<?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">OJDM</journal-id><journal-title-group><journal-title>Open Journal of Discrete Mathematics</journal-title></journal-title-group><issn pub-type="epub">2161-7635</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojdm.2014.44012</article-id><article-id pub-id-type="publisher-id">OJDM-50281</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>
 
 
  On a 3-Way Combinatorial Identity
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>arima</surname><given-names>Sood</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>Ashok</surname><given-names>Kumar Agarwal</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Centre for Advanced Study in Mathematics, Panjab University, Chandigarh, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>garimasood18@gmail.com(AS)</email>;<email>aka@pu.ac.in(AKA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>09</month><year>2014</year></pub-date><volume>04</volume><issue>04</issue><fpage>89</fpage><lpage>96</lpage><history><date date-type="received"><day>3</day>	<month>July</month>	<year>2014</year></date><date date-type="rev-recd"><day>2</day>	<month>August</month>	<year>2014</year>	</date><date date-type="accepted"><day>1</day>	<month>September</month>	<year>2014</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>
 
 
  Recently in [1] Goyal and Agarwal interpreted a generalized basic series as a generating function for a colour partition function and a weighted lattice path function. This led to an infinite family of combinatorial identities. Using Frobenius partitions, we in this paper extend the result of [1] and obtain an infinite family of 3-way combinatorial identities. We illustrate by an example that our main result has a potential of yielding Rogers-Ramanujan-MacMahon type identities with convolution property.
 
</p></abstract><kwd-group><kwd>Basic Series</kwd><kwd> Partitions</kwd><kwd> N-Colour Partitions</kwd><kwd> Frobenius Partitions</kwd><kwd> Lattice Paths</kwd><kwd> Generating Functions</kwd><kwd> Combinatorial Identities</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction, Definitions and the Main Results</title><p>A series involving factors like rising <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x6.png" xlink:type="simple"/></inline-formula>-factorial <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x7.png" xlink:type="simple"/></inline-formula> defined by:</p><disp-formula id="scirp.50281-formula14"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x8.png"  xlink:type="simple"/></disp-formula><p>is called basic series (or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x9.png" xlink:type="simple"/></inline-formula>-series, or Eulerian series).</p><p>Remark: Obviously,</p><disp-formula id="scirp.50281-formula15"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x10.png"  xlink:type="simple"/></disp-formula><p>if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x11.png" xlink:type="simple"/></inline-formula> is a positive integer.</p><p>The following two “sum-product” basic series identities are known as Rogers-Ramanujan identities:</p><disp-formula id="scirp.50281-formula16"><label>(*)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x12.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.50281-formula17"><label>(**)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x13.png"  xlink:type="simple"/></disp-formula><p>They were first discovered by Rogers [<xref ref-type="bibr" rid="scirp.50281-ref2">2</xref>] and rediscovered by Ramanujan in 1913. MacMahon [<xref ref-type="bibr" rid="scirp.50281-ref3">3</xref>] gave the following partition theoretic interpretations of (*) and (**), respectively:</p><p>Theorem (*). The number of partitions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x14.png" xlink:type="simple"/></inline-formula> into parts with minimal difference 2 equals the number of par- titions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x15.png" xlink:type="simple"/></inline-formula> into parts which are congruent to &#177;1 (mod 5).</p><p>Theorem (**). The number of partitions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x16.png" xlink:type="simple"/></inline-formula> into parts with minimal part 2 and minimal difference 2 equals the number of partitions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x17.png" xlink:type="simple"/></inline-formula> into parts which are congruent to &#177;2 (mod 5).</p><p>Partition theoretic interpretations of many more q-series identities like (*) and (**) have been given by several mathematicians (see, for instance, Gӧllnitz [<xref ref-type="bibr" rid="scirp.50281-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.50281-ref5">5</xref>] , Gordon [<xref ref-type="bibr" rid="scirp.50281-ref6">6</xref>] , Connor [<xref ref-type="bibr" rid="scirp.50281-ref7">7</xref>] , Hirschhorn [<xref ref-type="bibr" rid="scirp.50281-ref8">8</xref>] , Agarwal and Andrews [<xref ref-type="bibr" rid="scirp.50281-ref9">9</xref>] , Subbarao [<xref ref-type="bibr" rid="scirp.50281-ref10">10</xref>] , Subbarao and Agarwal [<xref ref-type="bibr" rid="scirp.50281-ref11">11</xref>] ).</p><p>In all these results, ordinary partitions were used. In [<xref ref-type="bibr" rid="scirp.50281-ref12">12</xref>] n-colour partitions were defined. Using these partitions several more basic series identities were interpreted combinatorially (see, for instance, [<xref ref-type="bibr" rid="scirp.50281-ref13">13</xref>] -[<xref ref-type="bibr" rid="scirp.50281-ref17">17</xref>] ). Recently in [<xref ref-type="bibr" rid="scirp.50281-ref1">1</xref>] the basic series,</p><disp-formula id="scirp.50281-formula18"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x18.png"  xlink:type="simple"/></disp-formula><p>was interpreted as generating function of two different combinatorial objects, viz., an n-colour partition function and a weighted lattice path function. This led to an infinte family of combinatorial identities. Our objective here is to extend the main result of [<xref ref-type="bibr" rid="scirp.50281-ref1">1</xref>] . This gives us an infinite family of 3-way identities which have the potential of yielding many Rogers-Ramanujan-MacMahon type combinatorial identities like Theorems (*)-(**). First we recall the following definitions from [<xref ref-type="bibr" rid="scirp.50281-ref12">12</xref>] :</p><p>Definition 1.1 A partition with “<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x19.png" xlink:type="simple"/></inline-formula>copies of n”, (also called an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x20.png" xlink:type="simple"/></inline-formula>-colour partition), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x21.png" xlink:type="simple"/></inline-formula>, is a partition in which a part of size n, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x22.png" xlink:type="simple"/></inline-formula>, can occur in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x23.png" xlink:type="simple"/></inline-formula> different colours denoted by subscripts<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x24.png" xlink:type="simple"/></inline-formula>. For example, the partitions of 2 with “<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x25.png" xlink:type="simple"/></inline-formula>copies of n” are:</p><disp-formula id="scirp.50281-formula19"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x26.png"  xlink:type="simple"/></disp-formula><p>Note that zeros are permitted if and only if t is greater than or equal to one.</p><p>Definition 1.2 The weighted difference of two elements <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x27.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x28.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x29.png" xlink:type="simple"/></inline-formula>, is defined by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x30.png" xlink:type="simple"/></inline-formula> and is denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x31.png" xlink:type="simple"/></inline-formula>.</p><p>Definition 1.3 A two-rowed array of non-negative integers,</p><disp-formula id="scirp.50281-formula20"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x32.png"  xlink:type="simple"/></disp-formula><p>with each row aligned in non-increasing order is called a generalized Frobenius partition or more simply an F-partition of ν,</p><p>if</p><disp-formula id="scirp.50281-formula21"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x33.png"  xlink:type="simple"/></disp-formula><p>Next, we recall the following description of lattice paths from [<xref ref-type="bibr" rid="scirp.50281-ref18">18</xref>] which we shall be considering in this paper.</p><p>All paths will be of finite length lying in the first quadrant. They will begin on the x-axis or on the y-axis and terminate on the x-axis. Only three moves are allowed at each step:</p><p>Northeast: from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x34.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x35.png" xlink:type="simple"/></inline-formula>,</p><p>Southeast: from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x36.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x37.png" xlink:type="simple"/></inline-formula>, only allowed if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x38.png" xlink:type="simple"/></inline-formula>,</p><p>Horizontal: from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x39.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x40.png" xlink:type="simple"/></inline-formula>, only allowed along x-axis.</p><p>The following terminology will be used in describing lattice paths:</p><p>PEAK: Either a vertex on the y-axis which is followed by a southeast step or a vertex preceded by a northeast step and followed by a southeast step.</p><p>VALLEY: A vertex preceded by a southeast step and followed by a northeast step. Note that a southeast step followed by a horizontal step followed by a northeast step does not constitute a valley.</p><p>MOUNTAIN: A section of the path which starts on either the x- or y-axis, which ends on the x-axis, and which does not touch the x-axis anywhere in between the end points. Every mountain has at least one peak and may have more than one.</p><p>PLAIN: A section of the path consisting of only horizontal steps which starts either on y-axis or at a vertex preceded by a southeast step and ends at a vertex followed by a northeast step.</p><p>The HEIGHT of a vertex is its y-coordinate. The WEIGHT of a vertex is its x-coordinate. The WEIGHT OF A PATH is the sum of the weights of its peaks.</p><p>For the related graphs the reader is referred to the following papers.</p><p>(a) T. Mansour, Counting peaks at height k in a Dyck path, Journal of Integer Sequences, 5 (2002), Article 02.1.1.</p><p>(b) T. Mansour, Statistics on Dyck paths, Journal of Integer Sequences 9:1 (2006), Article 06.1.5.</p><p>(c) P. Peart and W.J. Woan, Dyck paths with no peaks at height k, J. of Integer Sequences 4 (2001), Article 01.1.3.</p><p>(d) D. Merlini, R. Sprugnoli and M.C. Verri, Some statistics on Dyck paths, J. Statist. Plann. and Infer. 101 2002, 211-227.</p><p>Example: The following path has five peaks, three valleys, three mountains and one plain (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>In this example, there are two peaks of height three and three of height two, two valleys of height one and one of height zero.</p><p>The weight of this path is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x41.png" xlink:type="simple"/></inline-formula>.</p><p>The following result was proved in [<xref ref-type="bibr" rid="scirp.50281-ref15">15</xref>] .</p><p>Theorem 1.1 For a positive integer k, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x42.png" xlink:type="simple"/></inline-formula> denote the number of n-colour partitions of ν such that:</p><p>(1.1a) the parts are of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x43.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x44.png" xlink:type="simple"/></inline-formula>, if k is an odd and of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x45.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x46.png" xlink:type="simple"/></inline-formula>, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x47.png" xlink:type="simple"/></inline-formula> is even</p><p>(1.1b) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x48.png" xlink:type="simple"/></inline-formula> is the smallest or the only part in the partition, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x49.png" xlink:type="simple"/></inline-formula> and</p><p>(1.1c) the weighted difference between any two consecutive parts is nonnegative and is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x50.png" xlink:type="simple"/></inline-formula>.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x51.png" xlink:type="simple"/></inline-formula> denote the number of lattice paths of weight ν which start at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x52.png" xlink:type="simple"/></inline-formula>, such that,</p><p>(1.1d) they have no valley above height 0</p><p>(1.1e) there is a plain of length <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x53.png" xlink:type="simple"/></inline-formula> in the beginning of the path, other plains, if any, are of lengths which are multiples of 4 and</p><p>(1.1f) the height of each peak of odd (resp., even) weight is 1 (resp. 2) if k is odd and 2 (resp. 1) if k is even. Then</p><disp-formula id="scirp.50281-formula22"><label>(1.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x54.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.50281-formula23"><label>(1.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x55.png"  xlink:type="simple"/></disp-formula><p>In this paper we propose to prove the following theorems which extend Theorem 1.1 for odd and even k separately:</p><p>Theorem 1.2 For k an odd positive integer, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x56.png" xlink:type="simple"/></inline-formula> denote the number of F-partitions of ν such that:</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Lattice path</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1200184x57.png"/></fig><disp-formula id="scirp.50281-formula24"><label>(1.2a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x58.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.50281-formula25"><label>(1.2b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x59.png"  xlink:type="simple"/></disp-formula><p>(1.2c) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x60.png" xlink:type="simple"/></inline-formula>and,</p><p>(1.2d) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x61.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x62.png" xlink:type="simple"/></inline-formula></p><p>As in Theorem 1.1, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x63.png" xlink:type="simple"/></inline-formula> denote the number of n-colour partitions of ν such that:</p><p>(1.2e) the parts are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x64.png" xlink:type="simple"/></inline-formula>,</p><p>(1.2f) only the first copy of the odd parts and the second copy of the even parts are used, that is, the parts are of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x65.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x66.png" xlink:type="simple"/></inline-formula>,</p><p>(1.2g) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x67.png" xlink:type="simple"/></inline-formula> is the smallest or the only part in the partition, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x68.png" xlink:type="simple"/></inline-formula>, and,</p><p>(1.2h) the weighted difference of any two consecutive parts is non-negative and is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x69.png" xlink:type="simple"/></inline-formula>.</p><p>Then</p><disp-formula id="scirp.50281-formula26"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x70.png"  xlink:type="simple"/></disp-formula><p>Theorem 1.3 For k an even positive integer, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x71.png" xlink:type="simple"/></inline-formula> denote the number of F-partitions of ν such that:</p><disp-formula id="scirp.50281-formula27"><label>(1.3a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.50281-formula28"><label>(1.3b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x73.png"  xlink:type="simple"/></disp-formula><p>(1.3c) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x74.png" xlink:type="simple"/></inline-formula>and,</p><p>(1.3d) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x75.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x76.png" xlink:type="simple"/></inline-formula></p><p>As in Theorem 1.1, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x77.png" xlink:type="simple"/></inline-formula> denote the number of n-colour partitions of ν such that:</p><p>(1.3e) the parts are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x78.png" xlink:type="simple"/></inline-formula>,</p><p>(1.3f) only the second copy of the odd parts and the first copy of the even parts are used, that is, the parts are of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x79.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x80.png" xlink:type="simple"/></inline-formula>,</p><p>(1.3g) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x81.png" xlink:type="simple"/></inline-formula> is the smallest or only part in the partition, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x82.png" xlink:type="simple"/></inline-formula>,</p><p>(1.3h) the weighted difference of any two consecutive parts is non-negative and is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x83.png" xlink:type="simple"/></inline-formula>.</p><p>Then</p><disp-formula id="scirp.50281-formula29"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x84.png"  xlink:type="simple"/></disp-formula><p>In our next section we give the detailed proof of Theorem 1.2. The proofs of Theorem 1.2 and Theorem 1.3 are similar and hence the proof of Theorem 1.3 is omitted. The interested reader can supply it or obtain from the authors. In Section 3 we illustrate by an example that our results have the potential of yielding Rogers- Ramanujan-MacMahon type combinatorial identities.</p></sec><sec id="s2"><title>2. Proof of Theorem 1.2</title><p>We establish a one-one correspondence between the F-partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x85.png" xlink:type="simple"/></inline-formula> and n-colour partitions</p><p>enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x86.png" xlink:type="simple"/></inline-formula>. We do this by mapping each column <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x87.png" xlink:type="simple"/></inline-formula> of F-partitions to a single part <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x88.png" xlink:type="simple"/></inline-formula> of n-</p><p>colour partition. The mapping <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x89.png" xlink:type="simple"/></inline-formula> is:</p><disp-formula id="scirp.50281-formula30"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x90.png"  xlink:type="simple"/></disp-formula><p>and the inverse mapping <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x91.png" xlink:type="simple"/></inline-formula> is given by:</p><disp-formula id="scirp.50281-formula31"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x92.png"  xlink:type="simple"/></disp-formula><p>Clearly (2.1) and (1.2a) imply (1.2e). Also (2.1) and (1.2b) imply (1.2f). Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x93.png" xlink:type="simple"/></inline-formula> is the smallest part of the n-colour partition, we see that (2.1) and (1.2c) imply (1.2g). Now suppose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x94.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x95.png" xlink:type="simple"/></inline-formula>. Then since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x96.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x97.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.50281-formula32"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x98.png"  xlink:type="simple"/></disp-formula><p>which is non-negative and is divisible by 4 in view of (1.2d) and so (1.2h) follows.</p><p>To see the reverse implication we note that (2.2) and (1.2e) imply (1.2a).</p><p>(2.2) and (1.2f) imply (1.2b). Since if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x99.png" xlink:type="simple"/></inline-formula> is the smallest part then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x100.png" xlink:type="simple"/></inline-formula>, we see that (2.2) and (1.2g) imply (1.2c).</p><p>Now suppose<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x101.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x102.png" xlink:type="simple"/></inline-formula>are two consecutive parts in an n-colour partition with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x103.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x104.png" xlink:type="simple"/></inline-formula></p><p>Then in view of (2.2.),we have</p><disp-formula id="scirp.50281-formula33"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x105.png"  xlink:type="simple"/></disp-formula><p>Clearly (2.3) and (1.2h) imply (1.2d).</p><p>This completes the proof of Theorem 1.2.</p><p>To illustrate the bijection we have constructed, we give an example for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x106.png" xlink:type="simple"/></inline-formula> shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Thus</p><disp-formula id="scirp.50281-formula34"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x107.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. A Particular Case</title><p>By a little series manipulation, the following identity of Slater [<xref ref-type="bibr" rid="scirp.50281-ref19">19</xref>] (Equation (25)):</p><disp-formula id="scirp.50281-formula35"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x108.png"  xlink:type="simple"/></disp-formula><p>can be written in the following form:</p><disp-formula id="scirp.50281-formula36"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x109.png"  xlink:type="simple"/></disp-formula><p>Now an appeal to Theorem 1.1 gives the following 3-way combinatorial interpretation of Identity (3.2)</p><p>Theorem 3.1: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x110.png" xlink:type="simple"/></inline-formula> denote the number of partitions of ν into parts<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x111.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x112.png" xlink:type="simple"/></inline-formula> denote the number of partitions of ν into parts<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x113.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.50281-formula37"><label>(3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x114.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x115.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x116.png" xlink:type="simple"/></inline-formula> are as defined in Theorem 1.1.</p><p>Example.</p><disp-formula id="scirp.50281-formula38"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x117.png"  xlink:type="simple"/></disp-formula><p>Also</p><disp-formula id="scirp.50281-formula39"><graphic  xlink:href="http://html.scirp.org/file/1-1200184x118.png"  xlink:type="simple"/></disp-formula><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x119.png" xlink:type="simple"/></inline-formula>, <xref ref-type="table" rid="table2">Table 2</xref> shows the relevant partitions enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x120.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x121.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x122.png" xlink:type="simple"/></inline-formula> and <xref ref-type="table" rid="table3">Table 3</xref> shows the relevant lattice paths enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x123.png" xlink:type="simple"/></inline-formula>.</p><p>Our Theorem 1.2 provides a four way extension of (3.3) as follows:</p><disp-formula id="scirp.50281-formula40"><label>(3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1200184x124.png"  xlink:type="simple"/></disp-formula><p><xref ref-type="table" rid="table4">Table 4</xref> gives the relevant F-partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x125.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x126.png" xlink:type="simple"/></inline-formula>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Frobenius partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x127.png" xlink:type="simple"/></inline-formula> and their images under<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x128.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Frobenius partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x129.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Images under <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x130.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x131.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x132.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x133.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x134.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x135.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x136.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x137.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x138.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Number of partitions enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x139.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x140.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x141.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x142.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x143.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x144.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x145.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x146.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x147.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x148.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Empty partition</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Empty partition</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Empty partition</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1<sub>1</sub></td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2<sub>2</sub></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2, 1 + 1</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2 + 1, 1 + 1 + 1</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3<sub>1</sub> + 1<sub>1</sub></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 + 2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4, 2 + 2, 2 + 1 + 1, 1 + 1 + 1 + 1</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >5<sub>1</sub>, 4<sub>2</sub> + 1<sub>1</sub></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 + 2</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5, 4 + 1, 2 + 2 + 1, 2 + 1 + 1 + 1, 1 + 1 + 1 + 1 + 1</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >6<sub>2</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >6, 3 + 3, 2 + 2 + 2</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >5 + 1, 4 + 2, 4 + 1 + 1, 2 + 2 + 2, 2 + 2 + 1 + 1, 2 + 1 + 1 + 1 + 1 1 + 1 + 1 + 1 + 1 + 1</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5<sub>1 </sub>+ 2<sub>2</sub></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 + 2 + 2</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >7, 5 + 2, 5 + 1 + 1, 4 + 2 + 1, 4 + 1 + 1 + 1, 2 + 2 + 2 + 1, 2 + 2 + 1 + 1 + 1, 2 + 1 + 1 + 1 + 1 + 1, 1 + 1 + 1 + 1 + 1 + 1 + 1</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Number of lattice paths enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x149.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x150.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x151.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x152.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Empty lattice path with weight 0</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x153.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x154.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x155.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x156.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x157.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x158.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x159.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Number of Frobenius partitions enumerated by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x160.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x161.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x162.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Frobenius partitions enumerated by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x163.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Empty Frobenius partition with No column</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x164.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x165.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >No partition</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x166.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x167.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x168.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x169.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>4. Conclusion</title><p>The work done in this paper shows a nice interaction between the theory of basic series and combinatorics. Theorems 1.1, 1.2 and 1.3 give a 3-way combinatorial identity for each value of k. Thus we get infinitely many 3-way combinatorial identities from these theorems. In one particular case, viz., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1200184x170.png" xlink:type="simple"/></inline-formula>we get a 4-way com- binatorial interpretation of one well known basic series identity of L. J. Slater.</p><p>It would be of interest if more applications of Theorems 1.1, 1.2 and 1.3 can be found.</p></sec><sec id="s5"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.50281-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Goyal, M. and Agarwal, A.K. On a New Class of Combinatorial Identities. ARS Combinatoria. 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