<?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">JHEPGC</journal-id><journal-title-group><journal-title>Journal of High Energy Physics, Gravitation and Cosmology</journal-title></journal-title-group><issn pub-type="epub">2380-4327</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jhepgc.2016.24050</article-id><article-id pub-id-type="publisher-id">JHEPGC-70522</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>
 
 
  An Analytical Solution in the Complex Plane for the Luminosity Distance in Flat Cosmology
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lorenzo</surname><given-names>Zaninetti</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>Physics Department, Via P. Giuria 1, Turin, Italy</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>zaninetti@ph.unito.it</email></corresp></author-notes><pub-date pub-type="epub"><day>23</day><month>08</month><year>2016</year></pub-date><volume>02</volume><issue>04</issue><fpage>581</fpage><lpage>586</lpage><history><date date-type="received"><day>June</day>	<month>27,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>September</month>	<year>10,</year>	</date><date date-type="accepted"><day>September</day>	<month>13,</month>	<year>2016</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 present an analytical solution for the luminosity distance in spatially flat cosmology with pressureless matter and the cosmological constant. The complex analytical solution is made of a real part and a negligible imaginary part. The real part of the luminosity distance allows finding the two parameters H
  <sub>0</sub> and Ω
  <sub>M</sub> . A simple expression for the distance modulus for SNs of type Ia is reported in the framework of the mini-max approximation.
 
</p></abstract><kwd-group><kwd>Cosmology</kwd><kwd> Observational Cosmology</kwd><kwd> Distances</kwd><kwd> Redshifts</kwd><kwd> Radial Velocities</kwd><kwd> Spatial Distribution of Galaxies</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The luminosity distance in flat cosmology has been recently investigated using different approaches. A fitting formula which has a maximum relative error of 4% in the case of common cosmological parameters has been introduced by [<xref ref-type="bibr" rid="scirp.70522-ref1">1</xref>] . An approximate solution in terms of Pad&#233; approximants has been presented by [<xref ref-type="bibr" rid="scirp.70522-ref2">2</xref>] . The integral of the luminosity distance has been found in terms of elliptical integrals of the first kind by [<xref ref-type="bibr" rid="scirp.70522-ref3">3</xref>] .</p></sec><sec id="s2"><title>2. Flat Cosmology</title><p>Following Equation (2.1) in [<xref ref-type="bibr" rid="scirp.70522-ref2">2</xref>] , the luminosity distance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x4.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.70522-formula176"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x5.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x6.png" xlink:type="simple"/></inline-formula> is the Hubble constant expressed in km∙s<sup>−</sup><sup>1</sup>∙Mpc<sup>−1</sup>, c is the speed of light expressed in km∙s<sup>−1</sup>, z is the redshift, a is the scale-factor, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x7.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.70522-formula177"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x8.png"  xlink:type="simple"/></disp-formula><p>where G is the Newtonian gravitational constant and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x9.png" xlink:type="simple"/></inline-formula> is the mass density at the present time. We now introduce the indefinite integral</p><disp-formula id="scirp.70522-formula178"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x10.png"  xlink:type="simple"/></disp-formula><p>The solution is in terms of F, the Legendre integral or incomplete elliptic integral of the first kind</p><disp-formula id="scirp.70522-formula179"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x11.png"  xlink:type="simple"/></disp-formula><p>where the incomplete elliptic integral of the first kind is</p><disp-formula id="scirp.70522-formula180"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x12.png"  xlink:type="simple"/></disp-formula><p>see formula (19.2.4) in [<xref ref-type="bibr" rid="scirp.70522-ref4">4</xref>] , and</p><disp-formula id="scirp.70522-formula181"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x13.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula182"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x14.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula183"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x15.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula184"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x16.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula185"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x17.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula186"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x18.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula187"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula188"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x20.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula189"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x21.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70522-formula190"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x22.png"  xlink:type="simple"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x23.png" xlink:type="simple"/></inline-formula>. The incomplete elliptic integral <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x24.png" xlink:type="simple"/></inline-formula> of complex arguments is evaluated according to Equation (17.4.11) in [<xref ref-type="bibr" rid="scirp.70522-ref5">5</xref>] or Section 19.7 (ii) in [<xref ref-type="bibr" rid="scirp.70522-ref4">4</xref>] . The luminosity distance is</p><disp-formula id="scirp.70522-formula191"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x25.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x26.png" xlink:type="simple"/></inline-formula> means the real part.</p><p>The distance modulus is</p><disp-formula id="scirp.70522-formula192"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x27.png"  xlink:type="simple"/></disp-formula><p>An approximation can be found when the argument of the integral (1) is expanded about a = 1 in a Taylor series of order 10. The resulting Taylor approximation of order 10 to the luminosity distance, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x28.png" xlink:type="simple"/></inline-formula>, is</p><disp-formula id="scirp.70522-formula193"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x29.png"  xlink:type="simple"/></disp-formula><p>where we have reported the first few terms of the series. The goodness of the Taylor approximation is evaluated through the percentage error, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x30.png" xlink:type="simple"/></inline-formula>, which is</p><disp-formula id="scirp.70522-formula194"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x31.png"  xlink:type="simple"/></disp-formula><p>As an example when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula>, we obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula>. As an example with the above parameters, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x37.png" xlink:type="simple"/></inline-formula>has its angle in the complex plane, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x38.png" xlink:type="simple"/></inline-formula>, very small:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x39.png" xlink:type="simple"/></inline-formula>, which means that the solution is real for practical purposes. In the last years the Hubble Space Telescope (HST) has allowed the determination of the cosmological parameters through the modulus of the distance for SNs of type Ia, see [<xref ref-type="bibr" rid="scirp.70522-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.70522-ref10">10</xref>] . At the moment of writing the two unknown parameters, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x40.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x41.png" xlink:type="simple"/></inline-formula>, can be derived from two catalogs for the distance modulus of SNs of type Ia: 580 SNe in the Union 2.1 compilation, see [<xref ref-type="bibr" rid="scirp.70522-ref11">11</xref>] with data at http://supernova.lbl.gov/Union/, and 740 SNe in the joint light-curve analysis (JLA), see [<xref ref-type="bibr" rid="scirp.70522-ref12">12</xref>] with data at http://supernovae.in2p3.fr/sdss_snls_jla/ReadMe.html. This kind of analysis is not new and has been used, for example, by [<xref ref-type="bibr" rid="scirp.70522-ref13">13</xref>] .</p><p>The best fit for the distance modulus of SNs is obtained adopting the Levenberg- Marquardt method (subroutine MRQMIN in [<xref ref-type="bibr" rid="scirp.70522-ref14">14</xref>] ). The statistical parameters here adopted are the merit function or chi-square, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x42.png" xlink:type="simple"/></inline-formula>, the reduced chi-square, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x43.png" xlink:type="simple"/></inline-formula>and the maximum probability of obtaining a better fitting, Q, see Section 2.3 in [<xref ref-type="bibr" rid="scirp.70522-ref15">15</xref>] for more details. <xref ref-type="table" rid="table1">Table 1</xref> reports <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x44.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x45.png" xlink:type="simple"/></inline-formula> for the two catalogs of SNs and <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> display the best fits.</p><p>The Taylor approximation of order 10 to the distance modulus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x46.png" xlink:type="simple"/></inline-formula>, is</p><disp-formula id="scirp.70522-formula195"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x47.png"  xlink:type="simple"/></disp-formula><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Numerical values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x48.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x49.png" xlink:type="simple"/></inline-formula>and Q where k stands for the number of parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Compilation</th><th align="center" valign="middle" >SNs</th><th align="center" valign="middle" >k</th><th align="center" valign="middle" >Parameters</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x50.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x51.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Q</th></tr></thead><tr><td align="center" valign="middle" >Union 2.1</td><td align="center" valign="middle" >580</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x52.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x53.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >562.22</td><td align="center" valign="middle" >0.972</td><td align="center" valign="middle" >0.673</td></tr><tr><td align="center" valign="middle" >JLA</td><td align="center" valign="middle" >740</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x54.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x55.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >627.82</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.998</td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Hubble diagram for the Union 2.1 compilation. The solid line represents the best fit for the exact distance modulus in flat cosmology as represented by Equation (7), parameters as in first line of <xref ref-type="table" rid="table1">Table 1</xref></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2180143x56.png"/></fig><p>The above equation takes a simple expression when the minimax rational approximation is used, see [<xref ref-type="bibr" rid="scirp.70522-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.70522-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.70522-ref17">17</xref>] ; here we have used a polynomial of degree 3 for the numerator and degree 2 for the denominator. With the parameters of <xref ref-type="table" rid="table1">Table 1</xref> for the Union 2.1 compilation over the range in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x57.png" xlink:type="simple"/></inline-formula>, we obtain the following minimax approximation</p><disp-formula id="scirp.70522-formula196"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-2180143x58.png"  xlink:type="simple"/></disp-formula><p>the maximum error being 0.002956.</p></sec><sec id="s3"><title>3. Conclusion</title><p>We have presented an analytical approximation for the luminosity distance in terms of elliptical integrals with complex argument. The fit of the distance modulus of SNs of type Ia allows finding the pair <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x59.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-2180143x60.png" xlink:type="simple"/></inline-formula> for the Union 2.1 and JLA compilations.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Hubble diagram for the JLA compilation. The solid line represents the best fit for the exact distance modulus in flat cosmology as represented by Equation (7), parameters as in second line of <xref ref-type="table" rid="table1">Table 1</xref></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2180143x61.png"/></fig><p>A simple expression for the distance modulus relative to the Union 2.1 compilation is given through the minimax approximation applied to a Taylor expansion of the luminosity distance of order 10.</p></sec><sec id="s4"><title>Cite this paper</title><p>Zaninetti, L. (2016) An Analytical Solution in the Complex Plane for the Luminosity Distance in Flat Cosmology. Journal of High Energy Physics, Gravitation and Cosmology, 2, 581-586. http://dx.doi.org/10.4236/jhepgc.2016.24050</p></sec></body><back><ref-list><title>References</title><ref id="scirp.70522-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Pen, U.L. (1999) Analytical Fit to the Luminosity Distance for Flat Cosmologies with a Cosmological Constant. Astrophysical Journal Supplement Series, 120, 49. 
http://dx.doi.org/10.1086/313167</mixed-citation></ref><ref id="scirp.70522-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Adachi, M. and Kasai, M. (2012) An Analytical Approximation of the Luminosity Distance in Flat Cosmologies with a Cosmological Constant. Progress of Theoretical Physics, 127, 145. http://dx.doi.org/10.1143/PTP.127.145</mixed-citation></ref><ref id="scirp.70522-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Mészáros, A. and Rpa, J. (2013) A Curious Relation between the Flat Cosmological Model and the Elliptic Integral of the First Kind. Astronomy &amp; Astrophysics, 556, A13. 
http://dx.doi.org/10.1051/0004-6361/201322088</mixed-citation></ref><ref id="scirp.70522-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Olver, F.W.J., Lozier, D.W., Boisvert, R.F. and Clark, C.W. (2010) NIST Handbook of Mathematical Functions. Cambridge University Press, Cambridge.</mixed-citation></ref><ref id="scirp.70522-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Abramowitz, M. and Stegun, I.A. (1965) Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. Dover, New York.</mixed-citation></ref><ref id="scirp.70522-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Perlmutter, S., Aldering, G., della Valle, M., Deustua, S., Ellis, R.S., Fabbro, S., Fruchter, A., Goldhaber, G., Groom, D.E., Hook, I.M., Kim, A.G., Kim, M.Y., Knop, R.A., Lidman, C., McMahon, R.G., Nugent, P., Pain, R., Panagia, N., Pennypacker, C.R., Ruiz-Lapuente, P., Schaefer, B. and Walton, N. (1998) Discovery of a Supernova Explosion at Half the Age of the Universe. Nature, 391, 51. http://dx.doi.org/10.1038/34124</mixed-citation></ref><ref id="scirp.70522-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Garnavich, P.M., Kirshner, R.P., Challis, P., Tonry, J., Gilliland, R.L., Smith, R.C., Clocchiatti, A., Diercks, A., Filippenko, A.V., Hamuy, M., Hogan, C.J., Leibundgut, B., Phillips, M.M., Reiss, D., Riess, A.G., Schmidt, B.P., Schommer, R.A., Spyromilio, J., Stubbs, C., Suntzeff, N.B. and Wells, L. (1998) Constraints on Cosmological Models from Hubble Space Telescope Observations of High-z Supernovae. Astrophysical Journal Letters, 493, L53. http://dx.doi.org/10.1086/311140</mixed-citation></ref><ref id="scirp.70522-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Riess, A.G., Filippenko, A.V., Challis, P. and Clocchiatti, A. (1998) Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant. Astronomical Journal, 116, 1009. http://dx.doi.org/10.1086/300499</mixed-citation></ref><ref id="scirp.70522-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Knop, R.A., Aldering, G., Amanullah, R., Astier, P., Blanc, G., Burns, M.S., Conley, A., Deustua, S.E., Doi, M., Ellis, R., Fabbro, S., Folatelli, G., Fruchter, A.S., Garavini, G., Garmond, S., Garton, K., Gibbons, R., Goldhaber, G., Goobar, A., Groom, D.E., Hardin, D., Hook, I., Howell, D.A., Kim, A.G., Lee, B.C., Lidman, C., Mendez, J., Nobili, S., Nugent, P.E., Pain, R., Panagia, N., Pennypacker, C.R., Perlmutter, S., Quimby, R., Raux, J., Regnault, N., Ruiz-Lapuente, P., Sainton, G., Schaefer, B., Schahmaneche, K., Smith, E., Spadafora, A.L., Stanishev, V., Sullivan, M., Walton, N.A., Wang, L., Wood-Vasey, W.M. and Yasuda, N. (2003) New Constraints on  ,  , and w from an Independent Set of 11 High-Redshift Supernovae Observed with the Hubble Space Telescope. Astrophysical Journal Letters, 598, 102. http://dx.doi.org/10.1086/378560</mixed-citation></ref><ref id="scirp.70522-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Riess, A.G., Strolger, L.G., Casertano, S., Ferguson, H.C., Mobasher, B., Gold, B., Challis, P.J., Filippenko, A.V., Jha, S., Li, W., Tonry, J., Foley, R., Kirshner, R.P., Dickinson, M., MacDonald, E., Eisenstein, D., Livio, M., Younger, J., Xu, C., Dahlén, T. and Stern, D. (2007) New Hubble Space Telescope Discoveries of Type Ia Supernovae at z Greater than 1: Narrowing Constraints on the Early Behavior of Dark Energy. Astrophysical Journal Letters, 659, 98. http://dx.doi.org/10.1086/510378</mixed-citation></ref><ref id="scirp.70522-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Suzuki, N., Rubin, D., Lidman, C., Aldering, G., Amanullah, R., Barbary, K. and Barrientos, L.F. (2012) The Hubble Space Telescope Cluster Supernova Survey. V. Improving the Dark- Energy Constraints above z Greater than 1 and Building an Early-Type-Hosted Supernova Sample. Astrophysical Journal Letters, 746, 85.  
http://dx.doi.org/10.1088/0004-637X/746/1/85</mixed-citation></ref><ref id="scirp.70522-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Betoule, M., Kessler, R., Guy, J. and Mosher, J. (2014) Improved Cosmological Constraints from a Joint Analysis of the SDSS-II and SNLS Supernova Samples. Astronomy &amp; Astrophysics, 568, A22. http://dx.doi.org/10.1051/0004-6361/201423413</mixed-citation></ref><ref id="scirp.70522-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Oliveira, F.J. (2016) Cosmic Time Transformations in Cosmological Relativity. Journal of High Energy Physics, Gravitation and Cosmology, 2, 253.  
http://dx.doi.org/10.4236/jhepgc.2016.22022</mixed-citation></ref><ref id="scirp.70522-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Press, W.H., Teukolsky, S.A., Vetterling, W.T. and Flannery, B.P. (1992) Numerical Recipes in Fortran. The Art of Scientific Computing. Cambridge University Press, Cambridge.</mixed-citation></ref><ref id="scirp.70522-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Zaninetti, L. (2016) Pade Approximant and Minimax Rational Approximation in Standard Cosmology. Galaxies, 4, 4. http://www.mdpi.com/2075-4434/4/1/4</mixed-citation></ref><ref id="scirp.70522-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Remez, E. (1934) Sur la détermination des polyn&amp;ocirc;mes d’approximation de degré donnée. Comm. Soc. Math. Kharkov, 10, 41.</mixed-citation></ref><ref id="scirp.70522-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Remez, E. (1957) General Computation Methods of Chebyshev Approximation. The Problems with Linear Real Parameters. Publishing House of the Academy of Science of the Ukrainian SSR, Kiev.</mixed-citation></ref></ref-list></back></article>