  Hidden-color configurations are a key prediction of QCD with important
physical consequences. In this work we examine a QCD color-singlet
configuration in nuclei formed by combining six scalar $[u d]$ diquarks in a
strongly bound $\rm SU(3)_C$ channel. The resulting hexadiquark state is a
charge-2, spin-0, baryon number-4, isospin-0, color-singlet state. It
contributes to alpha clustering in light nuclei and to the additional binding
energy not saturated by ordinary nuclear forces in \he as well as the
alpha-nuclei sequence of interest for nuclear astrophysics. We show that the
strongly bound combination of six scalar isospin-0 $[ud]$ diquarks within the
nuclear wave function - relative to free nucleons - provides a natural
explanation of the EMC effect measured by the CLAS collaboration's comparison
of nuclear parton distribution function ratios for a large range of nuclei.
These experiments confirmed that the EMC effect; i.e., the distortion of quark
distributions within nuclei, is dominantly identified with the dynamics of
neutron-proton (``isophobic'') short-range correlations within the nuclear wave
function rather than proton-proton or neutron-neutron correlations.
