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Max-Born-Institut Berlin (MBI)

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i(pq - qp) = (h/2π),<br />

statistical<br />

of<br />

48<br />

<strong>Max</strong> <strong>Born</strong> • Paul Corkum<br />

In 1921, <strong>Max</strong> <strong>Born</strong> was appointed to a chair in Göttingen as the successor to Peter Debye.<br />

Together with James Franck, whose appointment to a post at Göttingen he made a precondition<br />

for accepting his own chair, and Robert Wichard Pohl, <strong>Born</strong> then became the founder of<br />

the famous Göttingen School. At this time <strong>Born</strong> began to concern himself with the quantum<br />

physics of atoms. Basic inadequacies had become apparent in Bohr’s treatment of the atom<br />

model. The conformity of quantum physics at the time with classical physics, maintained via<br />

the correspondence principle, had led to quantum rules that could be used to describe the simple<br />

hydrogen atom, but which already failed in their treatment of problems of even slightly<br />

greater complexity, such as the scattering of light and the influence of static magnetic and electric<br />

fields.<br />

The interest of <strong>Max</strong> <strong>Born</strong> and his colleagues in atomic physics was attracted by the lectures<br />

given by Niels Bohr in Göttingen in 1922. Initially, they sought a solution in Göttingen within<br />

the framework of many-body models oriented to classical physics. <strong>Born</strong>’s assistant, Werner Heisenberg,<br />

then succeeded in finding the solution during his famous trip to Heligoland in 1925.<br />

Heisenberg treated the spectral lines of the atom on the basis of a system of oscillators by<br />

replacing the classical amplitudes of the emitted radiation by quantum-theory amplitudes,<br />

which depend on two figures characterizing the transition from one state to another. He succeeded<br />

in transcribing Bohr’s quantum condition within the framework of the same assumptions<br />

and discovered that his formulation perfectly fulfilled the principle of the conservation of<br />

energy, which had been a problem for earlier treatments of semi-classical concepts.<br />

Fulfilling Ritz’s combination principle required the rule of noncommutative multiplication. After<br />

Heisenberg’s return from Heligoland, <strong>Born</strong> recognized that the result intuitively discovered by<br />

Heisenberg was the formation of a product of matrices. Today we know <strong>Max</strong> <strong>Born</strong>’s formulation,<br />

i(pq - qp) = (h/2π), which is also inscribed on his gravestone in Göttingen, in the form of<br />

Heisenberg’s commutation relations between the components of the operator of the space<br />

coordinate and the component of momentum. <strong>Born</strong> thus became the father of the matrix formulation<br />

of quantum theory.<br />

In the following years, <strong>Born</strong> devoted himself to the application of quantum mechanics to<br />

nonperiodic and time-dependent processes, especially of scattering theory. In 1933 he wrote<br />

his famous book on optics, which, when forced into exile in Edinburgh by the Nazis, he<br />

later revised with Emil Wolf and republished in 1959 as “The Principles of Optics”. This book,<br />

which we still use as a reference in my institute even today, has since become a standard<br />

work of modern optics.

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