Influence of dynamical dipolar coupling on spin-torque-induced excitations in a magnetic tunnel junction nanopillar J. Appl. Phys. 111, 07C906 (2012) Quasi-omnidirectional electrical spectrometer for studying spin dynamics in magnetic tunnel junctions Rev. Sci. Instrum. 83, 024710 (2012) Thermal-magnetic-electric oscillator based on spin-valve effect J. Appl. Phys. 111, 044315 (2012) Dependence of spin-transfer switching characteristics in magnetic tunnel junctions with synthetic free layers on coupling strength J. Appl. Phys. 111, 07C905 (2012) Electrical manipulation of spin polarization and generation of giant spin current using multi terminal spin injectors J. Appl. Phys. 111, 07C505 (2012) Additional information on J. Appl. Phys. FeCoV/TiN x and FeCoV/Ti multilayers having t FeCoV ϭ30-700 Å prepared by dc magnetron sputtering are investigated by x-ray diffraction, stress, and magnetization measurements. The x-ray diffraction data of the FeCoV/TiN x system show the presence of interstitial N atoms in the FeCoV layers due to reactive sputtering of Ti with nitrogen. The interstitial N causes an expansion of the FeCoV lattice in FeCoV/TiN x for small t FeCoV . However, for the samples with large t FeCoV , no lattice expansion is observed. In addition to the lattice expansion caused by the intake of N atoms, a change in the crystalline texture of FeCoV layers is also observed as indicated by the enhancement of the FeCoV͑200͒ peaks. The magnetic hysteresis measurements on the samples show that the easy direction of magnetization lies in the plane of the layers. They further show that there are easy and hard axes of magnetization within the plane of the FeCoV layers. The stress anisotropy present in the plane of the samples induces a magnetic anisotropy through magnetostrictive effects leading to the formation of the in-plane easy axis. The hysteresis and stress measurements carried out on these samples clearly show the influence of N on the in-plane magnetic anisotropy. The magnetoelastic energy in the case of the FeCoV/TiN x system, calculated from the stress data and from the magnetization measurements as a function of t FeCoV is found to agree over a large range of thickness, whereas the curves deviate significantly for small layer thickness. This deviation may be due to the role of the FeCoVN x phase. Hysteresis measurements also show that the remanence is about 95% for all the samples of the FeCoV/TiN x system. In contrast, the coercivity increases linearly with increasing t FeCoV in this system. The coercivity of the FeCoV/Ti system is larger and increases more rapidly with t FeCoV , as compared with the FeCoV/TiN x system. This behavior is attributed to a smaller grain size in the FeCoV/TiN x system due to the reactive sputtering of the Ti layers. However, there is no significant influence of N on the saturation magnetization of both systems.