(born March 13, 1899, Middletown, Conn., U.S.—died Oct. 27, 1980, Cambridge, Mass.) American physicist and mathematician who shared the Nobel Prize for Physics in 1977 with Philip W. Anderson and Sir Nevill F. Mott.
The prize honoured Van Vleck's contributions to the understanding of the behaviour of electrons in magnetic, noncrystalline solid materials.
Educated at the University of Wisconsin, Madison, and at Harvard University, where he received his Ph.D. in 1922, Van Vleck joined the faculty of the University of Minnesota, Minneapolis, in 1924. He taught at Wisconsin from 1928 to 1934, and he then went to Harvard, where he eventually served as chairman of the physics department (1945–49), dean of engineering and applied physics (1951–57), and Hollis professor of mathematics and natural philosophy (1951–69).
Van Vleck developed during the early 1930s the first fully articulated quantum mechanical theory of magnetism. Later he was a chief architect of the ligand field theory of molecular bonding. He contributed also to studies of the spectra of free molecules, of paramagnetic relaxation, and other topics. His publications include Quantum Principles and Line Spectra (1926) and The Theory of Electric and Magnetic Susceptibilities (1932).
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