Leigh Page | |
---|---|
Born | October 13, 1884 New Jersey, USA |
Died | September 14, 1952 New Haven, Connecticut, USA |
(aged 67)
Nationality | United States |
Fields | Physicist |
Institutions | Yale University |
Alma mater | Yale University |
Doctoral advisor | Henry Andrews Bumstead[1] |
Doctoral students | John Stuart Foster |
Known for | Conformal Invariance |
Leigh Page (October 13, 1884, New Jersey – September 14, 1952, New Haven, Connecticut) developed the theory of conformal invariance originally suggested by Harry Bateman. Chairman of Mathematical Physics at the Sloane Physics Laboratory of Yale University for over three decades, he is the namesake of Yale’s prestigious Leigh Page Prize Lectures.[2]
Contents |
Leigh Page was born October 13, 1884 in South Orange, New Jersey[3] to Edward Day Page & Nina Lee. He came to the Sheffield Scientific School “Sheff” at Yale in 1909 as an assistant professor in drawing and graduate student under Henry Andrews Bumstead.[1] He switched to physics in 1912, was appointed assistant professor of physics in 1916, and professor of mathematical physics in 1922, where he remained until his death in 1952. Devoting most of his time to teaching, Page conducted research and wrote several textbooks,[4][5][6][7] which appeared in various editions, often with the assistance of colleague Norman I. Adams, Jr. In 1967 Yale University sponsored the first of his namesake Leigh Page Prize Lectures, an honor since bestowed on several Nobel laureates and other notable physicists.
Page derived a complete electromagnetic theory, including Maxwell's equations, from only Coulomb's law and the Lorentz transformation.[8] His “emission theory” successfully explained blackbody radiation and other phenomena in electrodynamic terms,[9][10][11] but was eventually abandoned in favor of later theories of quantum mechanics.
Along with Norman I. Adams, Page established the relation between the “conformal transformation” and a constant relative acceleration.[12][13] This theory, known as “conformal relativity”, “conformal invariance”, or “conformal field theory”, is applied today as an invariance of gauge field theories for both electromagnetic and strong interactions. The symmetry of “conformal invariance” provides a valid approximation at very high energies or short distances when particle masses can safely be ignored.