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Rudolf Haag was born on 17 August, 1922 in Tübingen, Germany, is a German physicist. Discover Rudolf Haag'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 94 years old?

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Occupation N/A
Age 94 years old
Zodiac Sign Leo
Born 17 August, 1922
Birthday 17 August
Birthplace Tübingen, Germany
Date of death 2016
Died Place Neuhaus (Schliersee), Germany
Nationality Germany

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Rudolf Haag Height, Weight & Measurements

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Rudolf Haag Net Worth

His net worth has been growing significantly in 2023-2024. So, how much is Rudolf Haag worth at the age of 94 years old? Rudolf Haag’s income source is mostly from being a successful . He is from Germany. We have estimated Rudolf Haag's net worth, money, salary, income, and assets.

Net Worth in 2024 $1 Million - $5 Million
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1922

Rudolf Haag (17 August 1922 – 5 January 2016) was a German theoretical physicist, who mainly dealt with fundamental questions of quantum field theory.

He was one of the founders of the modern formulation of quantum field theory and he identified the formal structure in terms of the principle of locality and local observables.

He also made important advances in the foundations of quantum statistical mechanics.

Rudolf Haag was born on 17 August 1922, in Tübingen, a university town in the middle of Baden-Württemberg.

His family belonged to the cultured middle class.

Haag's mother was the writer and politician Anna Haag.

His father, Albert Haag, was a teacher of mathematics at a Gymnasium.

1939

After finishing high-school in 1939, he visited his sister in London shortly before the beginning of World War II.

He was interned as an enemy alien and spent the war in a camp of German civilians in Manitoba.

There he used his spare-time after the daily compulsory labour to study physics and mathematics as an autodidact.

1946

After the war, Haag returned to Germany and enrolled at the Technical University of Stuttgart in 1946, where he graduated as a physicist in 1948.

1948

In 1948, Haag married Käthe Fues, with whom he had four children, Albert, Friedrich, Elisabeth, and Ulrich.

After retirement, he moved together with his second wife Barbara Klie to Schliersee, a pastoral village in the Bavarian mountains.

1951

In 1951, he received his doctorate at the University of Munich under the supervision of Fritz Bopp and became his assistant until 1956.

1953

In April 1953, he joined the CERN theoretical study group in Copenhagen directed by Niels Bohr.

1954

After a year, he returned to his assistant position in Munich and completed the German habilitation in 1954.

1956

From 1956 to 1957 he worked with Werner Heisenberg at the Max Planck Institute for Physics in Göttingen.

1957

From 1957 to 1959, he was a visiting professor at Princeton University and from 1959 to 1960 he worked at the University of Marseille.

1960

He became a professor of Physics at the University of Illinois Urbana-Champaign in 1960.

1965

In 1965, he and Res Jost founded the journal Communications in Mathematical Physics.

1966

In 1966, he accepted the professorship position for theoretical physics at the University of Hamburg, where he stayed until he retired in 1987.

After retirement, he worked on the concept of the quantum physical event.

Haag developed an interest in music at an early age.

He began learning the violin, but later preferred the piano, which he played almost every day.

1973

Haag remained the first editor-in-chief until 1973.

2016

He died on 5 January 2016, in Fischhausen-Neuhaus, in southern Bavaria.

At the beginning of his career, Haag contributed significantly to the concepts of quantum field theory, including Haag's theorem, from which follows that the interaction picture of quantum mechanics does not exist in quantum field theory.

A new approach to the description of scattering processes of particles became necessary.

In the following years Haag developed what is known as Haag–Ruelle scattering theory.

During this work, he realized that the rigid relationship between fields and particles that had been postulated up to that point, did not exist, and that the particle interpretation should be based on Albert Einstein's principle of locality, which assigns operators to regions of spacetime.

These insights found their final formulation in the Haag–Kastler axioms for local observables of quantum field theories.

This framework uses elements of the theory of operator algebras and is therefore referred to as algebraic quantum field theory or, from the physical point of view, as local quantum physics.

This concept proved fruitful for understanding the fundamental properties of any theory in four-dimensional Minkowski space.

Without making assumptions about non-observable charge-changing fields, Haag, in collaboration with Sergio Doplicher and John E. Roberts, elucidated the possible structure of the superselection sectors of the observables in theories with short-range forces.

Sectors can always be composes with one another, each sector satisfies either para-Bose or para-Fermi statistics and for each sector there is a conjugate sector.

These insights correspond to the additivity of charges in the particle interpretation, to the Bose–Fermi alternative for particle statistics, and to the existence of antiparticles.

In the special case of simple sectors, a global gauge group and charge-carrying fields, which can generate all sectors from the vacuum state, were reconstructed from the observables.

These results were later generalized for arbitrary sectors in the Doplicher–Roberts duality theorem.

The application of these methods to theories in low-dimensional spaces also led to an understanding of the occurrence of braid group statistics and quantum groups.

In quantum statistical mechanics, Haag, together with Nicolaas M. Hugenholtz and Marinus Winnink, succeeded in generalizing the Gibbs–von Neumann characterization of thermal equilibrium states using the KMS condition (named after Ryogo Kubo, Paul C. Martin, and Julian Schwinger) in such a way that it extends to infinite systems in the thermodynamic limit.