The spectral analysis of three families of exceptional Laguerre polynomials
详细信息    查看全文
文摘
The Bochner Classification Theorem (1929) characterizes the polynomial sequences class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si1.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=6cca6d261bbe401e9b5a352eba2b46dd">class="imgLazyJSB inlineImage" height="15" width="46" 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-S0021904515001598-si1.gif">class="mathContainer hidden">class="mathCode">{pn}n=0, with class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si2.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=723a17cafe05f624fea5245b0474fe19" title="Click to view the MathML source">degpn=nclass="mathContainer hidden">class="mathCode">degpn=n that simultaneously form a complete set of eigenstates for a second-order differential operator and are orthogonal with respect to a positive Borel measure having finite moments of all orders. Indeed, up to a complex linear change of variable, only the classical Hermite, Laguerre, and Jacobi polynomials, with certain restrictions on the polynomial parameters, satisfy these conditions. In 2009, Gómez-Ullate, Kamran, and Milson found that for sequences class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si3.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=9537b63341f5d44c59ccb1c5535393d9">class="imgLazyJSB inlineImage" height="15" width="46" 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-S0021904515001598-si3.gif">class="mathContainer hidden">class="mathCode">{pn}n=1, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si2.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=723a17cafe05f624fea5245b0474fe19" title="Click to view the MathML source">degpn=nclass="mathContainer hidden">class="mathCode">degpn=n (without the constant polynomial), the only such sequences satisfying these conditions are the exceptional  class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si5.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=8ba8069a2ad35c81c6fb318a69fd3429" title="Click to view the MathML source">X1class="mathContainer hidden">class="mathCode">X1-Laguerre and class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si5.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=8ba8069a2ad35c81c6fb318a69fd3429" title="Click to view the MathML source">X1class="mathContainer hidden">class="mathCode">X1-Jacobi polynomials. Subsequently, during the past five years, several mathematicians and physicists have discovered and studied other exceptional orthogonal polynomials class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si7.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=071128957dc21be1f5674db307f3484f" title="Click to view the MathML source">{pn}n∈N0⧵Aclass="mathContainer hidden">class="mathCode">{pn}nN0A, where class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si13.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=20c0814113700bbe73fd23dc6a513425" title="Click to view the MathML source">Aclass="mathContainer hidden">class="mathCode">A is a finite subset of the non-negative integers class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si19.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=701b26bf7d6a6746a58b15ade358975e" title="Click to view the MathML source">N0class="mathContainer hidden">class="mathCode">N0 and where class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si2.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=723a17cafe05f624fea5245b0474fe19" title="Click to view the MathML source">degpn=nclass="mathContainer hidden">class="mathCode">degpn=n for all class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si11.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=b4faf92a40979fcf2f1e9580a2be2d6e" title="Click to view the MathML source">n∈N0⧵Aclass="mathContainer hidden">class="mathCode">nN0A. We call such a sequence an exceptional polynomial sequence of codimension class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si12.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=3e2bf59cb01110987e6eaa4721d232fa" title="Click to view the MathML source">|A|class="mathContainer hidden">class="mathCode">|A|, where the latter denotes the cardinality of class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si13.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=20c0814113700bbe73fd23dc6a513425" title="Click to view the MathML source">Aclass="mathContainer hidden">class="mathCode">A. All exceptional sequences with a non singular weight, found to date, have the remarkable feature that they form a complete orthogonal set in their natural Hilbert space setting.

Among the exceptional sets already known are two types of exceptional Laguerre polynomials, called the Type I and Type II exceptional Laguerre polynomials, each omitting class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021904515001598&_mathId=si14.gif&_user=111111111&_pii=S0021904515001598&_rdoc=1&_issn=00219045&md5=71acef71fbfd3d13184e1a8cac86b86a" title="Click to view the MathML source">mclass="mathContainer hidden">class="mathCode">m polynomials. In this paper, we briefly discuss these polynomials and construct the self-adjoint operators generated by their corresponding second-order differential expressions in the appropriate Hilbert spaces. In addition, we present a novel derivation of the Type III family of exceptional Laguerre polynomials along with a detailed disquisition of its properties. We include several representations of these polynomials, orthogonality, norms, completeness, the location of their local extrema and roots, root asymptotics, as well as a complete spectral study of the second-order Type III exceptional Laguerre differential expression.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700