Articles you may be interested inTunneling field-effect transistor with Ge/In0.53Ga0.47As heterostructure as tunneling junction J. Appl. Phys. 113, 094502 (2013); 10.1063/1.4794010 Band offset determination of mixed As/Sb type-II staggered gap heterostructure for n-channel tunnel field effect transistor application J. Appl. Phys. 113, 024319 (2013); 10.1063/1.4775606 Size, composition, and doping effects on In(Ga)As nanowire/Si tunnel diodes probed by conductive atomic force microscopy Appl. Phys. Lett. 101, 233102 (2012); 10.1063/1.4768001Defect assistant band alignment transition from staggered to broken gap in mixed As/Sb tunnel field effect transistor heterostructureWe use the envelope function formalism ͓M. G. Burt, J. Phys. Condens. Matter 4, 6651 ͑1992͔͒ with the rigorous boundary conditions ͓B. A. Foreman, Phys. Rev. B 48, 4964 ͑1993͔͒ to analyze the tunneling properties of holes across an abrupt InP/In 0.53 Ga 0.47 As heterojunction. We compare our results to those derived with boundary conditions obtained from an ad hoc ''symmetrized'' form of Burt's Hamiltonian. Our analysis includes the coupling between heavy, light, and spin-orbit bands. The percentage difference between the tunneling coefficients of heavy and light holes calculated in the two approaches increases ͑up to a maximum value of 30%͒ with the magnitude of the hole wave vector component parallel to the heterointerface. In addition, the tunneling coefficients of holes are found to be quite sensitive to the orientation of the hole wave vector parallel to the heterointerface. This sensitivity is particularly noticeable for large values of the hole transverse wave vector.