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Strongly Generalized Derivation

Updated 10 July 2026
  • Strongly generalized derivation is a Leibniz-type operator defined by an order‑n product identity using auxiliary families of maps to generalize standard derivation notions.
  • It encompasses classical derivations, generalized (σ,τ)-derivations, centralizers, and ternary derivations, linking various operator frameworks under one scheme.
  • Research in this area highlights automatic continuity results in Banach and C*-algebras and offers decomposition results in nonassociative and n‑ary settings with broad mathematical applications.

Strongly generalized derivation is a Leibniz-type operator notion whose most explicit formal definition in the recent literature is an order-nn product identity of the form

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],

with suitable auxiliary families of maps. In order $1$, this reduces to an (E,F,G,H)(E,F,G,H)-derivation,

D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),

which subsumes ordinary derivations, generalized derivations, generalized (σ,τ)(\sigma,\tau)-derivations, centralizers, homomorphisms, and ternary derivations. The phrase is not uniform across the broader derivation literature: many papers instead work with generalized derivations, quasiderivations, quasicentroids, or stronger constraints on generalized derivations, and these constitute the closest parallel frameworks in Banach, Lie, Hom, and nn-ary settings (Hosseini et al., 2023, Hosseini, 8 Sep 2025, Esfahani et al., 2022).

1. Formal definition and order structure

Let A\mathcal A and B\mathcal B be algebras and let nn be a positive integer. A linear mapping Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],0 is called a strongly generalized derivation of order Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],1 if there exist families of linear mappings

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],2

such that

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],3

A closely related formulation replaces the codomain algebra by a Banach Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],4-bimodule Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],5: then a linear mapping Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],6 is called a strongly generalized derivation of order Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],7 if there exist families

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],8

satisfying the same product identity (Hosseini et al., 2023, Hosseini, 8 Sep 2025).

The order-one case is singled out in both papers: Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],9 This is called an $1$0-derivation. The order-one format is the main vehicle for automatic continuity results on Banach algebras and $1$1-algebras, while the higher-order definition is designed to encompass finite sums of product-controlled terms (Hosseini et al., 2023, Hosseini, 8 Sep 2025).

The order hierarchy contains many standard notions as exact special cases. If $1$2 and $1$3, then

$1$4

so one recovers an ordinary derivation. If $1$5, $1$6, and $1$7, then

$1$8

which is the usual generalized derivation form. If $1$9, (E,F,G,H)(E,F,G,H)0, (E,F,G,H)(E,F,G,H)1, and (E,F,G,H)(E,F,G,H)2, then

(E,F,G,H)(E,F,G,H)3

so generalized (E,F,G,H)(E,F,G,H)4-derivations are included. If (E,F,G,H)(E,F,G,H)5, then

(E,F,G,H)(E,F,G,H)6

which is the ternary derivation form. If (E,F,G,H)(E,F,G,H)7 and either (E,F,G,H)(E,F,G,H)8 or (E,F,G,H)(E,F,G,H)9, then the identity collapses to homomorphism-like behavior (Hosseini et al., 2023, Hosseini, 8 Sep 2025).

The higher-order definition is also nontrivial in concrete families. Every D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),0-double derivation,

D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),1

is a strongly generalized derivation of order D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),2. If D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),3 is a higher derivation satisfying

D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),4

then each D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),5 is a strongly generalized derivation of suitable finite order D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),6, where

D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),7

These inclusions show that the order parameter organizes a wide class of “derivation-like” identities within one finite-sum scheme (Hosseini et al., 2023).

2. Relation to generalized derivations and earlier Leibniz-type frameworks

The strongest historical point of contact is the classical generalized derivation of Brešar type: a linear map D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),8 for which there exists an ordinary derivation D(ab)=E(a)F(b)+G(a)H(b),D(ab)=E(a)F(b)+G(a)H(b),9 such that

(σ,τ)(\sigma,\tau)0

This identity is the algebraic starting point of the differential-geometric construction in “Generalized derivations and general relativity” (Heller et al., 2013). In the Banach-algebra literature, the analogous notion is a pair (σ,τ)(\sigma,\tau)1 with

(σ,τ)(\sigma,\tau)2

where (σ,τ)(\sigma,\tau)3 is a derivation and (σ,τ)(\sigma,\tau)4 is called a generalized derivation (Esfahani et al., 2022). The order-one strongly generalized identity therefore enlarges two-sided Leibniz decompositions from one derivation companion to four auxiliary maps.

A second major comparison comes from the framework of (σ,τ)(\sigma,\tau)5-derivations and (σ,τ)(\sigma,\tau)6-derivations. An additive map (σ,τ)(\sigma,\tau)7 is an (σ,τ)(\sigma,\tau)8-derivation if

(σ,τ)(\sigma,\tau)9

and an additive map nn0 is a generalized nn1-derivation corresponding to an additive nn2 if

nn3

The most general class in that paper is the nn4-derivation: nn5 The paper explicitly notes that this framework includes ordinary derivations, generalized derivations, nn6-derivations, generalized nn7-derivations, ternary derivations, homomorphisms, and left/right centralizers (Hosseini, 2022). In this sense, the order-one strongly generalized derivation is aligned with a broader tradition in which Leibniz-type rules are encoded by finitely many product components.

A third adjacent notion is the generalized nn8-derivation. A usual nn9-derivation A\mathcal A0 satisfies

A\mathcal A1

and a generalized A\mathcal A2-derivation A\mathcal A3 associated with A\mathcal A4 satisfies

A\mathcal A5

That paper explicitly states that generalized A\mathcal A6-derivations are a A\mathcal A7-analogue of generalized derivations and notes that, when A\mathcal A8, the defining identity becomes the standard generalized derivation condition (Kaygorodov, 2011). This suggests that “strongly generalized derivation” is best read as one member of a wider Leibniz-type hierarchy rather than as a universally standardized term.

Several later papers do not define “strongly generalized derivation” as a separate formal notion. Instead, they study generalized derivations subject to stronger-looking conditions, including range restrictions into radicals, A\mathcal A9-centralizing and B\mathcal B0-commuting constraints, square-closure conditions such as B\mathcal B1 again being a generalized derivation, or additive decompositions into quasiderivation and quasicentroid parts (Esfahani et al., 2022, Bai et al., 2015, Zhou et al., 2014). In those settings, the strengthening is structural rather than terminological.

3. Automatic continuity on Banach algebras and B\mathcal B2-algebras

The main analytic development of the subject concerns automatic continuity. In the order-one setting on algebras, one of the earliest systematic results shows that if B\mathcal B3 and B\mathcal B4 are complex algebras, B\mathcal B5 is simple and unital, and B\mathcal B6 is a B\mathcal B7-derivation such that for some character B\mathcal B8,

B\mathcal B9

for some nn0, then

nn1

If nn2 and nn3 are normed algebras, then nn4 are continuous (Hosseini et al., 2023).

On operator algebras, a nn5-nn6-derivation

nn7

from a unital nn8-subalgebra nn9 into Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],00 is automatically continuous under explicit compatibility hypotheses. One version assumes Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],01,

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],02

and that Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],03 is Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],04-continuous; a second version assumes Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],05,

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],06

and that Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],07 is Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],08-continuous (Hosseini et al., 2023). Closely related results show that if

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],09

then on a unital Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],10-algebra Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],11 are generalized derivations and are automatically continuous in the Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],12-case and in the commutative case; on a unital algebra, Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],13 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],14 are generalized derivations, and if every derivation on the algebra is continuous, then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],15 are continuous (Hosseini et al., 2023).

Separating-space arguments extend these conclusions. If Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],16 is a Banach algebra, Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],17 a simple Banach algebra, and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],18 is both a continuous Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],19-derivation and a continuous Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],20-derivation, with Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],21 continuous and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],22 surjective, then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],23 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],24 are continuous, or else Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],25 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],26. If Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],27 is semiprime and either Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],28 is surjective with Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],29 continuous, or Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],30 is continuous with Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],31 surjective, then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],32 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],33 are continuous (Hosseini et al., 2023).

A later Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],34-algebra theorem shifts the codomain to a Banach Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],35-bimodule Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],36. Let Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],37 be a Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],38-algebra, Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],39 a Banach algebra, and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],40 an Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],41-derivation. If Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],42 are linear, Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],43 are continuous at Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],44, and one has either

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],45

or

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],46

for all Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],47, then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],48 is automatically continuous (Hosseini, 8 Sep 2025). Corollaries sharpen this in three directions: if at least one of Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],49 is a homomorphism, then every Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],50-derivation is continuous; if the separating-space annihilators

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],51

then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],52 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],53 are also continuous; and if Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],54 with Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],55 surjective and continuous at Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],56, then Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],57 are continuous (Hosseini, 8 Sep 2025).

These theorems place strongly generalized derivations in the same automatic-continuity lineage as Sakai’s continuity of derivations on Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],58-algebras, Ringrose’s continuity of bimodule derivations, and Johnson–Sinclair continuity on semisimple Banach algebras. The precise novelty is that continuity is forced for the asymmetric two-term identity

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],59

under mild algebraic side conditions rather than a classical Leibniz rule (Hosseini, 8 Sep 2025).

4. Decomposition phenomena in nonassociative, Hom-, and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],60-ary settings

A recurrent theme in nonassociative derivation theory is that generalized derivations admit a decomposition into a quasiderivation part and a centroid-like part. In Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],61-Lie algebras, a generalized derivation is a linear map Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],62 for which there exist Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],63 such that

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],64

The central structural theorem is

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],65

where Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],66 is the quasiderivation algebra and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],67 is the quasicentroid. The paper also proves that Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],68 and that quasiderivations embed as derivations in the larger algebra

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],69

via an explicit map Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],70 (Bai et al., 2015).

Exactly the same decomposition appears in multiplicative Hom-Jordan algebras: Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],71 There, generalized Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],72-derivations, quasiderivations, centroids, quasicentroids, and central derivations form a hierarchy

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],73

with

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],74

The paper further proves that quasiderivations can be embedded as derivations in a larger Hom-Jordan algebra Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],75 (Yao et al., 2019).

For multiplicative Hom-Lie superalgebras, the corresponding statement is again

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],76

The paper establishes closure properties such as Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],77 and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],78, and it embeds Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],79 into Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],80 for a suitable larger Hom-Lie superalgebra Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],81. If Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],82 is surjective and Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],83, then

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],84

(Zhou et al., 2014).

The same structural pattern extends to other nonassociative categories with variations in strength. For Lie triple systems,

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],85

and quasiderivations embed into derivations of a larger Lie triple system Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],86; if Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],87, then

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],88

(Zhou et al., 2014). For color Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],89-ary Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],90-algebras, the hierarchy

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],91

holds as well, and in the (anti)commutative case one has

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],92

with a direct-sum description

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],93

when the center vanishes (Kaygorodov et al., 2015).

These decomposition theorems do not usually employ the exact phrase “strongly generalized derivation.” A plausible implication is that, in nonassociative settings, the “strongly generalized” content is often encoded not by a new product formula but by a structural theorem identifying generalized derivations with sums of quasiderivation and quasicentroid-type components.

5. Banach-algebra generalized derivations under radical and centralizing constraints

A distinct but closely related direction studies generalized derivations on Banach algebras under strong spectral and radical hypotheses. Let Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],94 be a Banach algebra satisfying

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],95

For a derivation Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],96, one then has

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],97

As a consequence,

Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],98

and every derivation is spectrally infinitesimal: Dn(ab)=k=1n[Ek(a)Fk(b)+Gk(a)Hk(b)],D_n(ab)=\sum_{k=1}^{n}\bigl[E_k(a)F_k(b)+G_k(a)H_k(b)\bigr],99 These are the starting points for the paper’s analysis of generalized derivations $1$00 with

$1$01

(Esfahani et al., 2022).

If $1$02 has a right identity, the paper proves the equivalence

$1$03

Hence, in this setting, the only generalized derivations whose range lies in the radical are the derivations themselves. Under the same assumption, every generalized derivation is spectrally bounded: $1$04 This is one of the clearest examples in which a “stronger” generalized-derivation property collapses the operator back to an ordinary derivation (Esfahani et al., 2022).

The paper also studies $1$05-centralizing and $1$06-commuting generalized derivations. For $1$07,

$1$08

If $1$09 has a right identity and $1$10 is a generalized derivation, then the following are equivalent: $1$11 The associated set $1$12 of centralizing generalized derivations is a Banach algebra, and

$1$13

Thus centralizing generalized derivations are parametrized by the radical quotient (Esfahani et al., 2022).

A further strengthening asks when the square again defines a generalized derivation. If $1$14 is a generalized derivation and $1$15 has a right identity, then the following are equivalent: $1$16

$1$17

and

$1$18

The proof uses the computation

$1$19

so the mixed term $1$20 must vanish (Esfahani et al., 2022). This criterion is especially close in spirit to what some authors informally have in mind when speaking of stronger generalized-derivation conditions.

The same paper applies these results to group-related Banach algebras. For $1$21 when $1$22 is discrete amenable, for $1$23 when $1$24 is abelian non-discrete, and for certain introverted subspaces $1$25, the standing hypotheses

$1$26

hold, and the generalized-derivation theorems above apply (Esfahani et al., 2022).

6. Higher-order Leibniz formulas, rigidity examples, and geometric extensions

One of the broadest conceptual messages in the literature is that generalized derivation identities admit higher-iterate Leibniz formulas. For an ordinary derivation,

$1$27

For an $1$28-derivation $1$29 with $1$30,

$1$31

For a $1$32-derivation under $1$33,

$1$34

Without commutativity assumptions, the same paper derives a fully general formula using a non-commutative Newton expansion and the $1$35-product (Hosseini, 2022). These results do not define strongly generalized derivations, but they show that generalized product decompositions remain stable under iteration in a binomial or noncommutative-binomial form.

Rigidity can be equally important. For generalized shifts on $1$36, the restriction $1$37 is a $1$38-derivation if and only if there exists

$1$39

such that

$1$40

It is a $1$41-derivation if and only if

$1$42

It is not a Jordan derivation and not a Jordan triple derivation, and

$1$43

This is a particularly sharp example of how generalized-derivation behavior can force an operator to be trivial or identity-like (Arzanesh et al., 2021).

Generalized derivations also support extensions beyond pure algebra. For the commutative algebra $1$44 on a Lorentzian manifold $1$45 of dimension $1$46,

$1$47

The extra basis element is denoted

$1$48

so the generalized derivation module has dimension $1$49. In the corresponding geometry, the special metric ansatz with

$1$50

leads to a generalized Einstein–Hilbert action that reduces, for

$1$51

to the O’Hanlon action

$1$52

The paper also shows that the generalized Einstein equations with vanishing matter source are equivalent to a Kaluza–Klein theory satisfying the modified cylinder condition

$1$53

with a noncompact extra dimension (Heller et al., 2013). Although this is a theory of generalized derivations rather than strongly generalized derivations in the modern order-$1$54 sense, it demonstrates the conceptual breadth of derivation enlargements based on generalized Leibniz rules.

Taken together, these results show that “strongly generalized derivation” names a concrete modern definition, but also sits inside a larger mathematical landscape. In associative operator theory it is an order-$1$55 finite-sum Leibniz scheme with strong automatic continuity properties; in Banach-algebra theory it is mirrored by restrictive spectral, centralizing, and square-closure conditions on generalized derivations; and in nonassociative settings it is approached through decomposition theorems of the form $1$56 or $1$57.

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