We describe new constructions of graphs which exhibit perfect state transfer on continuoustime quantum walks. Our constructions are based on variants of the double cones [8,3,2] and the Cartesian graph products (which includes the n-cube Q n ) [11]. Some of our results include:and H is a circulant with odd eigenvalues, their weak product G × H has perfect state transfer. Also, if H is a regular graph with perfect state transfer at time t H and G is a graph where t H |V H | Spec(G) ⊆ 2Zπ, their lexicographic product G[H] has perfect state transfer. For example, these imply Q 2n × H and G[Q n ] have perfect state transfer, whenever H is any circulant with odd eigenvalues and G is any integral graph, for integer n ≥ 2. These complement constructions of perfect state transfer graphs based on Cartesian products. • The double cone K 2 +G on any connected graph G, has perfect state transfer if the weights of the cone edges are proportional to the Perron eigenvector of G. This generalizes results for double cone on regular graphs studied in [8, 3, 2].• For an infinite family G of regular graphs, there is a circulant connection so the graph K 1 + G • G + K 1 has perfect state transfer. In contrast, no perfect state transfer exists if a complete bipartite connection is used (even in the presence of weights) [2]. Moreover, we show that the cylindrical cone K 1 + G + K n + G + K 1 has no perfect state transfer, for any family G of regular graphs.We also describe a generalization of the path collapsing argument [10,11], which reduces questions about perfect state transfer to simpler (weighted) multigraphs, for graphs with equitable distance partitions. Our proofs exploit elementary spectral properties of the underlying graphs.Keywords: perfect state transfer, quantum walk, graph product, equitable partition.Recently, perfect state transfer in continuous-time quantum walks on graphs has received considerable attention. This is due to its potential applications for the transmission of quantum information over quantum networks. It was originally introduced by Bose [7] in the context of quantum walks on linear spin chains or paths. Another reason for this strong interest is due to the universal property *