The solutions (χ nlm) of the Schrödinger equation for the hydrogen atom contain the term exp(imϕ). When m = 0, functions χ nlm are real, however, in the cases of m ≠ 0, functions χ nlm are complex. Probability density distribution of χ 320 , χ 32±1 , or χ 32±2 was sculptured in a glass block (Figure 1). Each picture is symmetric about the z axis. It was compared with 3-D isosurface model such as Figure 2. By taking linear combinations of χ 32+1 and χ 32−1 , it is known to obtain the real atomic orbitals χ 3dzx and χ 3dyz. Similarly, from χ 32±2 and χ 32−2 , the real atomic orbitals χ 3dx 2 −y 2 and χ 3dxy are obtained. In this paper, this mathematical process is graphically visualized (Figure 3). The "doughnut(s)" are sliced by plane(s) containing the z axis. The number of the plane(s) equals the |m| value. As the plane is a nodal plane, by rounding the edge and attaching positive or negative sign to each lobe, the familiar "clover" type orbital is obtained. Probability density distribution in the 3-dimensional representation of hydrogen four 3d orbitals thus obtained was sculptured in a glass block (Figure 4). Isosurface models (Figure 3, bottom) can hardly show the entire region where an electron can be found. On the other hand, in the diagram of probability density distribution models (Figure 4), an electron is found everywhere around the nucleus. Number of conical nodes together with planar nodes in hydrogen 3d atomic orbitals is summarized in Table 1.