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A variational Monte Carlo method is used to generate sets of orthogonal trialfunctions, Psi_T(J^pi,T), for given quantum numbers in various light p-shellnuclei. These Psi_T are then used as input to Green's function Monte Carlocalculations of first, second, and higher excited (J^pi,T) states. Realistictwo- and three-nucleon interactions are used. We find that if the physicalexcited state is reasonably narrow, the GFMC energy converges to a stableresult. With the combined Argonne v_18 two-nucleon and Illinois-2 three-nucleoninteractions, the results for many second and higher states in A = 6--8 nucleiare close to the experimental values.Comment: Revised version with minor changes as accepted by Phys. Rev. C. 11  page

physical review. c. nuclear physics/physical review. c, nuclear physics

Quantum Monte Carlo calculations of excited states in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mn>6</mml:mn><mml:mo>–</mml:mo><mml:mn>8</mml:mn></mml:mrow></mml:math>nuclei

Quantum Monte Carlo calculations of excited states inA=6–8nuclei