<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2023.1310045</article-id><article-id pub-id-type="publisher-id">APM-128356</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>
 
 
  Some New Transformation Formulas for &lt;i&gt;q&lt;/i&gt;-Series through the Bailey Transform
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lijun</surname><given-names>Hao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Liangliang</surname><given-names>Xu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Science, Zhejiang Sci-Tech University, Hangzhou, China</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>10</month><year>2023</year></pub-date><volume>13</volume><issue>10</issue><fpage>651</fpage><lpage>661</lpage><history><date date-type="received"><day>6,</day>	<month>September</month>	<year>2023</year></date><date date-type="rev-recd"><day>15,</day>	<month>October</month>	<year>2023</year>	</date><date date-type="accepted"><day>18,</day>	<month>October</month>	<year>2023</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 literature, the Bailey transform has many applications in basic hypergeometric series. In this paper, we derive many new transformation formulas for 
  <em>q</em>-series by means of the Bailey transform. Meanwhile, We also obtain some new terminated identities. Furthermore, we establish a companion identity to the Rogers-Ramanujan identity labelled by number (23) on Slater’s list.
 
</p></abstract><kwd-group><kwd>&lt;i&gt;q&lt;/i&gt;-Series</kwd><kwd> Bailey Transform</kwd><kwd> Transformation Formulas</kwd><kwd> Rogers-Ramanujan Identities</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Throughout this paper, a , x and q are complex number with | q | &lt; 1 . Here and in what follows, we adopt the standard q-series notation [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] . For any positive integer n,</p><p>( a ; q ) 0 : = 1 ,   ( a ; q ) n : = ∏ k = 0 n − 1 ( 1 − a q k ) ,   ( a ; q ) ∞ : = ∏ k = 0 ∞ ( 1 − a q k ) ,</p><p>( a 1 , a 2 , a 3 , ⋯ , a m ; q ) n : = ( a 1 ; q ) n ( a 2 ; q ) n ( a 3 ; q ) n ⋯ ( a m ; q ) n ,</p><p>( a 1 , a 2 , a 3 , ⋯ , a m ; q ) ∞ : = ( a 1 ; q ) ∞ ( a 2 ; q ) ∞ ( a 3 ; q ) ∞ ⋯ ( a m ; q ) ∞ .</p><p>For convenience, we use ( a ) n to denote ( a ; q ) n . We will often use basic properties without reference, such as</p><p>( a ; q ) n + k = ( a ; q ) n ( a q n ; q ) k ,   ( a ; q ) ∞ = ( a ; q ) n ( a q n ; q ) ∞ .</p><p>The q-binomial coefficient is given for any nonnegative integers M and N by</p><p>[ N M ] q : = [ N M ] = ( ( q ; q ) N ( q ; q ) M ( q ; q ) N − M , if   N ≥ M , 0, otherwise .</p><p>Following Gasper and Rahman [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , the bilateral basic hypergeometric series is defined by</p><p>r ψ s [ a 1 , a 2 , ⋯ , a r b 1 , b 2 , ⋯ , b s ; q , z ] = ∑ n = − ∞ ∞ ( a 1 , a 2 , ⋯ , a r ; q ) n ( b 1 , b 2 , ⋯ , b s ; q ) n { ( − 1 ) n q ( n 2 ) } s − r z n ,</p><p>and the unilateral basic hypergeometric series is defined by</p><p>r ϕ s [ a 1 , a 2 , ⋯ , a r b 1 , b 2 , ⋯ , b s ; q , z ] = ∑ n = 0 ∞ ( a 1 , a 2 , ⋯ , a r ; q ) n ( q , b 1 , b 2 , ⋯ , b s ; q ) n { ( − 1 ) n q ( n 2 ) } 1 + s − r z n .</p><p>The Ramanujan’s 1 ψ 1 sum ( [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , Appendix (II. 29)), and the sum of a 1 ϕ 1 series, ( [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , Appendix (II.5)) are stated as follows.</p><p>1 ψ 1 [ a b ; q , z ] = ( q , b / a , a z , q / a z ; q ) ∞ ( b , q / a , z , b / a z ; q ) ∞ , (1.1)</p><p>1 ϕ 1 [ a c ; q , c a ] = ( c / a ; q ) ∞ ( c ; q ) ∞ . (1.2)</p><p>Among the other formulas needed for this paper, we have separately documented the q-binomial formula and its consequence ( [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] (1.3.2)) in the sequel,</p><p>∑ n ≥ 0 ( a ; q ) n ( q ; q ) n x n = ( a x ; q ) ∞ ( x ; q ) ∞ . (1.3)</p><p>Setting q → q 2 , a → ∞ , x → x q / a in (1.3), we have</p><p>∑ n ≥ 0 ( − 1 ) n q n 2 x n ( q 2 ; q 2 ) n = ( x q ; q 2 ) ∞ . (1.4)</p><p>Furthermore, Euler’s formulas (cf. [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , Corollary 2.2)</p><p>∑ n ≥ 0 q ( n 2 ) x n ( q ; q ) n = ( − x , q ) ∞   and   ∑ n ≥ 0 x n ( q ; q ) n = 1 ( x , q ) ∞ . (1.5)</p><p>Cauchy’s identity (cf. [<xref ref-type="bibr" rid="scirp.128356-ref2">2</xref>] , Theorem 3.3)</p><p>( x ; q ) n = ∑ k = 0 n ( − 1 ) k q ( k 2 ) [ n k ] x k , (1.6)</p><p>and the formula ( [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , Exercise 1.16) which is a special case of the Bailey-Daum sum ( [<xref ref-type="bibr" rid="scirp.128356-ref1">1</xref>] , (1.8.1))</p><p>∑ n ≥ 0 ( x ; q ) n q ( n + 1 2 ) ( q ; q ) n = ( − q ; q ) ∞ ( x q ; q 2 ) ∞ . (1.7)</p><p>Besides, if a ≠ 0,1 − b q n ≠ 0 , the following identity was given by Ramanujan [<xref ref-type="bibr" rid="scirp.128356-ref3">3</xref>] ,</p><p>∑ n ≥ 0 ( − b / a ; q ) n a n q n ( n + 1 ) / 2 ( q ; q ) n ( b q ; q ) n = ( − a q ; q ) ∞ ( b q ; q ) ∞ . (1.8)</p><p>A pair of sequences ( α n , β n ) is called a Bailey pair relative to a if</p><p>β n = ∑ r = 0 n α r ( q ; q ) n − r ( a q ; q ) n + r . (1.9)</p><p>And a conjugate Bailey pair relative to a is a pair of sequences ( δ n , γ n ) satisfying</p><p>γ n = ∑ k = n ∞ δ k ( q ; q ) k − n ( a q ; q ) k + n . (1.10)</p><p>In fact, the Bailey pair and the conjugate Bailey pair are the special cases of the following Bailey transform.</p><p>Lemma 1.1 ( [<xref ref-type="bibr" rid="scirp.128356-ref4">4</xref>] ). Let n be a nonnegative integer and { A n } n = 0 ∞ , { B n } n = 0 ∞ , { C n } n = 0 ∞ , { D n } n = 0 ∞ be sequences of complex numbers. Assuming convergence of the series, if</p><p>B n = ∑ j = 0 n   A j U n − j V n + j   and   C n = ∑ j = n ∞   D j U j − n V j + n , (1.11)</p><p>then</p><p>∑ n = 0 ∞   A n C n = ∑ n = 0 ∞   B n D n .</p><p>This terminology was first proposed by Slater [<xref ref-type="bibr" rid="scirp.128356-ref5">5</xref>] . Bailey transform is widely used in mathematics for a long time, especially, in the area of basic hypergeometric series. For example, Andrews [<xref ref-type="bibr" rid="scirp.128356-ref6">6</xref>] , Kim and Lovejoy [<xref ref-type="bibr" rid="scirp.128356-ref7">7</xref>] , and Lovejoy [<xref ref-type="bibr" rid="scirp.128356-ref8">8</xref>] established multiple sums Rogers-Ramanujan type identities and partial theta identities. Andrews and Warnaar [<xref ref-type="bibr" rid="scirp.128356-ref9">9</xref>] applied the Bailey transform to give another proof of false theta functions. Bailey [<xref ref-type="bibr" rid="scirp.128356-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.128356-ref10">10</xref>] , Bressoud [<xref ref-type="bibr" rid="scirp.128356-ref2">2</xref>] , and Slater [<xref ref-type="bibr" rid="scirp.128356-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.128356-ref12">12</xref>] used this transform to derive a number of identities of Rogers-Ramanujan type identities. Ji and Zhao [<xref ref-type="bibr" rid="scirp.128356-ref13">13</xref>] established the Hecke-Rogers identities for the universal mock theta functions by means of the Bailey transform.</p><p>Notice that if we take</p><p>U n = 1 ( q ; q ) n , V n = 1 ( a q ; q ) n</p><p>in lemma 1.1, the pair of sequences ( A n , B n ) is a Bailey pair relative to a, and the pair of sequences ( C n , D n ) is a conjugate Bailey pair relative to a.</p><p>The main motivation for this work came from some Bailey’s transform of M. E. Bachraoui which appear in [<xref ref-type="bibr" rid="scirp.128356-ref14">14</xref>] , specifically the ( V n ) is the constant sequences with value 1. Applying the ( [<xref ref-type="bibr" rid="scirp.128356-ref14">14</xref>] , Theorem 3, 4, 6) and choosing appropriate D n , we establish some new transformation formulas for q-series.</p></sec><sec id="s2"><title>2. Main Results</title><p>Theorem 2.1. We have</p><p>( a q 1 2 ; q ) ∞ ∑ n ≥ 0 ( a q 1 2 ) n ( 1 − q n ) ( x ; q ) n ( q ; q ) n 2 = ∑ n ≥ 0 ( − 1 ) n ( a x ) n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 . (2.1)</p><p>Corollary 2.2. There holds</p><p>x n ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n = ∑ k = 0 n ( − 1 ) k q ( k + 1 2 ) − n k ( 1 − q k ) ( x ; q ) k ( q ; q ) k [ n k ] , (2.2)</p><p>( q ; q ) ∞ ∑ n ≥ 1 q n ( − q ; q ) n − 1 ( q ; q ) n ( q ; q ) n − 1 = ∑ n ≥ 1 q ( n + 1 2 ) ( − q ; q ) n − 1 ( q ; q ) n ( q ; q ) n − 1 , (2.3)</p><p>( − 1 ; q ) ∞ ∑ n ≥ 1 ( − 1 ) n ( − q ; q ) n − 1 ( q ; q ) n ( q ; q ) n − 1 = ∑ n ≥ 1 ( − 1 ) n q ( n 2 ) ( − q ; q ) n − 1 ( q ; q ) n ( q ; q ) n − 1 . (2.4)</p><p>Theorem 2.3. We have</p><p>( c / a ; q ) ∞ ( c ; q ) ∞ ∑ n ≥ 0 ( c / a ) n ( 1 − q n ) ( x , a ; q ) n ( q ; q ) n 2 = ∑ n ≥ 0 ( − 1 ) n ( c x / a ) n q ( n 2 ) ( 1 − q n ) ( x − 1 , a ; q ) n ( q ; q ) n 2 ( c ; q ) n . (2.5)</p><p>Corollary 2.4. There holds</p><p>1 ( c ; q ) ∞ ∑ n ≥ 0 ( − 1 ) n c n q ( n 2 ) ( 1 − q n ) ( x ; q ) n ( q ; q ) n 2 = ∑ n ≥ 0 ( c x ) n q n ( n − 1 ) ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 ( c ; q ) n , (2.6)</p><p>∑ n ≥ 0 q ( n 2 ) ( 1 − q n ) ( q ; q ) n 2 ( − q n ; q ) ∞ = ∑ n ≥ 0 q n ( n − 1 ) ( 1 − q n ) ( q ; q ) n 2 . (2.7)</p><p>Theorem 2.5. We have</p><p>( a q 1 2 ; q ) ∞ ∑ n ≥ 0 ( a q 1 2 ) n ( x ; q ) n ( q ; q ) n = ∑ n ≥ 0 ( − 1 ) n ( a x ) n q n 2 2 ( q ; q ) n . (2.8)</p><p>Theorem 2.6. There holds</p><p>( c / a ; q ) ∞ ( c ; q ) ∞ ∑ n ≥ 0 ( c / a ) n ( x , a ; q ) n ( q ; q ) n = ∑ n ≥ 0 ( − 1 ) n ( c x / a ) n q ( n 2 ) ( a ; q ) n ( q , c ; q ) n . (2.9)</p><p>Corollary 2.7. We have</p><p>∑ n ≥ 0 ( c / a ) n ( a q k ; q ) n ( q ; q ) n = ( c q k ; q ) ∞ ( c / a ; q ) ∞ , (2.10)</p><p>1 ( c ; q ) ∞ ∑ n ≥ 0 ( − 1 ) n c n q ( n 2 ) ( x ; q ) n ( q ; q ) n = ∑ n ≥ 0 ( c x ) n q n ( n − 1 ) ( c , q ; q ) n . (2.11)</p><p>Remark. Setting c = − q , x = q in (2.11), we derive</p><p>1 ( − q ; q ) ∞ ∑ n = 0 ∞ q ( n + 1 2 ) = ∑ n ≥ 0 ( − 1 ) n q n 2 + n ( q 2 ; q 2 ) n .</p><p>Furthermore, we have</p><p>∑ n = 0 ∞   q ( n + 1 2 ) = ( q 2 ; q 2 ) ∞ ( − q ; q ) ∞ .</p><p>Combining the above two identities, we arrive at</p><p>∑ n ≥ 0 ( − 1 ) n q n 2 + n ( q 2 ; q 2 ) n = ( q 2 ; q 2 ) ∞ .</p><p>The above identity is a companion to number (23) on Slater’s list [<xref ref-type="bibr" rid="scirp.128356-ref12">12</xref>] as follows.</p><p>∑ n ≥ 0 ( − 1 ) n q n 2 ( q 2 ; q 2 ) n = ( q ; q 2 ) ∞ .</p><p>Theorem 2.8. We have</p><p>( − q 2 ; q 2 ) ∞ ∑ n ≥ 0 q n 2 ( x ; q 2 ) n ( x q 2 n + 2 ; q 4 ) ∞ ( q 2 ; q 2 ) n = ∑ n ≥ 0 q ( n + 1 2 ) ( x ; q 2 ) n ( q ; q ) n . (2.12)</p><p>Corollary 2.9. There holds</p><p>( − q 2 ; q 2 ) ∞ ∑ n ≥ 0   q n 2 ( q 2 n + 4 ; q 4 ) ∞ = ∑ n ≥ 0   q ( n + 1 2 ) ( − q ; q ) n , (2.13)</p><p>( − q 2 ; q 2 ) ∞ ∑ n ≥ 0 q n 2 ( q ; q 2 ) n ( q 2 n + 3 ; q 4 ) ∞ ( q 2 ; q 2 ) n = ∑ n ≥ 0 q ( n + 1 2 ) ( q ; q 2 ) n ( q ; q ) n . (2.14)</p><p>Theorem 2.10. We have</p><p>( − a q 3 ; q 2 ) ∞ ( b q 2 ; q 2 ) ∞ ∑ n ≥ 0 a n q n 2 + n ( − b a q ; q 2 ) n ( q 2 ; q 2 ) n = ∑ n ≥ 0 a n q ( n + 2 2 ) − 1 ( − b a q ; q 2 ) n ( q ; q ) n ( b q 2 ; q 2 ) n . (2.15)</p></sec><sec id="s3"><title>3. Proofs of Theorem 2.1 and Corollary 2.2</title><p>Proof of Theorem 2.1. Setting</p><p>A n = ( − 1 ) n q n 2 ( 1 − q n ) ( x ; q ) n ( q ; q ) n 2 ,   U n = q n 2 2 ( q ; q ) n , B n = x n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 ,   D n = ( − 1 ) n a n</p><p>and V n = 1 in Lemma 1.1, we obtain</p><p>C n = ∑ k = n ∞   D k U k − n V k + n = ∑ k ≥ 0   D n + k U k = ∑ k ≥ 0 ( − a ) n + k q k 2 2 ( q ; q ) k = ( − a ) n ∑ k ≥ 0 ( − 1 ) k a k q k 2 2 ( q ; q ) k = ( − 1 ) n a n ( a q 1 2 ; q ) ∞ , (3.1)</p><p>where the last step follows by (1.4).</p><p>Thus,</p><p>∑ n ≥ 0   A n C n = ( a q 1 2 ; q ) ∞ ∑ n ≥ 0 ( a q 1 2 ) n ( 1 − q n ) ( x ; q ) n ( q ; q ) n 2 = ∑ n ≥ 0   B n D n = ∑ n ≥ 0 ( − 1 ) n ( a x ) n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 .</p><p>This completes the proof. <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-5302337x61.png" xlink:type="simple"/></inline-formula></p><p>Proof of Corollary 2.2. Based on (1.4), we can rewrite (2.1) as follows</p><p>∑ m ≥ 0 ( − 1 ) m q m 2 2 a m ( q ; q ) m ∑ k ≥ 0 q k 2 ( 1 − q k ) ( x ; q ) k a k ( q ; q ) k 2 = ∑ n ≥ 0 ( − 1 ) n x n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n a n ( q ; q ) n 2 .</p><p>Equating terms of the corresponding powers of a n , we achieve</p><p>∑ k = 0 n ( − 1 ) n − k q ( n − k ) 2 2 ( q ; q ) n − k ⋅ q k 2 ( 1 − q k ) ( x ; q ) k ( q ; q ) k 2 = ( − 1 ) n x n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 ,</p><p>which is (2.2) by some basic simplifications. (2.3) (2.4) follow from (2.1) upon letting a = q 1 2 , x = − 1 ( a = − q − 1 2 , x = − 1 ), respectively. <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-5302337x67.png" xlink:type="simple"/></inline-formula></p></sec><sec id="s4"><title>4. Proofs of Theorem 2.3 and Corollary 2.4</title><p>Proof of Theorem 2.3. We now apply Lemma 1.1 with</p><p>A n = ( − 1 ) n q n 2 ( 1 − q n ) ( x ; q ) n ( q ; q ) n 2 , U n = q n 2 2 ( q ; q ) n , B n = x n q n 2 2 ( 1 − q n ) ( x − 1 ; q ) n ( q ; q ) n 2 , D n = ( − 1 ) n ( c / a ) n q − n 2 ( a ; q ) n ( c ; q ) n ,</p><p>and V n = 1 . We compute</p><p>C n = ∑ k ≥ 0 ( a ; q ) n + k ( c ; q ) n + k ( − 1 ) n + k ( c / a ) n + k q − n + k 2 ⋅ q k 2 2 ( q ; q ) k = ( − 1 ) n ( c / a ) n q − n 2 ( a ; q ) n ( c ; q ) n ∑ k ≥ 0 ( a q n ; q ) k ( c q n , q ; q ) k ( − 1 ) k q ( k 2 ) ( c / a ) k = ( − 1 ) n ( c / a ) n q − n 2 ( a ; q ) n ⋅ ( c / a ; q ) ∞ ( c ; q ) ∞ , (4.1)</p><p>where the last step follows by (1.2). Thus, we arrive at</p><p>∑ n ≥ 0   A n C n = ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ n ≥ 0 ( c / a ) n ( 1 − q n ) ( x , a ; q ) n ( q ; q ) n 2 = ∑ n ≥ 0   B n D n = ∑ n ≥ 0 ( − 1 ) n ( c x / a ) n q ( n 2 ) ( 1 − q n ) ( x − 1 , a ; q ) n ( q ; q ) n 2 ( c ; q ) n ,</p><p>which completes the proof.</p><p>Proof of Corollary 2.4. (2.6) follows from (2.5) upon letting a → ∞ and (2.7) follows from (2.6) by letting x = c = − 1 , which proves the desired formula.</p></sec><sec id="s5"><title>5. Proof of Theorem 2.5</title><p>Proof of Theorem 2.5. Setting</p><p>A n = ( − 1 ) n q n 2 ( x ; q ) n ( q ; q ) n ,   U n = q n 2 2 ( q ; q ) n ,   B n = x n q n 2 2 ( q ; q ) n ,   D n = ( − 1 ) n a n ,</p><p>and V n is the constant sequences with value 1 in Lemma 1.1. Due to (3.1), we have</p><p>C n = ( − 1 ) n a n ( a q 1 2 ; q ) ∞ .</p><p>Thus,</p><p>∑ n ≥ 0   A n C n = ( a q 1 2 ; q ) ∞ ∑ n ≥ 0 ( a q 1 2 ) n ( x ; q ) n ( q ; q ) n = ∑ n ≥ 0   B n D n = ∑ n ≥ 0 ( − 1 ) n ( a x ) n q n 2 2 ( q ; q ) n ,</p><p>which is (2.8). <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-5302337x78.png" xlink:type="simple"/></inline-formula></p><p>Notice that we use (1.4) to express the left-hand side of (2.8)</p><p>∑ k ≥ 0 ( − 1 ) k q k 2 2 a k ( q ; q ) k ∑ m ≥ 0 q m 2 ( x ; q ) m a m ( q ; q ) m = ∑ n ≥ 0 ( − 1 ) n x n q n 2 2 a n ( q ; q ) n . (5.1)</p><p>Now we equate the terms corresponding to a n in (5.1) to obtain</p><p>∑ k = 0 n ( − 1 ) n − k q ( n − k ) 2 2 ( q ; q ) n − k ⋅ q k 2 ( x ; q ) k ( q ; q ) k = ( − 1 ) n x n q n 2 2 ( q ; q ) n ,</p><p>which gives the following identity after straightforward simplifications.</p><p>x n = ∑ k = 0 n ( − 1 ) k q ( k + 1 2 ) − n k ( x ; q ) k [ n k ] .</p><p>The above identity appears in ( [<xref ref-type="bibr" rid="scirp.128356-ref4">4</xref>] , p. 157).</p></sec><sec id="s6"><title>6. Proofs of Theorem 2.6 and Corollary 2.7</title><p>Proof of Theorem 2.6. We apply Lemma 1.1 with</p><p>A n = ( − 1 ) n q n 2 ( x ; q ) n ( q ; q ) n ,   U n = q n 2 2 ( q ; q ) n ,   B n = x n q n 2 2 ( q ; q ) n , D n = ( − 1 ) n ( c / a ) n q − n 2 ( a ; q ) n ( c ; q ) n ,</p><p>and V n is the constant sequences with value 1. Then due to (4.1), we get</p><p>C n = ( − 1 ) n ( c / a ) n q − n 2 ( a ; q ) n ⋅ ( c / a ; q ) ∞ ( c ; q ) ∞ .</p><p>Thus,</p><p>∑ n ≥ 0   A n C n = ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ n ≥ 0 ( c / a ) n ( a , x ; q ) n ( q ; q ) n = ∑ n ≥ 0   B n D n = ( − 1 ) n ( c x / a ) n q ( n 2 ) ( a ; q ) n ( q , c ; q ) n ,</p><p>which yields the desired formula. <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-5302337x87.png" xlink:type="simple"/></inline-formula></p><p>Proof of Corollary 2.7. To prove (2.10), we first use (1.6) to express the left-hand side of (2.9) as powers series in x. Then</p><p>L. H. S. of (2.9) = ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ n ≥ 0 ( c / a ) n ( a ; q ) n ( q ; q ) n ∑ k = 0 n ( − 1 ) k q ( k 2 ) [ n k ] x k</p><p>= ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ k ≥ 0 ( − 1 ) k q ( k 2 ) x k ( q ; q ) k ∑ n = k ∞ ( c / a ) n ( a ; q ) n ( q ; q ) n − k = ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ k ≥ 0 ( − 1 ) k q ( k 2 ) x k ( q ; q ) k ∑ n = 0 ∞ ( c / a ) n + k ( a ; q ) n + k ( q ; q ) n = ( c / a ; q ) ∞ ( c ; q ) ∞ ∑ k ≥ 0 ( ∑ n ≥ 0 ( − 1 ) k q ( k 2 ) ( c / a ) n + k ( a ; q ) n + k ( q ; q ) k ( q ; q ) n ) x k .</p><p>Now equate the terms corresponding to x k in (2.9) to obtain</p><p>∑ n ≥ 0 ( − 1 ) k q ( k 2 ) ( c / a ) n + k ( a ; q ) n + k ( q ; q ) k ( q ; q ) n = ( c ; q ) ∞ ( c / a ; q ) ∞ ⋅ ( − 1 ) k ( c / a ) k q ( k 2 ) ( a ; q ) k ( c , q ; q ) k ,</p><p>which by some basic calculations down to (2.10). (2.11) follows easily from (2.9) upon letting a → ∞ .</p></sec><sec id="s7"><title>7. Proofs of Theorem 2.8 and Corollary 2.9</title><p>Proof of Theorem 2.8. Let us use Lemma 1.1 with a Bailey transform as follows:</p><p>A n = q n 2 + n ( q 2 ; q 2 ) n ,     U n = q n 2 + 2 n ( q 2 ; q 2 ) n ,     B n = q ( n + 2 2 ) − 1 ( q ; q ) n ,     D n = q − n ( x ; q 2 ) n ,     V n = 1.</p><p>We compute</p><p>C n = ∑ k ≥ 0   q − n − k ( x ; q 2 ) n + k ⋅ q k 2 + 2 k ( q 2 ; q 2 ) k = q − n ( x ; q 2 ) n ∑ k ≥ 0 q k ( k + 1 ) ( x q 2 n ; q 2 ) k ( q 2 ; q 2 ) k = q − n ( x ; q 2 ) n ( − q 2 ; q 2 ) ∞ ( x q 2 n + 2 ; q 4 ) ∞ ,</p><p>where in the last step, we used the (1.7) with q → q 2 , x → x q 2 n . Then by virtue of Lemma 1.1, we get</p><p>∑ n ≥ 0   A n C n = ( − q 2 ; q 2 ) ∞ ∑ n ≥ 0 q n 2 ( x ; q 2 ) n ( x q 2 n + 2 ; q 4 ) ∞ ( q 2 ; q 2 ) n = ∑ n ≥ 0   B n D n = ∑ n ≥ 0 q ( n + 1 2 ) ( x ; q 2 ) n ( q ; q ) n ,</p><p>which completes the proof.</p><p>Proof of Corollary 2.9. (2.13) and (2.14) follow from (2.12) by letting, respectively, x = q 2 and x = q .</p></sec><sec id="s8"><title>8. Proof of Theorem 2.10</title><p>Proof of Theorem 2.10. Let us use Lemma 1.1 with a Bailey transform as follows:</p><p>A n = q n 2 + n ( q 2 ; q 2 ) n ,     U n = q n 2 + 2 n ( q 2 ; q 2 ) n ,     B n = q ( n + 2 2 ) − 1 ( q ; q ) n ,     D n = a n ( − b a q ; q 2 ) n ( b q 2 ; q 2 ) n ,     V n = 1.</p><p>We compute</p><p>C n = ∑ k ≥ 0 a n + k ( − b a q ; q 2 ) n + k ( b q 2 ; q 2 ) n + k ⋅ q k 2 + 2 k ( q 2 ; q 2 ) k = a n ( − b a q ; q 2 ) n ( b q 2 ; q 2 ) n ∑ k ≥ 0 a k q k 2 + 2 k ( − b q 2 n + 1 / a ; q 2 ) k ( q 2 ; q 2 ) k ( b q 2 n + 2 ; q 2 ) k = a n ( − b a q ; q 2 ) n ( − a q 3 ; q 2 ) ∞ ( b q 2 ; q 2 ) ∞ ,</p><p>where in the last step, we used (1.8) by letting a = a q , b = b q 2 n . Then by virtue of Lemma 1.1, we get</p><p>∑ n ≥ 0   A n C n = ( − a q 3 ; q 2 ) ∞ ( b q 2 ; q 2 ) ∞ ∑ n ≥ 0 a n q n 2 + n ( − b a q ; q 2 ) n ( q 2 ; q 2 ) n = ∑ n ≥ 0   B n D n = ∑ n ≥ 0 a n q ( n + 2 2 ) − 1 ( − b a q ; q 2 ) n ( q ; q ) n ( b q 2 ; q 2 ) n ,</p><p>which completes the proof.</p></sec><sec id="s9"><title>9. Conclusion</title><p>By choosing some sequences, we can derive many identities from the Bailey transform. Furthermore, we should study the generalized Bailey transform [<xref ref-type="bibr" rid="scirp.128356-ref14">14</xref>] deeply to establish the multiple parameterized identities. On the other hand, we can also study the mock theta functions or the Rogers-Ramanujan identities through the Bailey transform.</p></sec><sec id="s10"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s11"><title>Cite this paper</title><p>Hao, L.J. and Xu, L.L. (2023) Some New Transformation Formulas for q-Series through the Bailey Transform. Advances in Pure Mathematics, 13, 651-661. https://doi.org/10.4236/apm.2023.1310045</p></sec></body><back><ref-list><title>References</title><ref id="scirp.128356-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Gasper, G. and Rahman, M. 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