An electrostatic particle accelerator is one of the two main types of particle accelerators, in which charged particles are accelerated to a high energy by passing through a static high voltage potential. This contrasts with the other category of particle accelerator, oscillating field particle accelerators, in which the particles are accelerated by passing successively through multiple voltage drops created by oscillating voltages on electrodes. Owing to their simpler design, historically electrostatic types were the first particle accelerators. The two main types are the Van de Graaf generator invented by Robert Van de Graaff in 1929, and the Cockcroft-Walton accelerator invented by John Cockcroft and Ernest Walton in 1932. The maximum particle energy produced by electrostatic accelerators is limited by the accelerating voltage on the machine, which is limited by insulation breakdown to a few megavolts. Oscillating accelerators do not have this limitation, so they can achieve higher particle energies than electrostatic machines.
However, these machines have advantages such as lower cost, the ability to produce continuous beams and higher beam currents that make them useful to industry, so they are by far the most widely used particle accelerators. They are used in industrial irradiating applications such as plastic shrink wrap production, high power X-ray machines, radiation therapy in medicine, radioisotope production, ion implanters in semiconductor production, and sterilization. Many universities worldwide have electrostatic accelerators for research purposes. More powerful accelerators usually incorporate an electrostatic machine as their first stage, to accelerate particles to a high enough velocity to inject into the main accelerator.
Electrostatic accelerators are occasionally confused with linear accelerators (linacs) simply because they both accelerate particles in a straight line. The difference between them is that an electrostatic accelerator accelerates a charged particle by passing it through a single DC potential difference between two electrodes, while a linear accelerator accelerates a particle by passing it successively through multiple voltage drops created between multiple accelerating electrodes with an oscillating voltage.
Although these machines accelerate atomic nuclei, the scope of application is not limited to the nuclear sciences of nuclear physics, nuclear astrophysics and nuclear chemistry. Indeed, those applications are outweighed by other uses of nuclear beams. Of the approximately 26,000 accelerators worldwide, ~44% are for radiotherapy, ~41% for ion implantation, ~9% for industrial processing and research, ~4% for biomedical and other low-energy research (less than 1% are higher energy machines).
These accelerators are being used for nuclear medicine in medical physics, sample analysis using techniques such as PIXE in the material sciences, depth profiling in solid state physics, and to a lesser extent secondary ion mass spectrometry in geologic and cosmochemical works, and even neutron beams can be made from the charged particles emerging from these accelerators to perform neutron crystallography in condensed matter physics. The principles used in electrostatic nuclear accelerators could be used to accelerate any charged particles, but particle physics operates at much higher energy regimes than these machines can achieve, and there are various better methods suited for making electron beams, so these accelerators are used for accelerating nuclei.
A special application of electrostatic particle accelerator are dust accelerators in which nanometer to micrometer sized electrically charged dust particles are accelerated to speeds up to 100 km/s. Dust accelerators are used for impact cratering studies, calibration of impact ionization dust detectors, and meteor studies.
Using a high voltage terminal kept at a static potential on the order of millions of volts, charged particles can be accelerated. In simple language, an electrostatic generator is basically a giant capacitor (although lacking plates). The high voltage is achieved either using the methods of Cockcroft & Walton or Van de Graaff, with the accelerators often being named after these inventors. Van de Graaff's original design places electrons on an insulating sheet, or belt, with a metal comb, and then the sheet physically transports the immobilized electrons to the terminal. Although at high voltage, the terminal is a conductor, and there is a corresponding comb inside the conductor which can pick up the electrons off the sheet; owing to Gauss's law, there is no electric field inside a conductor, so the electrons are not repulsed by the platform once they are inside. The belt is similar in style to a conventional conveyor belt, with one major exception: it is seamless. Thus, if the belt is broken, the accelerator must be disassembled to some degree in order to replace the belt, which, owing to its constant rotation and being made typically of a rubber, is not a particularly uncommon occurrence. The practical difficulty with belts led to a different medium for physically transporting the charges: a chain of pellets. Unlike a normal chain, this one is non-conducting from one end to the other, as both insulators and conductors are used in its construction. These types of accelerators are usually called Pelletrons.
Once the platform can be electrically charged by one of the above means, some source of positive ions is placed on the platform at the end of the beam line, which is why it's called the terminal. However, as the ion source is kept at a high potential, one cannot access the ion source for control or maintenance directly. Thus, methods such as plastic rods connected to various levers inside the terminal can branch out and be toggled remotely. Omitting practical problems, if the platform is positively charged, it will repel the ions of the same electric polarity, accelerating them. As E=qV, where E is the emerging energy, q is the ionic charge, and V is the terminal voltage, the maximum energy of particles accelerated in this manner is practically limited by the discharge limit of the high voltage platform, about 12 MV under ambient atmospheric conditions. This limit can be increased, for example, by keeping the HV platform in a tank of an insulating gas with a higher dielectric constant than air, such as SF6 which has dielectric constant roughly 2.5 times that of air. However, even in a tank of SF6 the maximum attainable voltage is around 30 MV. There could be other gases with even better insulating powers, but SF6 is also chemically inert and non-toxic. To increase the maximum acceleration energy further, the tandem concept was invented to use the same high voltage twice.
Conventionally, positively charged ions are accelerated because this is the polarity of the atomic nucleus. However, if one wants to use the same static electric potential twice to accelerate ions, then the polarity of the ions' charge must change from anions to cations or vice versa while they are inside the conductor where they will feel no electric force. It turns out to be simple to remove, or strip, electrons from an energetic ion. One of the properties of ion interaction with matter is the exchange of electrons, which is a way the ion can lose energy by depositing it within the matter, something we should intuitively expect of a projectile shot at a solid. However, as the target becomes thinner or the projectile becomes more energetic, the amount of energy deposited in the foil becomes less and less.
Tandems locate the ion source outside the terminal, which means that accessing the ion source while the terminal is at high voltage is significantly less difficult, especially if the terminal is inside a gas tank. So then an anion beam from a sputtering ion source is injected from a relatively lower voltage platform towards the high voltage terminal. Inside the terminal, the beam impinges on a thin foil (on the order of micrograms per square centimeter), often carbon or beryllium, stripping electrons from the ion beam so that they become cations. As it is difficult to make anions of more than -1 charge state, then the energy of particles emerging from a tandem is E=(q+1)V, where we have added the second acceleration potential from that anion to the positive charge state q emerging from the stripper foil; we are adding these different charge signs together because we are increasing the energy of the nucleus in each phase. In this sense, we can see clearly that a tandem can double the maximum energy of a proton beam, whose maximum charge state is merely +1, but the advantage gained by a tandem has diminishing returns as we go to higher mass, as, for example, one might easily get a 6+ charge state of a silicon beam.
It is not possible to make every element into an anion easily, so it is very rare for tandems to accelerate any noble gases heavier than helium, although KrF− and XeF− have been successfully produced and accelerated with a tandem. It is not uncommon to make compounds in order to get anions, however, and TiH2 might be extracted as TiH− and used to produce a proton beam, because these simple, and often weakly bound chemicals, will be broken apart at the terminal stripper foil. Anion ion beam production was a major subject of study for tandem accelerator application, and one can find recipes and yields for most elements in the Negative Ion Cookbook. Tandems can also be operated in terminal mode, where they function like a single-ended electrostatic accelerator, which is a more common and practical way to make beams of noble gases.
The name 'tandem' originates from this dual-use of the same high voltage, although tandems may also be named in the same style of conventional electrostatic accelerators based on the method of charging the terminal.
One trick which has to be considered with electrostatic accelerators is that usually vacuum beam lines are made of steel. However, one cannot very well connect a conducting pipe of steel from the high voltage terminal to the ground. Thus, many rings of a strong glass, like Pyrex, are assembled together in such a manner that their interface is a vacuum seal, like a copper gasket; a single long glass tube could implode under vacuum or fracture supporting its own weight. Importantly for the physics, these inter-spaced conducting rings help to make a more uniform electric field along the accelerating column. This beam line of glass rings is simply supported by compression at either end of the terminal. As the glass is non-conducting, it could be supported from the ground, but such supports near the terminal could induce a discharge of the terminal, depending on the design. Sometimes the compression is not sufficient, and the entire beam line may collapse and shatter. This idea is especially important to the design of tandems, because they naturally have longer beam lines, and the beam line must run through the terminal.
Most often electrostatic accelerators are arranged in a horizontal line. However, some tandems may have a "U" shape, and in principle the beam can be turned to any direction with a magnetic dipole at the terminal. Some electrostatic accelerators are arranged vertically, where either the ion source or, in the case of a "U" shaped vertical tandem, the terminal, is at the top of a tower. A tower arrangement can be a way to save space, and also the beam line connecting to the terminal made of glass rings can take some advantage of gravity as a natural source of compression.
In a single-ended electrostatic accelerator the charged particle is accelerated through a single potential difference between two electrodes, so the output particle energy is equal to the charge on the particle multiplied by the accelerating voltage
In a tandem accelerator the particle is accelerated twice by the same voltage, so the output energy is . If the charge is in conventional units of coulombs and the potential is in volts the particle energy will be given in joules. However because the charge on elementary particles is so small (the charge on the electron is 1.6x10−19 coulombs), the energy in joules is a very small number.
Since all elementary particles have charges which are multiples of the elementary charge on the electron, coulombs, particle physicists use a different unit to express particle energies, the electron volt (eV) which makes it easier to calculate. The electronvolt is equal to the energy a particle with a charge of 1e gains passing through a potential difference of one volt. In the above equation, if is measured in elementary charges e and is in volts, the particle energy is given in eV. For example, if an alpha particle which has a charge of 2e is accelerated through a voltage difference of one million volts (1 MV), it will have an energy of two million electron volts, abbreviated 2 MeV. The accelerating voltage on electrostatic machines is in the range 0.1 to 25 MV and the charge on particles is a few elementary charges, so the particle energy is in the low MeV range. More powerful accelerators can produce energies in the giga electron volt (GeV) range.
- According to William Barletta, director of USPAS, the US Particle Accelerator School, per Toni Feder, in Physics Today February 2010, "Accelerator school travels university circuit", p. 20
- Mocker, A.; Bugiel, S.; Auer, S.; Baust, G.; Collette, A.; Drake, K.; Fiege, K.; Grün, E.; Heckmann, F.; Helfert, S.; Hillier, J.; Kempf, S.; Matt, G.; Mellert, T.; Munsat, T.; Otto, K.; Postberg, F.; Röser, H. P.; Shu, A.; Strernovski, Z.; Srama, R. (September 2011). "A 2 MV Van de Graaff accelerator as a tool for planetary and impact physics research". Review of Scientific Instruments. 82 (9): 95111-95111-8. Bibcode:2011RScI...82i5111M. doi:10.1063/1.3637461. Retrieved 27 April 2022.
- Neukun, G.; Mehl, A.; Fechtig, H.; Zähringer, J. (March 1970). "Impact phenomena of micrometeorites on lunar surface material". Earth and Planetary Science Letters. 9 (1): 31. Bibcode:1970E&PSL...8...31N. doi:10.1016/0012-821X(70)90095-6. Retrieved 27 April 2022.
- Grün, E.; Fechtig, H.; Hanner, M.; Kissel, J.; Lindblad, B.A.; Linkert, D.; Maas, D.; Morfill, G.E.; Zook, H. (May 1992). "The Galileo Dust Detector". Space Science Reviews. 60 (1–4): 317-340. Bibcode:1992SSRv...60..317G. doi:10.1007/BF00216860. Retrieved 11 February 2022.
- Thomas, E.; Simolka, J.; DeLuca, M.; Horanyi, M.; Janches, D.; Marshall, R; Munsat, T.; Plane, J.; Sternovski, Z. (March 2017). "Experimental setup for the laboratory investigation of micrometeoroid ablation using a dust accelerator". Review of Scientific Instruments. 88 (3): id.034501. Bibcode:2017RScI...88c4501T. doi:10.1063/1.4977832. Retrieved 27 April 2022.
- Minehara, Eisuke; Abe, Shinichi; Yoshida, Tadashi; Sato, Yutaka; Kanda, Mamoru; Kobayashi, Chiaki; Hanashima, Susumu (1984). "On the production of the KrF- and XeF- Ion beams for the tandem electrostatic accelerators". Nuclear Instruments and Methods in Physics Research Section B. 5 (2): 217. Bibcode:1984NIMPB...5..217M. doi:10.1016/0168-583X(84)90513-5.
- Middleton, R: A Negative Ion Cookbook, University of Pennsylvania, unpublished, 1989 Online pdf
- Wegner, H.E.; Thieberger, P. (1977). "North-American MP tandem accelerators". Revue de Physique Appliquée. 12 (10): 1291–1301. doi:10.1051/rphysap:0197700120100129100. ISSN 0035-1687.
- Skorka, S.J. (1977). "The European MP-Tandems". Revue de Physique Appliquée. 12 (10): 1279–1290. doi:10.1051/rphysap:0197700120100127900. ISSN 0035-1687.