Our description of lass="boldFont">B depends on a fixed, but arbitrary, decomposition of lsi6" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si6.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=76c2f416c948479752dfcfb2f491844a" title="Click to view the MathML source">A1lass="mathContainer hidden">lass="mathCode"> of the form lsi7" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si7.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=d8145264d6acc0c993e10618ec4bb016" title="Click to view the MathML source">kx1⊕V0lass="mathContainer hidden">lass="mathCode">, for some non-zero element lsi8" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si8.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=e36df9d3704f96cc8e871ab99c9a90aa" title="Click to view the MathML source">x1lass="mathContainer hidden">lass="mathCode"> and some lsi9" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si9.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=e28e88db37c16c72733daa71a766de07" title="Click to view the MathML source">(d−1)lass="mathContainer hidden">lass="mathCode"> dimensional subspace lsi10" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si10.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=b576ab5449e4f39be2719dd34d99c3ca" title="Click to view the MathML source">V0lass="mathContainer hidden">lass="mathCode"> of lsi6" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si6.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=76c2f416c948479752dfcfb2f491844a" title="Click to view the MathML source">A1lass="mathContainer hidden">lass="mathCode">. Much information about lass="boldFont">B is already contained in the complex lsi11" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si11.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=a484cd7cfa90029bc520309cfe01d9bf">lass="imgLazyJSB inlineImage" height="18" width="87" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si11.gif">lass="mathContainer hidden">lass="mathCode">, which we call the skeleton of lass="boldFont">B. One striking feature of lass="boldFont">B is the fact that the skeleton of lass="boldFont">B is completely determined by the data lsi12" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si12.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=12e07350bfbe8ba10cc0c7abd621143f" title="Click to view the MathML source">(d,n)lass="mathContainer hidden">lass="mathCode">; no other information about A is used in the construction of lsi13" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si13.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=303780f786c38cee8a2ce32661acc6b2">lass="imgLazyJSB inlineImage" height="14" width="16" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si13.gif">lass="mathContainer hidden">lass="mathCode">.
The skeleton lsi13" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si13.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=303780f786c38cee8a2ce32661acc6b2">lass="imgLazyJSB inlineImage" height="14" width="16" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si13.gif">lass="mathContainer hidden">lass="mathCode"> is the mapping cone of lsi14" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si14.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=3c0decc6b09e5200a9ed7fc8f28b31a8" title="Click to view the MathML source">zero:K→Llass="mathContainer hidden">lass="mathCode">, where lsi15" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si15.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=644f1522c6197c13f697dba6749289c7" title="Click to view the MathML source">Llass="mathContainer hidden">lass="mathCode"> is a well known resolution of Buchsbaum and Eisenbud; lsi16" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si16.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=0e9d9fed6c57177363e9c926c69f3fa0" title="Click to view the MathML source">Klass="mathContainer hidden">lass="mathCode"> is the dual of lsi15" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si15.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=644f1522c6197c13f697dba6749289c7" title="Click to view the MathML source">Llass="mathContainer hidden">lass="mathCode">; and lsi15" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si15.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=644f1522c6197c13f697dba6749289c7" title="Click to view the MathML source">Llass="mathContainer hidden">lass="mathCode"> and lsi16" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si16.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=0e9d9fed6c57177363e9c926c69f3fa0" title="Click to view the MathML source">Klass="mathContainer hidden">lass="mathCode"> are comprised of Schur and Weyl modules associated to hooks, respectively. The decomposition of lsi13" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si13.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=303780f786c38cee8a2ce32661acc6b2">lass="imgLazyJSB inlineImage" height="14" width="16" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si13.gif">lass="mathContainer hidden">lass="mathCode"> into Schur and Weyl modules lifts to a decomposition of lass="boldFont">B; furthermore, lass="boldFont">B inherits the natural self-duality of lsi13" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si13.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=303780f786c38cee8a2ce32661acc6b2">lass="imgLazyJSB inlineImage" height="14" width="16" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si13.gif">lass="mathContainer hidden">lass="mathCode">.
The differentials of lass="boldFont">B are explicitly given, in a polynomial manner, in terms of the coefficients of a Macaulay inverse system for A . In light of the properties of lsi13" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si13.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=303780f786c38cee8a2ce32661acc6b2">lass="imgLazyJSB inlineImage" height="14" width="16" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0021869316000508-si13.gif">lass="mathContainer hidden">lass="mathCode">, the description of the differentials of lass="boldFont">B amounts to giving a minimal generating set of I , and, for the interior differentials, giving the coefficients of lsi8" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si8.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=e36df9d3704f96cc8e871ab99c9a90aa" title="Click to view the MathML source">x1lass="mathContainer hidden">lass="mathCode">. As an application we observe that every non-zero element of lsi6" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021869316000508&_mathId=si6.gif&_user=111111111&_pii=S0021869316000508&_rdoc=1&_issn=00218693&md5=76c2f416c948479752dfcfb2f491844a" title="Click to view the MathML source">A1lass="mathContainer hidden">lass="mathCode"> is a weak Lefschetz element for A.