<?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">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2015.68113</article-id><article-id pub-id-type="publisher-id">JMP-58188</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>
 
 
  Creation of a Non-Expanding, Non-Singular Universe
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>alter</surname><given-names>Petry</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>wpetry@meduse.de, petryw@uni-duesseldorf.de</email>;<email>Mathematical Institute, University of Duesseldorf, Duesseldorf, Germany</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>07</month><year>2015</year></pub-date><volume>06</volume><issue>08</issue><fpage>1085</fpage><lpage>1094</lpage><history><date date-type="received"><day>29</day>	<month>May</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>19</month>	<year>July</year>	</date><date date-type="accepted"><day>22</day>	<month>July</month>	<year>2015</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>
 
 
  A theory of gravitation in flat space-time is applied to homogeneous, isotropic cosmological models. There are non-singular cosmological models. A natural interpretation is a non-expanding universe. The redshift is an intrinsic effect and not a Doppler effect. The universe contains only energy in the beginning, i.e. no matter exists. In the course of time matter and radiation are created from energy where the whole energy is conserved. Matter increases with time but a certain time after the beginning of the universe the creation of matter is finished and the universe appears like a static one. A modified Hubble law is considered which may explain the high redshifts of objects in the universe without the assumption of dark energy.
 
</p></abstract><kwd-group><kwd>Universe</kwd><kwd> Non-Expanding</kwd><kwd> Non-Singular</kwd><kwd> Creation of Matter</kwd><kwd> Conservation of Total Energy</kwd><kwd>  Redshift Is No Doppler Effect</kwd><kwd> Modified Hubble Law</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Einstein’s general theory of relativity yields a singularity in the beginning of a homogeneous, isotropic universe. Hence, space and time do not exist before and are created in the beginning. The redshift is interpreted as Doppler effect which yields the expansion of space. This is the mainstream interpretation of cosmological models studied by general relativity. It is implied by the singularity of the models.</p><p>A theory of gravitation in flat space-time is studied by the author in several articles, e.g. in article [<xref ref-type="bibr" rid="scirp.58188-ref1">1</xref>] and in the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] . The theory of gravitation has a flat space-time metric. Gravitation is described by gravitational potentials which form a tensor of rank two. The source of these potentials is the total energy-momentum tensor including that of the gravitational field which is a tensor by this theory. This theory is a field theory in analogy to the well-known Maxwell’s electrodynamics. For weak gravitational fields the results of this theory agree with those of general relativity to measurable accuracy. In the beginning of the universe where strong gravitational fields work there are differences between the results of the two theories.</p><p>In the beginning of the universe only energy exists, i.e. there is no matter. In the curse of time matter and radiation are created at coasts of energy where the total energy is conserved. Non-singular cosmological models exist, i.e. a big bang doesn’t exist. The creation of matter is finished a certain time after the beginning of the universe, i.e. the creation of the universe is finished. It is now like a stationary universe. A natural interpretation is a non-stationary, non-expanding universe, the creation of which is finished. The redshift is an intrinsic gravitational effect and not a Doppler effect. A non-expanding universe is also experimentally indicated by several authors, e.g. the articles [<xref ref-type="bibr" rid="scirp.58188-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.58188-ref8">8</xref>] . Theoretical studies of a non-expanding universe are given by several authors (see e.g. [<xref ref-type="bibr" rid="scirp.58188-ref9">9</xref>] - [<xref ref-type="bibr" rid="scirp.58188-ref14">14</xref>] ). A fast increase of the inhomogeneity in the matter dominated universe by flat space-time theory of gravitation is given in article [<xref ref-type="bibr" rid="scirp.58188-ref15">15</xref>] . This is important to explain the presently observed inhomogeneity in the universe. General relativity gives only slow increase of the inhomogeneity which does not allow to explain the presently observed universe.</p><p>Chapter 2 contains the theory of gravitation in flat space-time which is a field theory. The metric is a flat space-time, e.g. the pseudo-Euclidean metric. The gravitational field satisfies covariant differential equations of order two with the total energy-momentum as source. Conservation of the total energy-momentum and the equations of motion for matter are stated (see e.g. article [<xref ref-type="bibr" rid="scirp.58188-ref1">1</xref>] and the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] ).</p><p>In Chapter 3 a homogeneous, isotropic universe is studied. The pseudo-Euclidean metric is used implying a flat space as indicated by measurements. The matter consists of dust and radiation. The universe is described by two functions. There is no singularity, i.e. no big bang. The absolute time is introduced. There is no age problem. A redshift formula is derived.</p><p>A modified Hubble law is described in Chapter 4 by the assumption that everybody is surrounded by a medium similar to that in electrodynamics. Absolute time is used and a modified Hubble law is derived. Quasars and galaxies with nearly the same redshift can have quite different distances as already experimentally indicated by Arp. Redshifts can give smaller distances of the objects than by the standard Hubble law. It may be that dark energy in the universe is not needed because the high redshifts are explained by the modified Hubble law.</p><p>The theory of gravitation in flat space-time and the general theory of relativity are compared with one another from the theoretical point of view in article [<xref ref-type="bibr" rid="scirp.58188-ref16">16</xref>] . A modified Hubble law is stated in article [<xref ref-type="bibr" rid="scirp.58188-ref17">17</xref>] which may be important to explain the high redshift of quasars without the assumption of dark energy. The existence of nearby quasars and galaxies with quite different redshifts is already stated by Arp [<xref ref-type="bibr" rid="scirp.58188-ref18">18</xref>] . This is also in agreement with the modified Hubble law in article [<xref ref-type="bibr" rid="scirp.58188-ref17">17</xref>] . Results about a non-singular, non-expanding universe can also be found in the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] .</p></sec><sec id="s2"><title>2. Gravitation in Flat Space-Time</title><p>A theory of gravitation in flat space-time is studied in several articles ( see e.g. article [<xref ref-type="bibr" rid="scirp.58188-ref1">1</xref>] and the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] ) gives for small gravitational fields the same results as general relativity to measurable accuracy. In this section the theory is shortly summarized.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x5.png" xlink:type="simple"/></inline-formula> be the coordinates of space-time and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x6.png" xlink:type="simple"/></inline-formula> the symmetric metric tensor of flat space-time with line-element</p><disp-formula id="scirp.58188-formula983"><label>. (3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x7.png"  xlink:type="simple"/></disp-formula><p>A special case is the pseudo-Euclidean geometry where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x8.png" xlink:type="simple"/></inline-formula> are the Cartesian coordinates, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x9.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x10.png" xlink:type="simple"/></inline-formula>. The gravitational field is described by a symmetric tensor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x11.png" xlink:type="simple"/></inline-formula>. The proper-time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x12.png" xlink:type="simple"/></inline-formula> is defined by</p><disp-formula id="scirp.58188-formula984"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x13.png"  xlink:type="simple"/></disp-formula><p>Put</p><disp-formula id="scirp.58188-formula985"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x14.png"  xlink:type="simple"/></disp-formula><p>Define the tensor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x15.png" xlink:type="simple"/></inline-formula> by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x16.png" xlink:type="simple"/></inline-formula>.</p><p>Then, the Lagrangian for the gravitational potentials <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x17.png" xlink:type="simple"/></inline-formula> is defined by</p><disp-formula id="scirp.58188-formula986"><label>(3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x18.png"  xlink:type="simple"/></disp-formula><p>where the bar/denotes the covariant derivative relative to the metric (3.1). Let k be the gravitational constant and put</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x19.png" xlink:type="simple"/></inline-formula>.</p><p>Then, the energy-momentum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x20.png" xlink:type="simple"/></inline-formula> of the gravitational field from the Lagrangian is</p><disp-formula id="scirp.58188-formula987"><label>(3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x21.png"  xlink:type="simple"/></disp-formula><p>This is a tensor whereas the energy-momentum of general relativity is not a tensor.</p><p>The energy-momentum tensor of matter is</p><disp-formula id="scirp.58188-formula988"><label>(3.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x22.png"  xlink:type="simple"/></disp-formula><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x23.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x24.png" xlink:type="simple"/></inline-formula> denote the density, the pressure and the four-velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x25.png" xlink:type="simple"/></inline-formula> of matter. It holds by relation (3.2)</p><disp-formula id="scirp.58188-formula989"><label>(3.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x26.png"  xlink:type="simple"/></disp-formula><p>Define the differential operator of order two</p><disp-formula id="scirp.58188-formula990"><label>. (3.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x27.png"  xlink:type="simple"/></disp-formula><p>Then, the field equations for the potentials from the Lagrangian (3.3) are</p><disp-formula id="scirp.58188-formula991"><label>(3.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x28.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x29.png" xlink:type="simple"/></inline-formula> is the total energy-momentum tensor of matter and of the gravitational field, i.e.</p><disp-formula id="scirp.58188-formula992"><label>(3.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x30.png"  xlink:type="simple"/></disp-formula><p>The equations of motion are</p><disp-formula id="scirp.58188-formula993"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x31.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.58188-formula994"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x32.png"  xlink:type="simple"/></disp-formula><p>is the symmetric energy-momentum tensor of matter. In addition to the field Equations (3.8) we have the conservation of the total energy-momentum tensor, i.e.</p><disp-formula id="scirp.58188-formula995"><label>(3.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x33.png"  xlink:type="simple"/></disp-formula><p>The field Equations (3.8) and the equations of motion (3.10) imply the conservation law (3.12) of the total energy-momentum. In addition, the field Equations (3.8) and the conservation law (3.12) of the total energy- momentum give the equations of motion (3.10).</p><p>The field Equations (3.8) are formally similar to those of general relativity with quite different meanings of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x34.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x35.png" xlink:type="simple"/></inline-formula>.</p><p>The theory of gravitation in flat space-time and that of general relativity are compared with one another from the theoretical point of view in article [<xref ref-type="bibr" rid="scirp.58188-ref16">16</xref>] .</p></sec><sec id="s3"><title>3. Homogeneous, Isotropic Universe</title><p>Flat space-time theory of gravitation is applied to a homogeneous, isotropic universe. The results can be found in several articles, especially in [<xref ref-type="bibr" rid="scirp.58188-ref11">11</xref>] and in the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] .</p><p>The metric is the pseudo-Euclidean geometry, i.e.</p><disp-formula id="scirp.58188-formula996"><label>(4.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x36.png"  xlink:type="simple"/></disp-formula><p>The potentials are</p><disp-formula id="scirp.58188-formula997"><label>(4.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x37.png"  xlink:type="simple"/></disp-formula><p>which implies the proper-time</p><disp-formula id="scirp.58188-formula998"><label>(4.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x38.png"  xlink:type="simple"/></disp-formula><p>Assume that matter is at rest, i.e.</p><disp-formula id="scirp.58188-formula999"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x39.png"  xlink:type="simple"/></disp-formula><p>which gives by (3.2) the four-velocity</p><disp-formula id="scirp.58188-formula1000"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x40.png"  xlink:type="simple"/></disp-formula><p>The matter tensor has the form</p><disp-formula id="scirp.58188-formula1001"><label>(4.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x41.png"  xlink:type="simple"/></disp-formula><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x42.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x43.png" xlink:type="simple"/></inline-formula> are the densities of matter and radiation and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x44.png" xlink:type="simple"/></inline-formula> is the pressure of radiation, i.e.</p><disp-formula id="scirp.58188-formula1002"><label>(4.5a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x45.png"  xlink:type="simple"/></disp-formula><p>The pressure of matter is that of dust, i.e.</p><disp-formula id="scirp.58188-formula1003"><label>(4.5b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x46.png"  xlink:type="simple"/></disp-formula><p>The energy-momentum tensor of gravitation is given by</p><disp-formula id="scirp.58188-formula1004"><label>(4.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x47.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.58188-formula1005"><label>(4.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x48.png"  xlink:type="simple"/></disp-formula><p>The prime denotes the time-derivative.</p><p>The equations for the gravitational field have the form</p><disp-formula id="scirp.58188-formula1006"><label>(4.8a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x49.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1007"><label>(4.8b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x50.png"  xlink:type="simple"/></disp-formula><p>The conservation of the total energy gives</p><disp-formula id="scirp.58188-formula1008"><label>(4.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x51.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x52.png" xlink:type="simple"/></inline-formula> is a constant of integration. The equations of motion imply under the assumption that matter and radiation do not interact with one another:</p><disp-formula id="scirp.58188-formula1009"><label>(4.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x53.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x54.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x55.png" xlink:type="simple"/></inline-formula> are the present densities at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x56.png" xlink:type="simple"/></inline-formula>.</p><p>The initial conditions for the differential Equations (4.8) are the values at present time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x57.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.58188-formula1010"><label>(4.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x58.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x59.png" xlink:type="simple"/></inline-formula> Is the Hubble constant and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x60.png" xlink:type="simple"/></inline-formula> is a further constant which is zero for general relativity.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x61.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x62.png" xlink:type="simple"/></inline-formula> be the well-known density parameters of radiation and matter. Put</p><disp-formula id="scirp.58188-formula1011"><label>(4.12a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x63.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.58188-formula1012"><label>(4.12b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x64.png"  xlink:type="simple"/></disp-formula><p>The it follows from (4.9) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x65.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.58188-formula1013"><label>(4.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x66.png"  xlink:type="simple"/></disp-formula><p>Longer calculations imply the relations</p><disp-formula id="scirp.58188-formula1014"><label>(4.14b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x67.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1015"><label>(4.14b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x68.png"  xlink:type="simple"/></disp-formula><p>The condition</p><disp-formula id="scirp.58188-formula1016"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x69.png"  xlink:type="simple"/></disp-formula><p>gives by the use of (4.12b) that the denominator of (4.14b) is positive for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x70.png" xlink:type="simple"/></inline-formula>. Hence, non-singular solutions exist. Let us assume</p><disp-formula id="scirp.58188-formula1017"><label>(4.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x71.png"  xlink:type="simple"/></disp-formula><p>then, there exists a time</p><disp-formula id="scirp.58188-formula1018"><label>(4.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x72.png"  xlink:type="simple"/></disp-formula><p>and for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x73.png" xlink:type="simple"/></inline-formula> holds</p><disp-formula id="scirp.58188-formula1019"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x74.png"  xlink:type="simple"/></disp-formula><p>We get for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x75.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.58188-formula1020"><label>(4.17a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1021"><label>(4.17b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x77.png"  xlink:type="simple"/></disp-formula><p>Put</p><disp-formula id="scirp.58188-formula1022"><label>(4.18a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x78.png"  xlink:type="simple"/></disp-formula><p>and assume</p><disp-formula id="scirp.58188-formula1023"><label>(4.18b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x79.png"  xlink:type="simple"/></disp-formula><p>then, the solutions are approximated by</p><disp-formula id="scirp.58188-formula1024"><label>(4.19a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x80.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1025"><label>(4.19b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x81.png"  xlink:type="simple"/></disp-formula><p>In the beginning of the universe, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x82.png" xlink:type="simple"/></inline-formula>, the functions are</p><disp-formula id="scirp.58188-formula1026"><label>(4.20a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x83.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1027"><label>(4.20b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x84.png"  xlink:type="simple"/></disp-formula><p>This means that the universe starts with a small positive value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula> at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula> and decreases till <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x88.png" xlink:type="simple"/></inline-formula>. Then, it increases to infinity as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x89.png" xlink:type="simple"/></inline-formula>. The function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x90.png" xlink:type="simple"/></inline-formula> is infinite at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x91.png" xlink:type="simple"/></inline-formula> and it is always decreases for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x92.png" xlink:type="simple"/></inline-formula> to a value a little bit smaller than 1. In the beginning of the universe there is no matter and no radiation. In the course of time matter and radiation are created. A certain time after the beginning of the universe the creation of matter is finished, i.e. the total universe is created. Hence, the universe appears as a static one. A static universe is also claimed by Watts [<xref ref-type="bibr" rid="scirp.58188-ref5">5</xref>] .</p><p>In addition to the time t there exist the proper time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x93.png" xlink:type="simple"/></inline-formula> defined by</p><disp-formula id="scirp.58188-formula1028"><label>(4.21a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x94.png"  xlink:type="simple"/></disp-formula><p>and the absolute time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x95.png" xlink:type="simple"/></inline-formula> defined by</p><disp-formula id="scirp.58188-formula1029"><label>(4.21b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x96.png"  xlink:type="simple"/></disp-formula><p>The proper time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x97.png" xlink:type="simple"/></inline-formula> is measured by atomic clocks. The introduction of the absolute time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x98.png" xlink:type="simple"/></inline-formula> gives</p><disp-formula id="scirp.58188-formula1030"><label>(4.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x99.png"  xlink:type="simple"/></disp-formula><p>i.e. the light-velocity in the universe is at every time equal to the vacuum light-velocity c.</p><p>The universe happens in the pseudo-Euclidean geometry with the time transformation (4.21b). Hence, space is not expanding.</p><p>Two light rays are emitted at distance r at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x100.png" xlink:type="simple"/></inline-formula> resp. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x101.png" xlink:type="simple"/></inline-formula>and they are received at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x102.png" xlink:type="simple"/></inline-formula> at time 0 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x103.png" xlink:type="simple"/></inline-formula>. Hence, it follows</p><disp-formula id="scirp.58188-formula1031"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x104.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1032"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x105.png"  xlink:type="simple"/></disp-formula><p>The last two relation yield</p><disp-formula id="scirp.58188-formula1033"><label>(4.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x106.png"  xlink:type="simple"/></disp-formula><p>Therefore, the time-intervals are at any time always identical.</p><p>The Equation (4.14b) is by the use of (4.14a) and the use of the absolute time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x107.png" xlink:type="simple"/></inline-formula> of (4.21b) rewritten the form</p><disp-formula id="scirp.58188-formula1034"><label>(4.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x108.png"  xlink:type="simple"/></disp-formula><p>The frequency <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x109.png" xlink:type="simple"/></inline-formula> of an atom emitted at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x110.png" xlink:type="simple"/></inline-formula> in the universe is by (4.22)</p><disp-formula id="scirp.58188-formula1035"><label>(4.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x111.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x112.png" xlink:type="simple"/></inline-formula> is the emitted frequency of the same atom at present time. By the use of (4.22) the change of the photon-energy during the motion of the photon in the universe is given by</p><disp-formula id="scirp.58188-formula1036"><graphic  xlink:href="http://html.scirp.org/file/8-7502273x113.png"  xlink:type="simple"/></disp-formula><p>Hence the frequency (energy) is not changed when light moves in the universe. Therefore, the measured redshift at the observer at present time is</p><disp-formula id="scirp.58188-formula1037"><label>(4.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x114.png"  xlink:type="simple"/></disp-formula><p>The redshift formula (4.26) implies by the use of (4.24), differentiation of (4.24) and the constant velocity of light c in the universe</p><disp-formula id="scirp.58188-formula1038"><label>(4.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x115.png"  xlink:type="simple"/></disp-formula><p>The age of the universe measured with absolute time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x116.png" xlink:type="simple"/></inline-formula> from time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x117.png" xlink:type="simple"/></inline-formula> till the present time is by the use of (4.24), (4.13), (4.15) and (4.16)</p><disp-formula id="scirp.58188-formula1039"><label>(4.28a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x118.png"  xlink:type="simple"/></disp-formula><p>The age of the universe from the beginning till <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x119.png" xlink:type="simple"/></inline-formula> is by the use of (4.24), (4.16) and (4.20a)</p><disp-formula id="scirp.58188-formula1040"><label>(4.28b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x120.png"  xlink:type="simple"/></disp-formula><p>Hence, the age of the universe measured with absolute time from the beginning till <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x121.png" xlink:type="simple"/></inline-formula> is very small compared to the total age of the universe.</p><p>There is no age problem for the universe by the use of the absolute time which is more natural than the proper time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x122.png" xlink:type="simple"/></inline-formula> by virtue of the constancy of the light-velocity c in the universe.</p><p>There exist several articles which require a universe with non-expanding space (see e.g. [<xref ref-type="bibr" rid="scirp.58188-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.58188-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.58188-ref12">12</xref>] ). Non- singular universes are studied in the articles [<xref ref-type="bibr" rid="scirp.58188-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.58188-ref14">14</xref>] .</p><p>A theoretical comparison of the theory of gravitation in flat space-time with general relativity is given in the article [<xref ref-type="bibr" rid="scirp.58188-ref16">16</xref>] . The total energy-momentum tensor of matter and gravitation is the source of the gravitational potentials whereas general relativity has only the energy-momentum of matter as source since the energy-mo- mentum of gravitation is not a tensor. Therefore, the Ricci tenor is used to describe the gravitational metric which implies non-Euclidean geometries. Experimental results indicate that the space of our universe is flat in agreement with flat space-time theory of gravitation. A flat space yields difficulties to be explained by general relativity since in the beginning of the universe there is a high matter density which implies high curvature. Therefore, the inflationary universe is introduced.</p><p>It is worth to mention that flat space-time theory of gravitation gives in the matter dominated universe a fast increase of the inhomogeneity of matter (see [<xref ref-type="bibr" rid="scirp.58188-ref15">15</xref>] ). This is necessary to explain the observed inhomogeneity by galaxies and quasars. General relativity has difficulties to explain this inhomogeneity because only weak increases can arise.</p></sec><sec id="s4"><title>4. Modified Hubble Law</title><p>The interpretation of an expanding space gives with recently observed high redshift quasars an acceleration of the expansion of the space. This is partly explained by the introduction of a cosmological constant in the general theory of relativity. This is also possible for flat space-time theory of gravitation.</p><p>Here we will consider another possibility. Let us assume that a body is surrounded by a medium analogous to that of electrodynamics with electric permittivity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x123.png" xlink:type="simple"/></inline-formula> and magnetic permeability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x124.png" xlink:type="simple"/></inline-formula>. We put</p><disp-formula id="scirp.58188-formula1041"><label>(5.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x125.png"  xlink:type="simple"/></disp-formula><p>We follow along the lines of article [<xref ref-type="bibr" rid="scirp.58188-ref17">17</xref>] and that of the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] . Put</p><disp-formula id="scirp.58188-formula1042"><label>(5.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x126.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.58188-formula1043"><label>(5.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x127.png"  xlink:type="simple"/></disp-formula><p>Then, the proper-time is given by</p><disp-formula id="scirp.58188-formula1044"><label>(5.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x128.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x129.png" xlink:type="simple"/></inline-formula> be the electric four-current density and consider the covariant differential equations</p><disp-formula id="scirp.58188-formula1045"><label>(5.5a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x130.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1046"><label>. (5.5b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x131.png"  xlink:type="simple"/></disp-formula><p>The electric and the magnetic field are defined by</p><disp-formula id="scirp.58188-formula1047"><label>(5.6a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x132.png"  xlink:type="simple"/></disp-formula><p>and the derived fields are</p><disp-formula id="scirp.58188-formula1048"><label>(5.6b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x133.png"  xlink:type="simple"/></disp-formula><p>Then, it follows from (5.5) with (5.2) and (5.3)</p><disp-formula id="scirp.58188-formula1049"><label>(5.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x134.png"  xlink:type="simple"/></disp-formula><p>and with the abbreviation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x135.png" xlink:type="simple"/></inline-formula> we have the well-known Maxwell equations in a medium</p><disp-formula id="scirp.58188-formula1050"><label>(5.8a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x136.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58188-formula1051"><label>(5.8b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x137.png"  xlink:type="simple"/></disp-formula><p>Let us now consider a medium in the universe described by the absolute time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x138.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x139.png" xlink:type="simple"/></inline-formula>. We define the approximating potentials</p><disp-formula id="scirp.58188-formula1052"><label>(5.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x140.png"  xlink:type="simple"/></disp-formula><p>The metric is given by</p><disp-formula id="scirp.58188-formula1053"><label>(5.10a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x141.png"  xlink:type="simple"/></disp-formula><p>and the proper-time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x142.png" xlink:type="simple"/></inline-formula> has the form</p><disp-formula id="scirp.58188-formula1054"><label>(5.10b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x143.png"  xlink:type="simple"/></disp-formula><p>Assume that an atom at rest emits a light ray at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7502273x144.png" xlink:type="simple"/></inline-formula> in the universe. The Equation (5.10b) gives for the proper-time</p><disp-formula id="scirp.58188-formula1055"><label>(5.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x145.png"  xlink:type="simple"/></disp-formula><p>Hence, the emitted frequency is</p><disp-formula id="scirp.58188-formula1056"><label>(5.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x146.png"  xlink:type="simple"/></disp-formula><p>Assume that the light-ray moves only a small part of his way to the observer in this medium. In the exterior of the medium relation (4.22) holds, i.e. the frequency is not changed during the motion. Hence, the redshift at the observer is</p><disp-formula id="scirp.58188-formula1057"><label>(5.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x147.png"  xlink:type="simple"/></disp-formula><p>which gives analogous to Section 4</p><disp-formula id="scirp.58188-formula1058"><label>(5.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x148.png"  xlink:type="simple"/></disp-formula><p>Hence, we get an intrinsic redshift by the medium, i.e. the standard Hubble law doesn’t give a real distance indicator. We must use the modified Hubble law (5.14).</p><p>We can assume</p><disp-formula id="scirp.58188-formula1059"><label>(5.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7502273x149.png"  xlink:type="simple"/></disp-formula><p>Then, we conclude:</p><p>(1) The linear modified Hubble law overestimates the Hubble constant.</p><p>(2) For a fixed redshift the resulting distance of the object is smaller than by the standard Hubble law.</p><p>(3) Quasars and galaxies with nearly the same distance can have quite different redshifts depending on the medium in which light is emitted (see e.g. Arp [<xref ref-type="bibr" rid="scirp.58188-ref18">18</xref>] ).</p><p>(4) Quasars may be nearer than by the standard Hubble law. Hence, the measured energy emitted from these quasars is smaller than generally assumed.</p><p>(5) It is possible that the assumption of dark energy in the universe is not necessary because the higher redshift implying the acceleration of the universe may be explained by the surrounding medium of the objects, as e.g. of galaxies and quasars.</p><p>All these results can be found in the article [<xref ref-type="bibr" rid="scirp.58188-ref17">17</xref>] and in the book [<xref ref-type="bibr" rid="scirp.58188-ref2">2</xref>] .</p></sec><sec id="s5"><title>5. Conclusion</title><p>The theory of gravitation in flat space-time gives a non-expanding, non-singular universe, i.e. there exists no big bang. The redshift is an intrinsic effect and not a Doppler effect. Space is not expanding. In the beginning of the universe only energy exists and no matter. In the course of time matter (dust) and radiation are created whereas the total energy is conserved. Matter increases with time and a certain time after the beginning the creation of matter is finished, i.e. the total universe appears static. A modified Hubble law is given which may explain the high redshifts of objects in the universe without the assumption of dark energy.</p></sec><sec id="s6"><title>Cite this paper</title><p>WalterPetry, (2015) Creation of a Non-Expanding, Non-Singular Universe. Journal of Modern Physics,06,1085-1094. doi: 10.4236/jmp.2015.68113</p></sec></body><back><ref-list><title>References</title><ref id="scirp.58188-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (1981) General Relativity and Gravitation, 13, 865-872. http://dx.doi.org/10.1007/BF00764272</mixed-citation></ref><ref id="scirp.58188-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2014) A Theory of Gravitation in Flat Space-Time. Science Publishing Group.</mixed-citation></ref><ref id="scirp.58188-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Lerner, L.J. (2005) arXiv: astro-phys. 0509611.</mixed-citation></ref><ref id="scirp.58188-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Lerner, L.J., Faloma, R. and Scarpa, R. (2014) International Journal of Modern Physics, D23, Article ID: 1450058.</mixed-citation></ref><ref id="scirp.58188-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Watts, A. (2014) “Settled Science” Paper Claims the Universe Is Static, Not Expanding.  
http://www.sci-news.com/astronomy/science-universe-is-not-expanding</mixed-citation></ref><ref id="scirp.58188-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Soares, D.S.L. (2006) arXiv: physics/0605098.</mixed-citation></ref><ref id="scirp.58188-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Afonso-Faus, A. (2010) arXiv: 1004.2251.</mixed-citation></ref><ref id="scirp.58188-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Alfonso-Faus, A. (2012) arXiv: 1207.0997.</mixed-citation></ref><ref id="scirp.58188-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2007) arXiv: 0705.4359.</mixed-citation></ref><ref id="scirp.58188-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Hartnett, J.G. (2011) arXiv: 1107.2485.</mixed-citation></ref><ref id="scirp.58188-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (1990) General Relativity and Gravitation, 22, 1045-1065. http://dx.doi.org/10.1007/BF00757815</mixed-citation></ref><ref id="scirp.58188-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (1997) Astrophysics and Space Science, 254, 305-317. http://dx.doi.org/10.1023/A:1000938931517</mixed-citation></ref><ref id="scirp.58188-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2011) arXiv: 1102.1063.</mixed-citation></ref><ref id="scirp.58188-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2013) Journal of Modern Physics, 4, 20-25. http://dx.doi.org/10.4236/jmp.2013.47A1003</mixed-citation></ref><ref id="scirp.58188-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (1996) Astrophysics and Space Science, 235, 41-57. http://dx.doi.org/10.1007/BF00643589</mixed-citation></ref><ref id="scirp.58188-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2014) Journal of Applied Mathematics and Physics, 2, 50.</mixed-citation></ref><ref id="scirp.58188-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Petry, W. (2013) Physics Essays, 26, 315.</mixed-citation></ref><ref id="scirp.58188-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Arp, H.C. (1988) Quasars, Redshifts and Controversies. Cambridge University Press, Cambridge.  
http://dx.doi.org/10.1017/CBO9780511564857</mixed-citation></ref></ref-list></back></article>