An attosecond XUV or x-ray pump-control scheme for the electron-spectral-line profiles of Fano and Auger resonances is proposed and studied. A weak pump resonantly excites the atom and creates the resonance, and then a second strong attosecond control pulse resonantly coupling the resonance to an valance excited state is applied at different time delays ($\mathrm{\ensuremath{\Delta}}{t}_{21}$). Resonance with lifetimes ($1/\mathrm{\ensuremath{\Gamma}}$) much longer than the pulse duration ($\ensuremath{\tau}$) is studied. It is found that the dynamic variations of the electron spectra can be partitioned into two or three regions with respect to the time delays and pulse area of the control pulse: explicitly, the overlap region ($\mathrm{\ensuremath{\Delta}}{t}_{21}l\ensuremath{\sim}4\ensuremath{\tau}$) and analysis region ($\mathrm{\ensuremath{\Delta}}{t}_{21}g\ensuremath{\sim}4\ensuremath{\tau}$) in the case with a sub-$\ensuremath{\pi}$-control pulse; and the overlap region ($\mathrm{\ensuremath{\Delta}}{t}_{21}l\ensuremath{\sim}4\ensuremath{\tau}$), reverse region ($\ensuremath{\sim}4\ensuremath{\tau}l\mathrm{\ensuremath{\Delta}}{t}_{21}l\ensuremath{\sim}2/\mathrm{\ensuremath{\Gamma}}$), and analysis region ($\mathrm{\ensuremath{\Delta}}{t}_{21}g\ensuremath{\sim}2/\mathrm{\ensuremath{\Gamma}}$) in the case with a sub-$2\ensuremath{\pi}$-control pulse. In the case with a sub-$\ensuremath{\pi}$-control pulse, the electron spectral line profiles do not change too much and only the degrees of asymmetries of the spectra are reduced in the overlap region, while in the analysis region, the main profiles of the electron spectra are maintained but with modulation structures. In the case with a sub-$2\ensuremath{\pi}$-control pulse, the electron spectral line profiles totally reverse the asymmetries in the overlap region, while in the reverse region, the electron spectra keep the reversed asymmetries but with modulation structures, and the electron spectra pertain the modulation structures in the analysis region but with the main profiles reversed. All these dynamic features of the electron spectra can be fully understood with the help of an analytic theory, which is also fully presented based on the time-dependent perturbation theory.