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For a harmonic oscillator perturbed by H′=λx4H' = \lambda x^4, the first-order energy shift is E(1)=λ⟨n∣x4∣n⟩E^{(1)} = \lambda \langle n|x^4|n\rangle, where (in the convention used here) ⟨n∣x4∣n⟩=3(2n2+2n+1)\langle n|x^4|n\rangle = 3(2n^2 + 2n + 1). For the ground state n=0n = 0 with λ=1\lambda = 1, what is E(1)E^{(1)}?