Age, Biography and Wiki

Jan Korringa was born on 31 March, 1915 in Heemstede, Netherlands, is a Dutch-American physicist. Discover Jan Korringa's Biography, Age, Height, Physical Stats, Dating/Affairs, Family and career updates. Learn How rich is he in this year and how he spends money? Also learn how he earned most of networth at the age of 100 years old?

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Occupation Theoretical physicist
Age 100 years old
Zodiac Sign Aries
Born 31 March, 1915
Birthday 31 March
Birthplace Heemstede, Netherlands
Date of death 9 October, 2015
Died Place Laguna Beach, California, U.S
Nationality Netherlands

We recommend you to check the complete list of Famous People born on 31 March. He is a member of famous with the age 100 years old group.

Jan Korringa Height, Weight & Measurements

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Jan Korringa Net Worth

His net worth has been growing significantly in 2023-2024. So, how much is Jan Korringa worth at the age of 100 years old? Jan Korringa’s income source is mostly from being a successful . He is from Netherlands. We have estimated Jan Korringa's net worth, money, salary, income, and assets.

Net Worth in 2024 $1 Million - $5 Million
Salary in 2024 Under Review
Net Worth in 2023 Pending
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Timeline

1915

Jan Korringa (31 March 1915 – 9 October 2015) was a Dutch American theoretical physicist, specializing in theoretical condensed matter physics.

He also contributed to the KKR Method.

Korringa received his undergraduate degree from the Delft University of Technology.

1937

In 1937, Korringa went to Leiden University, Netherlands, to pursue graduate studies.

After the closure of Leiden University, Korringa returned to Delft University of Technology.

1942

In 1942, he gave a Doctor of Philosophy from Delft University of Technology and published his thesis, Onderzoekingen op het gebied algebraïsche optiek (Essays in the area of science optics).

1946

In 1946, Korringa became an associate professor at the University of Leiden.

He was a protégé of Hendrik Kramers, who had been the first protégé of Niels Bohr, and who was a large influence on his interest in quantum mechanics.

1947

In a 1947 paper, Korringa showed how multiple scattering theory (MST) could be used to find the energy as a function of wavevector for electrons in a periodic solid.

1950

In 1950, Korringa showed that the spin relaxation rate divided by the square of the magnetic resonance field shift (the Knight shift) obtained from an NMR experiment is equal to a constant, κ, times the temperature T. The magnitude of the Korringa constant κ and its possible deviation from a constant value is the signature of the effects of strong correlations in the electron gas.

1952

In 1952, Korringa went to the United States and accepted a full professorship at Ohio State University.

He was a consultant at Oak Ridge National Laboratory for many years.

During the summers, he collaborated with a group at Chevron Corporation that developed nuclear magnetic resonance logging.

1954

In 1954, Walter Kohn (a Nobel laureate) and Norman Rostoker (a nuclear physicist), derived the same equations using the Kohn variational method.

Two of Korringa's students, Sam Faulkner and Harold Davis, started a program at the Oak Ridge National Laboratory using the Korringa-Kohn-Rostoker (KKR) band-theory equations to calculate the properties of solids.

Korringa realized that his equations could be used to calculate the electronic states of non-periodic solids for which Bloch’s theorem does not hold.

1958

In 1958 he published an approach, now called the average t-matrix approximation, for calculating the electronic states in random substitutional alloys.

That work continued to evolve and was later connected to the higher-level theory called the Coherent Potential Approximation (CPA).

Balázs Győrffy and Malcolm Stocks combined it with the KKR theory to obtain the KKR–CPA method, which is presently used for alloy calculations.

Korringa’s MST is the basis for numerous theoretical developments, including the locally self-consistent multiple scattering theory developed by Malcolm Stocks and Yang Wang that can be used to obtain the electronic and magnetic states of any ordered or disordered solid.

1962

In 1962, he was awarded a Guggenheim Foundation fellowship that he used for a sabbatical at the University of Besançon in France.