Johann Rafelski | |
---|---|
Born | |
Nationality | US, German |
Alma mater | Johann Wolfgang Goethe University Frankfurt am Main |
Known for | Structure of the Vacuum State and Energy in Strong External Field quantum electrodynamics and quantum chromodynamics, Muon-catalyzed fusion, Hadronization and Hagedorn temperature, Deconfinement of quarks (QGP) in relativistic heavy ion collisions, Strangeness as signature of quark–gluon plasma, quark matter |
Spouses | |
Children | Marc Rafelski, Susanne Rafelski |
Scientific career | |
Fields | Physicist |
Institutions | University of Arizona |
Doctoral advisor | Walter Greiner |
Johann Rafelski (born 19 May 1950) is a German-American theoretical physicist. He is a professor of physics at the University of Arizona in Tucson, [1] guest scientist at CERN (Geneva), [2] and has been LMU-Excellent Guest Professor at the Ludwig Maximilian University of Munich in Germany.
Rafelski's current research interests center around investigation of the vacuum structure of QCD and QED in the presence of strong fields; study of the QCD vacuum structure and deconfinement with strange particle production [3] in deconfined quark–gluon plasma formed in relativistic heavy ion collisions; the formation of matter out of quark–gluon plasma in the hadronization process, [4] also in the early Universe; [5] considering antimatter formation and annihilation. He has also contributed to the physics of table top muon-catalyzed fusion [6] and the ascent of ultrashort laser light pulses [7] as a new tool in this domain of physics. He contributed to understanding of neural nets and artificial intelligence [8] showing importance of neural plasticity and "sleep".
Rafelski studied physics at Johann Wolfgang Goethe University in Frankfurt, Germany, where he received his PhD in the spring of 1973 working with Walter Greiner on strong fields [9] and muonic atom tests of QED. [10] [11] In 1973 he began a series of postdoctoral fellowships: first at the University of Pennsylvania (Philadelphia) with Abraham Klein, then at the Argonne National Laboratory near Chicago where he worked with John W. Clark of Washington University in St. Louis and Michael Danos [12] [13] of National Bureau of Standards (now NIST). [14] In the spring of 1977, Rafelski moved for a few months to work at the GSI Helmholtz Centre for Heavy Ion Research in Germany, then continued on to a fellowship at CERN [15] where he worked with Rolf Hagedorn and John S. Bell; Rafelski remains associated with CERN to this day. [16]
In the fall of 1979 Rafelski was appointed tenured associate professor at Johann Wolfgang Goethe University where he taught for 4 years, while collaborating closely with Hagedorn, Berndt Müller and Gerhard Soff, whom Rafelski mentored in his PhD work. Rafelski then accepted the chair of Theoretical Physics at the University of Cape Town (South Africa) [17] where he created a Theoretical Physics and Astrophysics Institute before moving to The University of Arizona in the fall of 1987. During these years he was also a guest scientist at NIST in Washington, D.C. His interests in muon-catalyzed fusion and other table-top fusion methods led him to a collaboration led by Steven E. Jones [18] working at the Los Alamos National Laboratory. [19] The start-up of experimental work on quark–gluon plasma has led to another enduring collaboration with the University of Paris 7-Jussieu involving Jean Letessier. [20]
Rafelski has remained involved in the study of quark–gluon plasma (QGP) and advancing strangeness production as the pivotal QGP signature, [21] [16] for which the first experimental evidence was announced by CERN in February 2000 [22] and which has now become a new field of physics. [23] [24] [16] This work relates to his long-lasting studies of the structured quantum vacuum, [25] also known as Lorentz Invariant Aether.
Melting Hadrons, Boiling Quarks is a scientific book series edited by Rafelski. [26] The first volume of 2016 published as open-access under the Creative Commons license 4.0. [27] is subtitled 'From Hagedorn Temperature to ultra-relativistic heavy-ion collisions at CERN', and the volume in preparation was subtitled 'Quark–gluon plasma discovery at CERN'. In the foreword of the first volume, former director-general of CERN, Herwig Schopper, states that the book fulfills two purposes which have been neglected for a long time. [26] Primarily a festschrift (an 'honorary book'), it "...delivers the proper credit to physicist Rolf Hagedorn for his important role at the birth of a new research field"; and it describes how a development which he started just 50 years ago is "...closely connected to the most recent surprises in the new experimental domain of relativistic heavy ion physics...". [26]
Rafelski was born in Kraków, Poland, on May 19, 1950. In 1973 Rafelski married Helga Betz, with whom he had two children. Dr. Helga Rafelski died of cancer in 2000. In 2003 Rafelski married the American novelist Victoria Grossack. [31]
A gluon is a type of elementary particle that mediates the strong interaction between quarks, acting as the exchange particle for the interaction. Gluons are massless vector bosons, thereby having a spin of 1. Through the strong interaction, gluons bind quarks into groups according to quantum chromodynamics (QCD), forming hadrons such as protons and neutrons.
The
J/ψ
(J/psi) meson is a subatomic particle, a flavor-neutral meson consisting of a charm quark and a charm antiquark. Mesons formed by a bound state of a charm quark and a charm anti-quark are generally known as "charmonium" or psions. The
J/ψ
is the most common form of charmonium, due to its spin of 1 and its low rest mass. The
J/ψ
has a rest mass of 3.0969 GeV/c2, just above that of the
η
c, and a mean lifetime of 7.2×10−21 s. This lifetime was about a thousand times longer than expected.
High-energy nuclear physics studies the behavior of nuclear matter in energy regimes typical of high-energy physics. The primary focus of this field is the study of heavy-ion collisions, as compared to lighter atoms in other particle accelerators. At sufficient collision energies, these types of collisions are theorized to produce the quark–gluon plasma. In peripheral nuclear collisions at high energies one expects to obtain information on the electromagnetic production of leptons and mesons that are not accessible in electron–positron colliders due to their much smaller luminosities.
Hadronization is the process of the formation of hadrons out of quarks and gluons. There are two main branches of hadronization: quark-gluon plasma (QGP) transformation and colour string decay into hadrons. The transformation of quark-gluon plasma into hadrons is studied in lattice QCD numerical simulations, which are explored in relativistic heavy-ion experiments. Quark-gluon plasma hadronization occurred shortly after the Big Bang when the quark–gluon plasma cooled down to the Hagedorn temperature when free quarks and gluons cannot exist. In string breaking new hadrons are forming out of quarks, antiquarks and sometimes gluons, spontaneously created from the vacuum.
The STAR detector is one of the four experiments at the Relativistic Heavy Ion Collider (RHIC) in Brookhaven National Laboratory, United States.
Quark matter or QCD matter refers to any of a number of hypothetical phases of matter whose degrees of freedom include quarks and gluons, of which the prominent example is quark-gluon plasma. Several series of conferences in 2019, 2020, and 2021 were devoted to this topic.
The Hagedorn temperature,TH, is the temperature in theoretical physics where hadronic matter is no longer stable, and must either "evaporate" or convert into quark matter; as such, it can be thought of as the "boiling point" of hadronic matter. It was discovered by Rolf Hagedorn. The Hagedorn temperature exists because the amount of energy available is high enough that matter particle (quark–antiquark) pairs can be spontaneously pulled from vacuum. Thus, naively considered, a system at Hagedorn temperature can accommodate as much energy as one can put in, because the formed quarks provide new degrees of freedom, and thus the Hagedorn temperature would be an impassable absolute hot. However, if this phase is viewed as quarks instead, it becomes apparent that the matter has transformed into quark matter, which can be further heated.
In physical cosmology, the quark epoch was the period in the evolution of the early universe when the fundamental interactions of gravitation, electromagnetism, the strong interaction and the weak interaction had taken their present forms, but the temperature of the universe was still too high to allow quarks to bind together to form hadrons. The quark epoch began approximately 10−12 seconds after the Big Bang, when the preceding electroweak epoch ended as the electroweak interaction separated into the weak interaction and electromagnetism. During the quark epoch, the universe was filled with a dense, hot quark–gluon plasma, containing quarks, leptons and their antiparticles. Collisions between particles were too energetic to allow quarks to combine into mesons or baryons. The quark epoch ended when the universe was about 10−6 seconds old, when the average energy of particle interactions had fallen below the binding energy of hadrons. The following period, when quarks became confined within hadrons, is known as the hadron epoch.
Rolf Hagedorn was a German theoretical physicist who worked at CERN. He is known for the idea that hadronic matter has a "melting point". The Hagedorn temperature is named in his honor.
Quark–gluon plasma is an interacting localized assembly of quarks and gluons at thermal and chemical (abundance) equilibrium. The word plasma signals that free color charges are allowed. In a 1987 summary, Léon van Hove pointed out the equivalence of the three terms: quark gluon plasma, quark matter and a new state of matter. Since the temperature is above the Hagedorn temperature—and thus above the scale of light u,d-quark mass—the pressure exhibits the relativistic Stefan-Boltzmann format governed by temperature to the fourth power and many practically massless quark and gluon constituents. It can be said that QGP emerges to be the new phase of strongly interacting matter which manifests its physical properties in terms of nearly free dynamics of practically massless gluons and quarks. Both quarks and gluons must be present in conditions near chemical (yield) equilibrium with their colour charge open for a new state of matter to be referred to as QGP.
In high-energy nuclear physics, strangeness production in relativistic heavy-ion collisions is a signature and diagnostic tool of quark–gluon plasma (QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, heavier quark flavors such as strange and charm typically approach chemical equilibrium in a dynamic evolution process. QGP is an interacting localized assembly of quarks and gluons at thermal (kinetic) and not necessarily chemical (abundance) equilibrium. The word plasma signals that color charged particles are able to move in the volume occupied by the plasma. The abundance of strange quarks is formed in pair-production processes in collisions between constituents of the plasma, creating the chemical abundance equilibrium. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.
The NA49 experiment was a particle physics experiment that investigated the properties of quark–gluon plasma. The experiment's synonym was Ions/TPC-Hadrons. It took place in the North Area of the Super Proton Synchrotron (SPS) at CERN from 1991-2002.
The NA35 experiment was a particle physics experiment that took place in the North Area of the Super Proton Synchrotron (SPS) at CERN. It used a streamer chamber with comprehensive hadronic and electromagnetic calorimetry. This experiment was used to observe the properties of nucleus-nucleus collisions at 60 and 200 GeV/nucleon, to understand the degree of stopping and thermalization, determine the energy densities achievable in those conditions, and to measure other related properties and quantities.
Berndt O. Mueller is a German-born theoretical physicist who specializes in nuclear physics. He is a professor at Duke University.
Maurice René Michel Jacob was a French theoretical particle physicist.
Robert Elie Klapisch was a French engineer and physicist.
Emanuele Quercigh is an Italian particle physicist who works since 1964 at CERN, most known for the discovery of quark-gluon plasma (QGP). Quercigh moved as a child to Friuli with his mother and his younger brother after the early death of his father. Quercigh studied physics at the University of Milan in Italy, where he became assistant of professor Giuseppe Occhialini in 1959.
Helga Ernestine Rafelski, was a German particle physicist. She got her professional degree from Goethe-Universität Frankfurt am Main, her master's degree from University of Illinois at Chicago in 1977 and her PhD from University of Cape Town in 1988 under the advisement of Raoul D. Viollier. She studied muon-catalysed fusion and relativistic heavy-ion collisions.
Hannah Elfner is a German physicist who is Head of Simulations at the Helmholtz Centre for Heavy Ion Research and Professor of Physics at the Goethe University Frankfurt. She was named the 2021 Alfons and Gertrud Kassel Foundation Scientist of the Year.
Reinhard Stock is a German experimental physicist, specializing in heavy-ion physics.
Box 22, folder 8: Rafelski, biographical material and letters of recommendation, 1991