<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2015.38113</article-id><article-id pub-id-type="publisher-id">JAMP-59093</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>
 
 
  Modified Tunneling Radiation of Fermions from a Spherically Symmetric Spacetime with Dark Matter
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhongwen</surname><given-names>Feng</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaotao</surname><given-names>Zu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu, China</addr-line></aff><pub-date pub-type="epub"><day>26</day><month>08</month><year>2015</year></pub-date><volume>03</volume><issue>08</issue><fpage>931</fpage><lpage>936</lpage><history><date date-type="received"><day>7</day>	<month>June</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>19</month>	<year>August</year>	</date><date date-type="accepted"><day>26</day>	<month>August</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>
 
 
   In the paper, we use the generalized Dirac equation to study the Hawking temperature and entropy of a spherically symmetric spacetime with the dark matter. The results show that the dark matter can influence the thermodynamic properties of the black hole. Meanwhile, we find the GUP corrected temperature and entropy are not only determined by the nature of black but also related to the properties of tunneling particles. Besides, the GUP can slow down the increase of Hawking temperature and causes the remnants. 
 
</p></abstract><kwd-group><kwd>Generalized Uncertainty Principle</kwd><kwd> Spherically Symmetric Spacetime</kwd><kwd> Dark Matter</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Based on the quantum effect, people found that the black holes can radiate particles [<xref ref-type="bibr" rid="scirp.59093-ref1">1</xref>]. The radiation of black hole got researchers attention, many new methods were presented to study it [<xref ref-type="bibr" rid="scirp.59093-ref2">2</xref>]-[<xref ref-type="bibr" rid="scirp.59093-ref4">4</xref>]. Parikh and Wilzcek put forward the quantum tunneling method, which was an effective method to discuss the black hole’s Hawking radiation. With the help of the quantum tunneling method, they have calculated the massless scalar particle’s tunneling rate and Hawking temperature of the spherically symmetrical spacetime [<xref ref-type="bibr" rid="scirp.59093-ref5">5</xref>]. Then, Kerner and Mann developed the quantum tunneling method and studied the fermions tunneling from Schwarzschild (SC) spacetime [<xref ref-type="bibr" rid="scirp.59093-ref6">6</xref>]. Later, the tunneling behavior of particles with 0 spin, 1/2 spin, 1 spin and 3/2 spin from black holes were investigated via Hamilton-Jacobi ansatz, which is another quantum tunneling method. However, the results obtained in previous work showed that the standard Hawking temperature of black holes was inverse to their mass. As Hawking announced, the black hole would emit all their mass as the temperature increase, this process causes the black holes evaporate over. In other words, black holes would loss all their information, which was called as information paradox of black hole [<xref ref-type="bibr" rid="scirp.59093-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.59093-ref8">8</xref>].</p><p>In order to solve the information paradox problem, people proposed many kinds of correction theories. Recently, people studied the physical properties of the black hole via the generalized uncertainty principle (GUP) [<xref ref-type="bibr" rid="scirp.59093-ref9">9</xref>]-[<xref ref-type="bibr" rid="scirp.59093-ref11">11</xref>]. In quantum gravity theory and string theory, people believe the existence of the minimal observable length, which can be described by the GUP [<xref ref-type="bibr" rid="scirp.59093-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.59093-ref13">13</xref>] . In [ 14 ], based on the associative Heisenberg algebra</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x3.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x4.png" xlink:type="simple"/></inline-formula> is the momentum operator and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x5.png" xlink:type="simple"/></inline-formula> is the position operator. One kind of GUP is expressed as</p><disp-formula id="scirp.59093-formula20"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x6.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x7.png" xlink:type="simple"/></inline-formula> is a small value, which represents the effects of quantum gravity, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x8.png" xlink:type="simple"/></inline-formula>being the Planck</p><p>mass [<xref ref-type="bibr" rid="scirp.59093-ref15">15</xref>]. Adopted GUP, Banerjee and Ghosh investigated the thermodynamics of SC spacetime, their results showed that the black hole have remnant mass at the end of evolution [<xref ref-type="bibr" rid="scirp.59093-ref16">16</xref>]. Soon, combining with quantum tunneling method and GPU, the Hawking radiation of Schwarzschild black hole was studied by Nozari and Saghafi [<xref ref-type="bibr" rid="scirp.59093-ref17">17</xref>].</p><p>On other hand, astronomers predict 27% of the universe is dark matter. It is natural to think how can the dark matter influence the properties of black hole and whether different corrected methods deduce different results? In this paper, we will apply the GUP to investigate the Hawking temperature and entropy of spherically symmetric black hole with dark matter.</p><p>The remainder of the paper goes as follows. In Section 2, we overview of the spherically symmetric black hole with dark matter is provided. In Section 3, we corrected the Hawking temperature and entropy via GUP. The last section is the discussion and concludes.</p></sec><sec id="s2"><title>2. The Spherically Symmetric Spacetime with Dark Matter</title><p>In curved space-time, the line element of spherically symmetric black hole with dark matter can be expressed as [<xref ref-type="bibr" rid="scirp.59093-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.59093-ref19">19</xref>]</p><disp-formula id="scirp.59093-formula21"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x9.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.59093-formula22"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x10.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula23"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x11.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula24"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x12.png"  xlink:type="simple"/></disp-formula><p>In Equation (3)-Equation (5), the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x14.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x15.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x16.png" xlink:type="simple"/></inline-formula>are parameters of the spacetime, note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x17.png" xlink:type="simple"/></inline-formula> is a parameter of cold dark matter. In order to discuss the tunneling of the black hole, here we let parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x18.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x19.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x20.png" xlink:type="simple"/></inline-formula>, Equation (3) and Equation (4) become to</p><disp-formula id="scirp.59093-formula25"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x21.png"  xlink:type="simple"/></disp-formula><p>Note that Equation (5) and Equation (6) have the same expression. Thus, one can use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x22.png" xlink:type="simple"/></inline-formula> to replace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x23.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x24.png" xlink:type="simple"/></inline-formula>. Now, the metric of spherically symmetric black hole with dark matter is given by</p><disp-formula id="scirp.59093-formula26"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x25.png"  xlink:type="simple"/></disp-formula><p>The horizons of this black hole are determined by null super-surface equation. Now, assuming<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x26.png" xlink:type="simple"/></inline-formula>, by a simple calculate, the roots can be expressed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x27.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x28.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x29.png" xlink:type="simple"/></inline-formula>. According to the three roots, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x30.png" xlink:type="simple"/></inline-formula>can be written as</p><disp-formula id="scirp.59093-formula27"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x31.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x32.png" xlink:type="simple"/></inline-formula> is the cosmological horizon, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x33.png" xlink:type="simple"/></inline-formula>is the outer event horizon and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x34.png" xlink:type="simple"/></inline-formula> is the inner event horizon. The three roots satisfy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x35.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. The GUP Corrected Hawking Temperature and Entropy of Spherically Symmetric Black Hole with Dark Matter</title><p>According to the GUP, Chen et al. have rewritten the original Dirac equation into generalized form. The massless generalized Dirac equation in curved spacetime is [<xref ref-type="bibr" rid="scirp.59093-ref20">20</xref>]</p><disp-formula id="scirp.59093-formula28"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x36.png"  xlink:type="simple"/></disp-formula><p>In order to discussing the fermions tunneling from black hole, people assume fermions with 1/2 spin have two states: spin up state and spin down state. Here we only consider the spin up state. The wave function of the spin up state is</p><disp-formula id="scirp.59093-formula29"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x37.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x38.png" xlink:type="simple"/></inline-formula> is the action of up spin state of fermions, which can be expanded in powers of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x39.png" xlink:type="simple"/></inline-formula>.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x41.png" xlink:type="simple"/></inline-formula>are functions of coordinates<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x42.png" xlink:type="simple"/></inline-formula>. In order to solve Equation (9), one needs to find a tetrad, which can construct a gamma matrix. The tetrad is</p><disp-formula id="scirp.59093-formula30"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x43.png"  xlink:type="simple"/></disp-formula><p>Then, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x44.png" xlink:type="simple"/></inline-formula> matrices are</p><disp-formula id="scirp.59093-formula31"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x45.png"  xlink:type="simple"/></disp-formula><p>In Equation (12), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x46.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x47.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x48.png" xlink:type="simple"/></inline-formula>are Pauli matrices. Substituting Equation (10) and Equation (12) into Equation (9), then using WKB approximation and ignoring the higher order of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x49.png" xlink:type="simple"/></inline-formula>, one gets four Hamilton-Jacobi equations</p><disp-formula id="scirp.59093-formula32"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x50.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula33"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x51.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula34"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula35"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x53.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x54.png" xlink:type="simple"/></inline-formula>. For solving the four equations above, one needs to carry out separation of variables of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x55.png" xlink:type="simple"/></inline-formula>. Adopting the following ansatz for the separation of variables</p><disp-formula id="scirp.59093-formula36"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x56.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x57.png" xlink:type="simple"/></inline-formula> being the energy of this tunneling particle. One finds that Equation (15) and Equation (16) can be decoupled into the purely angular equation</p><disp-formula id="scirp.59093-formula37"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x58.png"  xlink:type="simple"/></disp-formula><p>In Equation (18), the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x59.png" xlink:type="simple"/></inline-formula> is a small coefficient associated with quantum gravity effective, it cannot be zero. Thus, we get an important relation</p><disp-formula id="scirp.59093-formula38"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x60.png"  xlink:type="simple"/></disp-formula><p>Now, substituting Equation (17) and Equation (19) into Equation (15) and Equation (16), keep the first order term of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x61.png" xlink:type="simple"/></inline-formula>, yields</p><disp-formula id="scirp.59093-formula39"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x62.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x63.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x64.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x65.png" xlink:type="simple"/></inline-formula>. Neglecting the higher order term of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x66.png" xlink:type="simple"/></inline-formula> and solving Equation (20) at the outer event horizon. The result of Equation (20) is</p><disp-formula id="scirp.59093-formula40"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x67.png"  xlink:type="simple"/></disp-formula><p>The plus (minus) means the outgoing (ingoing) wave. Here we only keep the imaginary part of Equation (24), because the real part <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x68.png" xlink:type="simple"/></inline-formula> do not contribution to calculate the tunneling rate. The tunneling rate of fermions is</p><disp-formula id="scirp.59093-formula41"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x69.png"  xlink:type="simple"/></disp-formula><p>Comparing with the Boltzman factor expression, the GUP corrected Hawking temperature of the black hole with dark matter is</p><disp-formula id="scirp.59093-formula42"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x70.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59093-formula43"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x73.png"  xlink:type="simple"/></disp-formula><p>Then, near the event horizon of the black hole, the position uncertainty of a particle can be expressed [<xref ref-type="bibr" rid="scirp.59093-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.59093-ref22">22</xref>]</p><disp-formula id="scirp.59093-formula44"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x74.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x75.png" xlink:type="simple"/></inline-formula> is a calibration factor and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x76.png" xlink:type="simple"/></inline-formula> is the event horizon of the black hole [<xref ref-type="bibr" rid="scirp.59093-ref23">23</xref>]. With the help of Equation (25), The temperature can be written as</p><disp-formula id="scirp.59093-formula45"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x77.png"  xlink:type="simple"/></disp-formula><p>In above equation, we set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x78.png" xlink:type="simple"/></inline-formula>. Obviously, the GUP corrected temperature is lower than the semi-clas- sical case. Besides, it is not only determined by parameters of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x79.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x80.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x81.png" xlink:type="simple"/></inline-formula> the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x82.png" xlink:type="simple"/></inline-formula>, which belongs to the effects of quantum gravity.</p></sec><sec id="s4"><title>4. Conclusions</title><p>In the previous work, people found that the GUP can cause the remnants of black holes. For calculating the remnants, we need neglect the parameters of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x84.png" xlink:type="simple"/></inline-formula>. The metric of SC black hole is recovered, Equation (26) becomes to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x85.png" xlink:type="simple"/></inline-formula>. When considering <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x86.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x87.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x88.png" xlink:type="simple"/></inline-formula>, the temperature of black hole will stop increasing. The remnants are</p><disp-formula id="scirp.59093-formula46"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/59093x89.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x90.png" xlink:type="simple"/></inline-formula>. Equation (27) implies that the remnant mass and temperature are relate to the Planck mass <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x91.png" xlink:type="simple"/></inline-formula> and the dimensionless parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x92.png" xlink:type="simple"/></inline-formula>.</p><p>In this work, with the help of GUP, we corrected the thermodynamic properties of spherically symmetric black hole with dark matter. We find that the GUP corrected temperatures is related to the properties of black hole (mass of black hole, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x93.png" xlink:type="simple"/></inline-formula>and dark matter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x94.png" xlink:type="simple"/></inline-formula>), and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/59093x95.png" xlink:type="simple"/></inline-formula>, which represents the effects of quantum gravity. In addition, we can obtain the same result when consider the down spin state of fermions. It implies that the GUP may solve the information paradox of the black hole.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is supported in part by the Natural Science Foundation of China (Grant No. 11178018).</p></sec><sec id="s6"><title>Cite this paper</title><p>Zhongwen Feng,Xiaotao Zu, (2015) Modified Tunneling Radiation of Fermions from a Spherically Symmetric Spacetime with Dark Matter. Journal of Applied Mathematics and Physics,03,931-936. doi: 10.4236/jamp.2015.38113</p></sec></body><back><ref-list><title>References</title><ref id="scirp.59093-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hawking, S.W. (1974) Particle Creation by Black Holes. Communications in Mathematical Physics, 43, 199. 
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