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copernicus1
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Sometimes we see the wave function broken into specific parts, like $$\psi_{\rm total}=\psi_{\rm space}\psi_{\rm spin}\psi_{\rm isospin}.$$ What determines which parts you include in writing down the wavefunction? For instance, why or why wouldn't we include the isospin part? This has important consequences because each part has a symmetry and has implications when trying to construct wavefunctions for identical bosons or fermions.