SVEP Polaroid operatorThe property (w) is a variant of Weyl's theorem, for a bounded operator T acting on a Banach space. In this note we consider the preservation of property (w) under a finite rank perturbation commuting with T , whenever T is polaroid, or T has analytical coreThe preservation of property (w) is also studied under commuting nilpotent or under injective quasi-nilpotent perturbations. The theory is exemplified in the case of some special classes of operators.In this paper we continue the study of the class of linear bounded operators defined on Banach spaces that verify property (w), a variant of Weyl's theorem introduced by V. Rakočević in [23] and studied in a more recent paper [8]. The preservation of property (w) under certain classes of perturbations has been investigated in [3,4,7]. In this paper we give further results on the preservation of property (w) in some special cases and improve previous results. Moreover, the theory is applied to several classes of operators. We begin by given some preliminary definitions and basic results.Let X be an infinite-dimensional complex Banach space and denote by L( X) the algebra of all bounded linear operators on X . A bounded operator T ∈ L( X) is said to be an upper semi-Fredholm operators if α(T ) := dim ker T < ∞ and T (X) is closed, while T ∈ L( X) is said to be lower semi-Fredholm if β(T ) := codim T (X) < ∞. Let Φ + (X) and Φ − (X) denote the class of all upper semi-Fredholm operators. The index of a semi-Fredholm operator is defined as ind T := α(T ) − β(T ). T ∈ L( X) is said to be a Fredholm operator if T ∈ Φ + (X) ∩ Φ − (X). The upper semi-Weyl operators W + (X) are defined as the class of upper semi-Fredholm operators having ind T 0. The lower semi-Weyl operators W − (X) are defined as the class of lower semi-Fredholm operators having ind T 0. The class of Weyl operators is defined byThese classes of operators generate the following spectra: the Weyl spectrum defined by σ w (T ) := λ ∈ C: λI − T / ∈ W (X) , the upper semi-Weyl spectrum (in literature called also Weyl essential approximate point spectrum) defined by σ uw (T ) := λ ∈ C: λI − T / ∈ W + (X) ,