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Superconductivity up to 30 K in charge neutrally doped BaFe2[As(1-x)P(x)]2has been ascribed to chemical pressure, caused by the shrinking unit cell. Butthe latter induces no superconductivity in [Ba(1-x)Sr(x)]Fe2As2 in spite of thesame volume range. We show that the spin-density-wave (SDW) state of BaFe2As2becomes suppressed in BaFe2[As(1-x)P(x)]2 by a subtle reorganization of thecrystal structure, where arsenic and phosphorus are located at differentcoordinates z(As), z(P). High-resolution X-ray diffraction experiments withBaFe2[As(1-x)P(x)]2 single crystals reveal almost unchanged Fe-P bonds, but acontraction of the Fe-As bonds, which remain nearly unchanged in[Ba(1-x)Sr(x)]Fe2As2. Since the Fe-As bond length is a gauge for the magneticmoment, our results show why the SDW is suppressed by P-, but not by Sr-doping.Only the Fe-P interaction increases the width of the iron 3d bands, whichdestabilizes the magnetic SDW ground state. The simultaneous contraction of theFe{As bonds is rather a consequence of the vanishing magnetism. Orderedstructure models of BaFe2[As(1-x)P(x)]2 obtained by DFT calculations agreeperfectly with the single-crystal X-ray structure determinations. Thecontraction of the Fe-As bonds saturates at doping levels above x = 0.3, whichcorrects the unreasonable linear decrease of the so-called pnictide height.

Different response of the crystal structure to isoelectronic doping in BaFe2[As(1-x)P(x)]2 and [Ba(1-x)Sr(x)]Fe2As2