Books as well as numerous articles have been written about hydrogen pa
ssivation in classical semiconductors such as Si and GaAs. The subject
has gained a renewed interest recently since hydrogen is widely consi
dered to saturate the hole conductivity of the wide bandgap semiconduc
tors GaN and ZnSe which are currently most promising for blue light em
itting devices. Other group-I impurities are capable of compensating t
he electrical conductivity of semiconductors both through directly neu
tralising (passivating) the impurity or providing space charge of pola
rity opposite to that of the dominating one. The paper reviews the sim
ilarities and differences between hydrogen and its light metallic neig
hbour in the periodic table, lithium. Also we provide a comparison wit
h the heavier interstitial copper which is known for its ability to pa
ssivate shallow accepters. Finally fundamental differences between sha
llow-level and deep level passivation will be addressed.