Inverse of the adjoint of the shift operator

In summary, the conversation is discussing the shift operator on the Hardy space, and the goal is to prove the identity (1-\lambda S^*)^{-1}S^*f(z)=\frac{f(z)-f(\lambda)}{z-\lambda}, where \lambda,z\in\mathbb{D}. The conversation also reveals that S^*=\frac{f(z)-f(0)}{z} and provides a hint to put (1-\lambda S^*) on the other side to prove the identity.
  • #1
Likemath2014
17
0
Hi there,

Let [itex]S[/itex] denote the shift operator on the Hardy space on the unit disc [itex]H^2[/itex], that is [itex](Sf)(z)=zf(z)[/itex].

My question is to show the following identity

[itex](1-\lambda S^*)^{-1}S^*f (z)=\frac{f(z)-f(\lambda)}{z-\lambda},[/itex]

where [itex]\lambda,z\in\mathbb{D}[/itex]

Thanks in advance
 
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  • #2
First of all, can you figure out what ##S^*## does exactly? This can be made easy if you can figure out an orthonormal basis of ##H^2##.
 
  • #3
Yes, [itex]S^*=\frac{f(z)-f(0)}{z}[/itex]. But my problem is with the term [itex](1-\lambda S^*)^{-1}[/itex].
 
  • #4
Just put it on the other side. So you need to prove

[tex]S^*f(z) = (1-\lambda S^*)\frac{f(z)-f(\lambda)}{z-\lambda}[/tex]
 
  • #5
for your help!

Hello,

First, let's define the adjoint of the shift operator. The adjoint, denoted by S^*, is the operator on the Hardy space H^2 such that for any two functions f and g in H^2, we have \langle Sf,g\rangle = \langle f,S^*g\rangle, where \langle \cdot,\cdot \rangle denotes the inner product on H^2.

Now, to prove the given identity, we will use the fact that the inverse of an operator A is given by (1-A)^{-1}=\sum_{n=0}^{\infty}A^n. So, we have

(1-\lambda S^*)^{-1}S^*f (z) = \sum_{n=0}^{\infty}(\lambda S^*)^nS^*f(z)

= \sum_{n=0}^{\infty}\lambda^n S^{*n}S^*f(z)

= \sum_{n=0}^{\infty}\lambda^n S^{*n+1}f(z)

Now, using the definition of the adjoint and the fact that (Sf)(z)=zf(z), we have

= \sum_{n=0}^{\infty}\lambda^n S^{*n+1}f(z)

= \sum_{n=0}^{\infty}\lambda^n zS^{*n}f(z)

= \sum_{n=0}^{\infty}\lambda^n zf(z)

= \frac{f(z)-f(\lambda)}{z-\lambda}

which proves the given identity.

I hope this helps. Let me know if you have any further questions.
 

1. What is the inverse of the adjoint of the shift operator?

The inverse of the adjoint of the shift operator is a mathematical operation that involves finding the inverse of the transpose of the shift operator. This operation is commonly used in linear algebra and functional analysis to solve equations and study the properties of linear transformations.

2. How is the inverse of the adjoint of the shift operator calculated?

The inverse of the adjoint of the shift operator is calculated by finding the inverse of the transpose of the shift operator. This can be done using various techniques such as matrix inversion, row reduction, or using the properties of inner product spaces.

3. What is the significance of the inverse of the adjoint of the shift operator?

The inverse of the adjoint of the shift operator is significant in studying the properties of linear transformations and solving equations involving these transformations. It also plays a crucial role in functional analysis and can be used to prove theorems and solve problems related to operator theory.

4. Can the inverse of the adjoint of the shift operator always be calculated?

No, the inverse of the adjoint of the shift operator cannot always be calculated. In some cases, the inverse may not exist or may be difficult to determine. This can happen when the shift operator is not invertible or when the dimension of the underlying vector space is infinite.

5. Are there any applications of the inverse of the adjoint of the shift operator in real life?

Yes, there are many applications of the inverse of the adjoint of the shift operator in real life. For example, it is used in signal processing to analyze and manipulate audio and video signals, in computer graphics for image transformations, and in engineering and physics for solving differential equations and studying dynamical systems.

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