Let T be a δ-Jordan Lie supertriple system. We first introduce the notions of generalized derivations and representations of T and present some properties. Also, we study the low dimension cohomology and the coboundary operator of T , and then we investigate the deformations and Nijenhuis operators of T by choosing some suitable cohomology.In [13], Okubo and Kamiya introduced the notion of δ-Jordan Lie triple system, where δ = ±1, which is a generalization of both Lie triple systems (δ = 1) and Jordan Lie triple systems (δ = −1). Later, Kamiya and Okubo [14] studied a construction of simple Jordan superalgebras from certain triple systems. Recently, Ma and Chen [7] discussed the cohomology theory, the deformations, Nijenhuis operators, abelian extensions and T * -extensions of δ-Jordan Lie triple system.As a natural generalization of Lie triple systems, Okubo [11] introduced the notion of Lie supertriple systems in the study of Yang-Baxter equations. Lie supertriple systems have many applications in high energy physics, and many important results on Lie supertriple systems have been obtained, see [8,11,14,15]. In [13], Okubo and Kamiya introduced the notion of δ-Jordan Lie supertriple system (they still call it Jordan Lie triple system), they presented some nontrivial examples and discussed their quasiclassical property. In the present paper, we hope to study generalized derivations, cohomology theories and deformations of δ-Jordan Lie supertriple systems.This paper is organized as follows. In Section 2, we recall the definition of δ-Jordan Lie supertriple systems and construct a kind of δ-Jordan Lie supertriple systems. Also, we study generalized derivation algebra of a δ-Jordan Lie supertriple system. In Section 3, we introduce notions of the representation and low dimension cohomology of a δ-Jordan Lie supertriple system. In Section 4, we consider the theory of deformations of a δ-Jordan Lie supertriple system by choosing a suitable cohomology. In Section 5, we study Nijenhuis operators for a δ-Jordan Lie supertriple system to describe trivial deformations.Remark 2.2. Clearly, T 0 is an ordinary δ-Jordan Lie triple system in [7]. Especially, the case of δ = 1 defines a Lie supertriple system while the other case of δ = −1 may be termed an anti Lie supertriple system as in [9]. Example 2.3. ([13]) Let (T, [·, ·]) be a δ-Jordan Lie superalgebra. Then (T, [·, ·, ·]) becomes a δ-Jordan Lie supertriple system, where [a, b, c] = [[a, b], c], for all a, b, c ∈ T .Example 2.4. Let T be a δ-Jordan Lie supertriple system and t an indeterminate. SetDefinition 2.5. Let T be a δ-Jordn Lie supertriple system and k a nonnegative integer. A homogeneous linear map D : T → T is said to be a homogeneous k-derivation of T if it satisfiesfor all a, b, c ∈ T , where |D| denotes the degree of D.We denote by Der(T ) = k≥0 Der k (T ), where Der k (T ) is the set of all homogeneous k-derivations of T . Obviously, Der(T ) is a subalgebra of End(T ) and has a normal Lie superalgebra structure via the bracket productDefinition 2.6. Let ...