Volker D. Burkert | |
---|---|
Nationality | German |
Occupation(s) | Physicist, academic and researcher |
Awards | Bonner Prize, American Physical Society, Outstanding Scientist Award, Governor of Virginia, USA Fellow, American Physical Society |
Academic background | |
Education | B.A. M.S. Physics PhD Philosophy |
Alma mater | Bonn University |
Academic work | |
Institutions | Thomas Jefferson National Accelerator Facility (Jefferson Lab/JLab) |
Volker D. Burkert is a German physicist,academic and researcher. He is a Principal Staff Scientist at the Thomas Jefferson National Accelerator Facility at Jefferson Lab (JLab) in Newport News,Virginia (USA). [1] He has made major contributions to the design of the CEBAF Large Acceptance Spectrometer (CLAS) that made it suitable for high luminosity operation in experiments studying spin-polarized electron scattering.
Beginning in 2002,Burkert developed the concept of a new large acceptance detector,CLAS12,tuned for the much higher rate capabilities that were needed to take full advantage of the doubling of the energy of the CEBAF machine to 12 GeV. CLAS12 has been in operation since 2018. Burkert's work contributed to JLab's flagship program investigating the three-dimensional structure of the proton. [2]
Burkert is a Fellow of the American Physical Society, [3] and the recipient of the 2019 Virginia Governor's Outstanding Scientist award. [4]
Burkert was educated at the University of Bonn in Germany,earning a BA in 1967,a master's degree in physics in 1969 and a PhD in 1975. After being awarded his doctorate,he continued to study in Bonn until 1981. [5]
Burkert began his career as a research associate at Bonn University in 1975. In 1978,he was promoted to the German equivalent of an assistant professorship,a position that he held until 1984. During this time he was also on leave as a Scientific Associate at the European Council for Nuclear Research (CERN) in Switzerland,where he joined the Axial Field Spectrometer (AFS) team at the proton-proton Intersecting Storage Rings (ISR). Following a sabbatical in the US in 1984,he joined the Continuous Electron Beam Accelerator Facility (CEBAF) in 1985 as a Staff Scientist,and worked on the development of instrumentation for nuclear physics experiments in two of the three planned experimental halls. [6]
In 1992,Burkert was promoted to the rank of Senior Staff Scientist and developed a broad research program to elucidate the internal structure of nucleons by investigating their excited states and so assisting theorists in their development of their quark models. Similar work was undertaken in research centers across Europe and Asia. In 2003,he took charge of the experimental department Hall B and the scientific research group,and led a team of scientists,engineers,and technicians in the pursuit of a high impact scientific program that explores the internal quark and gluon structure of protons,neutrons and atomic nuclei. [7] During this time,Burkert developed the conceptual design of a new spectrometer system,CLAS12,with an order of magnitude increase in operating luminosity over the original CLAS detector performance. He oversaw the design,construction and commissioning of the CLAS12 spectrometer system and ancillary equipment. [8]
Burkert has authored and co-authored over 500 scientific articles and has over 56,000 citations. [9] In his early years of research,he studied nucleon excitations involving high energy polarized electron beams and spin-polarized hydrogen and deuterium targets. [10] At the Bonn University electron accelerator,Burkert developed an electron-spin polarimeter to map the energy and strengths of several depolarizing resonances induced in the electron beam during the acceleration process in the synchrotron. The results enabled designing compensating measures to keep the polarization value high during the acceleration process as required for scientific experiments. [11]
Burkert's research at CERN focused on hard scattering processes employing two colliding proton beams each with beam energies up to 31 GeV. This led to the first direct determination of the gluon structure function of the proton. [12] At Jefferson Lab (CEBAF),Burkert led a research program focused on the experimental study of the structure of protons,neutrons and nuclei using high energy electron and photon beams,polarized hydrogen and deuterium targets and the CLAS detector system,suitably instrumented for high rate operation in intense electron beams. This opened up a high-impact scientific program of exclusive electron scattering measurements,where all particles generated in the interaction are detected and identified in CLAS. The required detector modifications enabled the discovery of the theoretically predicted deeply virtual Compton scattering (DVCS) process, [13] which provided the basis for an extensive program to construct 3D images of the proton's internal quark distribution as well their internal mechanical properties. These modifications were also critical for measurements that clarified the internal structure of a series of excited states of the proton as part of the NSTAR program.
Burkert has made major contributions to the design,construction and performance of CLAS. [6] The work on pressure distribution inside the proton provides insights into the strong interaction mechanisms internal to subatomic particles,and the cause of the extremely high pressure observed in protons for the first time. It further introduced a new area of research on the fundamental gravitational and mechanical properties of protons,neutrons and nuclei,which can provide access to the normal and shear stress inside subatomic particles,and their physical radii. [14] The results of this research through an extraction of the Compton Form Factors reveal a tomographic image of the nucleon. [15] This result is based on prior measurements of the differential cross sections and of the beam spin asymmetries in the hard exclusive electroproduction of photons on the proton over a wide kinematic range and with high statistical precision. [16]
Burkert reviewed the experimental findings in a large number of experiments in 2003-2004 had found evidence of the existence of an exotic baryon Ɵ+(1535) consisting of four quarks and one anti-quark,generated in photoproduction processes,e.g. on deuterium ɣd→K-(K+n)p as well as more massive states. Such exotic states would have quantum numbers that cannot be formed from only the 3 quarks present in nucleons or other baryons,but require combinations of four quarks and one anti-quark. He found that the experimental evidence for the Θ+(1535) state had significantly eroded with new precision data,and left only room for a hypothetical baryon state in the (K+n) system with a very narrow intrinsic energy-width of less than 500 KeV,rendering the existence of such a state highly unlikely. [17]
Reviews of the progress in the investigation of the electroexcitation of the excited nucleon resonances,both in experiment and in theory,highlight the transition amplitudes of the four lowest excited states. [18] These results show that the standard quark model of 3 valence quarks,consisting of up-quarks and down-quarks only,cannot explain the resonance transition amplitudes at small photon virtuality. Higher Fock states,including meson-baryon contributions,must be included. These results led the way towards resolving a longstanding controversy about the Roper resonance, [19] the lowest mass radial excitation of the ground state nucleon. Its transition amplitudes strongly deviate from the quark model predictions when probed at large distances that led to invoking more exotic interpretations of the resonance as a hybrid excitation [20] with gluons as structural parts of the wave function,and as a dynamically meson-baryon excitation. [21] This has been discussed in Progress in Nuclear and Particle Physics,and in the Review of Modern Physics. [22] Similar but smaller effects were also found for other excited states,Δ(1232)3/2+,N(1520)3/2−,and N(1535)1/2-,and indicates that this may be a fundamental contribution to resonance excitations in electromagnetic interactions.
The neutron is a subatomic particle, symbol
n
or
n0
, which has no electric charge, and a mass slightly greater than that of a proton. Protons and neutrons constitute the nuclei of atoms. Since protons and neutrons behave similarly within the nucleus, they are both referred to as nucleons. Nucleons have a mass of approximately one atomic mass unit, or dalton. Their properties and interactions are described by nuclear physics. Protons and neutrons are not elementary particles; each is composed of three quarks.
In physics and chemistry, a nucleon is either a proton or a neutron, considered in its role as a component of an atomic nucleus. The number of nucleons in a nucleus defines the atom's mass number.
Particle physics or high-energy physics is the study of fundamental particles and forces that constitute matter and radiation. The field also studies combinations of elementary particles up to the scale of protons and neutrons, while the study of combination of protons and neutrons is called nuclear physics.
A proton is a stable subatomic particle, symbol
p
, H+, or 1H+ with a positive electric charge of +1 e (elementary charge). Its mass is slightly less than the mass of a neutron and approximately 1836 times the mass of an electron (the proton-to-electron mass ratio). Protons and neutrons, each with a mass of approximately one atomic mass unit, are jointly referred to as nucleons (particles present in atomic nuclei).
In physics, a subatomic particle is a particle smaller than an atom. According to the Standard Model of particle physics, a subatomic particle can be either a composite particle, which is composed of other particles, or an elementary particle, which is not composed of other particles. Particle physics and nuclear physics study these particles and how they interact. Most force-carrying particles like photons or gluons are called bosons and, although they have quanta of energy, do not have rest mass or discrete diameters and are unlike the former particles that have rest mass and cannot overlap or combine which are called fermions. The W and Z bosons, however, are an exception to this rule and have relatively large rest masses at approximately 80 GeV and 90 GeV respectively.
A pentaquark is a human-made subatomic particle, consisting of four quarks and one antiquark bound together; they are not known to occur naturally, or exist outside of experiments specifically carried out to create them.
A hypernucleus is similar to a conventional atomic nucleus, but contains at least one hyperon in addition to the normal protons and neutrons. Hyperons are a category of baryon particles that carry non-zero strangeness quantum number, which is conserved by the strong and electromagnetic interactions.
The ISOLDE Radioactive Ion Beam Facility, is an on-line isotope separator facility located at the centre of the CERN accelerator complex on the Franco-Swiss border. Created in 1964, the ISOLDE facility started delivering radioactive ion beams (RIBs) to users in 1967. Originally located at the Synchro-Cyclotron (SC) accelerator, the facility has been upgraded several times most notably in 1992 when the whole facility was moved to be connected to CERN's ProtonSynchroton Booster (PSB). ISOLDE is currently the longest-running facility in operation at CERN, with continuous developments of the facility and its experiments keeping ISOLDE at the forefront of science with RIBs. ISOLDE benefits a wide range of physics communities with applications covering nuclear, atomic, molecular and solid-state physics, but also biophysics and astrophysics, as well as high-precision experiments looking for physics beyond the Standard Model. The facility is operated by the ISOLDE Collaboration, comprising CERN and sixteen (mostly) European countries. As of 2019, close to 1,000 experimentalists around the world are coming to ISOLDE to perform typically 50 different experiments per year.
Thomas Jefferson National Accelerator Facility (TJNAF), commonly called Jefferson Lab or JLab, is a US Department of Energy National Laboratory located in Newport News, Virginia.
GlueX is a particle physics experiment located at the Thomas Jefferson National Accelerator Facility (JLab) accelerator in Newport News, Virginia. Its primary purpose is to better understand the nature of confinement in quantum chromodynamics (QCD) by identifying a spectrum of hybrid and exotic mesons generated by the excitation of the gluonic field binding the quarks. Such mesonic states are predicted to exist outside of the well-established quark model, but none have been definitively identified by previous experiments. A broad high-statistics survey of known light mesons up to and including the is also underway.
Nathan Isgur was a theoretical physicist from the U.S. and Canada.
The Delta baryons are a family of subatomic particle made of three up or down quarks, the same constituent quarks that make up the more familiar protons and neutrons.
T2K is a particle physics experiment studying the oscillations of the accelerator neutrinos. The experiment is conducted in Japan by the international cooperation of about 500 physicists and engineers with over 60 research institutions from several countries from Europe, Asia and North America and it is a recognized CERN experiment (RE13). T2K collected data within its first phase of operation from 2010 till 2021. The second phase of data taking is expected to start in 2023 and last until commencement of the successor of T2K – the Hyper-Kamiokande experiment in 2027.
The lambda baryons (Λ) are a family of subatomic hadron particles containing one up quark, one down quark, and a third quark from a higher flavour generation, in a combination where the quantum wave function changes sign upon the flavour of any two quarks being swapped. They are thus baryons, with total isospin of 0, and have either neutral electric charge or the elementary charge +1.
The Roper resonance, also known as P11(1440) or N(1440)1/2+, is an unstable nucleon resonance with a mass of about 1,440 MeV/c2 and with a relatively wide full Breit-Wigner width Γ ≈ 300 MeV/c2. It contains three quarks (up (u) or down (d)) with total spin J = 1/2 and total isospin I = 1/2. In the quark model it is considered to be a radially excited three-quark state with radial quantum number N = 2 and positive parity. The Roper Resonance has been a subject of many studies because its mass is actually lower than three-quark states with radial quantum number N = 1. Only in the late 2000s was the lower-than-expected mass explained by theoretical calculations, revealing a quark core shielded by a dense cloud of mesons.
CEBAF Large Acceptance Spectrometer (CLAS) is a nuclear and particle physics detector located in the experimental Hall B at Jefferson Laboratory in Newport News, Virginia, United States. It is used to study the properties of the nuclear matter by the collaboration of over 200 physicists from many countries all around the world.
When embedded in an atomic nucleus, neutrons are (usually) stable particles. Outside the nucleus, free neutrons are unstable and have a mean lifetime of 877.75+0.50
−0.44 s or 879.6±0.8 s. Therefore, the half-life for this process is 611±1 s.
Joel Marshall Moss is an American experimental nuclear physicist.
The nucleon magnetic moments are the intrinsic magnetic dipole moments of the proton and neutron, symbols μp and μn. The nucleus of an atom comprises protons and neutrons, both nucleons that behave as small magnets. Their magnetic strengths are measured by their magnetic moments. The nucleons interact with normal matter through either the nuclear force or their magnetic moments, with the charged proton also interacting by the Coulomb force.