The second-order integrable Killing tensor with simple eigenvalues and vanishing Haantjes torsion is the key ingredient in construction of Liouville integrable systems of Stäckel type. We present two examples of the integrable systems on three-dimensional Euclidean space associated with the second-order Killing tensors possessing nontrivial torsion. Integrals of motion for these integrable systems are the second-and fourth-order polynomials in momenta, which are constructed using a special family of the Killing tensors. may be used as canonical coordinates for K in the domain where they are real, distinct, and functionally independent. In this domainand any distribution spanned by the n − 1 eigenvectors X i is completely integrable. Here N denotes the skew-symmetric (1, 2) Nijenhuis torsion tensor field associated with Kwhere X and Y are arbitrary vector fields and [. , .] denotes the commutator of two vector fields. This construction of the integrable distributions as orthogonal complements of each eigenvector field X i was slightly modified by Nijenhuis [29] and Haantjes [21] for the case where they enable K to possess torsion, but in a controlled manner. In this case, condition (1.1) is replaced by the weaker conditionwhere H is the skew-symmetric (1, 2) Haantjes tensor associated with K(1.2)The vanishing of the Haantjes tensor H is equivalent to the condition that the eigenvector fields of K commute after a reparameterization, and equivalent to the condition that any collection of n − 1 eigenvector fields is integrable. The algebraic relations between the Nijenhuis and Haantjes tensors are discussed in [10].