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#! ROHF and UHF-B-CCD(T)/cc-pVDZ $^{3}B@@1$ CH2 single-point energy (fzc, MO-basis $\langle ab|cd \rangle$ )

molecule ch2 {
    0 3
    c
    h 1 r
    h 1 r 2 a
    r = 1.1
    a = 109.0
}

set {
   reference    uhf
   basis        cc-pVDZ
   freeze_core  true
}

energy("bccd(t)")

escf = -38.917378694797030 #TEST
ebccd = -39.030833895315020 #TEST
ebccd_t = -39.032691827829460 #TEST
compare_values(escf, get_variable("SCF TOTAL ENERGY"), 7, "SCF energy") #TEST
compare_values(ebccd, get_variable("CCSD TOTAL ENERGY"), 7, "B-CCD energy") #TEST
compare_values(ebccd_t, get_variable("CCSD(T) TOTAL ENERGY"), 7, "B-CCD(T) energy") #TEST


# We should obtain the same result as above, but start with different orbitals
# Energy will be slightly different as the core is frozen 
set {
   reference    rohf
}

energy("bccd(t)")
escf = -38.91341670976116 #TEST
ebccd = -39.030807046983838 #TEST
ebccd_t = -39.032665163463861 #TEST
compare_values(escf, get_variable("SCF TOTAL ENERGY"), 7, "SCF energy") #TEST
compare_values(ebccd, get_variable("CCSD TOTAL ENERGY"), 7, "B-CCD energy") #TEST
compare_values(ebccd_t, get_variable("CCSD(T) TOTAL ENERGY"), 7, "B-CCD(T) energy") #TEST