The Padmakar-Ivan (PI) index is a Wiener-Szeged-like topological index which reflects certain structural features of organic molecules. The PI index of a graph G is the sum of all edges uv of G of the number of edges which are not equidistant from the vertices u and v. In this paper we obtain the second and third extremals of catacondensed hexagonal systems with respect to the PI index.
YARAHMADI, Z., & MORADI, S. (2010). Second and Third Extremals of Catacondensed Hexagonal Systems with Respect to the PI Index. Iranian Journal of Mathematical Chemistry, 1(Issue 1 (Special Issue on the Role of PI Index in Nanotechnology)), 95-103. doi: 10.22052/ijmc.2010.5139
MLA
Z. YARAHMADI; S. MORADI. "Second and Third Extremals of Catacondensed Hexagonal Systems with Respect to the PI Index", Iranian Journal of Mathematical Chemistry, 1, Issue 1 (Special Issue on the Role of PI Index in Nanotechnology), 2010, 95-103. doi: 10.22052/ijmc.2010.5139
HARVARD
YARAHMADI, Z., MORADI, S. (2010). 'Second and Third Extremals of Catacondensed Hexagonal Systems with Respect to the PI Index', Iranian Journal of Mathematical Chemistry, 1(Issue 1 (Special Issue on the Role of PI Index in Nanotechnology)), pp. 95-103. doi: 10.22052/ijmc.2010.5139
VANCOUVER
YARAHMADI, Z., MORADI, S. Second and Third Extremals of Catacondensed Hexagonal Systems with Respect to the PI Index. Iranian Journal of Mathematical Chemistry, 2010; 1(Issue 1 (Special Issue on the Role of PI Index in Nanotechnology)): 95-103. doi: 10.22052/ijmc.2010.5139