<?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.2016.47141</article-id><article-id pub-id-type="publisher-id">JAMP-68949</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>
 
 
  Skorohod Integral at Vacuum State on Guichardet-Fock Spaces
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jihong</surname><given-names>Zhang</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>Yongjun</surname><given-names>Li</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>Xiaochun</surname><given-names>Sun</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>College of Mathematics and Statistics, Northwest Normal University, Lanzhou, China</addr-line></aff><aff id="aff1"><addr-line>School of Mathematics, Lanzhou City University, Lanzhou, China</addr-line></aff><pub-date pub-type="epub"><day>30</day><month>06</month><year>2016</year></pub-date><volume>04</volume><issue>07</issue><fpage>1321</fpage><lpage>1326</lpage><history><date date-type="received"><day>23</day>	<month>May</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>16</month>	<year>July</year>	</date><date date-type="accepted"><day>19</day>	<month>July</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>
 
 
   In this paper, we define expectation of<em> f</em>∈<em>F</em>, i.e. <em>E</em>(<em>f</em>)=<em>f</em>(<em>?</em>), according to Wiener-Ito-Segal isomorphic relation between Guichardet-Fock space F and Wienerspace W. Meanwhile, we derive a formula for the expectation of random Hermite polynomial in Skorohod integral on Guichardet- Fock spaces. In particular, we prove that the anticipative Girsanov identities under the condition <em>E</em>(<em>H</em><sub>x</sub>(<em>δ</em>(<em>x</em>),‖<em>x</em><em></em>‖<sup>2</sup>)),n≥1 on Guichardet-Fock spaces.  
 
</p></abstract><kwd-group><kwd>Moment Identities</kwd><kwd> Girsanov Identities</kwd><kwd> Hermitpolynomial</kwd><kwd> Skorohod Integral</kwd><kwd> Guichardet-Fock Spaces</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The quantum stochastic calculus developed by Hudson and Parthasarathy [<xref ref-type="bibr" rid="scirp.68949-ref1">1</xref>] is essentially a noncommutative extension of classical Ito stochastic calculus. In thistheory, annihilation, creation, and number operator processes in boson Fock space play the role of “quantum noises” [<xref ref-type="bibr" rid="scirp.68949-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.68949-ref3">3</xref>], which are in continuous time. In 2002, Attal [<xref ref-type="bibr" rid="scirp.68949-ref4">4</xref>] discussed and extended quantum stochastic calculus by means of the Skorohod integral of anticipation processes and the related gradient operator on Guichardet-Fock spaces. Usually, Fock spaces as the models of the Particle Systems are widely used in quantumphysics. Meanwhile, vacuum states described by empty set on Guichardet-Fockspaces play very important role at quantum physics.</p><p>Recently Privault [<xref ref-type="bibr" rid="scirp.68949-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.68949-ref6">6</xref>] developed a Malliavin-type theory of stochastic calculus on Wiener spaces and showed its several interesting applications. In his article, Privault surveyed the moment identities for Skorohod integral and derived a formula for the expectation of random Hermit polynomials in Skorohod integral on Wiener spaces. It is well known that Guichardet-Fock space F and Wiener space W are Wiener-Ito-Segal isomorphic. Motivated by the above, we would like to study the expectation of random Hermit polynomials in Skorohod integral on Guichardet-Fock spaces. However, how to define the expectation on Guichardet-Fock spaces is the primary problem.</p><p>In this argument, we define expectation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x7.png" xlink:type="simple"/></inline-formula> according to isomorphic relation, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x8.png" xlink:type="simple"/></inline-formula>.</p><p>Meanwhile, we prove a moment identity for the Skorohod integrals and derive a formula for the expectation of random Hermite polynomial in Skorohod integral on Guichardet-Fock spaces. Particularly, under the condition<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x9.png" xlink:type="simple"/></inline-formula>, we prove the anticipative Girsanov identities on Guichardet-Fock spaces.</p><p>This paper is organized as follows. Section 2, we fix some necessarynotations and recall main notions and facts about Skorohod integral in Guichardet-Fock spaces. Section 3 and Section 4 state our main results.</p></sec><sec id="s2"><title>2. Notations</title><p>In this section, we fix some necessary notations and recall mainnotions in Guichardet-Fock spaces. For detail formulation of Skorohod integrals, we refer reader to [<xref ref-type="bibr" rid="scirp.68949-ref4">4</xref>].</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x10.png" xlink:type="simple"/></inline-formula> be the set of all nonnegative real numbers and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x11.png" xlink:type="simple"/></inline-formula> the finite power set of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x12.png" xlink:type="simple"/></inline-formula>, namely</p><disp-formula id="scirp.68949-formula331"><graphic  xlink:href="http://html.scirp.org/file/68949x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x14.png" xlink:type="simple"/></inline-formula> denotes the cardinality of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x15.png" xlink:type="simple"/></inline-formula> as a set. Particularly, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x16.png" xlink:type="simple"/></inline-formula> be an atom of measure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x17.png" xlink:type="simple"/></inline-formula>. We denote by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x18.png" xlink:type="simple"/></inline-formula> the usual space of square integral real-valued functions on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x19.png" xlink:type="simple"/></inline-formula>.</p><p>Fixing a complex separable Hilbert space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x20.png" xlink:type="simple"/></inline-formula>, Guichardet-Fock space tensor product<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x21.png" xlink:type="simple"/></inline-formula>, which we identify with the space of square-integrable functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x22.png" xlink:type="simple"/></inline-formula>, is denoted by F.</p><p>For a Hilbert space-valued map<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x23.png" xlink:type="simple"/></inline-formula>, let</p><disp-formula id="scirp.68949-formula332"><graphic  xlink:href="http://html.scirp.org/file/68949x24.png"  xlink:type="simple"/></disp-formula><p>denotes the Skorohod integral operator. For a vector space-valued map<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x25.png" xlink:type="simple"/></inline-formula>, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x26.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x27.png" xlink:type="simple"/></inline-formula> be the maps <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x28.png" xlink:type="simple"/></inline-formula> given by</p><disp-formula id="scirp.68949-formula333"><graphic  xlink:href="http://html.scirp.org/file/68949x29.png"  xlink:type="simple"/></disp-formula><p>respectively denote the stochastic gradient operator of f and the adapted gradient operator of f. Moreover, we write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x30.png" xlink:type="simple"/></inline-formula> for the domain of the stochastic gradient as anunbounded Hilbert apace operator:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x31.png" xlink:type="simple"/></inline-formula>.</p><p>Definition 2.1 The value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x32.png" xlink:type="simple"/></inline-formula> at empty set is called the expectation of f on Guichardet-Fock space and is denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x33.png" xlink:type="simple"/></inline-formula></p><p>Definition 2.2 For the map<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x34.png" xlink:type="simple"/></inline-formula>, the value of Skorohod integral <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x35.png" xlink:type="simple"/></inline-formula> at empty set is called the</p><p>expectation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x36.png" xlink:type="simple"/></inline-formula> on Guichardet-Fock space and is denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x37.png" xlink:type="simple"/></inline-formula> i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x38.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 2.1 Let x be a map<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x39.png" xlink:type="simple"/></inline-formula>, if x is square integrable and the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x40.png" xlink:type="simple"/></inline-formula> is integrable, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x41.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.68949-formula334"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x42.png"  xlink:type="simple"/></disp-formula><p>we denote</p><disp-formula id="scirp.68949-formula335"><graphic  xlink:href="http://html.scirp.org/file/68949x43.png"  xlink:type="simple"/></disp-formula><p>Lemma 2.2 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x44.png" xlink:type="simple"/></inline-formula> and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x45.png" xlink:type="simple"/></inline-formula> be Skorohod integrable, if the map</p><disp-formula id="scirp.68949-formula336"><graphic  xlink:href="http://html.scirp.org/file/68949x46.png"  xlink:type="simple"/></disp-formula><p>is integrable, then</p><disp-formula id="scirp.68949-formula337"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x47.png"  xlink:type="simple"/></disp-formula><p>Lemma 2.3 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x48.png" xlink:type="simple"/></inline-formula> be measurable. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x49.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula338"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x50.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x51.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x52.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 2.1 For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x53.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x54.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula339"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x55.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.68949-formula340"><graphic  xlink:href="http://html.scirp.org/file/68949x56.png"  xlink:type="simple"/></disp-formula><p>Lemma 2.4 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x57.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x58.png" xlink:type="simple"/></inline-formula>. Then for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x59.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.68949-formula341"><graphic  xlink:href="http://html.scirp.org/file/68949x60.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Random Hermit Polynomials</title><p>In Theorem 3.1 below, we compute the expectation of the random Hermit polynomial <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x61.png" xlink:type="simple"/></inline-formula> with respect to the Skorohod integral<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x62.png" xlink:type="simple"/></inline-formula>. This result will be applied in Section 4 to anticipate Girsanov identities on Guichardet-Fock spaces.</p><p>Theorem 3.1 For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x63.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x64.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula342"><graphic  xlink:href="http://html.scirp.org/file/68949x65.png"  xlink:type="simple"/></disp-formula><p>Especially, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x66.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.68949-formula343"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x67.png"  xlink:type="simple"/></disp-formula><p>then we have</p><disp-formula id="scirp.68949-formula344"><label>. (3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68949x68.png"  xlink:type="simple"/></disp-formula><p>Proof We divide two steps to prove the stability result.</p><p>Step 1. We first prove that for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x69.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.68949-formula345"><graphic  xlink:href="http://html.scirp.org/file/68949x70.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x71.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x72.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula346"><graphic  xlink:href="http://html.scirp.org/file/68949x73.png"  xlink:type="simple"/></disp-formula><p>replace 1 above with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x74.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula347"><graphic  xlink:href="http://html.scirp.org/file/68949x75.png"  xlink:type="simple"/></disp-formula><p>Hence, taking<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x76.png" xlink:type="simple"/></inline-formula>, we get</p><disp-formula id="scirp.68949-formula348"><graphic  xlink:href="http://html.scirp.org/file/68949x77.png"  xlink:type="simple"/></disp-formula><p>Step 2. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x78.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x79.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.68949-formula349"><graphic  xlink:href="http://html.scirp.org/file/68949x80.png"  xlink:type="simple"/></disp-formula><p>Hence, replacing 1 above with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x81.png" xlink:type="simple"/></inline-formula>, we get</p><disp-formula id="scirp.68949-formula350"><graphic  xlink:href="http://html.scirp.org/file/68949x82.png"  xlink:type="simple"/></disp-formula><p>thus letting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x83.png" xlink:type="simple"/></inline-formula> above, and use (2.3) in step 1, we get</p><disp-formula id="scirp.68949-formula351"><graphic  xlink:href="http://html.scirp.org/file/68949x84.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Girsanov Identities</title><p>Corollary 4.1 Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x85.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x86.png" xlink:type="simple"/></inline-formula> and that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x87.png" xlink:type="simple"/></inline-formula> holds (3.1). Then, we</p><p>have</p><disp-formula id="scirp.68949-formula352"><graphic  xlink:href="http://html.scirp.org/file/68949x88.png"  xlink:type="simple"/></disp-formula><p>Proof We have</p><disp-formula id="scirp.68949-formula353"><graphic  xlink:href="http://html.scirp.org/file/68949x89.png"  xlink:type="simple"/></disp-formula><p>hence</p><disp-formula id="scirp.68949-formula354"><graphic  xlink:href="http://html.scirp.org/file/68949x90.png"  xlink:type="simple"/></disp-formula><p>By Theorem 3.1 and Fubini theorem, we have</p><disp-formula id="scirp.68949-formula355"><graphic  xlink:href="http://html.scirp.org/file/68949x91.png"  xlink:type="simple"/></disp-formula><p>This shows that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x92.png" xlink:type="simple"/></inline-formula> is deterministic and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x93.png" xlink:type="simple"/></inline-formula> holds (3.1),</p><p>we have</p><disp-formula id="scirp.68949-formula356"><graphic  xlink:href="http://html.scirp.org/file/68949x94.png"  xlink:type="simple"/></disp-formula><p>i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x95.png" xlink:type="simple"/></inline-formula>has a centered Gaussian distribution with variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68949x96.png" xlink:type="simple"/></inline-formula> on Guichardet-Fock spaces.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors are extremely grateful to the referees for their valuable comments and suggestions on improvement of the first version of the present paper. The authors are supported by National Natural Science Foundation of China (No. 11261027 and No. 11461061), supported by scientific research projects in Colleges and Universities in gansu province (No. 2015A-122) and supported by doctoral research start-up fund project of Lanzhou City Universities (No. LZCU-BS2015-02) and SRPNWNU (No. NWNU-LKQW-14-2).</p></sec><sec id="s6"><title>Cite this paper</title><p>Jihong Zhang,Yongjun Li,Xiaochun Sun, (2016) Skorohod Integral at Vacuum State on Guichardet-Fock Spaces. Journal of Applied Mathematics and Physics,04,1321-1326. doi: 10.4236/jamp.2016.47141</p></sec></body><back><ref-list><title>References</title><ref id="scirp.68949-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hudson, R.L. and Parthasarathy, K.R. (1984) Quantum Ito’s Formula and Stochastic Evolutions. 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