<?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.2015.51004</article-id><article-id pub-id-type="publisher-id">APM-53315</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>
 
 
  Root-Patterns to Algebrising Partitions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ex</surname><given-names>L. Agacy</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>42 Brighton Street, Gulliver, Townsville, Australia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ragacy@iprimus.com.au</email></corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>01</month><year>2015</year></pub-date><volume>05</volume><issue>01</issue><fpage>31</fpage><lpage>41</lpage><history><date date-type="received"><day>26</day>	<month>December</month>	<year>2014</year></date><date date-type="rev-recd"><day>7</day>	<month>January</month>	<year>2015</year>	</date><date date-type="accepted"><day>22</day>	<month>January</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The study of the confluences of the roots of a given set of polynomials—root-pattern problem— does not appear to have been considered. We examine the situation, which leads us on to Young tableaux and tableaux representations. This in turn is found to be an aspect of multipartite partitions. We discover, and show, that partitions can be expressed algebraically and can be “differentiated” and “integrated”. We show a complete set of bipartite and tripartite partitions, indicating equivalences for the root-pattern problem, for select pairs and triples. Tables enumerating the number of bipartite and tripartite partitions, for small pairs and triples are given in an appendix.
 
</p></abstract><kwd-group><kwd>Combinatorics</kwd><kwd> Partitions</kwd><kwd> Polynomials</kwd><kwd> Root-Patterns</kwd><kwd> Tableaux</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We are interested in the “root-patterns” or confluences of the roots of a given set of polynomials―a topic one may have expected would have been studied in depth in the 19th century. However, apart from results on Resultants etc., there does not appear to have been much further development.</p><p>Motivation for consideration here arises from General Relativity where the classification of the Lanczos-Zund (3,1) spinor involves various confluences of the roots of two cubics [<xref ref-type="bibr" rid="scirp.53315-ref1">1</xref>] . This in turn relates to the important aspect of Invariants of the spinor―much like the confluences of roots of a quartic form the various algebraic types for the Weyl spinor (Petrov classification) and are linked to its Invariants.</p><p>It is shown here how the root-patterns problem becomes a problem in partitions. In this context, from bipartite partitions, an application to derivations of spinor factorizations in General Relativity has been made [<xref ref-type="bibr" rid="scirp.53315-ref2">2</xref>] .</p><p>For example, given a quadratic and two cubics, a root-pattern may be indicated by ab, aad, bce where a, b are the roots of the quadratic and a, a, b and b, c, e are the roots of each of the cubics.</p><p>Three observations may be made. Firstly, the order of the polynomials is immaterial and so the root-pattern is also aad, ab, bce, or bce, aad, ab etc. Secondly, although we have written the roots of each polynomial in “ascending letter” order, the confluences of the roots or root-pattern is unchanged if we rearrange the letter order for each polynomial’s roots. Then the last root-pattern is also ebc, ada, ab. Thirdly, for any root-pattern, we can replace any letter by any other, unused, letter as the actual value of the root is unimportant. This then allows an interchange of letters, e.g., bce, aad, ab with the interchange <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x5.png" xlink:type="simple"/></inline-formula> becomes ace, bbd, ba. In other words, any permutation of letters is allowed.</p><p>From an initial set S, a collection of elements of S where elements can be repeated, and shown juxtaposed, is just a list. A list with r elements is an r-element list and is the degree of the corresponding polynomial whose roots are the elements of the list or tuple. We define a root-pattern as just a collection of lists. Thus, the root-pattern ab, aad, bce is the collection of lists ab and aad and bce where the initial set is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x6.png" xlink:type="simple"/></inline-formula>. There are three elements in this root-pattern, a 2-element list or pair and two 3-element lists.</p><p>The number of lists in the collection is the number of polynomials. The number of components in a list is the degree of the polynomial.</p><p>If we take two polynomials, we refer to the binary case, for three polynomials, the ternary case etc.</p><p>The three observations we made earlier may now be formalized as the following rules.</p><p>1) Any two polynomials can be interchanged. This translates to any two lists in a root-pattern can be interchanged.</p><p>2) Any rearrangement of the ordering of roots of a polynomial translates as a rearrangement of the ordering of the roots in the corresponding list for that polynomial in the root-pattern.</p><p>3) Any permutation of the letters (roots) in the set of polynomials translates to a permutation of the letters in the root pattern.</p><p>It is the commonality or confluence of roots in the various polynomials that we are interested in.</p><p>We define two root-patterns A and B to be equivalent if B can be obtained from A by any of the three rules; otherwise they are inequivalent.</p><p>For the ternary case, the root patterns ab, aad, bce and bc, bvb, xcy are equivalent but neither are equivalent to aad, bb, acc.</p><p>For a given set of polynomials the various root-patterns, that is the combinations of the various roots, which include common roots, is of interest to us.</p><p>What we would like to obtain is the enumeration and the consequent collection of (inequivalent) root-patterns of several polynomials. More specifically, given m<sub>1</sub> linear forms, m<sub>2</sub> quadratics, ・・・, m<sub>n</sub> n-ics, enumerate and determine the set of inequivalent root-patterns. This is the “root-pattern’ problem.</p><p>Let us first consider a simple example.</p>Two Quadratics<p>The roots of two quadratics (two lists of pairs,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x7.png" xlink:type="simple"/></inline-formula>) are displayed in the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x8.png" xlink:type="simple"/></inline-formula> where the letters refer to the roots of the two polynomials. Besides using letters we also use corresponding numbers.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x9.png" xlink:type="simple"/></inline-formula>all roots equal.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x10.png" xlink:type="simple"/></inline-formula>roots of first are equal, which are common to one root of second.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x11.png" xlink:type="simple"/></inline-formula>roots of first are equal, but different to equal roots of second.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x12.png" xlink:type="simple"/></inline-formula>roots of first are equal, but distinct to each root of second.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x13.png" xlink:type="simple"/></inline-formula>both distinct roots of first are duplicated in second.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x14.png" xlink:type="simple"/></inline-formula>roots of first and second have a common root, with each of the others distinct.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x15.png" xlink:type="simple"/></inline-formula>all roots of both quadratics are different.</p><p>There are 7 inequivalent cases which can be written as rows</p><disp-formula id="scirp.53315-formula600"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x16.png"  xlink:type="simple"/></disp-formula><p>Note, for example, that a case written as ab, cc (12, 33) is essentially the same as cc, ab (33, 12) since the order of the quadratics is immaterial. Then too cc, ab (33, 12) is also the same as case 4 aa, bc (11, 23), since the letters (and numbers) used do not matter.</p></sec><sec id="s2"><title>2. Young Tableaux</title><p>It is seen that the roots of the two quadratics, displayed as rows, are instances of Young tableaux. We can always represent the roots of a set of polynomials as Young tableaux. For a polynomial of highest degree, say<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x17.png" xlink:type="simple"/></inline-formula>, we place its roots in a first or top row, and moving downwards to a second row with polynomials of the same or lesser degrees <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x18.png" xlink:type="simple"/></inline-formula> and so on, from top to bottom. The number of entries in row i is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x19.png" xlink:type="simple"/></inline-formula> and is the length of the row. Thus for a tableaux of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x20.png" xlink:type="simple"/></inline-formula> rows,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x21.png" xlink:type="simple"/></inline-formula>. The root-patterns of any number of polynomials can be displayed as Young tableaux.</p><p>As the order of roots of a polynomial in any row is immaterial we will take it that the numbers in each row of a Young tableau are always arranged in weakly increasing order.</p><p>A question arises as to whether every tableau can be ordered so that every row and column is weakly increasing. This is in fact not so. For any permutation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x22.png" xlink:type="simple"/></inline-formula> and row interchanges, the tableau (with weakly increasing rows)</p><disp-formula id="scirp.53315-formula601"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x23.png"  xlink:type="simple"/></disp-formula><p>cannot be displayed as one with weakly increasing columns, also allowing for the interchange of any rows.</p><sec id="s2_1"><title>2.1. Tableau Representation</title><p>We will take it that the numbers used in any tableau of n rows will be consecutive, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x24.png" xlink:type="simple"/></inline-formula>(the largest number in the tableau). Should any tableau contain q non-consecutive numbers we can always replace them so that we have consecutive numbering<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x25.png" xlink:type="simple"/></inline-formula>.</p><p>We now construct a different numbering on a tableau T. For a given T we form n-tuples or lists and there will be at most q of them. We will write the n-tuples or lists in sequence which we call the tableau representation. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x26.png" xlink:type="simple"/></inline-formula> entry of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x27.png" xlink:type="simple"/></inline-formula> tuple will be the number of times the number j appears in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x28.png" xlink:type="simple"/></inline-formula> row. Thus for the tableau T with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x29.png" xlink:type="simple"/></inline-formula> rows and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x30.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.53315-formula602"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x31.png"  xlink:type="simple"/></disp-formula><p>count the number of times 1 appears in the first row of the tableau, next the number of times 1 appears in the second row and so on, written as 110, the first 3-tuple or list. Then count the number of times 2 appears in the first row, next the number of times 2 appears in the second row and so on, to get 002 etc., so that finally we construct the tableau representation 110, 002, 120, 100 of T.</p><p>From this representation, the tableau can be reconstructed as follows.</p><p>1) The sum of the first components of each triple tells us the length of the first row; similarly for the second and third. Thus for T we have a 3-rowed tableau with row lengths<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x32.png" xlink:type="simple"/></inline-formula>.</p><p>2) Since there are four triples there will be 4 different numbers 1, 2, 3, 4 used.</p><p>3) The first component of each 3-tuple tells us that the first row contains one 1, one 3 and one 4, so the first row is 134. Similarly the second row is 133 and the third row is 22. Putting these together, one row under another, in order, recovers T.</p><p>In the tableau representation of a set of polynomials, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x33.png" xlink:type="simple"/></inline-formula> tuple refers to the number j, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x34.png" xlink:type="simple"/></inline-formula> number in a tuple refers to the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x35.png" xlink:type="simple"/></inline-formula> row of the tableau.</p><p>The 7 tableaux for two quadratics, namely</p><disp-formula id="scirp.53315-formula603"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x36.png"  xlink:type="simple"/></disp-formula><p>have the 7 tableaux representations</p><disp-formula id="scirp.53315-formula604"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x37.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Nil-Addition and the Algebraic Representations of Partitions</title><p>Partitions may be represented in two ways: for example the partitions of the number (4) are: 4, 3 + 1, 2 + 2, 2 + 1 + 1, 1 + 1 + 1 + 1 and a second way as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x38.png" xlink:type="simple"/></inline-formula>. This latter notation is manifested by extracting, from the following products, the terms of degree 4</p><disp-formula id="scirp.53315-formula605"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x39.png"  xlink:type="simple"/></disp-formula><p>so that we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x40.png" xlink:type="simple"/></inline-formula> where the exponents are the partitions</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x41.png" xlink:type="simple"/></inline-formula>which is the second notation.</p><p>The general rule for partitions of a single variable is given by a generating function [<xref ref-type="bibr" rid="scirp.53315-ref3">3</xref>] . Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x42.png" xlink:type="simple"/></inline-formula> be a set of positive intergers, usually<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x43.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.53315-formula606"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x44.png"  xlink:type="simple"/></disp-formula><p>where the exponent of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x45.png" xlink:type="simple"/></inline-formula> is the partition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x46.png" xlink:type="simple"/></inline-formula> This is seen in the above parttioning of the number (4).</p><p>For bipartite partitions the generating function for a set of pairs <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x47.png" xlink:type="simple"/></inline-formula> of positive integers, usually <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x48.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.53315-formula607"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x49.png"  xlink:type="simple"/></disp-formula><p>Expanding as a power series in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x50.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x51.png" xlink:type="simple"/></inline-formula>, the coefficient of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x52.png" xlink:type="simple"/></inline-formula> is the number of bipartite partitions of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x53.png" xlink:type="simple"/></inline-formula>. The process can be computerized and short tables of bipartite and tripartite partitions are displayed in the Appendix.</p><p>We will use the first notation, however, and consider bipartite partitions here.</p><p>The pair (2,1) has the following 4 (bi)partitions:</p><disp-formula id="scirp.53315-formula608"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x54.png"  xlink:type="simple"/></disp-formula><p>We have used a delimiting comma here, rather than the usual summation sign, since we will now use the summation sign to express the partitions as a “sum”</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x55.png" xlink:type="simple"/></inline-formula>.</p><p>Any (bipartite) partition is a tuple/list of parts: thus, the partition 11, 10 has parts 11 and 10. Each part is comprised of components; the part 10 has components 1 and 0. Partitions are then shown as their tableau representations. Thus we can talk of a partition or a tableau representation of a tableau, and construct a tableau that represents the partition1.</p><p>The + symbol used here needs more definition. Whilst it will be legitimate to write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x57.png" xlink:type="simple"/></inline-formula> there will be no point in writing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x58.png" xlink:type="simple"/></inline-formula> since we are only interested in the single partition, not multiples of it. We avoid such “multiples” of partitions by adopting the rule for addition of a partition</p><disp-formula id="scirp.53315-formula609"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x59.png"  xlink:type="simple"/></disp-formula><p>We refer to the rule as the nil-addition of a partition.</p><p>The root-patterns of two quadratics, written (2,2) can then be shown as the sum of the 7 tableau representations, so that we now write</p><disp-formula id="scirp.53315-formula610"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x60.png"  xlink:type="simple"/></disp-formula><p>Note that the tableau representations <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x61.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x62.png" xlink:type="simple"/></inline-formula> are equivalent respectively to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x63.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x64.png" xlink:type="simple"/></inline-formula>, the first by interchange of rows; the second, by interchanging the numbers 1 and 3 and then</p><p>interchanging rows. The root patterns are equivalent for these two. Including the latter two equivalent tableaux representations to the 7 above, we have</p><disp-formula id="scirp.53315-formula611"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x65.png"  xlink:type="simple"/></disp-formula><p>This is exactly the expression of the pair (2,2) into its 9 bipartite partitions.</p><p>The 7 tableau representations (or corresponding partitions) for the roots of two quadratics are a subset of the full set of tableau representations of all partitions of (2,2).</p><p>It is convenient to call the sum of all partitions of a given number, pair, triple etc., its partition representation.</p>Algebraic Representation<p>Parts and hence partitions of a number, pair of numbers etc., can be represented algebraically. For the bipartite case let x represent the tuple 10 and y the tuple 01. Then put<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x66.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x67.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x68.png" xlink:type="simple"/></inline-formula> etc. Such representations of parts or tableau representations we refer to as algebraic representations. The representation by monomials transfers partitions to algebraic notation obeying rules we have yet to set up</p><p>Let us denote the concatenation of two tuples by a concatenation (circle) symbol <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x69.png" xlink:type="simple"/></inline-formula>2, as a concatenating operator, so that 20,01 is written <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x70.png" xlink:type="simple"/></inline-formula> and 10,10,01 is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x71.png" xlink:type="simple"/></inline-formula> This notation will apply to all concatenation of tuples.</p><p>Besides the concatenation symbol<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x73.png" xlink:type="simple"/></inline-formula>, we introduce an extension symbol <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x74.png" xlink:type="simple"/></inline-formula> as an extension (or integrating) operator and develop some rules for “circle and extension multiplication”. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x75.png" xlink:type="simple"/></inline-formula> be monomials.</p><p>We define the following laws</p><disp-formula id="scirp.53315-formula612"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula613"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula614"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula615"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula616"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x80.png"  xlink:type="simple"/></disp-formula><p>where ac etc., is the ordinary (dot・) multiplication of two monomials.</p><p>It is easily seen that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x81.png" xlink:type="simple"/></inline-formula>, so that both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x82.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x83.png" xlink:type="simple"/></inline-formula> are commutative.</p><p>Rules (2), (3) and (4) allow us to simplify some of the calculations that are used, by employing simplified rules. Thus with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x84.png" xlink:type="simple"/></inline-formula> in rule 4 we have</p><disp-formula id="scirp.53315-formula617"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x85.png"  xlink:type="simple"/></disp-formula><p>using nil-addition. Most often we will therefore use rule 4′</p><disp-formula id="scirp.53315-formula618"><label>(4′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x86.png"  xlink:type="simple"/></disp-formula><p>Then with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x87.png" xlink:type="simple"/></inline-formula> in 4′, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x88.png" xlink:type="simple"/></inline-formula> which, also with nil-addition, gives a simple rule 5′ which we will very frequently employ</p><disp-formula id="scirp.53315-formula619"><label>(5′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x89.png"  xlink:type="simple"/></disp-formula><p>The term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x90.png" xlink:type="simple"/></inline-formula> is a monomial and the term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x91.png" xlink:type="simple"/></inline-formula> is a concatenated term. It is clear that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x92.png" xlink:type="simple"/></inline-formula>.</p><p>Rule 5 is a distributive law, and for simplified versions we have</p><disp-formula id="scirp.53315-formula620"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x93.png"  xlink:type="simple"/></disp-formula><p>Collating the rules that will be frequently used we have</p><disp-formula id="scirp.53315-formula621"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x94.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula622"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x95.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula623"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula624"><label>(4′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x97.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula625"><label>(5′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x98.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula626"><label>(6′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x99.png"  xlink:type="simple"/></disp-formula><p>Note that (5′) is derivable from (4′) and that the rhs of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x100.png" xlink:type="simple"/></inline-formula> consists of a monomial part <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x101.png" xlink:type="simple"/></inline-formula> and a concatenated part<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x102.png" xlink:type="simple"/></inline-formula>. It is also easily seen that</p><disp-formula id="scirp.53315-formula627"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x103.png"  xlink:type="simple"/></disp-formula><p>In these shortened versions of the original laws it may be convenient to use the terminology of an integating operator instead of that of the extension operator, using the symbol i rather than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x104.png" xlink:type="simple"/></inline-formula>. With this notation we rewrite laws (4′), (5′) and (6′) as</p><disp-formula id="scirp.53315-formula628"><label>(4′′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula629"><label>(5′′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x106.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula630"><label>(6′′)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5300652x107.png"  xlink:type="simple"/></disp-formula><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula>then rule (5′) gives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x110.png" xlink:type="simple"/></inline-formula>. In terms of tuples where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x111.png" xlink:type="simple"/></inline-formula>, y = 01 the monomial expression<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x112.png" xlink:type="simple"/></inline-formula>, where we see that the (dot) product <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x113.png" xlink:type="simple"/></inline-formula>or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x114.png" xlink:type="simple"/></inline-formula> is the mere addition of the components 01 and 21.</p><p>The left table below shows an example of the use of the extension operator employed “algebraically”, with the rhs consisting of monomials, including concatenations of them. The right table shows the interpretation of these as tableau representations.</p><disp-formula id="scirp.53315-formula631"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula632"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x117.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula633"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x119.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula634"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x121.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula635"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x123.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53315-formula636"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x125.png"  xlink:type="simple"/></disp-formula><p>Example 1. Suppose we wish to obtain the tableau representation of (2,2) associated with the roots of two quadratics. It consists of the 9 partitions</p><disp-formula id="scirp.53315-formula637"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x127.png"  xlink:type="simple"/></disp-formula><p>We can construct the (2,2) partition representation from the algebraic representation of (2,1) The algebraic representation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x128.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.53315-formula638"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x129.png"  xlink:type="simple"/></disp-formula><p>To get the (2,2) algebraic representation from the (2,1) algebraic representation we multiply it by 01, that is by the monomial y, using the extension operator<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x130.png" xlink:type="simple"/></inline-formula>.</p><p>Taking each of the 4 terms separately we get, making simplifications and writing terms with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x131.png" xlink:type="simple"/></inline-formula> preceding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x132.png" xlink:type="simple"/></inline-formula> to reorder monomials in circle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x133.png" xlink:type="simple"/></inline-formula> products,</p><disp-formula id="scirp.53315-formula639"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x134.png"  xlink:type="simple"/></disp-formula><p>Adding these up we have the algebraic representation of (2,2)</p><disp-formula id="scirp.53315-formula640"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x135.png"  xlink:type="simple"/></disp-formula><p>Ignoring the irrelevant numerical coefficients (nil-addition) in this 9 term algebraic representation of (2,2) we have</p><disp-formula id="scirp.53315-formula641"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x136.png"  xlink:type="simple"/></disp-formula><p>In terms of the partition representation this is</p><disp-formula id="scirp.53315-formula642"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x137.png"  xlink:type="simple"/></disp-formula><p>The actual tableau corresponding to each term in these expressions is easily constructed. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x138.png" xlink:type="simple"/></inline-formula></p><p>In the algebraic representation, the terms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x140.png" xlink:type="simple"/></inline-formula> are equivalent (interchange <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x141.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x142.png" xlink:type="simple"/></inline-formula>), as also the terms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x143.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x144.png" xlink:type="simple"/></inline-formula>. The tableau representation is the equivalence of pairs 21, 01 and 12, 10 and pairs 20, 01, 01 and 10, 10, 02.</p><p>Thus we may consider the (2,2) partitioning as consisting of 7 inequivalent pairs. We may take this by defining an order (dominance) algebraically on the variables, say, x &gt; y (thus ignoring the term<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x145.png" xlink:type="simple"/></inline-formula>) or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x146.png" xlink:type="simple"/></inline-formula> (ignoring the latter term).</p><p>Alternatively we could “symmetrize” the expression and consider the set of symmetrised terms,</p><disp-formula id="scirp.53315-formula643"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x147.png"  xlink:type="simple"/></disp-formula><p>which are 7.</p><p>So really the problem of finding the number of inequivalent root-patterns of a set of polynomials (two quadratics here) is subsumed as that of determining the set of symmetrized partitions, a subset of all partitions corresponding to all tableau representations of the polynomials.</p></sec></sec><sec id="s3"><title>3. Differentiation of Partitions</title><p>Partitons now being expressed algebraically, provide an opportunity to introduce “differentiation”.</p><p>If a and b are monomials in x (they must be of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x148.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x149.png" xlink:type="simple"/></inline-formula>) we define a derivative operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x150.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.53315-formula644"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x151.png"  xlink:type="simple"/></disp-formula><p>In practice we may just differentiate a monomial and ignore any coefficients. The derivative operator can be extended to a partial derivative operator such as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x152.png" xlink:type="simple"/></inline-formula> in an obvious way etc.</p><p>Example 2. The tableau and algebraic partitioning of numbers (3) and (4) is</p><disp-formula id="scirp.53315-formula645"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x153.png"  xlink:type="simple"/></disp-formula><p>Ordinary differentiation of the latter (also using 2.) gives</p><disp-formula id="scirp.53315-formula646"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x154.png"  xlink:type="simple"/></disp-formula><p>which, ignoring coefficients, reduces to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x155.png" xlink:type="simple"/></inline-formula> which is precisely the partitioning of (3).</p><p>The tableau and algebraic partitioning of the bivariate partitions (2,1) and (2,2) is</p><disp-formula id="scirp.53315-formula647"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x156.png"  xlink:type="simple"/></disp-formula><p>Differentiating the latter with respect to y gives</p><disp-formula id="scirp.53315-formula648"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x157.png"  xlink:type="simple"/></disp-formula><p>which all amounts to, ignoring coefficients,</p><disp-formula id="scirp.53315-formula649"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x158.png"  xlink:type="simple"/></disp-formula><p>precisely the partitioning of (2,1). <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x159.png" xlink:type="simple"/></inline-formula></p><p>The process of differentiation in the example has exhibited the “downgrading” of partitions―from (4) to (3) and from (2,2) to (2,1). The reverse process of “integrating” or “upgrading” was performed in Example 1 in deriving the partitioning of (2,2) from (2,1).</p></sec><sec id="s4"><title>4. Display of Partitioning for Low Degree Polynomials</title><p>The partition representations of low degree polynomials are displayed. Equivalent partitions are superscripted alike. The first-listed partition is the dominant one. Partitions of all different row lengths are necessarily all inequivalent. Partitions with equal row lengths will have partition equivalents. The algebraic representations can easily be constructed from the tableau representations.</p><sec id="s4_1"><title>4.1. Binary Root Patterns</title><sec id="s4_1_1"><title>4.1.1. Two Quadratics (2,2)</title><p>There are 9 possible partitions with 7 being inequivalent.</p><disp-formula id="scirp.53315-formula650"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x160.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_1_2"><title>4.1.2. Cubic and Quadratic (3,2)</title><p>As the polynomials are of different degrees all partitions are inequivalent. There are 16 inequivalent partitions.</p><disp-formula id="scirp.53315-formula651"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x161.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_1_3"><title>4.1.3. Two Cubics (3,3)</title><p>The total number of partitions is 31. The number of inequivalent ones (here) is 21.</p><disp-formula id="scirp.53315-formula652"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x162.png"  xlink:type="simple"/></disp-formula><p>Other partitions, equivalent to some listed here, are:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x163.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x164.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x165.png" xlink:type="simple"/></inline-formula> etc.</p></sec></sec><sec id="s4_2"><title>4.2. Ternary Root-Patterns</title><sec id="s4_2_1"><title>4.2.1. A Cubic and Two Linear Forms (3,1,1)</title><p>The total number of partitions is 21. The number of inequivalent ones is 17.</p><disp-formula id="scirp.53315-formula653"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x166.png"  xlink:type="simple"/></disp-formula><p>It is easily seen that a partition is equivalent to a given partition if the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x167.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x168.png" xlink:type="simple"/></inline-formula> entries of each part of the partition are interchanged―corresponding to row interchanges in the tableau view of the partitions. More generally, any permutation of the numbers of a permutation gives an equivalent partition. Interchange of the parts of a partition produces an equivalent partition.</p></sec><sec id="s4_2_2"><title>4.2.2. Two Quadratics and a Linear Form (2,2,1)</title><p>The total number of partitions is 26. The number of inequivalent ones is 20.</p><disp-formula id="scirp.53315-formula654"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x169.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_2_3"><title>4.2.3. Three Quadratics (2,2,2)</title><p>The total number of partitions is 66. The number of inequivalent ones is 51.</p><disp-formula id="scirp.53315-formula655"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x170.png"  xlink:type="simple"/></disp-formula></sec></sec></sec><sec id="s5"><title>Appendix</title><sec id="s5_1"><title>1. Bipartite Partitions</title><p>The table shows the number of bipartite partitions for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x171.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x172.png" xlink:type="simple"/></inline-formula> which is the coefficient of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x173.png" xlink:type="simple"/></inline-formula> in a power series expansion of</p><disp-formula id="scirp.53315-formula656"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x174.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5_2"><title>2. Tripartite Partitions</title><p>The tables show the number of tripartite partitions for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x175.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x176.png" xlink:type="simple"/></inline-formula> which is the coefficient of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5300652x177.png" xlink:type="simple"/></inline-formula> in a power series expansion of</p><disp-formula id="scirp.53315-formula657"><graphic  xlink:href="http://html.scirp.org/file/4-5300652x178.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.53315-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Agacy, R.L. and Briggs, J.R. (1994) Algebraic Classification of the Lanczos Tensor by Means of Its (3,1) Spinor Equivalent. Tensor, 55, 223-234.</mixed-citation></ref><ref id="scirp.53315-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Agacy, R.L. (2002) Spinor Factorizations for Relativity. General Relativity and Gravitation, 34, 1617-1624.http://dx.doi.org/10.1023/A:1020116122418</mixed-citation></ref><ref id="scirp.53315-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Andrews, G.E. (1984) The Theory of Partitions. Cambridge University Press, Cambridge. http://dx.doi.org/10.1017/CBO9780511608650</mixed-citation></ref></ref-list></back></article>