<?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.2013.39098</article-id><article-id pub-id-type="publisher-id">APM-41127</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>
 
 
  Value Distribution of L-Functions with Rational Moving Targets
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>atthew</surname><given-names>Cardwell</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>Zhuan</surname><given-names>Ye</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Intelligent Medical Objects, Inc., Northbrook, USA</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematical Sciences, Northern Illinois University, DeKalb, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mcardwell@e-imo.com(AC)</email>;<email>ye@math.niu.edu(ZY)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>28</day><month>11</month><year>2013</year></pub-date><volume>03</volume><issue>09</issue><fpage>719</fpage><lpage>723</lpage><history><date date-type="received"><day>August</day>	<month>26,</month>	<year>2013</year></date><date date-type="rev-recd"><day>September</day>	<month>26,</month>	<year>2013</year>	</date><date date-type="accepted"><day>October</day>	<month>1,</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>
 
 
   We prove some value-distribution results for a class of L-functions with rational moving targets. The class contains Selberg class, as well as the Riemann-zeta function. 
 
</p></abstract><kwd-group><kwd>Value Distribution; Moving Target; &lt;i&gt;L&lt;/i&gt;-Function; Selberg Class</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We define the class <img src="6-5300523\e0410378-5315-47df-bbfa-9cb568132086.jpg" /> to be the collection of functions</p><p><img src="6-5300523\86c5d9be-3da8-460e-966c-d132486f0689.jpg" />satisfying Ramanujan hypothesisAnalytic continuation and Functional equation. We also denote the degree of a function <img src="6-5300523\3e037c53-060f-4de3-8597-45692d44562d.jpg" /> by <img src="6-5300523\b343a44b-a3d3-4605-9dcf-3316d6edc370.jpg" /> which is a non-negative real number. We refer the reader to Chapter six of [<xref ref-type="bibr" rid="scirp.41127-ref1">1</xref>] for a complete definitions. Obviously, the class <img src="6-5300523\df037d71-64de-4dd8-ad2c-7df577a968c8.jpg" /> contains the Selberg class. Also every function in the class <img src="6-5300523\bca8692f-3cd7-483b-b649-0addf477343e.jpg" /> is an <img src="6-5300523\c552cb6d-9032-443c-aacd-48e98527ad3f.jpg" />-function and the Riemann-zeta function is in the class. In this paper, we prove a value-distribution theorem for the class <img src="6-5300523\a83b074d-1dbe-4d60-8f21-db658d3046ba.jpg" /> with rational moving targets. The theorem generalizes the value-distribution results in Chapter seven of [<xref ref-type="bibr" rid="scirp.41127-ref1">1</xref>] from fixed targets to moving targets.</p><p>Theorem. Assume that <img src="6-5300523\546f6cb0-53d3-4ea2-b4eb-cec3c6546627.jpg" /> and <img src="6-5300523\28ef2524-a39e-4be6-8b45-83c8179eccd9.jpg" /> is a rational function with<img src="6-5300523\afdb4a46-7bd7-4786-a3b6-7afc9742ffcf.jpg" />. Let the roots of the equation <img src="6-5300523\d631ee9e-dff5-4193-b707-68156a8842d0.jpg" /> be denoted by<img src="6-5300523\3123b0f5-16f5-457a-a271-85d250eb4447.jpg" />. Then</p><p>(I) For any<img src="6-5300523\786095b0-01de-49cf-983a-a6db19b71306.jpg" />,</p><p><img src="6-5300523\186becd0-40c7-44aa-82ab-c0c0670b303e.jpg" /></p><p>(II) For sufficiently large negative<img src="6-5300523\f427dc31-f7bb-4a33-87e5-7f36ec456f6a.jpg" />,</p><p><img src="6-5300523\752adb26-826a-4532-8cf9-6ca89cb65a71.jpg" /></p><p>Proof of (I). It is known that if<img src="6-5300523\fa429c53-e368-4597-bd44-8308fa4a1ca6.jpg" />, then</p><p><img src="6-5300523\5679fddc-cd7d-4093-baa2-8d27d72c30a4.jpg" /></p><p>where <img src="6-5300523\f0dd07a5-c52b-4626-9345-ade20da9c85c.jpg" /> is the index of the first non-zero term of the sequence of<img src="6-5300523\66a46cee-1ca4-4743-87ff-fafdb0fe7395.jpg" />, <img src="6-5300523\4915b1b5-9bbb-438e-93af-9e62fabadfc4.jpg" />with<img src="6-5300523\48a13d57-db9a-4147-8851-b2b29b8f2539.jpg" />. Since<img src="6-5300523\4c9afc4a-d4aa-4ebe-9e95-b8a250956902.jpg" />, there exists <img src="6-5300523\5535ef69-b1e8-4cfd-a1d4-4c6f496e7546.jpg" /> such that <img src="6-5300523\9f43a623-f680-4021-bea2-22a1c80fcf99.jpg" /> for<img src="6-5300523\955f91af-89f4-4837-9edb-19d5059df0b4.jpg" />. It follows that <img src="6-5300523\8be7a475-0489-42d5-a1ee-c29a6a8437a4.jpg" /> for all real part of zeros of the function<img src="6-5300523\9a783d0a-b96f-46f1-a33d-06090acad9a2.jpg" />. We set <img src="6-5300523\152bf63a-ca40-4f4b-9eb4-4e7b233d98e7.jpg" /> where the degrees of <img src="6-5300523\bf35de15-f992-4212-bcff-5aa402d0580d.jpg" /> are<img src="6-5300523\8e07e287-a2ed-4cb5-b3fd-0f9f4dd5c98b.jpg" />, respectively; and define</p><p><img src="6-5300523\7d36ed06-73d8-43ed-9a62-5de8f8d07987.jpg" /></p><p>Thus, there is <img src="6-5300523\f3166580-c2ba-4124-be29-2f85db2365fd.jpg" /> such that <img src="6-5300523\3f1e7938-36f2-4969-aec7-f01771722884.jpg" /> is analytic in the region <img src="6-5300523\77c02461-0c49-48dd-ae53-ba79f0387191.jpg" /> since <img src="6-5300523\6e6f85a0-18ef-4947-8bbe-52318488ab4d.jpg" /> is a meromorphic function in <img src="6-5300523\13321adc-38de-485f-b819-44bee53756cb.jpg" /> with the only pole at<img src="6-5300523\a7605126-8a7b-4ff9-9f26-95db19003284.jpg" />. We apply Littlewood’s argument principle [<xref ref-type="bibr" rid="scirp.41127-ref3">3</xref>] to <img src="6-5300523\e33be5ae-d8d0-4362-b154-97ee5fb7fec3.jpg" /> in the rectangle <img src="6-5300523\4e0890ba-d530-4021-8e1d-2ec056b1bd56.jpg" /> where <img src="6-5300523\178e8ce0-203c-482b-8bf3-6ca3542a5a91.jpg" /> are parameters satisfying<img src="6-5300523\e952c56c-6282-4885-a379-b7e9b0393ad9.jpg" />. Thus,</p><p><img src="6-5300523\d834a516-56bf-460b-9390-005377964357.jpg" /></p><p>where the given logarithm is defined as in Littlewood’s argument principle [<xref ref-type="bibr" rid="scirp.41127-ref3">3</xref>]. To prove our result, however, we first decompose our auxiliary function by</p><disp-formula id="scirp.41127-formula123414"><label>(1)</label><graphic position="anchor" xlink:href="6-5300523\f9752511-8f0d-48fc-9940-3d10cfba2270.jpg"  xlink:type="simple"/></disp-formula><p>Without loss of generality, we may assume that <img src="6-5300523\5d92f48b-fa78-451c-912c-86112a3f7b3b.jpg" /> whenever <img src="6-5300523\a7937023-290d-474a-b197-44f8a61eda8e.jpg" /> since we can always write <img src="6-5300523\f38ccee5-e3d5-411f-8e12-be19e2ec1c8f.jpg" /> for <img src="6-5300523\54225504-3367-4dca-8e33-b406dca7f932.jpg" /> due to our choice of the parameters which define the rectangle<img src="6-5300523\3380d0c0-57a4-4dc7-bb25-0ae27ca70e3b.jpg" />. However, the modification will guarantee in the case of <img src="6-5300523\f473ddfe-88c9-41de-abbc-d5efef609637.jpg" /> that <img src="6-5300523\613d3fe4-bc83-428f-b2af-3bb450ffb5ad.jpg" /> exhibit polynomial growth, which is necessary for our proof. In the case of<img src="6-5300523\5eda8f56-ecd5-4309-a5a8-99e78ca7c617.jpg" />, <img src="6-5300523\e884dc6f-ef7e-4792-a0ae-dd54db0aebfa.jpg" />already exhibits polynomial growth, and no such adjustment is necessary. We now integrate the logarithm of <img src="6-5300523\a5cffdcb-3d86-4dfb-bd66-057dffb28505.jpg" /> to get</p><p><img src="6-5300523\28c5bc6c-ea08-4337-bc6c-bc2404f28cc8.jpg" /></p><p>where the <img src="6-5300523\40f32983-59cf-4f6b-882d-225af868d53a.jpg" /> terms are the integrals of the maximum contribution from writing <img src="6-5300523\77e3687c-7c4a-4068-aeb7-7bdb40e2f70b.jpg" /> as a sum of logarithms. By our choice of<img src="6-5300523\1cccc507-794d-4066-9f34-46bc3a836cb1.jpg" />, both <img src="6-5300523\c2842783-05b6-4212-9317-ebf8ac0f5a23.jpg" /> and <img src="6-5300523\5b8738d4-a880-4bb4-b370-5b11bb6abfcd.jpg" /> are analytic in <img src="6-5300523\79e91384-0342-47a4-ad45-69c7e561cf2b.jpg" /><img src="6-5300523\a4fc529f-7e62-4cdc-8dfa-34b5287aab36.jpg" />Hence, Cauchy’s Theorem gives</p><disp-formula id="scirp.41127-formula123415"><label>(2)</label><graphic position="anchor" xlink:href="6-5300523\a2c98af7-e0cc-41c6-9755-c3958097ef40.jpg"  xlink:type="simple"/></disp-formula><p>To connect this integral with Littlewood’s argument principle [<xref ref-type="bibr" rid="scirp.41127-ref3">3</xref>], we note that the definition of <img src="6-5300523\574b9607-650d-4fad-8ec3-0ac5fb8bec76.jpg" /> guarantees that</p><disp-formula id="scirp.41127-formula123416"><label>(3)</label><graphic position="anchor" xlink:href="6-5300523\96b88337-e7bf-444c-8a45-a2916ed114ee.jpg"  xlink:type="simple"/></disp-formula><p>In light of (2) and because the quantity given in (3) is imaginary-valued, we get for <img src="6-5300523\b880427d-bfc5-473d-8ae3-01d07838470a.jpg" /></p><disp-formula id="scirp.41127-formula123417"><label>(4)</label><graphic position="anchor" xlink:href="6-5300523\ece397e7-17f7-486c-8cb6-e3466bbe8e8e.jpg"  xlink:type="simple"/></disp-formula><p>for instance.</p><p>We now estimate<img src="6-5300523\6515637b-e36d-4cd7-8f2f-27407b06c022.jpg" />. For <img src="6-5300523\c91fadff-da6c-4c8c-93ac-c0881c7de778.jpg" /> large enough, we have for <img src="6-5300523\07d51cf7-bb05-4037-afa4-c5dce7e58500.jpg" /> (since<img src="6-5300523\767bc142-41a0-4807-81e2-b26246fc93fa.jpg" />),</p><p><img src="6-5300523\ed5da9f2-c702-45da-a00f-3c2bf31e1a28.jpg" /></p><p>Then for <img src="6-5300523\d86ba872-8cc3-488e-9124-ee4e1796b086.jpg" /> large enough, <img src="6-5300523\6c8e783e-24f5-4678-80b4-69865a3644f5.jpg" />, we find in a similar fashion that</p><p><img src="6-5300523\e2d2adca-6f35-4700-b69f-081716a61987.jpg" /></p><p>Since we have the same estimate for<img src="6-5300523\9c616a2c-415e-42b4-b485-0b9d324a0726.jpg" />, we find that</p><p><img src="6-5300523\fce44dd6-7196-4590-9b0a-ed5f54f70543.jpg" /></p><p>where the final bound follows from Jensen’s inequality. It is known [<xref ref-type="bibr" rid="scirp.41127-ref2">2</xref>] that for<img src="6-5300523\e2fe5bd2-4690-476c-9bea-f0688e8013db.jpg" />,</p><p><img src="6-5300523\ee75e898-93dd-4989-af16-4c56fdf701d3.jpg" /></p><p>Hence, <img src="6-5300523\45cebd46-6472-4770-baf3-1a1aa3b54c42.jpg" />uniformly in <img src="6-5300523\0b2bbd7c-64b0-44de-b45b-7c7dfb63eb8f.jpg" />.</p><p>We next move to estimate<img src="6-5300523\75b33fd5-05a0-4061-a682-d0127dd71dbd.jpg" />. For sufficiently large positive real number<img src="6-5300523\a20c0338-6773-44de-8085-1e7c8f7b6260.jpg" />, we have</p><disp-formula id="scirp.41127-formula123418"><label>(5)</label><graphic position="anchor" xlink:href="6-5300523\56f96668-1c64-4c19-9d9f-b71255761470.jpg"  xlink:type="simple"/></disp-formula><p>so</p><p><img src="6-5300523\822ce147-546c-45ac-ae00-0d15c7bcf231.jpg" /></p><p>since<img src="6-5300523\859671b5-f208-4697-a2c0-e17ef13ccbff.jpg" />. Furthermore,</p><p><img src="6-5300523\a5f213ba-12c7-4898-b09c-ef42b4afe105.jpg" /></p><p>Since we may take <img src="6-5300523\e6c8ddc8-cdc8-4b91-8100-7ea5233f0c0b.jpg" /> large enough so that</p><p><img src="6-5300523\b114a901-7875-40eb-89f9-87c4f3cb0055.jpg" />, we may write <img src="6-5300523\960de7c3-0ff1-498b-9695-4b0a5a2bb22c.jpg" /> using a Taylor series expansion in the rectangle<img src="6-5300523\ef07785d-0f97-4838-be8f-e95023631648.jpg" />. For<img src="6-5300523\83974459-afbe-401c-9e8d-153c4b061c70.jpg" />, we have after taking real parts that</p><p><img src="6-5300523\ae16ca0d-5725-4d5d-8361-aeaeb2b85d2c.jpg" /></p><p>We now observe that for sufficiently large T and some constant M we have</p><p><img src="6-5300523\b57dfff7-7166-4685-8116-0593ab95e531.jpg" /></p><p>for <img src="6-5300523\bb018eda-207f-4b6b-bf50-42709ba27588.jpg" /> and</p><p><img src="6-5300523\0686cd1c-919e-4fc4-ac65-fa852b5ff80c.jpg" /></p><p>for sufficiently large<img src="6-5300523\98198332-2424-4fc4-83e9-09bdb0cdf308.jpg" />. In light of these bounds and the definition of<img src="6-5300523\b119e421-6405-4b4c-ba3a-0a1095c289cc.jpg" />, we have (6)</p><p>where the last equality holds because <img src="6-5300523\1ff9f30d-1a55-4c90-bb9e-6e5db3a676fb.jpg" /> could be sufficiently large. Replacing <img src="6-5300523\7f84df87-fd70-4f12-9378-660b6b7b325a.jpg" /> by <img src="6-5300523\fc99acfe-3ea8-449e-a28c-4d82f87bbd70.jpg" /> in the above computations, we see analogously that<img src="6-5300523\201d4be2-c4c6-4af0-9428-752f60ee1885.jpg" />.</p><p>Finally, we estimate <img src="6-5300523\14a1c276-2d6a-4934-a93b-4a81fa96cd8c.jpg" /> and<img src="6-5300523\f6f7e526-00b9-4f35-ab86-ddce66793dc5.jpg" />. We show the computation for <img src="6-5300523\bf33beed-fe88-46b1-8412-4d31204dfce4.jpg" /> explicitly and note that the bound for <img src="6-5300523\8470f9f6-9e27-40b8-a622-0b047965725e.jpg" /> follows analogously. We first suppose that <img src="6-5300523\e080ebd2-82ad-415d-bf46-30f65cb4705f.jpg" /> has exactly <img src="6-5300523\6988a314-e4d1-4003-bb6f-4a9441813a30.jpg" /> zeros for<img src="6-5300523\6e16962b-cd57-49b5-882a-cca1742a5d19.jpg" />. Then, there are at most <img src="6-5300523\343de58a-5bdd-4354-a5de-28eab33ce984.jpg" /> subintervals, counting for multiplicities, in which <img src="6-5300523\92b35ccc-2c4d-45ec-a12a-7b2a82b4c084.jpg" /> is of constant sign. Thus,</p><disp-formula id="scirp.41127-formula123419"><label>(7)</label><graphic position="anchor" xlink:href="6-5300523\cab02915-044f-44c9-a72b-78edf409352f.jpg"  xlink:type="simple"/></disp-formula><p>It remains to estimate<img src="6-5300523\01fc8291-2512-4b10-afc6-a5d7ac41445b.jpg" />. To this end, we define</p><p><img src="6-5300523\7b3e751b-2c2d-48b3-95ad-c69a5c1e6872.jpg" /></p><p>Then</p><p><img src="6-5300523\ab4610f6-21f4-48bc-b64a-60172cd08fc3.jpg" /></p><p>so that if <img src="6-5300523\e68813f2-9a0d-4113-8823-d731eaedd214.jpg" /> for<img src="6-5300523\d80b3aca-a91c-4d2c-9658-5e594c050a53.jpg" />, then<img src="6-5300523\5b7bd92c-be8b-4061-a99c-cdad438cb7db.jpg" />.</p><p>Now let <img src="6-5300523\9730d424-b275-48a1-9261-02fd20043c78.jpg" /> and<img src="6-5300523\717e1d19-2817-4346-b4d6-4c72de102a31.jpg" />, and choose <img src="6-5300523\d08a99a0-5be0-47d2-84f3-13fff860f671.jpg" /> large enough so that<img src="6-5300523\df09e44f-e213-4076-8b04-f9d4a79b912c.jpg" />. Then <img src="6-5300523\82cc3c5c-9ec8-49ca-b468-131c56796ce8.jpg" /> for<img src="6-5300523\81b48b64-85fb-4590-ba3a-38948be38aaf.jpg" />, showing that no zeros or poles of <img src="6-5300523\efe7833d-af5d-420a-a598-308538be84ec.jpg" /> are located in<img src="6-5300523\a644e198-fccb-4067-bca8-57eb2591434a.jpg" />. Thus, both <img src="6-5300523\9a2a1b59-406e-47b5-bbe3-a7d9b7ad5dfd.jpg" /> and <img src="6-5300523\c6e748c0-2064-4021-9c22-26805a0f4dc2.jpg" /> are analytic in<img src="6-5300523\2d8bc499-9f8b-4afc-b96e-45c870768606.jpg" />. Letting <img src="6-5300523\d0638e87-3e4d-4868-9001-94ab35208d1d.jpg" /> denote the number of zeros of <img src="6-5300523\2bb7d4ad-1288-49c7-a397-3ee4a5d4c435.jpg" /> in<img src="6-5300523\c4e76951-fa62-437f-9c98-cb6b276e9607.jpg" />, we have</p><p><img src="6-5300523\d1ec89bd-47e0-4dae-add0-11bb7c7b14b5.jpg" /></p><p>By Jensen’s formula</p><p><img src="6-5300523\bdd04e61-3c27-451c-88b9-6925bfa062b1.jpg" /></p><p>and so</p><disp-formula id="scirp.41127-formula123420"><label>(8)</label><graphic position="anchor" xlink:href="6-5300523\201afb04-ed80-4a15-8ad4-cbec1f6be7a8.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.41127-formula123421"><label>(6)</label><graphic position="anchor" xlink:href="6-5300523\1c5aecee-c50f-47b0-bf0a-6850c6fa45cd.jpg"  xlink:type="simple"/></disp-formula><p>By (5), <img src="6-5300523\fe2452c8-8c1d-4326-b4b3-f9b76d0976c8.jpg" />is bounded. Further, it is clear from a property of <img src="6-5300523\7d5de550-fa61-459b-9f81-31ffc36c47d1.jpg" /> functions that we have</p><p><img src="6-5300523\f46daf0d-1b11-4930-a14f-01f2c3e7fff3.jpg" /></p><p>for some positive absolute numbers <img src="6-5300523\f2c41f9c-fa45-45cc-a747-384afc1538e6.jpg" /> in any vertical strip of bounded width. The same estimate must hold for <img src="6-5300523\6b171eee-c751-4c07-89f6-c132f242e921.jpg" /> as well. Thus, the integral in (8) is<img src="6-5300523\ceb5137e-3fdd-41e4-8cfa-94ac9aa18144.jpg" />, implying that <img src="6-5300523\15fc0c5b-6699-410e-bd0f-359445c434a9.jpg" /> . Since the interval<img src="6-5300523\f8dad4fe-a087-4d34-8965-42d8d66266e1.jpg" />, it follows that</p><p><img src="6-5300523\2ebd00d6-4790-4e6c-912c-5a932e190dfa.jpg" /></p><p>With this bound, we integrate (7) to deduce that</p><p><img src="6-5300523\9497dcbe-93b1-4428-85cb-5f7b78fef2ba.jpg" /></p><p>As previously noted, we may bound <img src="6-5300523\e4ceb551-d7f9-4158-b2a6-f654b788d3c7.jpg" /> in the same way. Thus, we attain the desired bounds for <img src="6-5300523\bfbc723c-dce0-4693-8876-66f7ee1074a9.jpg" /> and<img src="6-5300523\f0a5900a-eae3-43e1-896f-f3a3bffef9db.jpg" />. Consequently, the first part of the theorem is proved by using (4).</p><p>Proof of (II). As in the proof of the first part of the theorem, we conclude that there exists a real number <img src="6-5300523\adfe3dbe-e4a9-48d6-a86a-4007c6bc9de4.jpg" /> for which the real parts <img src="6-5300523\a7d07866-bc5d-4485-a8ab-ca111ff3b5fc.jpg" /> of all <img src="6-5300523\2d59703d-c691-4db7-8d5e-9a3dec65be5c.jpg" />-values satisfy<img src="6-5300523\86306600-f425-41a6-84f8-e60c33d0c9ba.jpg" />; and also, there exist <img src="6-5300523\c9b027f7-9f7d-49f6-97d1-1d43e9e9cd60.jpg" /> for each rational function <img src="6-5300523\13bf0890-7989-4823-84ff-5d3aa9fa6068.jpg" /> such that no zeros of <img src="6-5300523\2836223b-81bf-45ae-8bf2-3bc265258884.jpg" /> lie in the quarter-plane<img src="6-5300523\64866cbf-07c2-45e6-9d27-630e65269335.jpg" />. As before, we define the rectangle <img src="6-5300523\6fa19e66-b209-4e86-a37e-223df923fe6b.jpg" /> where <img src="6-5300523\316700ef-c36f-4e48-9438-7f030336084b.jpg" /> are parameters satisfying <img src="6-5300523\51011f35-3eb2-4a4c-9f10-0f7925719d13.jpg" />.</p><p>Proceeding as in the proof of the first part of the theorem, we see that</p><p><img src="6-5300523\019f8e3f-18ca-4682-aeb2-afdf21ecf6bb.jpg" /></p><p>for <img src="6-5300523\4a120d24-9d82-4ab9-b87a-ccc598fc39f1.jpg" /> where <img src="6-5300523\e6e5bdb1-7938-47cd-86a8-984e5b706d5a.jpg" /> is defined as in (1). In the equation above, we note that we have chosen to compute <img src="6-5300523\bf630ccb-5f04-4ccd-81b0-405db9066d20.jpg" /> separately. Indeed, this is the only estimate that we will need. For the integrals<img src="6-5300523\bbed9cb3-0178-43b9-a3e7-a2f1b308088a.jpg" />, <img src="6-5300523\a1821272-72ab-4a89-ae48-fde57841c603.jpg" />and<img src="6-5300523\e3523706-680b-4d9c-a844-311dab53a0b9.jpg" />, the bounds given as in the proof of the first part of the theorem still hold. First, integral <img src="6-5300523\16b98e28-8d71-444f-b5dc-0e3b012b6e45.jpg" /> is unchanged. On the other hand, the integrals <img src="6-5300523\d5992215-6b84-4cb0-9213-38f03ef56a87.jpg" /> have changed by our choice of<img src="6-5300523\648eaae8-34e0-429c-a225-5a837824e333.jpg" />, but, as we have done as before, we still have the desired bound since the only requirement is that we consider <img src="6-5300523\0ff4892c-4a92-4a6c-92d7-7c4d21553ee0.jpg" /><img src="6-5300523\a38a222b-e486-4470-a9f5-7a15d7654d8e.jpg" /> in a vertical strip of fixed width, which we have in this case.</p><p>We now bound<img src="6-5300523\4a6cc218-9717-4d82-8220-506635c3791f.jpg" />. Since<img src="6-5300523\43568aaa-54ed-4a35-a82a-31aa3382678e.jpg" />, we have by the functional equation in the definition of <img src="6-5300523\7013f930-1a02-4660-8f3a-87c997e379a8.jpg" /> function,</p><p><img src="6-5300523\3fdcae0b-10af-4ac6-acb1-4b41487b8214.jpg" /></p><p>Taking logarithms, we get</p><disp-formula id="scirp.41127-formula123422"><label>(9)</label><graphic position="anchor" xlink:href="6-5300523\7ab96d4c-7159-4488-a913-7d237b6e5b2f.jpg"  xlink:type="simple"/></disp-formula><p>Since, for<img src="6-5300523\6ac278f6-e904-4ffe-bc30-d5d8bb36d7fe.jpg" />, we have, uniformly in<img src="6-5300523\9171fcc2-7975-41f2-9ee0-900cf2aa3134.jpg" />,</p><p><img src="6-5300523\74a82260-fac1-4478-882a-52e09e73b272.jpg" /></p><p>where <img src="6-5300523\7c0d0844-144f-4ab2-bb30-b8d1ed91abe1.jpg" /> are two constants. It follows, for <img src="6-5300523\9caa090f-fe77-4134-b17c-aae30a99c297.jpg" /> as<img src="6-5300523\bada0550-7842-4e53-a08e-ed331875b175.jpg" />, that</p><p><img src="6-5300523\6d7c4b6a-ef0f-401d-aedf-5d6d9c59617f.jpg" /></p><p>We now consider the last term in (9). Since,</p><p><img src="6-5300523\733f3b13-b0bf-4b74-9b2f-78fd8dcac0a0.jpg" /></p><p>and noting<img src="6-5300523\e75bdb42-ae3a-4c1f-8391-ff3936b729e6.jpg" />, we have for any <img src="6-5300523\b8450773-0c20-4ca5-9257-2f78ca521966.jpg" /> and <img src="6-5300523\33c5771a-9cd9-476a-a0fa-0d4724211c05.jpg" /></p><p><img src="6-5300523\a29b82b8-2088-4d32-941b-f242454b757d.jpg" /></p><p>for sufficiently large<img src="6-5300523\8da80ce2-8ebf-4d04-b93c-1635d7271319.jpg" />. Then we see the quotient</p><p><img src="6-5300523\e621f576-503d-418b-a726-b60c176dfa41.jpg" /></p><p>when <img src="6-5300523\0a10507b-04aa-4f3b-921e-d325ebd67181.jpg" /> is large enough so that</p><p><img src="6-5300523\d505e44a-1c7e-4c2e-99aa-4e0c3c1afda2.jpg" /></p><p>Therefore, we find that</p><p><img src="6-5300523\6da27d3f-7775-4044-8577-1aafb81adc72.jpg" /></p><p>Integrating in light of these estimates, we see</p><p><img src="6-5300523\bb309459-8d77-4e58-93c0-70da9a420877.jpg" /></p><p>The first integral is<img src="6-5300523\8d6bac9e-7b25-4587-8149-daf7346b4a73.jpg" />, and the second integral is <img src="6-5300523\c01fc017-4953-42e3-9fed-b65cfdf6b585.jpg" /> for sufficiently large and negative <img src="6-5300523\938c22f3-14cc-401c-bae8-18e83815a317.jpg" /> by the method used to derive (6). Hence,</p><p><img src="6-5300523\31e3aa1e-5365-420b-af59-c6fd66af63e4.jpg" /></p><p>With the estimates for the<img src="6-5300523\79ffc8c0-9423-4640-a234-34383ecdbe62.jpg" />’s, we have proved the second part of the theorem.</p></sec><sec id="s2"><title>REFERENCES</title></sec><sec id="s3"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.41127-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">J. Steuding, “Value Distribution of L-Functions,” Number 1877 in Lecture Notes in Mathematics, Springer, 2007.</mixed-citation></ref><ref id="scirp.41127-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">H. S. A. Potter, “The Mean Values of Certain Dirichlet Series I,” Proceedings London Mathematical Society, Vol. 46, No. 2, 1940, pp. 467-468. http://dx.doi.org/10.1112/plms/s2-46.1.467</mixed-citation></ref><ref id="scirp.41127-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">E. C. Titchmarsh, “The Theory of Functions,” 2nd Edition, Oxford, 1939.</mixed-citation></ref></ref-list></back></article>