ldots,\alpha}_{k+1},1,\beta,\beta;f]. (50)

To calculate the coefficientsμ1,μ2\mu_{1},\mu_{2}, we identify the coefficients off(1)f(-1)andf(β)f^{\prime}(\beta)in (47) and (50). Taking into account (4), we deduce,

μ1=2(1+β)(1+α)k+1<0μ2=(βα)k+1(β1)c2.0=(βα)(β1)11(xα)kdx==(βα)(β1)uk+1vk+1k+1<0\begin{gathered}\mu_{1}=-2(1+\beta)(1+\alpha)^{k+1}<0\\ \mu_{2}=-(\beta-\alpha)^{k+1}(\beta-1)c_{2,0}=-(\beta-\alpha)(\beta-1)\int_{-1}^{1}(x-\alpha)^{k}dx=\\ =-(\beta-\alpha)(\beta-1)\frac{u^{k+1}-v^{k+1}}{k+1}<0\end{gathered}

It follows that the rest of the formula(F5)\left(\mathrm{F}_{5}\right)is of the simple form. This remainder is again given by formula (43) where, this time,kkis odd.

Theorem 5 is therefore completely proven.
The formula

11f(x)dx=213[12f(16)+f(2)]119D3[f]\int_{-1}^{1}f(x)dx=\frac{2}{13}\left[12f\left(-\frac{1}{6}\right)+f(2)\right]-\frac{11}{9}D_{3}[f]

is an example of a formula of the type (F5\mathrm{F}_{5}25.
Whenp=3,z1=1,z2=α,z3=1p=3,z_{1}=-1,z_{2}=\alpha,z_{3}=1, We havep=3p^{\prime}=3and we are still in the same situationpq1=1p^{\prime}-q-1=1or in the casepq1=2p^{\prime}--q-1=2. Forα(1.1)\alpha\in(-1,1)We studied the simplicity of the rest of this formula in a previous work [9]. In this case, when the formula has a degree of accuracym1m-1The rest is either in simple form or not in simple form depending on whether(1)k2+k3+1sg(c1,k11c3,k31)(-1)^{k_{2}+k_{3}+1}\mathrm{sg}\left(c_{1,k_{1}-1}c_{3,k_{3}-1}\right)is equal to 1 or -1.

We find the simplicity of the rest of Simpson's formula by takingk1=k3=1,k2=2,α=0k_{1}=k_{3}=1,k_{2}=2,\alpha=0. In this caseq=0q=0Andc1.0=c3.0=13c_{1,0}=c_{3,0}=\frac{1}{3}are indeed positive. Note that the simplicity of the rest of Simpson's formula is also obtained from Theorem 10 by takingρ=σ=m=1\rho=\sigma=m=1Indeed, this formula can also be obtained by takingk1=k2=k3=1k_{1}=k_{2}=k_{3}=1,α=0\alpha=0but then you have to takeq=1q=1In the first interpretation, we are in the casepq1=2p^{\prime}-q-1=2, but in the second interpretation in the casepq1=1p^{\prime}-q-1=1.

For Simpson's formula, we also have,

R*[f]=23[1,1,0,0,0,1;f]23[1,0,0,0,1,1;f]==43[1,1,0,0,1,1;f]\begin{gathered}R^{*}[f]=-\frac{2}{3}[-1,-1,0,0,0,1;f]-\frac{2}{3}[-1,0,0,0,1,1;f]=\\ =-\frac{4}{3}[-1,-1,0,0,1,1;f]\end{gathered}

As another example, consider the quadrature formula of DG SANIKIDZE [11],

11f(x)dx=1210[51f(1)42f(1)6f"(1)+\displaystyle\int_{-1}^{1}f(x)dx=\frac{1}{210}\left[-51f(-1)-42f^{\prime}(-1)-6f^{\prime\prime}(-1)+\right. (51)
+432f(0)48f(0)+40f"(0)+39f(1)]+R[f]\displaystyle\left.\quad+432f(0)-48f^{\prime}(0)+40f^{\prime\prime}(0)+39f(1)\right]+R[f]

In this casek1=3,k2=3,k3=1,α=0,c1.2=135<0,c3.0==1370>0k_{1}=3,k_{2}=3,k_{3}=1,\alpha=0,c_{1,2}=-\frac{1}{35}<0,c_{3,0}==\frac{13}{70}>0And(1)khas+khas+1sg(c1,k11c3,k31)=1(-1)^{k_{\mathrm{a}}+k_{\mathrm{a}}+1}\mathrm{sg}\left(c_{1,k_{1}-1}\cdot c_{3,k_{3}-1}\right)=1.

The remainder, equal to835D7[f]-\frac{8}{35}D_{7}[f], of this formula is therefore of degree of accuracy 6 and is of the simple form.

Regarding the formula given by DG SANIKIDZE (formula (11)) in his work [11], the simplicity of the remainder cannot be sufficiently recognized*).
26. The application of Theorem 9 generally requires the calculation of the coefficientsμi\mu_{i}of formula (35).

Assuming that formula (1) has a degree of accuracy equal tom+q1(q0)m+q-1(q\geq 0)we have for everythingjjverifying inequalities

k=max(k1+1,k2+1,,kp+1)jm+q+1k=\max\left(k_{1}+1,k_{2}+1,\ldots,k_{p}+1\right)\leqq j\leqq m+q+1 (52)

an equality of the form

R*[f]=i=1m+pjμi(j)[y1,y2,,yi+j;f]R^{*}[f]=\sum_{i=1}^{m+p^{\prime}-j}\mu_{i}^{(j)}\left[y_{1},y_{2},\ldots,y_{i+j};f\right] (53)

THEμi(j)\mu_{i}^{(j)}being independent of the functionffWe
then have

μi=μi(m+q+1),i=1.2,,pq1.\mu_{i}=\mu_{i}^{(m+q+1)},i=1,2,\ldots,p^{\prime}-q-1. (54)

Starting with the coefficientsμi(k),i=1.2,,m+pk\mu_{i}^{(k)},i=1,2,\ldots,m+p^{\prime}-kwe can successively calculate the coefficientsμi(j)\mu_{i}^{(j)}Fori=1.2,,m+pk,j=k,k+1,,m+q+1i=1,2,\ldots,m+p^{\prime}--k,j=k,k+1,\ldots,m+q+1using recurrence formulas

μi(j+1)=(yj+i+1yi)v=1iμv(j)\displaystyle\mu_{i}^{(j+1)}=-\left(y_{j+i+1}-y_{i}\right)\sum_{v=1}^{i}\mu_{v}^{(j)} (55)
i=1.2,,m+pj1,j=k,k+1,,m+q\displaystyle i=1,2,\ldots,m+p^{\prime}-j-1,\quad j=k,\quad k+1,\ldots,m+q

Applying this method gives us, in the case of formula (51),k=3k=3,

70R*[f]=12[1,1,1,1,;f]28[1,1,1.0;f]\displaystyle 0R^{*}[f]=2[-1,-1,-1,-1,;f]-8[-1,-1,-0;f]-
11[1,1,0,0;f]+76[1,0,0,0;f]\displaystyle-1[-1,-00;f]+6[-000;f]-
80[0,0,0,0;f]+44[0,0,0,1;f]13[0,0,1,1;f]\displaystyle-0[000;f]+4[001;f]-3[011;f]
00footnotetext: *). It follows from the above that in this formula one can always takeξ=η\xi=\eta.

and, using formulas (55) we find

35R*[f]=12[1,1,1,1,0,0,0,0,1;f]52[1,1,1,0,0,0,0,1,1;f]\begin{gathered}35R^{*}[f]=-12[-1,-1,-1,-1,0,0,0,0,1;f]-\\ -52[-1,-1,-1,0,0,0,0,1,1;f]\end{gathered}

This formula clearly highlights the simplicity of the remainder.
27. The preceding method can be applied, in general, to linear combinations.HAS[f]A[f]of a finite number of values ​​of the functionffand some of its derivatives, respecting, of course, the assumptions that were highlighted in our previous work [9]. For example, the linear functional

HAS[f]=f(1)f(0)f"(0)A[f]=f(1)-f(0)-f^{\prime\prime\prime}(0) (56)

is of degree of accuracy 0 but, obviously, cannot be put in the form (35). The linear functional (56) is defined for any functionffhaving a continuous derivative of order 3 on an intervalEEcontaining[0.1][0,1]butnnIt's not a simple form. Otherwise, for everythingffthere would be at least one pointξ\xibelonging to the interior ofEEsuch as one has

HAS[f]=f(ξ).A[f]=f^{\prime}(\xi). (57)

If we takef(x)=x3+x2f(x)=x^{3}+x^{2}equality (57) becomes3ξ2+2ξ+4=03\xi^{2}+2\xi+4=0which is not verified by any real value ofξ\xi.

§ 3

  1. 28.

    If the coefficientsμi\mu_{i}Since the terms in formula (35) are all of the same sign (and not all zero), we can deduce the simplicity of the remainder.R[f]R[f]without making the assumption3duno3\mathrm{du}\mathrm{no}.17 on the monotony of the sequence(yi)i=1m+p\left(y_{i}\right)_{i=1}^{m+p^{\prime}}.

Thus, we can state results analogous to that expressed by Theorem 11 when the nodesziz_{i}, without coinciding with points -1 and 1, are not necessarily all in (1.1-1,1). Taking into account (18) and (49), we deduce that (zi21,i=1.2,,pz_{i}^{2}\neq 1,i=1,2,\ldots,p) sg(μ1μ2)==sg(1)i=1p(ki+sgki)+1\left(\mu_{1}\mu_{2}\right)==\operatorname{sg}(-1)^{\sum_{i=1}^{p}\left(k_{i}^{\prime}+\mathrm{sg}^{\prime}k_{i}^{\prime}\right)+1}
Therefore, if the degree of accuracy ism+p2m+p-2, the simple p for is not of the form sime that the sumi=1(ki+sgki)\sum_{i=1}\left(k_{i}^{\prime}+\operatorname{sg}k_{i}^{\prime}\right)is odd or even.
29. Consider the formula of type (1)

11f(x)dx=i=1pcif(zi)+R[f]\int_{-1}^{1}f(x)dx=\sum_{i=1}^{p}c_{i}f\left(z_{i}\right)+R[f] (58)

the knotsziz_{i}being simple, distinct and different from the points1.1.𝐏𝐨𝐮𝐫\mathbf{-1,1.\penalty 10000\ Pour\penalty 10000\ }Let's clarify the ideas, suppose that1<z1<z2<<zp<1-1<z_{1}<z_{2}<\ldots<z_{p}<1So if we assume that the remainder of formula (58) vanishes for every polynomial of degreepp, we deduce the formula

R*[f]=i=1p(zi21)L(zi)ci[1,z1,z2,,zp,1,zi;f]R^{*}[f]=-\sum_{i=1}^{p}\left(z_{i}^{2}-1\right)l^{\prime}\left(z_{i}\right)c_{i}\left[-1,z_{1},z_{2},\ldots,z_{p},1,z_{i};f\right] (59)

OrL(x)=i=1p(xzi)l(x)=\prod_{i=1}^{p}\left(x-z_{i}\right)
The proof of formula (59) presents no difficulties. The difference between the two sides of this inequality is a linear combination of the values ​​at the points 1.1,z1,z2,,zp-1,1,z_{1},z_{2},\ldots,z_{p}of the functionffand which vanishes over any polynomial of degreep+1p+1Therefore, it is identically null.

From formula (59) we deduce
THEOREM 12. If in the quadrature formula (58) the coefficientscic_{i}are alternately positive and negative (cici+1<0,i=1.2,,p1c_{i}c_{i+1}<0,i=1,2,\ldots,p-1) and if the degree of accuracy of this formula is equal topp, its remainder is of simple form.

It is always assumed that1<z1<z2<<zp<1-1<z_{1}<z_{2}<\ldots<z_{p}<1
In particular, we have

11f(x)dx=2[f(16)f(0)+f(16)]+1345D4[f]11f(x)dx=2[f(3360)f(1360)+f(0)f(1360)++f(3360)]+382137800D6[f]\begin{gathered}\int_{-1}^{1}f(x)dx=2\left[f\left(-\frac{1}{\sqrt{6}}\right)-f(0)+f\left(\frac{1}{\sqrt{6}}\right)\right]+\frac{13}{45}D_{4}[f]\\ \int_{-1}^{1}f(x)dx=2\left[f\left(-\sqrt{\frac{33}{60}}\right)-f\left(-\sqrt{\frac{13}{60}}\right)+f(0)-f\left(\sqrt{\frac{13}{60}}\right)+\right.\\ \left.+f\left(\sqrt{\frac{33}{60}}\right)\right]+\frac{3821}{37800}D_{6}[f]\end{gathered}

which are valid for any functionffcontinues over the interval[1.1][-1,1]S. E. MIKELADZE gave these formulas [4], assuming thatffadmits a derivative4th 4^{\text{ième }}respectively a derivative6th 6^{\text{ième }}continue on[1.1][-1,1].

The existence of formulas of the form considered in Theorem 12 was studied by S.N. Bernstein [1].
30. The preceding results can easily be generalized. We will simply state the following result with respect to formula (1): Ifp>1,1z1<z2<<zp1p>1,-1\leqq z_{1}<z_{2}<\ldots<z_{p}\leqq 1, if the formula has a degree of
accuracym+pp2m+p^{\prime}-p-2and if(1)kici,ki1ci+1,ki+11>0(-1)^{k_{i}}c_{i,k_{i-1}}c_{i+1,k_{i+1^{-1}}}>0Fori=1.2i=1,2,,p1\cdots,p-1The rest is of simple form.

For example, the remainder of the quadrature formula

11f(x)dx=18[[3f(1)+3f(1)+16f(0)3f(13)3f(13)]+46135D4[f]\begin{gathered}\int_{-1}^{1}f(x)dx=\frac{1}{8}\left[\left[3f(-1)+3f(1)+16f(0)-3f\left(-\frac{1}{3}\right)-3f\left(\frac{1}{3}\right)\right]+\right.\\ -\frac{46}{135}D_{4}[f]\end{gathered}

is simple.
In the case of the formula

11f(x)dx=12[f(1)+2f(0)+f(1)]13D2[f]\int_{-1}^{1}f(x)dx=\frac{1}{2}[f(-1)+2f(0)+f(1)]-\frac{1}{3}D_{2}[f]

We haveR*[f]=[1,1,0,1;f]+[1,0,0,1;f][1,0,1,1;f]==12{[1,1,0,0;f]+[0,0,1,1;f]}R^{*}[f]=-[-1,-1,0,1;f]+[-1,0,0,1;f]-[-1,0,1,1;f]==-\frac{1}{2}\{[-1,-1,0,0;f]+[0,0,1,1;f]\}and the simplicity of the rest does not result from the previous remark, but rather from theorem 9.

84

  1. 31.

    In this section we will make some remarks on certain generalizations of Theorem 7. HE SALZER studied [10], as an extension of Chebyshev's formulas (34), the formulas

0exf(x)dx=1mi=1mf(zi)+R[f]\displaystyle\int_{0}^{\infty}e^{-x}f(x)dx=\frac{1}{m}\sum_{i=1}^{m}f\left(z_{i}\right)+R[f] (60)
ex2f(x)dx=πmi=1mf(zi)+R[f]\displaystyle\int_{-\infty}^{\infty}e^{-x^{2}}\cdot f(x)dx=\frac{\sqrt{\pi}}{m}\sum_{i=1}^{m}f\left(z_{i}\right)+R[f] (61)

degree of accuracym\geqq mThese are Chebyshev's formulas for the semi-infinite and infinite intervals.

We are taking now as a set\mathscr{F}the set of continuous functionsffon the intervalE=[0,+)E=[0,+\infty)respectively on the intervalE=(,+)E=(-\infty,+\infty)and for which the integral of the first member 7 exists.\mathcal{F}still contains all polynomials andR[f]R[f]is a linear functional defined on\mathscr{F}32.
Formula (60) does not exist form=3m=3and formula (61) does not exist form=4m=4(and for larger values ​​ofmm)

Chebyshev's formulas (60) form=1.2m=1,2and Chebyshev's formulas (61) form=1, 2, 3m=1,2,3have residues of the simple form and are written respectively

0exf(x)dx=f(1)+D2[f]\displaystyle\int_{0}^{\infty}e^{-x}f(x)dx=f(1)+D_{2}[f] (62)
exf(x)dx=12[f(0)+f(2)]+2D3[f]\displaystyle\int_{-\infty}^{\infty}e^{-x}f(x)dx=\frac{1}{2}[f(0)+f(2)]+2D_{3}[f] (63)
1πex2f(x)dx=f(0)+12D2[f]\displaystyle\frac{1}{\sqrt{\pi}}\int_{-\infty}^{\infty}e^{-x^{2}}f(x)dx=f(0)+\frac{1}{2}D_{2}[f] (64)
1πex2f(x)dx=12[f(12)+f(12)]+12D4[f]\displaystyle\frac{1}{\sqrt{\pi}}\int_{-\infty}^{\infty}e^{-x^{2}}f(x)dx=\frac{1}{2}\left[f\left(-\frac{1}{\sqrt{2}}\right)+f\left(\frac{1}{\sqrt{2}}\right)\right]+\frac{1}{2}D_{4}[f] (65)
1πex2f(x)dx=13[f(32)+f(0)+f(32)]+38D4[f]\displaystyle\frac{1}{\sqrt{\pi}}\int_{-\infty}^{\infty}e^{-x^{2}}f(x)dx=\frac{1}{3}\left[f\left(-\frac{\sqrt{3}}{2}\right)+f(0)+f\left(\frac{\sqrt{3}}{2}\right)\right]+\frac{3}{8}D_{4}[f] (66)
  1. 33.

    The proof of formulas (62)-(65) presents no difficulties since these formulas do not change if the terms are added to the right-hand side.0.f(1),0.f(2),0.f(0),0.f(12)+0.f(12)0.f^{\prime}(1),0.f^{\prime}(2),0.f^{\prime}(0),0.f^{\prime}\left(\frac{1}{\sqrt{2}}\right)+0.f^{\prime}\left(-\frac{1}{\sqrt{2}}\right)respectively and the rest of these formulas can therefore be written

R[f]=0(x1)2ex[1.1,x;f]dxR[f]=0x(x2)2ex[0,2,2,x;f]dxπR[f]=x2ex2[0.0,x;f]dxπR[f]=(x212)2ex2[12,12,12,12,x;f]dx\begin{gathered}R[f]=\int_{0}^{\infty}(x-1)^{2}e^{-x}[1,1,x;f]dx\\ R[f]=\int_{0}^{\infty}x(x-2)^{2}e^{-x}[0,2,2,x;f]dx\\ \sqrt{\pi}R[f]=\int_{-\infty}^{\infty}x^{2}e^{-x^{2}}[0,0,x;f]dx\\ \sqrt{\pi}R[f]=\int_{-\infty}^{\infty}\left(x^{2}-\frac{1}{2}\right)^{2}e^{-x^{2}}\left[-\frac{1}{\sqrt{2}},-\frac{1}{\sqrt{2}},\frac{1}{\sqrt{2}},\frac{1}{\sqrt{2}},x;f\right]dx\end{gathered}

respectively.

It follows that formulas (62) - (65) are valid for any functionfWf\in\mathbb{F}differentiable.
34. On formula (66) we will establish only a less general result. The rest of this formula can be written

πR[f]=x(x234)ex2[0,32,32,x;f]dx\sqrt{\pi}R[f]=\int_{-\infty}^{\infty}x\left(x^{2}-\frac{3}{4}\right)e^{-x^{2}}\left[0,-\frac{\sqrt{3}}{2},\frac{\sqrt{3}}{2},x;f\right]dx

and the parts integration formula

πR[f]=(x22+18)ex2[0,32,32,x;f]|+\displaystyle\sqrt{\pi}R[f]=-\left.\left(\frac{x^{2}}{2}+\frac{1}{8}\right)e^{-x^{2}}\left[0,-\frac{\sqrt{3}}{2},\frac{\sqrt{3}}{2},x;f\right]\right|_{-\infty}^{\infty}+
+(x22+18)[0,32,32,x,x;f]ex2dx\displaystyle\quad+\int_{-\infty}^{\infty}\left(\frac{x^{2}}{2}+\frac{1}{8}\right)\left[0,-\frac{\sqrt{3}}{2},\frac{\sqrt{3}}{2},x,x;f\right]e^{-x^{2}}dx

It follows that formula (66) is true for any functionfffor which the integral of the second member exists (in particular for any polynomial).

BIBLIOGRAPHY

[1] Bernstein S., Some applications of the parametric method to the study of quadrature formulas. Communic. Kharkow (4) 15, 1, 3-29 (1938). . 1959.

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[7] - 53-122 (1952). Supra numerică to him Gauss. Studii
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[8] - și Cerc. St. Iași, 6, 29-57 (1955). linear approximation of the analysis. [9] - On the remainder in certain formulas
Mathematica 1 (24), 95-142 (1959). quadrature formulas over semi-infinite [10] Salzer Herbert E., Equally weighted quadvand Phys., XXXIV, 54-63 (1955). and infinite intervals'. Journan of mazdelenimi raznostiami. Sobsc. Acad. [11] Sanikidze DG, Interpolirovanie (1960). [12] Steffensen JF, Interpolation, 1950.

1964

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