@mmoderwell

Fe8Co3Mn2N1 (requested SG: P4/mmm #123, calculated SG: P1 #1, optimized: 395 steps, cell relaxed (isotropic))

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); imaginary modes detected; min freq = -2.04 THz

Phase diagram of MnFe4Co4N; eabovehull: 0.505384 eV/atom; predicted_stable: False

Fe4Co4Mn1N1 (requested space group: P4mm #99, optimized: 51 steps, cell relaxed (isotropic))

Phase diagram of CrFe6Co3N; eabovehull: 1.340589 eV/atom; predicted_stable: False

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); imaginary modes detected; min freq = -8.02 THz

Fe6Co3Cr1N1.5 (requested SG: P6/m #175, calculated SG: P1 #1, optimized: 400 steps, cell relaxed (isotropic))

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); imaginary modes detected; min freq = -2.74 THz

Phase diagram of MnFe4Co5N2; eabovehull: 0.317240 eV/atom; predicted_stable: False

Fe4Co5Mn1N2 (requested SG: P-3m1 #164, calculated SG: P1 #1, optimized: 400 steps, cell relaxed (isotropic))

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); no imaginary modes; min freq = -0.03 THz

Phase diagram of MnFe5(Co2N)2; eabovehull: 0.117499 eV/atom; predicted_stable: False

Fe5Co4Mn1N2 (requested SG: Pmmm #47, calculated SG: P1 #1, optimized: 253 steps, cell relaxed (isotropic))

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); no imaginary modes; min freq = -0.09 THz

Phase diagram of MnFe5(Co2N)2; eabovehull: 0.179289 eV/atom; predicted_stable: False

Fe5Co4Mn1N2 (requested space group: P1 #1, optimized: 233 steps, cell relaxed (isotropic))

Phonon band structure (supercell [2, 2, 2], Δ=0.01 Å); no imaginary modes; min freq = -0.07 THz

Phase diagram of Ti2MnFe4Co3B2; eabovehull: 0.237298 eV/atom; predicted_stable: False

Fe4Co3Mn1Ti2B2 (requested SG: P6 #168, calculated SG: P1 #1, optimized: 189 steps, cell relaxed (isotropic))

Phase diagram of Ti2MnFe4Co3B2; eabovehull: 0.205637 eV/atom; predicted_stable: False