<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.411A3002</article-id><article-id pub-id-type="publisher-id">AM-38300</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Approximation by Splines of Hermite Type
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uri</surname><given-names>K. Dem’yanovich</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Irina</surname><given-names>G. Burova</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Faculty of Mathematics and Mechanics, St. Petersburg State University, St. Petersburg, Russia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Yuri.Demjanovich@gmail.com(UKD)</email>;<email>burovaig@mail.ru(IGB)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>18</day><month>10</month><year>2013</year></pub-date><volume>04</volume><issue>11</issue><fpage>5</fpage><lpage>10</lpage><history><date date-type="received"><day>July</day>	<month>24,</month>	<year>2013</year></date><date date-type="rev-recd"><day>August</day>	<month>24,</month>	<year>2013</year>	</date><date date-type="accepted"><day>August</day>	<month>31,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   The approximation evaluations by polynomial splines are well-known. They are obtained by the similarity principle; in the case of non-polynomial splines the implementation of this principle is difficult. Another method for obtaining of the evaluations was discussed earlier (see [1]) in the case of nonpolynomial splines of Lagrange type. The aim of this paper is to obtain the evaluations of approximation by non-polynomial splines of Hermite type. Considering a linearly independent system of column-vectors<inline-formula><inline-graphic xlink:href="dit_197865d8-1c35-418b-9dd7-6394cac42a26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="dit_a81210c2-f305-4f61-9d25-e52accd94ddb.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="dit_2078b0fa-91da-4e4b-b49b-a33a423fce80.png" xlink:type="simple"/></inline-formula> be square matrix. Supposing that <inline-formula><inline-graphic xlink:href="dit_d57e83ae-dbdd-455f-a146-946e84793fc2.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="dit_17a58a6a-cf01-4bd9-9e01-01bb9f4a9c2d.png" xlink:type="simple"/></inline-formula> are columns with components from the linear space <inline-formula><inline-graphic xlink:href="dit_4b3a9207-78fd-4ee4-a69a-cdc0e48ac88b.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="dit_2b141c1c-d8a5-4457-845a-9fab3a2efab9.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="dit_beffd9fa-dac9-4ae1-91ff-26025557b3ca.png" xlink:type="simple"/></inline-formula> be vector with components <inline-formula><inline-graphic xlink:href="dit_176a1400-70f0-4ff8-81ea-563e58c13817.png" xlink:type="simple"/></inline-formula> belonging to conjugate space <inline-formula><inline-graphic xlink:href="dit_f3f37a57-c036-471f-b717-cb0f2472f088.png" xlink:type="simple"/></inline-formula>. For an element <inline-formula><inline-graphic xlink:href="dit_2d1534d1-3f18-4d3d-afe3-3a8635a3e11b.png" xlink:type="simple"/></inline-formula> we consider a linear combination of elements <inline-formula><inline-graphic xlink:href="dit_ab64523b-a0c9-4f88-adb3-30cbd2c0109f.png" xlink:type="simple"/></inline-formula> By definition, put <inline-formula><inline-graphic xlink:href="dit_b06b542e-cd58-4bc9-b6da-87dedce11d55.png" xlink:type="simple"/></inline-formula>. The discussions are based on the next assertion. The following relation holds: <inline-formula><inline-graphic xlink:href="dit_b4e6051d-5bd3-4fca-8260-490680d5ae00.png" xlink:type="simple"/></inline-formula> where the second factor on the right-hand side is the determinant of a block-matrix of order m + 2. Using this assertion, we get the representation of residual of approximation by minimal splines of Hermite type. Taking into account the representation, we get evaluations of the residual and calculate relevant constants. As a result the obtained evaluations are exact ones for components of generated vector-function <inline-formula><inline-graphic xlink:href="dit_ed8afa3a-a228-41eb-b08a-ad68bf050e57.png" xlink:type="simple"/></inline-formula>.  
    
 
</p></abstract><kwd-group><kwd>Splines; Errors of Approximations</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Representation of Approximation Residual</title><p>For convenience we shall give scheme of representation of the approximation residual in general situation (see also [<xref ref-type="bibr" rid="scirp.38300-ref1">1</xref>]).</p><p>We consider a linearly independent system of columnvectors <img src="2-7401746\c6b4c72b-b28c-4522-b78e-c9d34eca43e7.jpg" /> (where m is a natural number)</p><p>in the space<img src="2-7401746\34bf6a53-5a48-43f1-bf6e-72dd7877bd9c.jpg" />. The matrix <img src="2-7401746\18138c7d-0217-4b9b-9bf7-7eb402e148b9.jpg" /> composed of these columns is denoted by</p><disp-formula id="scirp.38300-formula62507"><label>(1)</label><graphic position="anchor" xlink:href="2-7401746\05e12c94-d54e-49f6-a5f0-827999bed628.jpg"  xlink:type="simple"/></disp-formula><p>Let <img src="2-7401746\ada989e7-9eb0-4d78-9691-eebf3d4e4528.jpg" /> be linear space.</p><p>Suppose that <img src="2-7401746\35d5f60d-e9e6-418d-b9ba-cbb32ca49862.jpg" /> and</p><p><img src="2-7401746\3e3a73dc-6765-486c-a12a-6cec7ec70807.jpg" />are columns with components belonging to the space<img src="2-7401746\228cfb6d-1528-47e7-930e-53d8f5e041af.jpg" />; assume the relation</p><disp-formula id="scirp.38300-formula62508"><label>(2)</label><graphic position="anchor" xlink:href="2-7401746\3b0d5ba6-2c4e-4cea-829b-d11785119f11.jpg"  xlink:type="simple"/></disp-formula><p>is valid; matrix A is defined by (1).</p><p>Let <img src="2-7401746\9cc2882b-b87c-46d8-b734-69e91ca53db9.jpg" /> be vector with components</p><p><img src="2-7401746\dd0c73e7-4537-4649-a1d8-b5b1eb9fad18.jpg" />belonging to conjugate space<img src="2-7401746\554690a3-465e-4d10-8f5f-741b132c0998.jpg" />.</p><p>For an element <img src="2-7401746\973c44c9-4a67-4e53-a37c-a6cb25c67a50.jpg" /> we consider a linear combination of elements<img src="2-7401746\50ad5e56-437c-4f93-8758-43c58dc6c260.jpg" />:</p><disp-formula id="scirp.38300-formula62509"><label>(3)</label><graphic position="anchor" xlink:href="2-7401746\c373073b-decf-4595-816e-b062e24f2e9d.jpg"  xlink:type="simple"/></disp-formula><p>From (2) and (3) it follows that</p><disp-formula id="scirp.38300-formula62510"><label>(4)</label><graphic position="anchor" xlink:href="2-7401746\5be8c87b-35a1-4af6-bf79-1d30b8665d05.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="2-7401746\9c34314d-61bb-4bf2-9ab7-fc98a4cf1e8f.jpg" /> denotes the column-vector in<img src="2-7401746\4f546906-0aaf-499a-9083-2aef94b4d88e.jpg" />namely,<img src="2-7401746\09ced6e2-024e-4ddf-ac70-89be165ed29d.jpg" />. The outer round brackets in (4) mean the inner product of <img src="2-7401746\b8c7c961-b6e9-4a0c-8493-0e6fa4f43770.jpg" />-dimensional vectors.</p><p>Theorem 1 The following relation holds:</p><disp-formula id="scirp.38300-formula62511"><label>(5)</label><graphic position="anchor" xlink:href="2-7401746\e9e9c2ad-b919-44e0-ba29-90822ff32196.jpg"  xlink:type="simple"/></disp-formula><p>where the second factor on the right-hand side is the determinant of a block-matrix of order<img src="2-7401746\d7320b88-04d4-4b69-bbfd-8fbe437fb81f.jpg" />.</p><p>Proof By (4), we have <img src="2-7401746\dfe81fab-a8ff-4492-ae8d-20d2ff58ddb2.jpg" /> Hence</p><disp-formula id="scirp.38300-formula62512"><label>(6)</label><graphic position="anchor" xlink:href="2-7401746\e769933b-1abf-44cb-8a56-68d60df70c85.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="2-7401746\1c3e1767-e7e2-44d0-9864-59c2e6deb9e4.jpg" /> is the cofactor of an entry <img src="2-7401746\a7c86c24-2a07-4e1a-bce9-e79a2b3c65bd.jpg" /> of the matrix<img src="2-7401746\1646d1ad-8ce4-4acd-a4e6-36f2ad0c3da5.jpg" />. By (6), we can represent the difference <img src="2-7401746\d3c2ee3b-3fbf-439d-9276-0cf7cfa8c662.jpg" /> as the product of determinants, written as</p><disp-formula id="scirp.38300-formula62513"><label>(7)</label><graphic position="anchor" xlink:href="2-7401746\a628482c-8c4f-4550-8a0d-cddc66687dcd.jpg"  xlink:type="simple"/></disp-formula><p>The equality (7) is equivalent to the equality (5).</p></sec><sec id="s2"><title>2. Representation of the Remainder of Approximation by Elementary Hermite Type Splines</title><p>On <img src="2-7401746\924d4a4e-faf9-47ff-968f-01df2b82caf7.jpg" /> we consider a grid of the form</p><p><img src="2-7401746\d7685cea-2c06-4ff2-acee-12fbc44c7a3c.jpg" /></p><p><img src="2-7401746\73c4d9a0-ad38-4993-8cc9-1f07b0e4e0e4.jpg" /></p><p>We set</p><p><img src="2-7401746\fe54bc21-8418-4fe6-871d-4c9e585fd1d4.jpg" /></p><p>Let <img src="2-7401746\2243f2d7-e57c-423c-9426-ad972992c800.jpg" /> be <img src="2-7401746\3adf73fa-c18c-4897-b414-adfd593dcd79.jpg" />-component vector-function with components in<img src="2-7401746\fd7a289f-678f-4b0d-8e03-48f0a346e531.jpg" />. We assume that Wronskian of the components is separated from zero.</p><p>Consider function<img src="2-7401746\431b62d0-241b-4697-9410-e15e902434de.jpg" />, <img src="2-7401746\1e6b157d-5534-439f-914a-602f188d53f5.jpg" />, and introduce notation</p><disp-formula id="scirp.38300-formula62514"><label>(8)</label><graphic position="anchor" xlink:href="2-7401746\e973bd1a-e068-4da3-9b82-c89bbe59b5d0.jpg"  xlink:type="simple"/></disp-formula><p>Let symbol <img src="2-7401746\ad556780-3fa0-4f05-b998-ba9f168b2b70.jpg" /> denote the number of elements of a set<img src="2-7401746\827c34d1-6fe6-419c-9529-06d4e63f85b1.jpg" />.</p><p>We assume that natural numbers <img src="2-7401746\40a52d72-d616-4904-a7f9-9ad8da9de7cd.jpg" /> comply with relations<img src="2-7401746\7646f008-ea71-4cdc-9feb-666831d943ce.jpg" />, <img src="2-7401746\19ea56dd-532e-42b1-b5ed-85c2cda8ff71.jpg" />,<img src="2-7401746\eb2e8837-d453-43fd-918b-c8cb40297265.jpg" />.</p><p>By definition, put</p><p><img src="2-7401746\db0abd55-1747-4db6-b12d-29d11066583b.jpg" /></p><p>where<img src="2-7401746\18e4ed70-6263-4e97-a2e6-30226f41d506.jpg" />. Obviously<img src="2-7401746\140e21bc-0882-473f-a874-77b712c7825c.jpg" />.</p><p>We introduce the functions <img src="2-7401746\9adf4ad2-ba9a-49ff-b331-9ed61cc79f09.jpg" /> by the approximate relations</p><disp-formula id="scirp.38300-formula62515"><label>(9)</label><graphic position="anchor" xlink:href="2-7401746\25b8e68a-b0b2-4576-8483-3275965b7135.jpg"  xlink:type="simple"/></disp-formula><p><img src="2-7401746\d4b0601d-e7d8-4d5e-9b0a-d4944ba7b271.jpg" /></p><p>Consider square matrix <img src="2-7401746\b41ce29c-490a-49bb-874b-208151cac304.jpg" /> of the order <img src="2-7401746\8a8d637c-c353-4562-b17c-cd3dd8e8e861.jpg" /> (see notation (8)),</p><p><img src="2-7401746\987c967a-9c89-4574-a651-d7008aaf85bc.jpg" /></p><p>and vector-function</p><p><img src="2-7401746\fb509c21-66b2-46b4-8851-0fa26746ed9f.jpg" /></p><p>then the relations (9) may be rewritten as</p><p><img src="2-7401746\29d88823-5055-4d8e-a856-45686b20f9b8.jpg" /></p><p><img src="2-7401746\692aef4d-0287-4b39-b882-878f55ac4733.jpg" /></p><p>It can be proved (for example, see [<xref ref-type="bibr" rid="scirp.38300-ref2">2</xref>]) that the matrix <img src="2-7401746\d022ae15-0956-44c6-bcae-9de39022bb39.jpg" /> is invertible. Hence the functions <img src="2-7401746\b31456c3-6ddb-4d7c-8436-a99d2123fe9c.jpg" /> are defined uniquely and they are linear independent. If<img src="2-7401746\cae52f69-51cb-4ab7-98d9-d8aacb04e12d.jpg" />, <img src="2-7401746\26bf89b4-9b2f-4847-971a-73c6e929d6af.jpg" />, then the functions <img src="2-7401746\02181211-60f5-4600-a63a-fca8f4745080.jpg" /> belong to<img src="2-7401746\2376d2ec-d621-40f0-91e3-36057be2630a.jpg" />, and functional system <img src="2-7401746\5bab57f3-82c5-468c-a330-e19ade4c6f8f.jpg" /> defined by formula</p><p><img src="2-7401746\12c33406-eebc-44f6-a961-7eec7feba386.jpg" /></p><p>is biorthogonal to the system <img src="2-7401746\19523b0e-bc5d-4a0c-ab36-92ce7beac736.jpg" /> so that</p><p><img src="2-7401746\f3067604-0943-456f-a6e5-42e1bd5779d5.jpg" /></p><p>Rewrite the system (9) in the form</p><disp-formula id="scirp.38300-formula62516"><label>(10)</label><graphic position="anchor" xlink:href="2-7401746\7e05ac2f-79e8-4eec-8e6a-2287eaeac18b.jpg"  xlink:type="simple"/></disp-formula><p>Under condition <img src="2-7401746\eca2b937-a12e-47af-8da3-448aef27645c.jpg" /> we have</p><p><img src="2-7401746\716c5a1f-b751-4e27-bb4d-e013e5d9584e.jpg" /></p><p>Analogously on the adjacent interval we get</p><p><img src="2-7401746\c2f09a3b-7d92-4df7-88b5-4577dba336ab.jpg" /></p><p>Discuss the linear space</p><p><img src="2-7401746\2e617037-336e-4fff-8599-9617dbc50787.jpg" /></p><p>where <img src="2-7401746\60637c2d-0e8b-4c86-a00a-c2965a765ad4.jpg" /> is the linear hull of the elements in the curly brackets and <img src="2-7401746\c5eca7ba-2d94-47f2-8afd-94ce889315c9.jpg" /> means the closure of the linear hull in the topology of pointwise convergence.</p><p>We call <img src="2-7401746\4283ae5c-418a-4c23-9432-752e3fec81bd.jpg" /> the space of elementary Hermite type <img src="2-7401746\6232527e-1914-4307-9e33-1982eab48010.jpg" />-splines.</p><p>By definition, put</p><p><img src="2-7401746\1f31504a-b7ed-41c3-95ea-b35bc5f2873b.jpg" /></p><p>We consider the function <img src="2-7401746\aa941391-6de5-4a73-ba15-5f3d5f05ba4c.jpg" /> defined by</p><disp-formula id="scirp.38300-formula62517"><label>(11)</label><graphic position="anchor" xlink:href="2-7401746\cfcada41-7702-42f0-a167-d30e59a1236b.jpg"  xlink:type="simple"/></disp-formula><p>Theorem 2 For<img src="2-7401746\013ac43c-6de1-46ae-8b63-4663e940cd63.jpg" />, <img src="2-7401746\a40b8647-ea1a-4e6e-bec9-6d01f06d1705.jpg" />,</p><disp-formula id="scirp.38300-formula62518"><label>(12)</label><graphic position="anchor" xlink:href="2-7401746\79f1d4e0-78bb-4621-b10b-988f1264d4b1.jpg"  xlink:type="simple"/></disp-formula><p>where the second factor on the right-hand side is the determinant of the square matrix of order <img src="2-7401746\86d89d53-1561-4961-a266-416b23126899.jpg" /> written in the block form.</p><p>Proof We can obtain the identity (12) by expanding the second determinant of right part of (12) and by usage of the relations (10)-(11) (cf. [<xref ref-type="bibr" rid="scirp.38300-ref1">1</xref>]).</p></sec><sec id="s3"><title>3. Some Auxiliary Assertions</title><p>Let<img src="2-7401746\46c9b4c9-fd6b-483e-bac5-239c2f2c894c.jpg" />, <img src="2-7401746\3c263442-3c63-432d-b4dd-03614c1550a9.jpg" />be natural numbers with property<img src="2-7401746\18987b0c-51d0-4eec-87b5-a0762d1aec4d.jpg" />; let <img src="2-7401746\7a13b54e-15b9-4ee2-be18-abaad5aff75d.jpg" /> be real numbers, which comply with inequalities <img src="2-7401746\cd6f904b-a753-41ff-8f3d-e4fdb9169025.jpg" />. Let us put</p><p><img src="2-7401746\94dab4ad-8009-4684-996a-9022b3b51589.jpg" />,<img src="2-7401746\e83687cf-fe70-49ed-9af5-eabafbc01ee4.jpg" />.</p><p>Lemma 1 For arbitrary <img src="2-7401746\00807ba9-24bf-4eeb-abef-4cb1ec73ae9e.jpg" />-component vector-function <img src="2-7401746\79fa62f7-4cc8-4e61-a15e-31955b81a62a.jpg" /> the representation</p><disp-formula id="scirp.38300-formula62519"><label>(13)</label><graphic position="anchor" xlink:href="2-7401746\59503581-c26f-4deb-9b59-f1cec7cc98c6.jpg"  xlink:type="simple"/></disp-formula><p>is valid; here <img src="2-7401746\897647e5-fb1a-4519-88d6-122269de0d88.jpg" /> is a linear operator of integration over parallelepiped</p><p><img src="2-7401746\55f06b0e-eb0d-4dff-8a98-0f68e3ddeb9c.jpg" /></p><p>with nonnegative kernel.</p><p>Proof We consider the case <img src="2-7401746\38f8d46e-25da-4f4e-9cd7-491920ccc684.jpg" /> <img src="2-7401746\9326dfa4-d0a5-489e-b0ac-90ea30361594.jpg" /> <img src="2-7401746\7496469b-a7df-4000-ac90-9df5ae2960fb.jpg" />,<img src="2-7401746\7ca8bc37-d796-45bc-af20-91c96e14b8eb.jpg" />. Introduce value <img src="2-7401746\8a7aed30-bd41-4e72-aa6f-1fe8e904d6cb.jpg" /> with property <img src="2-7401746\643747ac-4415-416e-9311-a6f88508172f.jpg" /> and use notation</p><disp-formula id="scirp.38300-formula62520"><label>(14)</label><graphic position="anchor" xlink:href="2-7401746\1d4e7539-660f-466d-9d92-eff9bddd0645.jpg"  xlink:type="simple"/></disp-formula><p>so that<img src="2-7401746\7d568508-1f1a-4208-9915-66b302399699.jpg" />.</p><p>Using the additivity property of determinants and integrals and applying the Newton?-Leibnitz formula, we find</p><p><img src="2-7401746\9ae0b167-ca5a-453a-ac0b-1e665d31d100.jpg" /></p><p>where<img src="2-7401746\1078a0f7-282a-4fdf-952f-c178e933fcc8.jpg" />,</p><disp-formula id="scirp.38300-formula62521"><label>(15)</label><graphic position="anchor" xlink:href="2-7401746\0ccda7cd-1a1d-425f-bda5-bb4951d70264.jpg"  xlink:type="simple"/></disp-formula><p>Similarly,</p><p><img src="2-7401746\3ca4129a-501a-4922-a186-b878507c08c9.jpg" /></p><p>where</p><disp-formula id="scirp.38300-formula62522"><label>(16)</label><graphic position="anchor" xlink:href="2-7401746\2cc77354-9ab6-46bc-bf1c-bfaa7fd0e62c.jpg"  xlink:type="simple"/></disp-formula><p>Finally</p><p><img src="2-7401746\401f180a-1879-4802-851e-6a86df0b05f1.jpg" /></p><p>where</p><disp-formula id="scirp.38300-formula62523"><label>(17)</label><graphic position="anchor" xlink:href="2-7401746\f2a22826-2e6a-4a75-a4d4-eda6a22bd2b9.jpg"  xlink:type="simple"/></disp-formula><p>Integral operators <img src="2-7401746\055d9f63-ef6b-4888-95e1-03c075ac5de2.jpg" /> can be rewritten in the form</p><p><img src="2-7401746\88f7aace-3985-4a44-b701-224ccf77f88e.jpg" /></p><p>where<img src="2-7401746\31c9eb88-5dca-4166-aa12-ecc6b3edc663.jpg" />, and</p><p><img src="2-7401746\2a204d9c-a597-4f16-9151-552c496e2463.jpg" />.</p><p>It is obvious that</p><disp-formula id="scirp.38300-formula62524"><label>(18)</label><graphic position="anchor" xlink:href="2-7401746\08d99736-1e8b-4b92-8cce-b08137e70b1b.jpg"  xlink:type="simple"/></disp-formula><p>Since the lower limit is no more than the upper one in the integrals in (15)-(17), the result of integration is nonnegative for any nonnegative continuous function<img src="2-7401746\05cf6b5f-cfae-413f-9aa5-01e604ce9f75.jpg" />. Hence the integral operations<img src="2-7401746\39e0006f-af90-4e87-8989-2fdba91c39ac.jpg" />, have nonnegative kernels By (17) we have</p><disp-formula id="scirp.38300-formula62525"><label>(19)</label><graphic position="anchor" xlink:href="2-7401746\a19561d8-bc68-47e2-9b63-668e48bf1689.jpg"  xlink:type="simple"/></disp-formula><p>Recall that vector-function <img src="2-7401746\06a0dce7-7a08-4048-ad2a-5e6dcf4a3b63.jpg" /> is continuously differentiable in neighborhood of the point<img src="2-7401746\b4013a2a-dc6c-4a5f-8422-6a80328f05c1.jpg" />, and passaging to limit as<img src="2-7401746\8e25915c-3952-41eb-aea3-83656944f855.jpg" />, we get</p><disp-formula id="scirp.38300-formula62526"><label>(20)</label><graphic position="anchor" xlink:href="2-7401746\61d17d25-2a36-4ef8-9809-db3b343fe725.jpg"  xlink:type="simple"/></disp-formula><p>It follows easily that relation (20) can be written in the form</p><p><img src="2-7401746\18544bb3-9ca8-469e-b929-576079e7527b.jpg" /></p><p>where<img src="2-7401746\2e08aae0-1d14-45d5-898b-d7650f008ad3.jpg" />, and the operator <img src="2-7401746\397d7e38-8263-4dc8-bf12-8e952d95c5dc.jpg" /> is defined by identity</p><disp-formula id="scirp.38300-formula62527"><label>(21)</label><graphic position="anchor" xlink:href="2-7401746\b8595378-4c85-4cc4-8150-540e5e611b57.jpg"  xlink:type="simple"/></disp-formula><p>By relations (18) and (21) we see that the integral operator <img src="2-7401746\0e25f606-9ecd-4753-9643-b17d55a056ce.jpg" /> may be represented in the form</p><p><img src="2-7401746\a4d259fe-bcbf-48b0-bdad-6bbe7d7e6526.jpg" /></p><p>where<img src="2-7401746\cbcd9c08-cb96-442c-830f-55372ee87fd6.jpg" />, and <img src="2-7401746\ae28ab55-0531-41d2-a4ba-1ff65597e8e7.jpg" /> is nonnegative function Taking into account (14), we obtain <img src="2-7401746\91f0c17b-a931-40c0-b909-2367344814f3.jpg" />, where<img src="2-7401746\4d1a73f2-4e87-48ff-9db5-cea758f0c12b.jpg" />, <img src="2-7401746\65fe20ac-85f0-45a8-9149-ecaf83ffc70c.jpg" />,<img src="2-7401746\f1b0d589-d174-4d52-9077-ac45911c3dd9.jpg" />. Thus the assertion is true in discussed case.</p><p>Now consider the case of<img src="2-7401746\ce9f1786-be97-4d88-badb-bc0debcea402.jpg" />, <img src="2-7401746\37c8a0ce-4bb4-43bd-b0b4-1d0cacd16bfb.jpg" />,<img src="2-7401746\cf7a292d-7b39-45f6-ac2b-02627b207086.jpg" />.</p><p>Let <img src="2-7401746\173011b3-ee4d-4ba7-b5e6-c2af78e16bfb.jpg" /> is new variable,<img src="2-7401746\73ac4cde-e063-41bf-818a-4080962ffbf9.jpg" />; by definition put</p><disp-formula id="scirp.38300-formula62528"><label>(22)</label><graphic position="anchor" xlink:href="2-7401746\6936b350-ff7a-4399-b0bf-757817877776.jpg"  xlink:type="simple"/></disp-formula><p>so that<img src="2-7401746\ff22e523-0879-4a20-a8dd-0676be2e8057.jpg" />.</p><p>Under condition <img src="2-7401746\4e8a6702-9a13-4b93-8947-db4df8ed68ed.jpg" /> according to Taylor formula we have</p><p><img src="2-7401746\a02bc719-cdbc-4c5b-a574-70cb1120522b.jpg" /></p><p>whence we get</p><p><img src="2-7401746\2675a9e0-14f5-4ec5-9f37-ff5b6c630a7c.jpg" /></p><p>Thus by (21) we obtain</p><p><img src="2-7401746\b88f5ea4-b359-430c-915e-25cf4a41f36d.jpg" /></p><p>where</p><disp-formula id="scirp.38300-formula62529"><label>(23)</label><graphic position="anchor" xlink:href="2-7401746\21006dd4-8be2-4c9b-ba5b-60f84f97bb1f.jpg"  xlink:type="simple"/></disp-formula><p>It follows in the standard way that</p><p><img src="2-7401746\4a997741-73cd-43bc-9aa1-96e1b4faf137.jpg" /></p><p>where<img src="2-7401746\7823ba12-f945-40cb-80fd-bcaba8db2a39.jpg" />,<img src="2-7401746\e5afedcc-884a-4c78-b370-a2ed0959b40e.jpg" />.</p><p>Passaging to limit under <img src="2-7401746\1babe863-5130-4067-b8cb-972dfad5ad3d.jpg" /> we obtain</p><p><img src="2-7401746\3db205e9-0b9d-42af-a2ba-5422685250c7.jpg" /></p><p>taking into account (23), we rewrite the formula in the form</p><p><img src="2-7401746\08073557-04f1-408b-8f59-9809eb5f8255.jpg" /></p><p>Thus</p><p><img src="2-7401746\caf30309-af91-4e27-a7bd-218377f44f60.jpg" /></p><p>where</p><p><img src="2-7401746\3df12e82-a61e-4ce7-a88e-fae0e2f05443.jpg" /></p><p>here <img src="2-7401746\250c4ed7-2806-4a37-8044-cca9e0c8c1d4.jpg" /> and <img src="2-7401746\d2fc522f-e328-4322-8f26-cc74da8a2ebf.jpg" /> is nonnegative function.</p><p>Now recall notation (22); we obtain <img src="2-7401746\71418526-cdcc-47b8-b093-7f034d311d3c.jpg" />, where<img src="2-7401746\2853aa2c-99e4-4867-9061-aa4e098365f3.jpg" />,<img src="2-7401746\4ce1d7ff-0034-4a97-96c9-cf88ad71e5ee.jpg" />. This completes the proof in discussed case.</p><p>For an arbitrary natural <img src="2-7401746\7fe4f392-a9be-4488-8805-4c7d343749f7.jpg" /> one can obtain a similar representation via multiple integrals with the lower integration limit less than the upper one. Analogously the assertion is proved for<img src="2-7401746\3b414419-f2a0-4801-948e-b680b8e1f012.jpg" />. This completes the proof.</p><p>Denote <img src="2-7401746\d686ae62-f351-453f-ac0d-7264868b30cb.jpg" /> and introduce the function <img src="2-7401746\53ab051f-8132-439c-88c3-6da0435d12c4.jpg" /></p><p>Lemma 2 If suppositions of Lemma 1 are fulfilled, then</p><disp-formula id="scirp.38300-formula62530"><label>(24)</label><graphic position="anchor" xlink:href="2-7401746\d98312d0-c311-48f6-99fe-f3beecf101ee.jpg"  xlink:type="simple"/></disp-formula><p>Proof Substituting vector-function <img src="2-7401746\dea42889-6f5f-4042-b64b-846ea239bba0.jpg" /> for <img src="2-7401746\94d2d78e-acb4-4f10-9aa9-e44024a2ce2a.jpg" /> in (13), we have</p><disp-formula id="scirp.38300-formula62531"><label>(25)</label><graphic position="anchor" xlink:href="2-7401746\71bf9fd5-600c-42df-965c-63d11ab763dc.jpg"  xlink:type="simple"/></disp-formula><p>The determinant on the right-hand side of (25) contains a lower triangular matrix with entries <img src="2-7401746\fde8a79b-62bc-40ee-9257-2ff5881bb8d8.jpg" /> at the main diagonal so that right-hand side is equal to</p><disp-formula id="scirp.38300-formula62532"><label>(26)</label><graphic position="anchor" xlink:href="2-7401746\41c3b3f0-2f8b-4934-8a31-9b7c8ab7a197.jpg"  xlink:type="simple"/></disp-formula><p>The left-hand side contains the determinant of matrix, which appears in Hermite interpolation problem</p><p><img src="2-7401746\4ea80c7a-e068-48f6-8ee8-adbe7da522fd.jpg" /></p><p>where <img src="2-7401746\cc431a0c-a4f9-4f36-a592-373ceaaab073.jpg" /> are prescribed numbers and</p><p><img src="2-7401746\506c0978-2c91-4b1f-a270-c9ea31e3d561.jpg" />. Value of the mentioned determinant is known (see [<xref ref-type="bibr" rid="scirp.38300-ref3">3</xref>], p. 43); it is equal to</p><disp-formula id="scirp.38300-formula62533"><label>(27)</label><graphic position="anchor" xlink:href="2-7401746\d7ffe0fa-e64b-4e24-ba1c-f1d66156b937.jpg"  xlink:type="simple"/></disp-formula><p>Equating of (26) to (27) gives (24). It completes the proof.</p></sec><sec id="s4"><title>4. Evaluations of Approximation by Splines of Hermite Type</title><p>We assume that <img src="2-7401746\e6e03c51-28d6-4154-9b58-d082f4b76b08.jpg" /> and</p><disp-formula id="scirp.38300-formula62534"><label>(28)</label><graphic position="anchor" xlink:href="2-7401746\508f3f11-dfe4-4063-9066-d60c70dbf4bc.jpg"  xlink:type="simple"/></disp-formula><p>By the uniform continuity of the function under consideration on [a,b], from (28) we conclude that for any <img src="2-7401746\2cea0e61-f3fe-452a-8b90-744f4f477eee.jpg" /> there exists <img src="2-7401746\af9445da-cd6d-4cb0-ab8e-cfbe0cc511a6.jpg" /> such that for <img src="2-7401746\8464d893-2fb0-4164-846d-32f9c1247f4d.jpg" /> and <img src="2-7401746\9f241573-b226-4764-aeb5-716eaa2c6757.jpg" /></p><disp-formula id="scirp.38300-formula62535"><label>(29)</label><graphic position="anchor" xlink:href="2-7401746\4765c74d-9570-410a-b3f0-aa7ce2c91b13.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="2-7401746\4d691821-e290-49ee-807f-ac3ed07a879c.jpg" />.</p><p>By definition, put</p><p><img src="2-7401746\0adebe7f-2b39-421a-b53e-760928160f64.jpg" /></p><p>Lemma 3 Under the assumption (29), for <img src="2-7401746\7b6bb822-32a2-4cca-8d37-ba8da1f65e67.jpg" /> the inequality</p><disp-formula id="scirp.38300-formula62536"><label>(30)</label><graphic position="anchor" xlink:href="2-7401746\f7c0b6e0-7859-46fc-a3b4-b4f3e1a31876.jpg"  xlink:type="simple"/></disp-formula><p>is true; here<img src="2-7401746\866d5460-c736-454c-a7c2-27ac219c1087.jpg" />, <img src="2-7401746\a32ea34d-346a-4dd2-a770-a19e6734ebbf.jpg" />, <img src="2-7401746\cbfd3e19-988e-4c7e-b728-7c831ef6a774.jpg" />,<img src="2-7401746\cdaabd44-a51c-4747-a22d-78396d428163.jpg" />.</p><p>Proof We use Lemma 1 and represent <img src="2-7401746\fccb4a04-795b-44ea-bd49-f28f5271ca3c.jpg" /> in the form (13) for<img src="2-7401746\e8783a48-5ebc-4dbf-ac6e-a9e20f0f8632.jpg" />, <img src="2-7401746\9ef81f6a-008d-4051-9927-b6bbabe1d554.jpg" />, <img src="2-7401746\5aba87b3-4f2d-421d-b060-99f206e182df.jpg" />, <img src="2-7401746\2c8fea3d-073b-4be4-acee-51fc9dda1848.jpg" />,<img src="2-7401746\2da27156-6a63-4cfb-92df-38a43df6eb04.jpg" />. As a result, we find</p><p><img src="2-7401746\322b8483-3a54-414c-8064-44784960a1d0.jpg" /></p><p>Using the estimate (29), the positiveness of the kernel of the integral operation<img src="2-7401746\25db5ac4-36b2-4d74-99fa-b5f8e59e134d.jpg" />, and the relation (24) obtained in Lemma 2, we derive the estimate (4.3) for<img src="2-7401746\fc910166-bafd-4336-bd5b-5031f8a698bc.jpg" />.</p><p>Now we set</p><disp-formula id="scirp.38300-formula62537"><label>(31)</label><graphic position="anchor" xlink:href="2-7401746\5acf7925-3e4d-401a-9108-13337f9a87d8.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.38300-formula62538"><label>(32)</label><graphic position="anchor" xlink:href="2-7401746\dd015a9e-e4c4-43ed-badb-4a7fd72f72c9.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.38300-formula62539"><label>(33)</label><graphic position="anchor" xlink:href="2-7401746\8d4e9daf-e580-477d-beaa-2a92808005ac.jpg"  xlink:type="simple"/></disp-formula><p>Lemma 4 If<img src="2-7401746\42eb91a3-0f44-422e-a2d9-c3ac88e61e6a.jpg" />, then for <img src="2-7401746\69e9872d-4c8e-4eae-9d93-94ff5a46ca97.jpg" /> the following inequality holds:</p><disp-formula id="scirp.38300-formula62540"><label>(34)</label><graphic position="anchor" xlink:href="2-7401746\c8c8c182-6aee-4b73-a902-c932e9a920ac.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.38300-formula62541"><label>(35)</label><graphic position="anchor" xlink:href="2-7401746\5bcc146b-2711-4ab1-8ba9-f9507e184dbf.jpg"  xlink:type="simple"/></disp-formula><p>and the maximum is taken over</p><p><img src="2-7401746\01da55ac-5443-43cc-aa4d-aaa89f8875db.jpg" /></p><p>Proof By (31)-(33) the relation (13) may be written in the form</p><p><img src="2-7401746\afc73a1b-609c-4122-a82b-6fd56fa6b093.jpg" /></p><p>It is clear that conditions of Lemma 1 and Lemma 2 are fulfilled, and therefore the kernel of integral operator <img src="2-7401746\67bd4f16-76ac-49b3-9a55-aa223790a36e.jpg" /> is nonnegative. By Lemma 2 we get evaluation (34)-(35).</p><p>Theorem 3 If <img src="2-7401746\a35c655c-5358-4223-978c-b04be747bf74.jpg" /> and (29) holds, then for <img src="2-7401746\354bff15-0293-4737-956a-67d6e963dcce.jpg" /></p><disp-formula id="scirp.38300-formula62542"><label>(36)</label><graphic position="anchor" xlink:href="2-7401746\00cde2cf-fcb6-4458-93f7-9f38154a71f2.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="2-7401746\d959ae73-1adf-4588-8c50-2c175431eabd.jpg" /> is defined by (35)</p><p>Proof Usage (34)-(35) in (12) gives the evaluation (36).</p><p>Corollary 1 Under the assumptions of Theorem 3, the interpolation <img src="2-7401746\07d4a9a6-27ab-46b8-abd1-5594b8ba86c1.jpg" /> of a function <img src="2-7401746\1a933be7-686e-4dbf-9605-222ecd62d9ab.jpg" /> is exact on elements of the space<img src="2-7401746\c7e74257-d042-4ae6-a5b1-3e9e9b0cbf2d.jpg" />, i.e.,</p><disp-formula id="scirp.38300-formula62543"><label>(37)</label><graphic position="anchor" xlink:href="2-7401746\f3758096-d0c2-4119-9728-a52d3196373f.jpg"  xlink:type="simple"/></disp-formula><p>Proof If identity <img src="2-7401746\88c45d0e-eb67-4095-9cbb-c3bc87b02f4a.jpg" /> is fulfilled for a number<img src="2-7401746\a585b3ce-ce7b-40ae-bf43-955a5b5f8e8f.jpg" />, <img src="2-7401746\f26e13ec-b8a2-4c67-855a-5921edbb0a0a.jpg" />, then in (33) the determinant <img src="2-7401746\fff10a3c-f3fd-4e52-8a2e-932042647260.jpg" /> includes two identical rows; therefore<img src="2-7401746\997a3b13-c373-4864-9e0d-619b6af1f7e1.jpg" />. Thus the relation (37) is true.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>The work is partially supported by the Russian Foundation for Basic Research (grant No. 13-01-00096).</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.38300-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Yu. K. Dem’yanovich, “Approximation by Minimal Splines,” Journal of Mathematical Sciences, Vol. 193, No. 2, 2013, pp. 261-266.</mixed-citation></ref><ref id="scirp.38300-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">I. G. Burova and Yu. K. Dem’yanovich, “Theory of Minimal Splines,” St.-Petersburg University Press, St.-Petersburg, 2000.</mixed-citation></ref><ref id="scirp.38300-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">A. O. Gelfond, “Calculation of Finite Differences,” Nauka Press, Moscow, 1967.</mixed-citation></ref></ref-list></back></article>