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Zarantonello Fixed-Point Iteration

Updated 9 July 2026
  • Zarantonello fixed-point iteration is a relaxed fixed-point scheme in Hilbert spaces that uses adaptive step sizes to drive convergence towards fixed points.
  • It generalizes classical projection methods to include firmly nonexpansive mappings, cutter operators, and cyclic compositions for solving common fixed-point problems.
  • The method extends to adaptive iterative linearized Galerkin schemes and is benchmarked against modern acceleration techniques like optimized Halpern anchoring for improved convergence rates.

Zarantonello fixed-point iteration is the Hilbert-space scheme

xk+1=xk+θk(Txkxk),k=0,1,2,,x_{k+1}=x_k+\theta_k(Tx_k-x_k), \qquad k=0,1,2,\dots,

for an operator T:HHT:H\to H with nonempty fixed point set FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset. In modern fixed-point terminology it is often called a relaxed fixed-point iteration. Equivalently, with

Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,

one has xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k. The method is classical in the setting of metric projections onto closed convex sets, but later work places it in a much broader framework that includes firmly nonexpansive mappings, resolvents of maximal monotone operators, subgradient projectors, cutter operators, cyclic compositions, and adaptive iterative linearized Galerkin schemes for strongly monotone nonlinear equations (Cegielski et al., 2012, Heid et al., 2019).

1. Canonical formulation and classical projection setting

Let HH be a real Hilbert space with inner product ,\langle\cdot,\cdot\rangle and norm \|\cdot\|. The iteration

xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)

moves from xkx_k in the direction of the fixed-point residual T:HHT:H\to H0, scaled by a relaxation parameter T:HHT:H\to H1. In the classical projection setting, T:HHT:H\to H2 is the metric projection T:HHT:H\to H3 onto a nonempty, closed and convex set T:HHT:H\to H4, so that

T:HHT:H\to H5

Zarantonello’s original work focuses on metric projections. The crucial structural fact is that T:HHT:H\to H6 is firmly nonexpansive: T:HHT:H\to H7 In particular, T:HHT:H\to H8 is nonexpansive and quasi-nonexpansive, and its fixed point set is exactly T:HHT:H\to H9. This places the iteration in a setting where the relaxed operator inherits strong metric regularity properties.

The interval FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset0 is characteristic for the relaxation parameter. For many classes of operators considered in the modern literature, including cutters and firmly nonexpansive maps, constant relaxation FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset1 leads to convergence under suitable assumptions, and variable relaxation FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset2 for some FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset3 also fits the standard convergence framework (Cegielski et al., 2012). A common misconception is that the method is specific to orthogonal projection. In fact, the same template appears for nonexpansive mappings with nonempty fixed point set, firmly nonexpansive mappings, cutter operators, and projection-type operators such as subgradient projectors.

2. Geometric operator classes and the cutter framework

A central generalization replaces the single projection operator by a cutter. For FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset4, define the half-space

FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset5

An operator FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset6 is called a cutter if

FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset7

equivalently, if

FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset8

or, in rewritten form,

FixT={xHTx=x}\operatorname{Fix}T=\{x\in H\mid Tx=x\}\neq\emptyset9

Geometrically, the hyperplane through Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,0 with normal Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,1 cuts the space into two half-spaces, containing Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,2 and Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,3 on opposite sides.

This framework unifies several operator classes. Orthogonal projections Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,4, resolvents of maximal monotone operators, subgradient projectors, and firmly nonexpansive mappings are all cutters. If Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,5, then Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,6 is closed and convex. Every cutter is quasi-nonexpansive: Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,7

Within this language, the Zarantonello iteration is simply the usual relaxation of a cutter. If one defines

Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,8

then setting Tθk:=(1θk)I+θkT,T_{\theta_k}:=(1-\theta_k)I+\theta_k T,9 yields

xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k0

which is exactly the relaxed operator underlying Zarantonello iteration. Thus the classical scheme is a special case of a generalized relaxation in which the step can depend on the current state (Cegielski et al., 2012).

3. Cyclic compositions, extrapolation, and local acceleration

The cutter framework is particularly useful for common fixed point problems. Given a finite family of cutter operators xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k1 with nonempty common fixed point set

xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k2

one may form the cyclic composition

xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k3

The basic cyclic scheme is then the Picard iteration

xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k4

which reduces to the classical cyclic projection method when xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k5.

The generalized Zarantonello-type scheme for the composite operator takes the form

xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k6

with xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k7 and a step size function xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k8. When xk+1=Tθkxkx_{k+1}=T_{\theta_k}x_k9 outside HH0, the paper terms this an extrapolation of HH1: the step along HH2 is larger than in the basic Zarantonello iteration.

A distinguished choice is the maximal step size

HH3

where HH4 and HH5. This choice is constructed so that HH6 is again a cutter. In this way, the classical single-operator iteration extends systematically to composite operators, state-dependent step sizes, and local acceleration strategies of Dos Santos type (Cegielski et al., 2012).

The Dos Santos principle is line-search-like but remains within the fixed-point geometry. For projection methods onto hyperplanes or related feasibility operators, the accelerated point on the line HH7 is selected by a problem-specific formula for HH8. The paper emphasizes that this acceleration is local: each step is optimally adjusted along the current line, but global speed-up is not guaranteed a priori.

4. Convergence mechanisms

For a cutter HH9, the relaxed operator

,\langle\cdot,\cdot\rangle0

is strongly quasi-nonexpansive for ,\langle\cdot,\cdot\rangle1. This property is the analytical basis for convergence of Zarantonello-type iterations in the cutter setting (Cegielski et al., 2012).

For cyclic composites, the central convergence statement is expressed for

,\langle\cdot,\cdot\rangle2

Under the common fixed point assumption and the cutter hypotheses on the factors ,\langle\cdot,\cdot\rangle3, one has the estimate

,\langle\cdot,\cdot\rangle4

This yields Fejér monotonicity with respect to ,\langle\cdot,\cdot\rangle5, and in particular ,\langle\cdot,\cdot\rangle6.

The demiclosedness assumptions identify the weak limit. If ,\langle\cdot,\cdot\rangle7 is demiclosed at ,\langle\cdot,\cdot\rangle8, then every weak cluster point belongs to ,\langle\cdot,\cdot\rangle9, and Fejér arguments give weak convergence of the whole sequence to a point in \|\cdot\|0. If each \|\cdot\|1 is demiclosed at \|\cdot\|2, then the limit lies in the common fixed point set

\|\cdot\|3

These results generalize the single-operator picture in two directions. First, they allow families of operators treated through their composition. Second, they allow extrapolation parameters \|\cdot\|4 that may exceed \|\cdot\|5, provided the induced operator remains strongly quasi-nonexpansive. The standard restriction \|\cdot\|6 therefore survives in a broadened form rather than disappearing.

5. Strongly monotone equations and adaptive iterative linearized Galerkin schemes

A second modern realization of Zarantonello iteration arises in the solution of nonlinear operator equations

\|\cdot\|7

on a real Hilbert space \|\cdot\|8, where \|\cdot\|9 is Lipschitz continuous and strongly monotone. In the unified iterative linearization framework, one chooses xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)0, or more precisely xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)1 with xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)2 the Riesz map. The iteration then becomes

xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)3

and in weak form

xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)4

This is exactly the Zarantonello fixed-point iteration in that framework (Heid et al., 2019).

The paper assumes Lipschitz continuity with constant xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)5, strong monotonicity with constant xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)6, and the existence of a Gâteaux differentiable potential xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)7 with xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)8. For Zarantonello iteration, the energy decrease condition holds for any

xk+1=xk+θk(Txkxk)x_{k+1}=x_k+\theta_k(Tx_k-x_k)9

Under these assumptions, the general convergence theory yields convergence of xkx_k0 to the unique solution xkx_k1.

The same framework is coupled to Galerkin discretization. On a finite-dimensional subspace xkx_k2, the discrete Zarantonello iteration reads

xkx_k3

Adaptive iterative linearized Galerkin algorithms monitor the linearization error

xkx_k4

against a posteriori estimator values

xkx_k5

and iterate on the current space while xkx_k6. When xkx_k7, the space is enriched and the process repeats. In the finite element applications studied in the paper, this yields convergence xkx_k8 and linear decay of a combined energy-estimator quantity. The numerical comparisons reported there place Zarantonello alongside Kačanov and Newton iterations: Zarantonello is globally convergent under the monotonicity assumptions and fits naturally into adaptive finite element discretizations, but it is slower in iteration count than Newton when high accuracy is sought (Heid et al., 2019).

Recent complexity theory places classical relaxed fixed-point methods in a sharper hierarchy. For nonexpansive and contractive operators, optimized Halpern-type anchoring yields exact optimal worst-case rates for the squared fixed-point residual xkx_k9. In the nonexpansive case, the optimized Halpern rate is

T:HHT:H\to H00

while in the contractive case the optimal rate is of order T:HHT:H\to H01, and for maximal T:HHT:H\to H02-strongly monotone inclusions the corresponding optimal proximal-point residual rate is of order T:HHT:H\to H03 (Park et al., 2022).

This has a direct consequence for the interpretation of classical Zarantonello-type iterations. Relaxed Picard, Krasnosel’skiĭ–Mann, projection, and resolvent schemes belong to the broad class of deterministic fixed-point methods driven by evaluations of a nonexpansive or averaged operator. In the abstract residual metric used in the complexity analysis, classical relaxed projection and Mann-type schemes with T:HHT:H\to H04 residual behavior are therefore strictly suboptimal, whereas optimized Halpern-type anchoring is optimal (Park et al., 2022). This does not invalidate the classical method; it locates it as a baseline iteration whose convergence guarantees are robust but not complexity-optimal in the black-box model.

A related but terminologically distinct interpretation appears for linear systems. The paper “Zur iterativen Loesung von linearen Gleichungssystemen” studies a fixed-point iteration

T:HHT:H\to H05

and modifies it to

T:HHT:H\to H06

so that the new iteration matrix has spectral radius less than one, even when the original iteration diverges. That paper does not use the name “Zarantonello,” and presents the method through state feedback, eigenvalue placement, and Riccati equations; the connection is conceptual rather than terminological (Karl et al., 2013). It nevertheless illustrates a recurrent theme in the modern reading of Zarantonello’s iteration: a problematic fixed-point map is altered by a structured relaxation or feedback mechanism so that convergence becomes enforceable.

Taken together, these developments suggest a stable taxonomy. Zarantonello fixed-point iteration is the basic relaxation process

T:HHT:H\to H07

for projection, nonexpansive, firmly nonexpansive, cutter, and monotone-operator settings. Cyclic composition and extrapolation extend it to common fixed point problems; adaptive ILG places it in PDE discretization; and optimized Halpern-type methods define the current complexity frontier against which the classical scheme is measured.

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