Home Geometric approach to the Moore–Penrose inverse and the polar decomposition of perturbations by operator ideals
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Geometric approach to the Moore–Penrose inverse and the polar decomposition of perturbations by operator ideals

  • Eduardo Chiumiento EMAIL logo and Pedro Massey
Published/Copyright: May 15, 2024

Abstract

We study the Moore–Penrose inverse of perturbations by a proper symmetrically-normed ideal of a closed range operator on a Hilbert space. We show that the notion of essential codimension of projections gives a characterization of subsets of such perturbations in which the Moore–Penrose inverse is continuous with respect to the metric induced by the operator ideal. These subsets are maximal satisfying the continuity property, and they carry the structure of real analytic Banach manifolds, which are acted upon transitively by the Banach–Lie group consisting of invertible operators associated with the ideal. This geometric construction allows us to prove that the Moore–Penrose inverse is indeed a real bianalytic map between infinite-dimensional manifolds. We use these results to study the polar decomposition of closed range operators from a similar geometric perspective. At this point we prove that operator monotone functions are real analytic in the norm of any proper symmetrically-normed ideal. Finally, we show that the maps defined by the operator modulus and the polar factor in the polar decomposition of closed range operators are real analytic fiber bundles.


Communicated by Maria Gordina


Funding statement: This research was partially supported by CONICET (PIP 2021/2023 11220200103209CO), ANPCyT (2015 1505/ 2017 0883) and FCE-UNLP (11X974).

A Appendix

In this section we present a proof of Lemma 2. Hence, we let 𝔖 be a symmetrically-normed ideal, ν a positive Borel measure on ( 0 , ) and we let h : [ 0 , ) 𝔖 sa be a function satisfying:

  1. h ( t ) 𝔖 q ( t ) , where q ( t ) is a bounded, continuous, positive and non-increasing function such that 0 q ( t ) 𝑑 ν ( t ) < .

  2. For δ > 0 we have h ( t + δ ) - h ( t ) 𝔖 α δ r ( t ) , where α > 0 and r : [ 0 , ) [ 0 , ) is a continuous and non-increasing function such that

    lim t r ( t ) = 0 and 0 r ( t ) 𝑑 ν ( t ) < .

Recall that the operator 0 h ( t ) 𝑑 ν ( t ) ( ) sa is determined by the identity

0 h ( t ) 𝑑 ν ( t ) x , y = 0 h ( t ) x , y 𝑑 ν ( t ) , x , y .

Since 𝔖 , item (i) above shows that 0 h ( t ) 𝑑 ν ( t ) < . Then the previous facts imply that for every p 1 ,

0 h ( t ) 𝑑 ν ( t ) 0 h ( t ) 𝑑 ν ( t ) , 0 h ( t ) 𝑑 ν ( t ) = m = 1 [ m - 1 2 p , m 2 p ) h ( t ) 𝑑 ν ( t ) ,

where the series converges in the operator norm. We now introduce the sequence

R p = m = 1 ν ( [ m - 1 2 p , m 2 p ) ) h ( m 2 p ) 𝔖 sa , p 1 ,

where we have used that h ( t ) 𝔖 q ( t ) is a decreasing function,

m = 1 ν ( [ m - 1 2 p , m 2 p ) ) h ( m 2 p ) 𝔖 m = 1 ν ( [ m - 1 2 p , m 2 p ) ) q ( m 2 p ) 0 q ( t ) 𝑑 ν ( t ) < ,

so that the series defining R p is absolutely convergent in 𝔖 (and hence determines an element in 𝔖 sa ). By item (ii) above we get that for m , p 1 :

(A.1) h ( m 2 p ) - h ( m - 1 2 p + t ) h ( m 2 p ) - h ( m - 1 2 p + t ) 𝔖 α 2 p r ( m - 1 2 p ) for  t [ 0 , 1 2 p ) ,

where we have used that m 2 p = ( m - 1 2 p + t ) + δ for some δ [ 0 , 2 - p ] , and that r ( m - 1 2 p + t ) r ( m - 1 2 p ) for t [ 0 , 2 - p ) . By the same item we also get that there exists η 1 such that for p 1 we have that

(A.2) m = 1 r ( m - 1 2 p ) ν ( [ m - 1 2 p , m 2 p ) ) η 0 r ( t ) 𝑑 ν ( t ) .

Therefore, we get that

(A.3) R p - 0 h ( t ) 𝑑 ν ( t ) α η 2 p 0 r ( t ) 𝑑 ν ( t ) p 0 .

We now show that { R p } p 1 is a Cauchy sequence in 𝔖 : indeed, for p 1 we have that

R p = m = 1 ( ν ( [ 2 m - 2 2 p + 1 , 2 m - 1 2 p + 1 ) ) + ν ( [ 2 m - 1 2 p + 1 , 2 m 2 p + 1 ) ) ) h ( 2 m 2 p + 1 )

and hence,

R p + 1 - R p = m = 1 ν ( [ 2 m - 2 2 p + 1 , 2 m - 1 2 p + 1 ) ) ( h ( 2 m - 1 2 p + 1 ) - h ( 2 m 2 p + 1 ) ) .

The previous identity implies that

R p + 1 - R p 𝔖 m = 1 ν ( [ 2 m - 2 2 p + 1 , 2 m - 1 2 p + 1 ) ) α 2 p + 1 r ( 2 m - 1 2 p + 1 ) α η 2 p + 1 0 r ( t ) 𝑑 ν ( t ) .

This last fact shows that { R p } p 1 is a Cauchy sequence in 𝔖 so that it converges to an operator R 𝔖 sa ; but then, { R p } p 1 also converges to R in the operator norm. The previous comments together with (A.3) imply that R = 0 h ( t ) 𝑑 ν ( t ) 𝔖 sa . On the other hand, using (A.1), we have that

| h ( m - 1 2 p + δ ) 𝔖 - h ( m 2 p ) 𝔖 | h ( m - 1 2 p + δ ) - h ( m 2 p ) 𝔖 α 2 p r ( m - 1 2 p ) for  δ [ 0 , 1 2 p ) .

Hence, using the previous fact and (A.2), we get that

(A.4) | 0 h ( t ) d ν ( t ) - m = 1 ν ( [ m - 1 2 p , m 2 p ) ) h ( m 2 p ) 𝔖 | α η 2 p 0 r ( t ) 𝑑 ν ( t ) .

Since R p - 0 h ( t ) 𝑑 ν ( t ) 𝔖 0 when p , given ϵ > 0 there exists p 0 1 such that if p p 0 , then

0 h ( t ) 𝑑 ν ( t ) 𝔖 R p 𝔖 + ϵ .

On the other hand, (A.4) shows that there exists p 1 p 0 such that for p p 1 we get that

0 h ( t ) 𝑑 ν ( t ) 𝔖 R p 𝔖 + ϵ m = 1 ν ( [ m - 1 2 p , m 2 p ) ) h ( m 2 p ) 𝔖 + ϵ 0 h ( t ) 𝔖 𝑑 ν ( t ) + 2 ϵ .

Acknowledgements

We thank the reviewer for his/her careful reading of this work and helpful comments.

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Received: 2024-01-03
Revised: 2024-04-30
Published Online: 2024-05-15
Published in Print: 2025-02-01

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