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Jan Korringa

Jan Korringa is a physics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand Jan Korringa rather than just read about it. In short: 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.

Jan Korringa — main illustration
Jan Korringa — illustration

Key takeaways

  • Jan Korringa belongs to physics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect Jan Korringa to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of Jan Korringa from memory before moving on to harder problems.

Reference excerpt

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.

Education and career Korringa received his undergraduate degree from the Delft University of Technology. 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. 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). 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. 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. In 1962, he was awarded a Guggenheim Foundation fellowship that he used for a sabbatical at the University of Besançon in France. 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. 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. 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. 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.

References

Illustrations

Jan Korringa illustration

Worked examples

Example 1 — a first encounter with Jan Korringa

Start with the simplest possible case. Write down what Jan Korringa claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In physics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to Jan Korringa before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about Jan Korringa ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of Jan Korringa

In research
Jan Korringa appears in physics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses Jan Korringa in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
Jan Korringa is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1915 births, 2015 deaths, 20th-century Dutch physicists, so understanding it makes those chapters shorter.
In everyday life
Look for Jan Korringa outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.

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How to study Jan Korringa in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Jan Korringa means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain Jan Korringa out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Jan Korringa in simple terms?

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.

Why does Jan Korringa matter?

Because it connects several physics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study Jan Korringa?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on Jan Korringa.

Tags

  • 1915 births
  • 2015 deaths
  • 20th-century Dutch physicists
  • Academic staff of Leiden University
  • American men centenarians
  • Delft University of Technology alumni
  • Dutch emigrants to the United States
  • Dutch men centenarians
  • Fellows of the American Physical Society
  • Ohio State University faculty
  • People from Heemstede
  • Theoretical physicists

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