<?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">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2013.31001</article-id><article-id pub-id-type="publisher-id">APM-26506</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>
 
 
  Applications of Multivalent Functions Associated with Generalized Fractional Integral Operator
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ae</surname><given-names>Ho Choi</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics Education, Daegu National University of Education, Daegu, South Korea</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>choijh@dnue.ac.kr</email></corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>01</month><year>2013</year></pub-date><volume>03</volume><issue>01</issue><fpage>1</fpage><lpage>5</lpage><history><date date-type="received"><day>August</day>	<month>29,</month>	<year>2012</year></date><date date-type="rev-recd"><day>October</day>	<month>29,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>10,</month>	<year>2012</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><html>
 <head></head>
 
   
   By using a method based upon the Briot-Bouquet differential subordination, we investigate some subordination properties of the generalized fractional integral operator 
   <img style="width:51px;height:18px;" alt="" src="Edit_c2920cea-e33a-4675-8579-738a6c2f46fd.bmp" width="54" height="18" />
    
   which was defined by Owa, Saigo and Srivastava [1]. Some interesting further consequences are also considered. 
   
  
 
</html></p></abstract><kwd-group><kwd>Multivalent Functions; Subordination; Gaussian Hypergeometric Function; Fractional Integral Operator</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let <img src="1-5300306\1474ed05-fbf0-4a39-9f46-aea8a766c292.jpg" /> denote the class of functions <img src="1-5300306\217eb0af-82ef-444f-b85d-180e55859fec.jpg" /> of the form</p><disp-formula id="scirp.26506-formula7825"><label>(1.1)</label><graphic position="anchor" xlink:href="1-5300306\8d1e2d9f-cd97-47c8-979a-8831a2632dba.jpg"  xlink:type="simple"/></disp-formula><p>which are analytic in the open unit disk <img src="1-5300306\e118ba4b-5712-493c-bf64-177944f896f0.jpg" /> Also let f and g be analytic in <img src="1-5300306\07473aed-a07b-479d-835c-d5f9860244bd.jpg" /> with<img src="1-5300306\6c433387-8906-4007-aa73-5196e88984ca.jpg" />. Then we say that f is subordinate to g in<img src="1-5300306\414d219c-95e6-4c14-a377-de6be25e1263.jpg" />, written <img src="1-5300306\80b29436-38dc-421f-84b3-4eeb791def33.jpg" /> or<img src="1-5300306\2ef3732d-ed4b-428f-a8d1-cb673aab20fd.jpg" />, if there exists the Schwarz function w, analytic in <img src="1-5300306\fe1af975-12fc-426e-bbd3-6f9b3c25758a.jpg" /> such that<img src="1-5300306\2ee8bf1c-8762-40c7-8389-45eb8568287b.jpg" />, <img src="1-5300306\94d2de2a-aee3-4091-8561-8b6db4f8f565.jpg" />and<img src="1-5300306\74ce64d0-ec06-4119-bbda-e4bf54c217f8.jpg" />. We also observe that</p><p><img src="1-5300306\0206986b-f770-4efd-b388-1bc6d875aef3.jpg" /></p><p>if and only if</p><p><img src="1-5300306\44ef975d-95ff-4543-8784-ca1c4313b0be.jpg" /></p><p>whenever <img src="1-5300306\074cbdea-2e97-42b5-a046-b2f75cc1b995.jpg" /> is univalent in<img src="1-5300306\48f41399-ea77-4efe-a953-7955ab582e31.jpg" />.</p><p>Let a, b and c be complex numbers with<img src="1-5300306\f2af82be-692e-43fc-ac7f-2255c70bb1ca.jpg" />. Then the Gaussian/classical hypergeometric function <img src="1-5300306\ba713963-e430-4c3d-9288-96904416f8eb.jpg" /> is defined by</p><disp-formula id="scirp.26506-formula7826"><label>(1.2)</label><graphic position="anchor" xlink:href="1-5300306\0cc08ce0-b819-4ac2-a846-b1f0beb59f22.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-5300306\6352bf42-e051-4da8-aa54-adaff34fa583.jpg" /> is the Pochhammer symbol defined, in terms of the Gamma function, by</p><disp-formula id="scirp.26506-formula7827"><label>(1.3)</label><graphic position="anchor" xlink:href="1-5300306\4bc3f12a-bba0-476a-b6d5-7917cc9db549.jpg"  xlink:type="simple"/></disp-formula><p>The hypergeometric function <img src="1-5300306\9bca6815-e863-48ec-bd18-4725abc6af92.jpg" /> is analytic in <img src="1-5300306\cfce5e22-b3e6-41f0-8266-392c41d815cc.jpg" /> and if a or b is a negative integer, then it reduces to a polynomial.</p><p>For each A and B such that<img src="1-5300306\c47c9755-dc8c-4637-9c62-9eed392f4225.jpg" />, let us define the function</p><disp-formula id="scirp.26506-formula7828"><label>(1.4)</label><graphic position="anchor" xlink:href="1-5300306\d5983f43-869c-4a42-a7ff-6fc6b80a078d.jpg"  xlink:type="simple"/></disp-formula><p>It is well known that<img src="1-5300306\424ea5f0-4fb7-48df-b2b5-7758f0935dfe.jpg" />, for<img src="1-5300306\69f91126-34cf-41fb-9810-dce48dcbf809.jpg" />, is the conformal map of the unit disk onto the disk symmetrical respect to the real axis having the center <img src="1-5300306\be9d0802-820b-4093-a62d-f5ff8ef7bfa4.jpg" /> and the radius<img src="1-5300306\84d87532-21bb-4552-b2de-0805eec630e3.jpg" />. The boundary circle cuts the real axis at the points <img src="1-5300306\222b2b5f-67d2-4bdf-abf9-5808bc0f3c64.jpg" /> and<img src="1-5300306\2054c4cc-7ccc-427a-98e5-5c9acf595d79.jpg" />.</p><p>Many essentially equivalent definitions of fractional calculus have been given in the literature (cf., e.g. [2,3]). We state here the following definition due to Saigo [<xref ref-type="bibr" rid="scirp.26506-ref4">4</xref>] (see also [1,5]).</p><p>Definition 1. For<img src="1-5300306\563a485c-ea8d-4e32-929e-07fcc54c5e14.jpg" />, <img src="1-5300306\62a8d1ce-99fe-45a7-94d3-6f52f5b2e5bc.jpg" />, the fractional integral operator <img src="1-5300306\175df57c-82ed-45b6-8144-6b7794e2f646.jpg" /> is defined by</p><disp-formula id="scirp.26506-formula7829"><label>(1.5)</label><graphic position="anchor" xlink:href="1-5300306\742fd14d-b9cb-4a57-83f1-1613b502b5f9.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-5300306\b9cb1bbb-7f0e-4a47-adb9-ea47baadca86.jpg" /> is the Gaussian hypergeometric function defined by (1.2) and <img src="1-5300306\b02b743f-cb5c-45e3-9cea-bf841f8654af.jpg" /> is taken to be an analytic function in a simply-connected region of the z-plane containing the origin with the order</p><p><img src="1-5300306\1851c65b-4d46-4463-8529-ddecd52588cd.jpg" /></p><p>for<img src="1-5300306\ff23eaee-8b05-4d87-9c09-5f2f55786189.jpg" />, and the multiplicity of <img src="1-5300306\6cb7d305-6d4c-420f-8d6f-bed073021637.jpg" /> is removed by requiring that <img src="1-5300306\fd1650af-bf78-45f6-860f-b0eb5138e9a8.jpg" /> to be real when<img src="1-5300306\9dc607a6-ae81-4d37-9f9b-be5ea7e96c46.jpg" />.</p><p>The definition (1.5) is an interesting extension of both the Riemann-Liouville and Erd&#233;lyi-Kober fractional operators in terms of Gauss’s hypergeometric functions.</p><p>With the aid of the above definition, Owa, Saigo and Srivastava [<xref ref-type="bibr" rid="scirp.26506-ref1">1</xref>] defined a modification of the fractional integral operator <img src="1-5300306\4f721f81-47d0-43d0-95eb-c566f64493f9.jpg" /> by</p><disp-formula id="scirp.26506-formula7830"><label>(1.6)</label><graphic position="anchor" xlink:href="1-5300306\0d031533-b1d9-41e7-a22e-3c998a2314b2.jpg"  xlink:type="simple"/></disp-formula><p>for <img src="1-5300306\f3ab7583-51e5-4f5b-a27f-334f70d91915.jpg" /> and<img src="1-5300306\fc95d91b-ab31-4b92-8338-2f649b22ded3.jpg" />. Then it is observed that <img src="1-5300306\a91adbe8-906b-4362-88f6-73b5ea662b76.jpg" /> also maps <img src="1-5300306\10d2f21a-71f5-4462-a84c-ed2f48b2f289.jpg" /> onto itself as follows:</p><disp-formula id="scirp.26506-formula7831"><label>(1.7)</label><graphic position="anchor" xlink:href="1-5300306\853569ac-8c72-46ac-ba56-f7672d618097.jpg"  xlink:type="simple"/></disp-formula><p>We note that<img src="1-5300306\05b60931-751b-4771-b12a-9a0367f73d55.jpg" />, where the operator <img src="1-5300306\b3532317-6c53-43bb-8cee-106e14b63434.jpg" /> was introduced and studied by Jung, Kim and Srivastava [<xref ref-type="bibr" rid="scirp.26506-ref6">6</xref>] (see also [<xref ref-type="bibr" rid="scirp.26506-ref7">7</xref>]).</p><p>It is easily verified from (1.7) that</p><disp-formula id="scirp.26506-formula7832"><label>(1.8)</label><graphic position="anchor" xlink:href="1-5300306\225d29ef-10cf-4e3a-a9b6-df4127534d74.jpg"  xlink:type="simple"/></disp-formula><p>The identity (1.8) plays an important and significant role in obtaining our results.</p><p>Recently, by using the general theory of differential subordination, several authors (see, e.g. [7-9]) considered some interesting properties of multivalent functions associated with various integral operators. In this manuscript, we shall derive some subordination properties of the fractional integral operator <img src="1-5300306\02029644-72e6-401e-8d0d-071ffe1b8a5a.jpg" /> by using the technique of differential subordination.</p></sec><sec id="s2"><title>2. Main Results</title><p>In order to establish our results, we shall need the following lemma due to Miller and Mocanu [<xref ref-type="bibr" rid="scirp.26506-ref10">10</xref>].</p><p>Lemma 1. Let <img src="1-5300306\46e9a7c1-eaba-4544-8830-82b29f364b74.jpg" /> be analytic and convex univalent in <img src="1-5300306\a773ac3e-f99e-4009-b794-8a864a2ed76b.jpg" /> with<img src="1-5300306\0f9c1b11-6187-452e-9082-c2a936291dfa.jpg" />, and let <img src="1-5300306\37a150c1-de3f-4823-96c9-6484f1b42496.jpg" /> be analytic in<img src="1-5300306\8d1bfe5a-75b2-4102-87eb-b2a63d9a573a.jpg" />. If</p><disp-formula id="scirp.26506-formula7833"><label>(2.1)</label><graphic position="anchor" xlink:href="1-5300306\510360ff-36f3-4f46-ba35-d5647f77fadc.jpg"  xlink:type="simple"/></disp-formula><p>then for <img src="1-5300306\22a0d2c9-a027-4f85-8146-0c6765219d33.jpg" /> and<img src="1-5300306\262d7860-0a8b-44d9-919e-0b448308629c.jpg" />,</p><disp-formula id="scirp.26506-formula7834"><label>(2.2)</label><graphic position="anchor" xlink:href="1-5300306\4229331c-1360-40fb-956b-a78f5d3df7cd.jpg"  xlink:type="simple"/></disp-formula><p>We begin by proving the following theorem.</p><p>Theorem 1. Let<img src="1-5300306\431afa44-653e-4331-b350-55cc5e9c5118.jpg" />, <img src="1-5300306\25c633ab-dff2-4dbc-afb2-49ec2a8c6b77.jpg" />, <img src="1-5300306\af3915fe-4b30-44c9-9d29-c2c698a00441.jpg" />, <img src="1-5300306\fce39582-984c-4654-a4a9-ae1813c3fa0f.jpg" />, <img src="1-5300306\8ad99cde-6cd7-4a19-b9df-6b3fbba6d06a.jpg" />and<img src="1-5300306\85707462-0ab4-48e0-967e-7b03aaf345cb.jpg" />, and let</p><p><img src="1-5300306\2133520a-c207-4268-9db0-78f4d16e72cd.jpg" />. Suppose that</p><disp-formula id="scirp.26506-formula7835"><label>(2.3)</label><graphic position="anchor" xlink:href="1-5300306\95b4044f-6da3-4bd2-b714-c1dafa11883a.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.26506-formula7836"><label>(2.4)</label><graphic position="anchor" xlink:href="1-5300306\a3cfc276-b18e-42a4-bf87-a7464a12c034.jpg"  xlink:type="simple"/></disp-formula><p>and <img src="1-5300306\0c90d685-2169-4835-82b0-3fa511249377.jpg" /> is given by (1.3).</p><p>1) If<img src="1-5300306\aa9b7d30-a1ca-4406-9702-2c0b06c43c0d.jpg" />, then</p><disp-formula id="scirp.26506-formula7837"><label>(2.5)</label><graphic position="anchor" xlink:href="1-5300306\62720b41-e542-4c33-84b9-2cdf5638ed3e.jpg"  xlink:type="simple"/></disp-formula><p>2) If <img src="1-5300306\5cc46001-d71f-4f04-be2b-4fad595b6b9c.jpg" /> and<img src="1-5300306\9d5d5e6c-9125-48e3-8d01-f23f9713b1b2.jpg" />, then</p><disp-formula id="scirp.26506-formula7838"><label>(2.6)</label><graphic position="anchor" xlink:href="1-5300306\c87b9c20-4d4c-4fa7-b0e7-899a1477bc42.jpg"  xlink:type="simple"/></disp-formula><p>The result is sharp.</p><p>Proof. 1) If we set</p><p><img src="1-5300306\f6f78498-0551-49b2-9010-e88572f26990.jpg" /></p><p>then, from (1.7) we see that</p><disp-formula id="scirp.26506-formula7839"><label>(2.7)</label><graphic position="anchor" xlink:href="1-5300306\ab23bca0-67d8-488d-9128-76e98e2249c8.jpg"  xlink:type="simple"/></disp-formula><p>For <img src="1-5300306\2dbaab4b-20ab-4407-9081-e247207c0105.jpg" /> and<img src="1-5300306\86b36623-2d43-48d4-9326-9fade40510b2.jpg" />, it follows from (2.3) that</p><disp-formula id="scirp.26506-formula7840"><label>(2.8)</label><graphic position="anchor" xlink:href="1-5300306\39f30edb-b00d-418b-8b7f-bbd636a9e2f5.jpg"  xlink:type="simple"/></disp-formula><p>which implies that</p><p><img src="1-5300306\c254d2a3-b43b-4dd0-ba37-fa924356c04a.jpg" /></p><p>2) Let</p><disp-formula id="scirp.26506-formula7841"><label>(2.9)</label><graphic position="anchor" xlink:href="1-5300306\deb39cb6-912f-4779-bc4e-b310a28c9532.jpg"  xlink:type="simple"/></disp-formula><p>Then the function <img src="1-5300306\a7bea178-6f34-4223-9063-a3f4d833c8e9.jpg" /> is analytic in<img src="1-5300306\1b3cfd95-22e8-411f-86da-992d88c44dd6.jpg" />. Using (1.8) and (2.9), we have</p><disp-formula id="scirp.26506-formula7842"><label>(2.10)</label><graphic position="anchor" xlink:href="1-5300306\4f4fc82c-1b1e-496d-9e6c-dc7ea5a04197.jpg"  xlink:type="simple"/></disp-formula><p>From (2.5), (2.9) and (2.10) we obtain</p><p><img src="1-5300306\128464b2-c836-4fe2-b613-503b7f8bd169.jpg" /></p><p>Thus, by applying Lemma 1, we observe that</p><p><img src="1-5300306\84d3e61b-f63f-4123-9f72-e437e5ddfb96.jpg" /></p><p>or</p><disp-formula id="scirp.26506-formula7843"><label>(2.11)</label><graphic position="anchor" xlink:href="1-5300306\7112e916-2574-4a25-a3f0-7a2d013fb06f.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-5300306\e633dbb4-c708-4256-8193-2e48f8482efa.jpg" /> is analytic in <img src="1-5300306\b2727d5d-59c0-4808-b9d0-3089593fba36.jpg" /> with <img src="1-5300306\a15f0324-0b87-4a0f-a247-ea82010013b5.jpg" /> and<img src="1-5300306\e622b3d0-d82a-4209-8077-c57c5c0f3883.jpg" />. In view of <img src="1-5300306\ca8871d7-5198-44b4-8b7d-1f2d4eb54e63.jpg" /> and <img src="1-5300306\fcf39ef2-662e-4661-9645-02effd263fa1.jpg" />, we conclude from (2.11) that</p><disp-formula id="scirp.26506-formula7844"><label>(2.12)</label><graphic position="anchor" xlink:href="1-5300306\bbf35b44-5363-41bb-bf81-a252854242ab.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="1-5300306\97aaabd8-676d-462a-8949-71b61eb3726b.jpg" /> for <img src="1-5300306\c03af5a9-2108-4a6a-b2f0-afd95022cfcb.jpg" /> and<img src="1-5300306\da837d8f-9294-4daf-9396-4dafc4f8bf9c.jpg" />, from (2.12) we see that the inequality (2.6) holds.</p><p>To prove sharpness, we take <img src="1-5300306\f25abd52-3843-4f3f-a5d3-ec67904b4304.jpg" /> defined by</p><p><img src="1-5300306\0826b179-bd26-4092-9e84-ff5640d90b52.jpg" /></p><p>For this function we find that</p><p><img src="1-5300306\efd04c7d-d4d4-4d48-952e-9f8cde61fc76.jpg" /></p><p>and</p><p><img src="1-5300306\9b84c07a-4709-4b4b-9980-550aa5fa64ca.jpg" /></p><p>Hence the proof of Theorem 1 is evidently completed.</p><p>Theorem 2. Let<img src="1-5300306\768df6ec-e6db-4655-afea-f5e583a2900c.jpg" />, <img src="1-5300306\b6903c0f-6655-4687-bc30-8a62218c3c14.jpg" />, <img src="1-5300306\e6a9654e-f93e-4731-bea6-bdbca7591d4a.jpg" />, <img src="1-5300306\5495c8b4-36bc-43b9-b62c-e88fb3d561d5.jpg" />, <img src="1-5300306\57101981-bb16-4a1c-b347-0ef9048298f9.jpg" />and<img src="1-5300306\b8e8ec71-8648-4328-83e4-2587363acf63.jpg" />. Suppose that</p><p><img src="1-5300306\9ab2b8cd-0e77-4db3-a5e2-07286c2dbf01.jpg" />, <img src="1-5300306\9c4d5b9e-5f1e-4ded-8925-a7783a6964e4.jpg" />and <img src="1-5300306\24ddab0b-258e-47ad-a2f3-fe6874841e82.jpg" />. If the sequence <img src="1-5300306\60b5b188-b73a-4ca1-9c50-66569ad959d9.jpg" /> is nondecreasing with</p><disp-formula id="scirp.26506-formula7845"><label>(2.13)</label><graphic position="anchor" xlink:href="1-5300306\feb7a6f2-026c-4414-bf58-213f9df47d33.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-5300306\f1f9046a-a414-4658-8341-8448fd457ead.jpg" /> is given by <img src="1-5300306\5426a627-1ba1-4f33-9f68-5bcd992fcfe8.jpg" /> and satisfies the condition<img src="1-5300306\908a727e-85a7-4b99-b38a-b88c5d213718.jpg" />, then</p><disp-formula id="scirp.26506-formula7846"><label>(2.14)</label><graphic position="anchor" xlink:href="1-5300306\e6e1260d-e4e9-45ac-b9fa-d89e4354c7c6.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.26506-formula7847"><label>(2.15)</label><graphic position="anchor" xlink:href="1-5300306\a0417207-c866-4f69-a3f2-459f9ef3d8c4.jpg"  xlink:type="simple"/></disp-formula><p>Each of the bounds in (2.14) and (2.15) is best possible for<img src="1-5300306\8292c9ec-de4e-42b5-89e9-2217deb1cd9f.jpg" />.</p><p>Proof. We prove the bound in (2.14). The bound in (2.15) is immediately obtained from (2.14) and will be omitted. Let</p><p><img src="1-5300306\40ccac47-6391-4c95-85b2-64a78a0fa8a3.jpg" /></p><p>Then, from (1.7) we observe that</p><p><img src="1-5300306\bb329ab5-b90b-425a-8707-23d5910841fa.jpg" /></p><p>where, for convenience,</p><p><img src="1-5300306\5d322fc4-e837-4b14-83f6-773ce9a6f262.jpg" /></p><p>It is easily seen from (2.4) and (2.13) that <img src="1-5300306\46d4c8c2-77d1-48a1-96ef-948f8f447a30.jpg" /> and</p><disp-formula id="scirp.26506-formula7848"><label>(2.16)</label><graphic position="anchor" xlink:href="1-5300306\c438a6fc-6eb1-46af-b91e-00f034aa54c3.jpg"  xlink:type="simple"/></disp-formula><p>Hence, by applying (2.3) and (2.16), we have</p><p><img src="1-5300306\96180232-fbca-434c-aaae-7b1c3fcf30fb.jpg" /></p><p>which readily yields the inequality (2.14).</p><p>If we take<img src="1-5300306\cf4369c7-c094-47c4-9f81-c5d32e3a80b9.jpg" />, then</p><p><img src="1-5300306\65d73dbd-1197-41f4-9a0d-c37f7902ca87.jpg" /></p><p>This show that the bound in (2.14) is best possible for each m, which proves Theorem 2.</p><p>Finally, we consider the generalized Bernardi-LiveraLivingston integral operator <img src="1-5300306\bc4e323f-000c-4496-a1db-139a338bd05f.jpg" /> defined by (cf. [11-13])</p><disp-formula id="scirp.26506-formula7849"><label>(2.17)</label><graphic position="anchor" xlink:href="1-5300306\19fe0ec0-6bee-4ef4-bfb3-12f08cf69205.jpg"  xlink:type="simple"/></disp-formula><p>Theorem 3. Let<img src="1-5300306\43ae4860-55fb-4de5-bdac-2e4c8891aa6f.jpg" />, <img src="1-5300306\1e9dad6d-c485-4ed9-b5de-0c1f2cfafc57.jpg" />, <img src="1-5300306\2bc949fa-b5cf-4661-80f6-a7b0cf48da2f.jpg" />, <img src="1-5300306\bed8c74a-043b-414f-87c8-03a0e1d1353e.jpg" />, <img src="1-5300306\851d7bdf-4203-41e0-98f4-fe80438fcd5d.jpg" />, <img src="1-5300306\26f1d0a9-a626-4e29-9fa1-82f29e125d1d.jpg" />and<img src="1-5300306\8c6fe982-b7e5-4195-9727-4841e137c201.jpg" />and let<img src="1-5300306\c337c644-c05e-41fd-9415-2366af5e55d3.jpg" />. Suppose that</p><disp-formula id="scirp.26506-formula7850"><label>(2.18)</label><graphic position="anchor" xlink:href="1-5300306\95afcd82-cabe-4f93-b4dd-6acf0f38a836.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="1-5300306\ed34c798-e096-4592-bba6-079aae22c7d3.jpg" /></p><p>and <img src="1-5300306\c30a69c4-8de9-44ab-9e86-94f3530c7e37.jpg" /> is given by (1.3).</p><p>1) If<img src="1-5300306\b8d09ce9-bb72-40c7-8943-3b030ec9f6f1.jpg" />, then</p><disp-formula id="scirp.26506-formula7851"><label>(2.19)</label><graphic position="anchor" xlink:href="1-5300306\71318c52-54a4-499f-81b3-3a51c07da19d.jpg"  xlink:type="simple"/></disp-formula><p>2) If <img src="1-5300306\84aa0915-b648-4288-9f7f-74749acb8155.jpg" /> and<img src="1-5300306\466dcf21-adf8-4321-9cc4-039122ac95d5.jpg" />, then</p><disp-formula id="scirp.26506-formula7852"><label>(2.20)</label><graphic position="anchor" xlink:href="1-5300306\0d59473e-82a6-420a-bab3-8aa021a521dd.jpg"  xlink:type="simple"/></disp-formula><p>The result is sharp.</p><p>Proof. 1) If we put</p><p><img src="1-5300306\9fc901d9-a7e4-4c3b-bd77-048b9c447154.jpg" /></p><p>then, from (1.7) and (2.17) we have</p><p><img src="1-5300306\cedbc73d-0ad1-4a87-add8-ad3e7a651d97.jpg" /></p><p>Therefore, by using same techniques as in the proof of Theorem 1 1), we obtain the desired result.</p><p>2) From (2.17) we have</p><disp-formula id="scirp.26506-formula7853"><label>(2.21)</label><graphic position="anchor" xlink:href="1-5300306\a0bac703-e488-4ce7-a920-6c8e993f86f9.jpg"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.26506-formula7854"><label>(2.22)</label><graphic position="anchor" xlink:href="1-5300306\41251557-d8d8-4da3-80fa-0127393eef5d.jpg"  xlink:type="simple"/></disp-formula><p>Then, by virtue of (2.21), (2.22) and (2.19), we observe that</p><p><img src="1-5300306\f7e29533-fb77-48e0-b715-55dd5d9591f2.jpg" /></p><p>Hence, by applying the same argument as in the proof of Theorem 1 2), we obtain (2.20), which evidently proves Theorem 3.</p></sec><sec id="s3"><title>3. 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