Excitation of isobaric analog states from <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mo>(</mml:mo><mml:mmultiscripts><mml:mi>He</mml:mi><mml:mprescripts /><mml:none /><mml:mn>3</mml:mn></mml:mmultiscripts><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math> …

Differential cross sections of $(p,n)$ and $(^{3}\mathrm{He},t)$ charge-exchange reactions leading to the excitation isobaric analog state (IAS) target nucleus are calculated with distorted wave Born approximation. The $G$-matrix double-folding method is employed determine nucleus-nucleus optical potential within framework Lane model. $G$ matrices obtained from a Brueckner-Hartree-Fock calculation using Argonne Av18 nucleon-nucleon potential. Target densities have been taken Skyrme-Hartree-Fock calculations which predict values for neutron skin thickness heavy nuclei compatible current existing data. Calculations compared experimental data $(p,n)\mathrm{IAS}$ on $^{14}\mathrm{C}$ at ${E}_{\mathrm{lab}}=135$ MeV $^{48}\mathrm{Ca}$ ${E}_{\mathrm{lab}}=134$ ${E}_{\mathrm{lab}}=160$ MeV, $(^{3}\mathrm{He},t)\mathrm{IAS}$ $^{58}\mathrm{Ni},$ $^{90}\mathrm{Zr},$ $^{208}\mathrm{Pb}$ ${E}_{\mathrm{lab}}=420$ MeV. Experimental results well described without necessity any rescaling strength A clear improvement in description differential $^{58}\mathrm{Ni}$ $^{90}\mathrm{Zr}$ targets found when excess density used transition densities. Our show that isospin dependences play non-negligible role