...
首页> 外文期刊>Complex analysis and operator theory >A Complete Spectral Analysis of Generalized Gribov-Intissar's Operator in Bargmann Space
【24h】

A Complete Spectral Analysis of Generalized Gribov-Intissar's Operator in Bargmann Space

机译:广义Gribov-Intissar在Bargmann Space中的完整光谱分析

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

In the Bargmann representation, we study mathematically rigorously some interesting spectral properties of generalized Gribov-Intissar's operator: H,,=ap+1ap+1+apap+iap(a+a)ap(p=0,1,2...) where a and a are the creation and annihilation operators; [a,a]=I. (,,)R3 are respectively the four coupling, the intercept and the triple coupling of Pomeron and i2=-1. Firstly, the domain of the operator is defined precisely and it is shown that the minimal and the maximal version of the operator are identical; here as well as in many subsequent stages of the analysis we use extensively the representation of the operators in the Bargmann space of analytic functions. Then it is proved that H,, has compact resolvent and thus its spectrum consists of complex eigenvalues. Furthermore, H,, generates a strongly continuous semigroup such that for all t0 and a constant c>0 the estimate ||e-tH,,||ect holds, and the operator e-t(H,,+c) is compact for all t>0. Moreover, the solutions of the Cauchy problem dudt+H,,u=0 can be expanded as a series in the eigenvectors of H,,. Similar results concerning the associated semigroups are established for the operator H,, for =0. If p=0, =0 and iR then H,, is the displaced harmonic oscillator. Secondly If p=1, the Reggeon field theory (Boreskov et al. in Phys Atomic Nucl 69(10):1765-1780, 2006; Gribov in Sov. Phys. JETP 26(2):414-423, 1968) is governed by H,,. In this case for >0,>0, let sigma(,,)0 be the smallest eigenvalue of H,,, we show in this paper that sigma(,,) is positive, increasing and analytic function on the whole real line with respect to and that the spectral radius of H,,-1 converges to that of H0,,-1 as goes to zero. Hence we can exploit the structure of H,,-1 as goes to zero to deduce the main results of Ando-Zerner established (Ando and Zerner in Commun Math Phys 93:123-139, 1984) on the function sigma(0,,). Thirdly, If ==0, we consider the generalized operator Hp,m=ap(am+am)ap; (p,m=1,2,...) of -iH0,0, acting on Bargmann space. For this operator, we find some conditions on the parameters p and m for that Hp,m to be completely indeterminate. It follows from these conditions that Hp,m is entire of the type minimal. And by applying the main result of the authors (Intissar and Intissar in Complex Anal Oper Theory 11(3):491-505, 2017), we show that Hp,m and Hp,m+Hp,m are connected at the chaotic operators (where Hp,m is the adjoint of the Hp,m).
机译:在Bargmann表示中,我们在数学上严格地研究了广义Gribov-Intissar的操作员的一些有趣的光谱特性:H ,, = AP + 1AP + 1 + APAP + IAP(A + A)AP(P = 0,1,2 ... )其中A和A是创造和湮灭运营商; [A,A] = I。 (,)R3分别是PoMeron和I2 = -1的四个耦合,截距和三重耦合。首先,正是定义了操作员的域,并显示了操作员的最小和最大版本是相同的;这里以及在分析的许多后续阶段中,我们在分析函数的Bargmann空间中广泛使用了运营商的表示。然后证明H ,,具有紧凑的分辨率,因此其谱由复杂的特征值组成。此外,H ,,,为所有T0和常数C> 0产生强烈连续的半群,估计|| e_ ,, || ect,以及操作员ET(H,+ C)为所有t> 0。此外,Cauchy问题DUDT + H的溶液,例如u = 0可以在H的特征向量中扩展为串联。与= 0的操作员H建立类似的关于相关联的半群的结果。如果p = 0,则= 0和IR,则为H,是位移的谐波振荡器。其次,如果p = 1,那么reggeon场理论(Borykov等人。在phys原子核查69(10):1765-1780,2006; Gribov在Sov。物理。Jetp 26(2):414-423,1968)受到约束在h ,,。在这种情况下,对于> 0,> 0,让Sigma(,,)0是H的最小特征值,,,00在本文中展示了Sigma(,)是整个实际线上的正,增加和分析功能尊重并且H ,, - 1的光谱半径会聚到H0 ,, - 1的变为零。因此,我们可以利用H的结构,, - - 1的结构为零,推断成立的Ando-Zerner的主要结果(ANDO和Zerner在Commmal Math Phys 93:123-139,1984)上的函数sigma(0 ,,, )。第三,如果== 0,我们考虑广义操作员HP,M = AP(AM + AM)AP; (p,m = 1,2,......)的-ih0,0,作用于argmann空间。对于此运算符,我们在参数P和M上找到一些条件,对于该HP,m是完全不确定的。从这些条件下,HP,M是整个最小的条件。并通过应用作者的主要结果(复杂肛门操作中的Intissar和Intissar理论11(3):491-505,2017),我们显示HP,M和HP,M + HP,M在混沌运算符中连接(其中HP,M是HP,M的伴随。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号