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The spectral resolution of Laguerre operators in right definite and left definite spaces.

机译:Laguerre算子在右定和左定空间中的光谱分辨率。

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摘要

The connection between the singular Sturm-Liouville problem and the differential operator generated by the Laguerre differential equation {dollar}xyprimeprime + (1 + alpha - x)yprime + lambda y = 0{dollar} is considered for {dollar}all alpha{dollar} in both the right and left definite cases.; First, the boundary value Sturm-Liouville problem is considered on an interval, {dollar}(a,b),{dollar} where both {dollar}a{dollar} and {dollar}b{dollar} are singular points. We use the Weyl {dollar}m(lambda){dollar} function to find {dollar}Lsp2(a, b; w){dollar} solutions near a and b. Using these we define abstract boundary conditions. These, in turn, assist us to define a self-adjoint differential operator and to derive its resolvent. We then discuss the spectral functions and the generalized Fourier transform of an arbitrary function in {dollar}Lsp2(a, b; w).{dollar}; Second, in the right definite case, a shifted Laguerre equation when {dollar}alpha {lcub}-{rcub}1{dollar} are introduced. We show that both Laguerre operators given by {dollar}ly = lbrack {lcub}-{rcub}(xsp{lcub}alpha+1{rcub}esp{lcub}-x{rcub}yprime)primerbrack /xspalpha esp{lcub}-x{rcub},{dollar} when {dollar}alpha {lcub}-{rcub}1,{dollar} respectively, are self-adjoint under the norm {dollar}(y, z) = intsbsp{lcub}0{rcub}{lcub}infty{rcub} xspalpha esp{lcub}-x{rcub}y bar z dx.{dollar} It is also shown that the spectral resolution of the Laguerre differential operator for all {dollar}alpha {lcub}-{rcub}1.{dollar}; Finally, in the left definite case, the Laguerre operators given by {dollar}ly = lbrack {lcub}-{rcub}(xsp{lcub}alpha+1{rcub} esp{lcub}-x{rcub} yprime)prime + xspalpha esp{lcub}-x{rcub} yrbrack /xspalpha esp{lcub}-x{rcub},{dollar} when {dollar}alpha {lcub}-{rcub}1,{dollar} respectively, are shown to be self-adjoint under the energy norm {dollar}langle y, zrangle = intsbsp{lcub}0{rcub}{lcub}infty{rcub} lbrack (xsp{lcub}alpha+1{rcub} esp{lcub}-x{rcub})yprimebar zprime + xspalpha esp{lcub}-x{rcub} y bar zrbrack dx.{dollar} The spectra for both the shifted, {dollar}alpha {lcub}-{rcub}1,{dollar} Laguerre equations are discrete, {dollar}{lcub}n - alpha + 1{rcub}sbsp{lcub}n=0{rcub}{lcub}infty{rcub}{dollar} and {dollar}{lcub}n + 1{rcub}sbsp{lcub}n=0{rcub}{lcub}infty{rcub},{dollar} with eigenfunctions {dollar}{lcub}xsp{lcub}-alpha{rcub}Lsbsp{lcub}n{rcub}{lcub}(-alpha){rcub}(x){rcub}sbsp{lcub}n=0{rcub}{lcub}infty{rcub}{dollar} and {dollar}{lcub}Lsbsp{lcub}n{rcub}{lcub}(alpha){rcub}(x){rcub}sbsp{lcub}n=0{rcub}{lcub}infty{rcub}{dollar}, respectively. Their spectral resolutions in {dollar}Lsp2(0, infty; xspalpha esp{lcub}-x{rcub}){dollar} hold in the new space {dollar}Hsp1(0, infty; xsp{lcub}alpha+1{rcub} esp{lcub}-x{rcub}, xspalpha esp{lcub}-x{rcub}){dollar} as well.
机译:对于{dollar} all alpha {dollar},考虑奇异Sturm-Liouville问题和由Laguerre微分方程{dol} xyprimeprime +(1 + alpha-x)yprime + lambda y = 0 {dollar}生成的微分算子之间的联系。 }在左右确定的情况下。首先,在一个区间{美元}(a,b),{美元}上考虑边界值Sturm-Liouville问题,其中{美元} a {美元}和{美元} b {美元}都是奇异点。我们使用Weyl {dollar} m(lambda){dollar}函数在a和b附近找到{dollar} Lsp2(a,b; w){dollar}解。使用这些我们定义抽象边界条件。这些反过来又帮助我们定义了一个自伴微分算子并导出了它的分解。然后,我们讨论频谱函数和{splash} Lsp2(a,b; w)中任意函数的广义傅里叶变换。其次,在右定情况下,引入了{dollar} alpha {lcub}-{rcub} 1 {dollar}时的移位Laguerre方程。我们显示{dollar} ly = lbrack {lcub}-{rcub}(xsp {lcub} alpha + 1 {rcub} esp {lcub} -x {rcub} yprime)给出的两个Laguerre运算符primerbrack / xspalpha esp {lcub} -x {rcub},{dollar},当{dollar} alpha {lcub}-{rcub} 1,{dollar}分别在范本{dollar}(y,z)= intsbsp {lcub} 0 { rcub} {lcub} infty {rcub} xspalpha esp {lcub} -x {rcub} y bar z dx。{dollar}还显示了所有{dollar} alpha {lcub}-的Laguerre微分算子的光谱分辨率{rcub} 1. {dollar};最后,在左定情况下,由{dollar} ly = lbrack {lcub}-{rcub}(xsp {lcub} alpha + 1 {rcub} esp {lcub} -x {rcub} yprime)给出的Laguerre运算符素数+ xspalpha esp {lcub} -x {rcub} yrbrack / xspalpha esp {lcub} -x {rcub},{dollar}当{dollar} alpha {lcub}-{rcub} 1,{dollar}分别显示为self -在能量范数下的伴随{美元} langle y,zrangle = intsbsp {lcub} 0 {rcub} {lcub} infty {rcub} lbrack(xsp {lcub} alpha + 1 {rcub} esp {lcub} -x {rcub} } yprimebar zprime + xspalpha esp {lcub} -x {rcub} y bar zrbrack dx。{dollar}位移的{dollar} alpha {lcub}-{rcub} 1,{dollar}拉盖尔方程的光谱都是离散的, {dollar} {lcub} n-alpha + 1 {rcub} sbsp {lcub} n = 0 {rcub} {lcub} infty {rcub} {dollar}和{dollar} {lcub} n +1 {rcub} sbsp {lcub } n = 0 {rcub} {lcub} infty {rcub},{dollar}具有本征函数{dollar} {lcub} xsp {lcub} -alpha {rcub} Lsbsp {lcub} n {rcub} {lcub}(-alpha) {rcub}(x){rcub} sbsp {lcub} n = 0 {rcub} {lcub} infty {rcub} {dollar}和{dollar} {lcub} Lsbsp {lcub} n {rcub} {lcub}(alpha) {rcub}(x){rcub} sbsp {lcub} n = 0 {rcub} {lcub} infty {rcub} {dollar}。它们在{dollar} Lsp2(0,infty; xspalpha esp {lcub} -x {rcub}){dollar}中的光谱分辨率在新空间{dollar} Hsp1(0,infty; xsp {lcub} alpha + 1 {rcub } esp {lcub} -x {rcub},xspalpha esp {lcub} -x {rcub}){dollar}。

著录项

  • 作者

    Hajmirzaahmad, Mojdeh.;

  • 作者单位

    The Pennsylvania State University.;

  • 授予单位 The Pennsylvania State University.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 1990
  • 页码 136 p.
  • 总页数 136
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 数学;
  • 关键词

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