Gargamelle was a heavy liquid bubble chamber detector in operation at CERN between 1970 and 1979. It was designed to detect neutrinos and antineutrinos, which were produced with a beam from the Proton Synchrotron (PS) between 1970 and 1976, before the detector was moved to the Super Proton Synchrotron (SPS). [1] In 1979 an irreparable crack was discovered in the bubble chamber, and the detector was decommissioned. It is currently part of the "Microcosm" exhibition at CERN, open to the public.
Gargamelle is famous for being the experiment where neutral currents were discovered. Found in July 1973, neutral currents were the first experimental indication of the existence of the Z0 boson, and consequently a major step towards the verification of the electroweak theory.
Gargamelle can refer to both the bubble chamber detector itself, or the high-energy physics experiment by the same name. The name itself is derived from a 16th-century novel by François Rabelais, The Life of Gargantua and of Pantagruel , in which the giantess Gargamelle is the mother of Gargantua. [1]
In a series of separate works in the 1960s Sheldon Glashow, Steven Weinberg, and Abdus Salam came up with a theory that unified electromagnetic and weak interaction between elementary particles—the electroweak theory—for which they shared the 1979 Nobel Prize in Physics. [2] Their theory predicted the existence of the W± and Z0 bosons as propagators of the weak force. W± bosons have electric charge, either positive (W+) or negative (W−), the Z0, however, has no charge. Exchange of a Z0 boson transfers momentum, spin, and energy but leaves the particle's quantum numbers unaffected—charge, flavor, baryon number, lepton number, etc. Since there is no transfer of electric charge, the exchange of a Z0 is referred to as "neutral current". Neutral currents were a prediction of the electroweak theory.
In 1960 Melvin Schwartz proposed a method of producing an energetic neutrino beam. [3] Such a beam was then used by Schwartz and others in an experiment in 1962 at Brookhaven which showed that there are different types of neutrinos: muon neutrinos and electron neutrinos. Schwartz shared the 1988 Nobel Prize in Physics for this discovery. [4] Prior to Schwartz' idea weak interactions had been studied only in the decay of elementary particles, especially strange particles. Using these new neutrino beams greatly increased the energy available for the study of the weak interaction. Gargamelle was one of the first experiments that made use of a neutrino beam, produced with a proton beam from the PS.
A bubble chamber is simply a container filled with a superheated liquid. A charged particle travelling through the chamber will leave an ionization track, around which the liquid vaporizes, forming microscopic bubbles. The entire chamber is subject to a constant magnetic field, causing the tracks of the charged particles to curve. The radius of curvature is proportional to the momentum of the particle. The tracks are photographed, and by studying the tracks one can learn about the properties of the particles detected. The neutrino beam which travelled through the Gargamelle bubble chamber did not leave any tracks in the detector, since neutrinos have no charge. Interactions with neutrinos were therefore detected, by observing particles produced by the interactions of the neutrinos with the constituents of matter. Neutrinos have extremely small cross sections, i.e., the probability of interaction is very small. Whereas bubble chambers typically are filled with liquid hydrogen, Gargamelle was filled with a heavy liquid—CBrF3 (Freon)—increasing the probability of seeing neutrino interactions. [1]
The domain of neutrino physics was in rapid expansion in the 60's. Neutrino experiments using bubble chambers were already running at the first synchrotron at CERN, the PS, and the question of the next generation of bubble chambers had been on the agenda for some time. André Lagarrigue, an esteemed physicist at the École Polytechnique in Paris, and some of his colleagues, wrote the first published report, dated 10 February 1964, proposing the construction of a heavy liquid chamber to be built under the supervision of CERN. [5] He formed a collaboration consisting of seven laboratories: École Polytechnique Paris, RWTH Aachen, ULB Bruxelles, Istituto di Fisica dell'Università di Milano, LAL Orsay, University College London and CERN. [6] The group met in Milan in 1968 to list the physics priorities for the experiment: today Gargamelle is famous for its discovery of the neutral currents, but while preparing the physics program the topic was not even discussed, and in the final proposal it is ranked as fifth in priority. [7] At the time there was no consensus around the electroweak theory, which might explain the list of priorities. Also, earlier experiments looking for neutral currents in the decay of the neutral kaon into two charged leptons, had measured very small limits of around 10−7.
Due to budgetary crisis, the experiment was not approved in 1966, contrary to what was expected. Victor Weisskopf, Director General at CERN, and Bernard Grégory, Scientific Director, decided to commit the money themselves, the latter offering a loan to CERN to cover the instalment due for 1966. [5] The final contract was signed on 2 December 1965, making this the first time in CERN's history that an investment of this kind was not approved by the council, but by the Director General using his executive authority.
The Gargamelle chamber was entirely constructed at Saclay. Though the construction was delayed by about two years, it was finally assembled at CERN in December 1970, and the first important run occurred in March 1971. [5]
Gargamelle was 4.8 meters long and 2 meters in diameter, and held 12 cubic meters of heavy liquid Freon. To bend the tracks of charged particles, Gargamelle was surrounded by a magnet providing a 2 Tesla field. The coils of the magnet were made of copper cooled down with water, and followed the oblong shape of Gargamelle. In order to maintain the liquid at an adequate temperature several water tubes surrounded the chamber body, to regulate the temperature. The entire installation weighed more than 1000 tons.
When recording an event, the chamber was illuminated and photographed. The illumination system emitted light that was scattered at 90° by the bubbles, and sent to the optics. The light source consisted of 21 point flashes disposed at the ends of the chamber body and over one half of the cylinder. [8] The optics were situated in the opposite half of the cylinder, distributed in two rows parallel to the chamber axis, each rows having four optics. The objective was made by an assembly of lenses with a 90° angular field followed by a divergent lens which extends the field to 110°.
Gargamelle was designed for neutrino and antineutrino detection. The source of neutrinos and antineutrinos was a proton beam at an energy of 26 GeV from the PS. The protons were extracted by a magnet and then directed through an appropriate array of quadrupole and dipole magnets, providing the necessary degrees of freedom in position and orientation for adjusting the beam onto target. The target was a cylinder of beryllium, 90 cm long and 5 mm in diameter. [8] The target material was chosen so that the hadrons produced in the collision was mainly pions and kaons, which both decay to neutrinos. The produced pions and kaons have a variety of angles and energies, and consequently their decay product will also have huge momentum spread. As neutrinos have no charge, they cannot be focused with electric or magnetic fields. Instead, one focuses the secondary particles by using a magnetic horn, invented by Nobel laurate Simon van der Meer. The shape of the horn and the strength of the magnetic field can be tuned to select a range of particles that are to be best focused, resulting in a focused neutrino beam with a chosen range of energy as the kaons and pions decay. By reversing the current through the horn, one could produce an antineutrino beam. Gargamelle ran alternately in a neutrino and an antineutrino beam. The invention of van der Meer increased the neutrino flux by a factor of 20. The neutrino beam had an energy between 1 and 10 GeV.
After being focused, the pions and kaons were directed through a 70 m long tunnel, allowing them to decay. Pions and kaons that did not decay hit a shielding in the end of the tunnel and were absorbed. When decaying, pions and kaons normally decay in π→μ + ν and K→μ + ν, meaning that the flux of neutrinos would be proportional to the flux of muons. As the muons were not absorbed as hadrons, the flux of charged muons was stopped by an electromagnetic slowing down process in the long shielding. The neutrino flux was measured through the corresponding muon flux by means of six planes of silicium-gold detectors placed at various depths in shielding. [8]
During the years 1971-1976 large improvements factors were obtained in the intensity, first with a new injector for the PS — the Proton Synchrotron Booster — and secondly by the careful study of beam optics.
The first main quest of Gargamelle was to search for evidence of hard-scattering of muon-neutrinos and antineutrinos off nucleons. The priorities changed in March 1972, when the first hints of the existence of hadronic neutral current became obvious. [9] It was then decided to make a two-prong attack in the search for neutral current candidates. One line would search for leptonic events — events involving the interaction with an electron in the liquid, e.g.
ν
μ +
e−
→
ν
μ +
e−
or
ν
μ +
e−
→
ν
μ +
e−
. The other line would search for hadronic events — involving a neutrino scattered from a hadron, e.g.
ν
+
p
→
ν
+
p
,
ν
+
n
→
ν
+
p
+
π−
or
p
→
ν
+
n
+
π+
, plus events with many hadrons. The leptonic events have small cross-sections, but correspondingly small background. The hadronic events have larger backgrounds, most extensively due to neutrons produced when neutrinos interact in the material around the chamber. Neutrons, being of no charge, would not be detected in the bubble chamber, and the detection of their interactions would mimic neutral currents events. In order to reduce the neutron background, the energy of the hadronic events had to be greater than 1 GeV.
The first example of a leptonic event was found in December 1972 at Gargamelle by a graduate student from Aachen. By March 1973 166 hadronic events had been found, 102 events with the neutrino beam and 64 events with the antineutrino beam. [9] However, the question of neutron background hung over the interpretation of the hadronic events. The problem was solved by studying the charged current events which also had an associated neutron interaction which satisfied the hadronic event selection. [10] In this way one has a monitor of the neutron background flux. On the 19th of July 1973 the Gargamelle collaboration presented the discovery of neutral currents at a seminar at CERN.
The Gargamelle collaboration discovered both leptonic neutral currents — events involving the interaction of a neutrino with an electron — and hadronic neutral currents — events when a neutrino is scattered from a nucleon. The discovery was very important as it was in support of the electroweak theory, today a pillar of the Standard Model. The final experimental proof the electroweak theory came in 1983, when the UA1 and UA2 collaboration discovered the W± and Z0 bosons.
Initially the first priority of the Gargamelle had been to measure the neutrino and antineutrino cross-sections and structure functions. The reason for this was to test the quark model of the nucleon. Firstly the neutrino and antineutrino cross-sections were shown to be linear with energy, which is what one expects for the scattering of point-like constituents in the nucleon. Combining the neutrino and antineutrino structure functions allowed the net number of quarks in the nucleon to be determined, and this was in good agreement with 3. In addition comparing the neutrino results with results from Stanford Linear Accelerator Center (SLAC) in the US, using an electron beam, one found that quarks had fractional charges, and experimentally proved the values of these charges: +2⁄3 e, −1⁄3 e. The results were published in 1975, providing crucial evidence for the existence of quarks. [11]
In nuclear physics and particle physics, the weak interaction, also called the weak force, is one of the four known fundamental interactions, with the others being electromagnetism, the strong interaction, and gravitation. It is the mechanism of interaction between subatomic particles that is responsible for the radioactive decay of atoms: The weak interaction participates in nuclear fission and nuclear fusion. The theory describing its behaviour and effects is sometimes called quantum flavordynamics (QFD); however, the term QFD is rarely used, because the weak force is better understood by electroweak theory (EWT).
In particle physics, a pion or pi meson, denoted with the Greek letter pi, is any of three subatomic particles:
π0
,
π+
, and
π−
. Each pion consists of a quark and an antiquark and is therefore a meson. Pions are the lightest mesons and, more generally, the lightest hadrons. They are unstable, with the charged pions
π+
and
π−
decaying after a mean lifetime of 26.033 nanoseconds, and the neutral pion
π0
decaying after a much shorter lifetime of 85 attoseconds. Charged pions most often decay into muons and muon neutrinos, while neutral pions generally decay into gamma rays.
The Standard Model of particle physics is the theory describing three of the four known fundamental forces in the universe and classifying all known elementary particles. It was developed in stages throughout the latter half of the 20th century, through the work of many scientists worldwide, with the current formulation being finalized in the mid-1970s upon experimental confirmation of the existence of quarks. Since then, proof of the top quark (1995), the tau neutrino (2000), and the Higgs boson (2012) have added further credence to the Standard Model. In addition, the Standard Model has predicted various properties of weak neutral currents and the W and Z bosons with great accuracy.
The tau, also called the tau lepton, tau particle, tauon or tau electron, is an elementary particle similar to the electron, with negative electric charge and a spin of 1/2. Like the electron, the muon, and the three neutrinos, the tau is a lepton, and like all elementary particles with half-integer spin, the tau has a corresponding antiparticle of opposite charge but equal mass and spin. In the tau's case, this is the "antitau". Tau particles are denoted by the symbol
τ−
and the antitaus by
τ+
.
In particle physics, the W and Z bosons are vector bosons that are together known as the weak bosons or more generally as the intermediate vector bosons. These elementary particles mediate the weak interaction; the respective symbols are
W+
,
W−
, and
Z0
. The
W±
bosons have either a positive or negative electric charge of 1 elementary charge and are each other's antiparticles. The
Z0
boson is electrically neutral and is its own antiparticle. The three particles each have a spin of 1. The
W±
bosons have a magnetic moment, but the
Z0
has none. All three of these particles are very short-lived, with a half-life of about 3×10−25 s. Their experimental discovery was pivotal in establishing what is now called the Standard Model of particle physics.
Jack Steinberger was a German-born American physicist noted for his work with neutrinos, the subatomic particles considered to be elementary constituents of matter. He was a recipient of the 1988 Nobel Prize in Physics, along with Leon M. Lederman and Melvin Schwartz, for the discovery of the muon neutrino. Through his career as an experimental particle physicist, he held positions at the University of California, Berkeley, Columbia University (1950–68), and the CERN (1968–86). He was also a recipient of the United States National Medal of Science in 1988, and the Matteucci Medal from the Italian Academy of Sciences in 1990.
Weak neutral current interactions are one of the ways in which subatomic particles can interact by means of the weak force. These interactions are mediated by the Z boson. The discovery of weak neutral currents was a significant step toward the unification of electromagnetism and the weak force into the electroweak force, and led to the discovery of the W and Z bosons.
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.
CDHS was a neutrino experiment at CERN taking data from 1976 until 1984. The experiment was officially referred to as WA1. CDHS was a collaboration of groups from CERN, Dortmund, Heidelberg, Saclay and later Warsaw. The collaboration was led by Jack Steinberger. The experiment was designed to study deep inelastic neutrino interactions in iron.
The NA58 experiment, or COMPASS is a 60-metre-long fixed-target experiment at the M2 beam line of the SPS at CERN. The experimental hall is located at the CERN North Area, close to the French village of Prévessin-Moëns. The experiment is a two-staged spectrometer with numerous tracking detectors, particle identification and calorimetry. The physics results are extracted by recording and analysing the final states of the scattering processes.
A magnetic horn or neutrino horn is a high-current, pulsed focusing device, invented by the Dutch physicist Simon van der Meer in CERN, that selects pions and focuses them into a sharp beam. The original application of the magnetic horn was in the context of neutrino physics, where beams of pions have to be tightly focused. When the pions then decay into muons and neutrinos or antineutrinos, a focused neutrino beam is obtained.
The Big European Bubble Chamber (BEBC) is a large detector formerly used to study particle physics at CERN. The chamber body, a stainless-steel vessel, was filled with 35 cubic metres of superheated liquid hydrogen, liquid deuterium, or a neon-hydrogen mixture, whose sensitivity was regulated by means of a movable piston weighing 2 tons. The liquids at typical operation temperatures around 27 K were placed under overpressure of about 5 standard atmospheres (510 kPa). The piston expansion, synchronized with the charged particle beam crossing the chamber volume, caused a rapid pressure drop; in consequence the liquid reached its boiling point. During each expansion, charged particles ionized the atoms of the liquid as they passed through it and the energy deposited by them initiated boiling along their path, leaving trails of tiny bubbles. These tracks were photographed by the five cameras mounted on top of the chamber. The stereo photographs were subsequently scanned and all events finally evaluated by a team of scientists. After each expansion, the pressure was increased again to stop the boiling. The bubble chamber was then ready again for a new cycle of beam exposure.
The NA62 experiment is a fixed-target particle physics experiment in the North Area of the SPS accelerator at CERN. The experiment was approved in February 2007. Data taking began in 2015, and the experiment is expected to become the first in the world to probe the decays of the charged kaon with probabilities down to 10−12. The experiment's spokesperson is Giuseppe Ruggiero. The collaboration involves 308 participants from 33 institutions and 16 countries around the world.
NA31 is a CERN experiment which was proposed in 1982 as a measurement of |η00 /η+-|2 by the CERN-Edinburgh-Mainz-Pisa-Siegen collaboration. It took data between 1986 and 1989, using a proton beam from the SPS through the K4 neutral beam-line. Its aim was to experimentally prove direct CP-violation.
Herbert Hwa-sen Chen was a Chinese-born American theoretical and experimental physicist at the University of California at Irvine known for his contributions in the field of neutrino detection. Chen's work on observations of elastic neutrino-electron scattering provided important experimental support for the electroweak theory of the standard model of particle physics. In 1984 Chen realized that the deuterium of heavy water could be used as a detector that would distinguish the flavors of solar neutrinos. This idea led Chen to develop plans for the Sudbury Neutrino Observatory that would eventually make fundamental measurements demonstrating that neutrinos were particles with mass.
André Lagarrigue (1924 – 14 January 1975) was a French particle physicist. Being the initiator of the Gargamelle experiment at CERN, his work was of paramount importance in the discovery of neutral currents — the first experimental indication of the existence of the Z0 boson. This major discovery was a step towards verification of the electroweak theory, today a pillar of the Standard Model.
]
The Enhanced NeUtrino BEams from kaon Tagging or ENUBET is an ERC funded project that aims at producing an artificial neutrino beam in which the flavor, flux and energy of the produced neutrinos are known with unprecedented precision.
An accelerator neutrino is a human-generated neutrino or antineutrino obtained using particle accelerators, in which beam of protons is accelerated and collided with a fixed target, producing mesons which then decay into neutrinos. Depending on the energy of the accelerated protons and whether mesons decay in flight or at rest it is possible to generate neutrinos of a different flavour, energy and angular distribution. Accelerator neutrinos are used to study neutrino interactions and neutrino oscillations taking advantage of high intensity of neutrino beams, as well as a possibility to control and understand their type and kinematic properties to a much greater extent than for neutrinos from other sources.
Dieter Haidt is a German physicist, known for his contribution to the 1973 discovery of weak neutral currents. The discovery was made in the Gargamelle experiment, which used a heavy liquid bubble chamber detector in operation at CERN from 1970 to 1979.
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