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The total energies and various bound state properties of the excited $2^1S(L = 0)-{}^{\infty}{}^4{}^3$He atoms, are determined to very high numerical accuracy. The convergence of the results obtained for some electron-nuclear and electron-electron expectation values and, in particular, for the electron-nuclear and electron-electron cusp values, is discussed. The field component of the isotope shift and lowest order QED correction are estimated for the states in the He and He atoms. We also apply our highly accurate methods to numerical computations of the excited states (for = 3 and 4) in two-electron atomic systems.

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