The decrease in atomic radii from left to right across the first row of the d-block is small and irregular. In the first row of the d-block, as the nuclear charge increases across the period, each additional electron enters the penultimate 3d orbital which increases the shielding experienced by the 4s electrons. This results in a relatively small difference in the effective nuclear charge as the shielding effect nullifies, to a large extent, the increase in nuclear charge. As the atomic radius decreases with increasing relative atomic mass, the density increases.
The first ionization energy increases from left to right across the first row of the d-block. In the first row of the d-block, as the nuclear charge increases each additional electron enters the penultimate 3d orbital. These 3d electrons efficiently shields the 4s electrons from the nucleus. Thus the increase nuclear attraction for the outer 4s electrons is minimal across the period. This results in relatively small changes in the energy required to remove an outer 4s electron.
The d-block elements form metallic structures. Electrons are available from both 4s and 3d orbitals for delocalization to form metallic bonds. This results in relatively high melting points and boiling points. The melting and boiling points drop at Mn (half filled) and Zn (filled). The d orbitals make the electrons less available for metallic bonding.
orbitals close to the ligand are pushed to slightly higher energy levels than those farther away. The orbitals split into two groups. When an electron moves from a D orbital of lower energy to orbital higher energy, light is absorbed in the visible region of the spectrum. The frequency of light absorb depends on the energy difference between the split the levels. Different ligands split the D energy levels by a different amount. So different ligands different colors to be absorbed.
Formed with the transition element ions because the d electrons in transition elements do not shield the outer electrons very well from the nuclear charge