The NA63 experiment aims to study the radiation process in strong electromagnetic fields. Located at CERN, in the North Area. It is a fixed-target experiment which uses the H4 secondary electron beams from the SPS, which are directed onto different targets. Those are made from a variety of elements, ranging from the relatively light carbon and silicon, through the heavier iron and tin to tungsten, gold and lead and are either amorphous or mono-crystals (made up of diamond for example).
This experiment is part of the SPS research programme and began taking data in 2010 with Mr Ulrik Ingerslev Uggerhoj as spokesperson. [1]
One of the main objectives of NA63 is to study the trident “Klein-like” production. This phenomenon happens in very strong electromagnetic fields, when an electron in motion penetrates the field and emits an electron/positron pair. For this to happen, the field must be greater than the so-called critical field E0 = 1.32*10^16 V/cm-1, [2] which is impossible to produce in a laboratory. However, in the case of crystalline targets, [3] the penetrating particles experience an electromagnetic field close to that theoretical critical one. Indeed, if the electrons enter the crystal with a small angle of incidence to a crystallographic direction (axis or plane) in a single crystal, the electrical fields of its constituents add coherently, producing a total field around 10^11 V/cm which then has become continuous and macroscopic. If the crystal is rotated from an amorphous configuration, then in the rest frame of the electron, the nuclear fields add coherently in the motion direction and the total field can finally reach the sought 10^16 V/cm. [2]
In such fields, an electron may gain an energy corresponding to the production of a new electron-positron pair, if it is transported over a distance given by the quantum mechanical uncertainty of its location : Δd= ƛ = ħ/mc. Thus, significant production of new particles is expected – and observed [2] – once the field in the electron rest frame becomes critical.
Such fields are generally only seen in astrophysical phenomena, such as highly magnetized neutron stars, black holes (where it is the gravitational field that is strong instead of the electromagnetic field as in NA63) where the Hawking radiation is a close analogue and, perhaps, in the cosmic accelerators that give rise to cosmic rays of the highest known energies. Using a special approach employing crystalline targets and energetic beams from the SPS (~ 100GeV), NA63 has managed to test processes at such fields in the laboratory.
Another line of enquiry for NA63 is the effect of strong electromagnetic fields on the duration of the process of photon emission. Specifically, fields of a critical magnitude have an intriguing effect on how long it takes for an electron to emit a photon.
An electron entering an electric field is accelerated, and therefore must lose part of its energy in the form of a photon via the Bremsstrahlung effect - the process by which a charged particle emits electromagnetic radiation when being decelerated upon passing an atom, for instance in a solid material. By exploiting the relativistic phenomena of time dilatation and length contraction, the NA63 experiment has shown that this process of photon emission is not instantaneous, but rather, takes time. [4] Because the process takes time, the photon production can be influenced experimentally. For non-relativistic particles this time is so short that investigations are very difficult, if not excluded. But for the relativistic particles used by NA63, their time is ‘slowed’ by a factor of about half a million due to the relativistic effect of time dilatation, making investigations possible.
In a critical electromagnetic field, on the contrary, electrons are deflected so violently that they don't have enough time to radiate photons. So adjusting the electromagnetic field past a critical level can modify the emerging radiation spectrum of a beam of electrons: increase the field and the relative radiation yield from the beam diminishes. NA63 is investigating such effects, and one of the main results shown so far is the measurement of quantum corrections to synchrotron radiation [5] that is normally only observed in its classical form in a synchrotron (storage) ring.
Radiation reaction is a long-standing problem in electrodynamics. Briefly formulated it concerns the back-reaction of an emitted photon on the charged particle that emits it. In the classical theory, the solutions of the equations of motion lead to absurd consequences, e.g conflicts with either energy conservation or causality. In the quantum version, the so-called Quantum electrodynamics (QED), the problem is in principle solved as the techniques required are known. However, the calculational difficulties involved are serious, and only comparatively simple problems have been solved. It turns out that strong fields is a route to addressing the problem experimentally, and (members of) the NA63 collaboration has paved the way theoretically [6] as well as experimentally. [7]
The effects of strong fields and emission times are relevant in many other branches of physics, ranging from the so-called “bubble-regime” in plasma wakefields used for extremely high-gradient particle acceleration, through astrophysical objects such as magnetars (heavily magnetized neutron stars) to intense lasers and heavy-ion collisions. The concepts studied at NA63 even apply in a gravitational analogue – Hawking radiation from black holes – which remains to be detected. Finally, although a much ‘cleaner’ environment can be achieved with electron-laser interactions to address the problem of radiation reaction experimentally, lasers of sufficient intensity to enable thorough investigations are still some years, perhaps decades, ahead of us. With electron-crystal interactions, NA63 has addressed the problem experimentally already.
The Unruh effect might have been observed for the first time in the high energy channeling radiation explored by NA63. [7] [8]
The electron is a subatomic particle with a negative one elementary electric charge. Electrons belong to the first generation of the lepton particle family, and are generally thought to be elementary particles because they have no known components or substructure. The electron's mass is approximately 1/1836 that of the proton. Quantum mechanical properties of the electron include an intrinsic angular momentum (spin) of a half-integer value, expressed in units of the reduced Planck constant, ħ. Being fermions, no two electrons can occupy the same quantum state, per the Pauli exclusion principle. Like all elementary particles, electrons exhibit properties of both particles and waves: They can collide with other particles and can be diffracted like light. The wave properties of electrons are easier to observe with experiments than those of other particles like neutrons and protons because electrons have a lower mass and hence a longer de Broglie wavelength for a given energy.
A photon is an elementary particle that is a quantum of the electromagnetic field, including electromagnetic radiation such as light and radio waves, and the force carrier for the electromagnetic force. Photons are massless particles that always move at the speed of light measured in vacuum. The photon belongs to the class of boson particles.
The photoelectric effect is the emission of electrons from a material caused by electromagnetic radiation such as ultraviolet light. Electrons emitted in this manner are called photoelectrons. The phenomenon is studied in condensed matter physics, solid state, and quantum chemistry to draw inferences about the properties of atoms, molecules and solids. The effect has found use in electronic devices specialized for light detection and precisely timed electron emission.
In particle physics, quantum electrodynamics (QED) is the relativistic quantum field theory of electrodynamics. In essence, it describes how light and matter interact and is the first theory where full agreement between quantum mechanics and special relativity is achieved. QED mathematically describes all phenomena involving electrically charged particles interacting by means of exchange of photons and represents the quantum counterpart of classical electromagnetism giving a complete account of matter and light interaction.
Wave-particle duality is the concept in quantum mechanics that quantum entities exhibit particle or wave properties according to the experimental circumstances. It expresses the inability of the classical concepts such as particle or wave to fully describe the behavior of quantum objects. During the 19th and early 20th centuries, light was found to behave as a wave then later discovered to have a particulate behavior, whereas electrons behaved like particles in early experiments then later discovered to have wavelike behavior. The concept of duality arose to name these seeming contradictions.
Antihydrogen is the antimatter counterpart of hydrogen. Whereas the common hydrogen atom is composed of an electron and proton, the antihydrogen atom is made up of a positron and antiproton. Scientists hope that studying antihydrogen may shed light on the question of why there is more matter than antimatter in the observable universe, known as the baryon asymmetry problem. Antihydrogen is produced artificially in particle accelerators.
A timeline of atomic and subatomic physics, including particle physics.
Synchrotron radiation is the electromagnetic radiation emitted when relativistic charged particles are subject to an acceleration perpendicular to their velocity. It is produced artificially in some types of particle accelerators or naturally by fast electrons moving through magnetic fields. The radiation produced in this way has a characteristic polarization, and the frequencies generated can range over a large portion of the electromagnetic spectrum.
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In experimental and applied particle physics, nuclear physics, and nuclear engineering, a particle detector, also known as a radiation detector, is a device used to detect, track, and/or identify ionizing particles, such as those produced by nuclear decay, cosmic radiation, or reactions in a particle accelerator. Detectors can measure the particle energy and other attributes such as momentum, spin, charge, particle type, in addition to merely registering the presence of the particle.
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Two-photon physics, also called gamma–gamma physics, is a branch of particle physics that describes the interactions between two photons. Normally, beams of light pass through each other unperturbed. Inside an optical material, and if the intensity of the beams is high enough, the beams may affect each other through a variety of non-linear effects. In pure vacuum, some weak scattering of light by light exists as well. Also, above some threshold of this center-of-mass energy of the system of the two photons, matter can be created.
In particle physics, the history of quantum field theory starts with its creation by Paul Dirac, when he attempted to quantize the electromagnetic field in the late 1920s. Major advances in the theory were made in the 1940s and 1950s, leading to the introduction of renormalized quantum electrodynamics (QED). The field theory behind QED was so accurate and successful in predictions that efforts were made to apply the same basic concepts for the other forces of nature. Beginning in 1954, the parallel was found by way of gauge theory, leading by the late 1970s, to quantum field models of strong nuclear force and weak nuclear force, united in the modern Standard Model of particle physics.
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In the physics of electromagnetism, the Abraham–Lorentz force is the reaction force on an accelerating charged particle caused by the particle emitting electromagnetic radiation by self-interaction. It is also called the radiation reaction force, the radiation damping force, or the self-force. It is named after the physicists Max Abraham and Hendrik Lorentz.
A particle accelerator is a machine that uses electromagnetic fields to propel charged particles to very high speeds and energies to contain them in well-defined beams. Small accelerators are used for fundamental research in particle physics. Accelerators are also used as synchrotron light sources for the study of condensed matter physics. Smaller particle accelerators are used in a wide variety of applications, including particle therapy for oncological purposes, radioisotope production for medical diagnostics, ion implanters for the manufacture of semiconductors, and accelerator mass spectrometers for measurements of rare isotopes such as radiocarbon.
The timeline of quantum mechanics is a list of key events in the history of quantum mechanics, quantum field theories and quantum chemistry.
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The Research Institute for Nuclear Problems of Belarusian State University is a research institute in Minsk, Belarus. Its main fields of research are nuclear physics, particle physics, materials science and nanotechnology.
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