Particle beam: Difference between revisions

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{{Short description|Stream of charged, or less frequently neutral particles}}
{{Refimprove|date=November 2008}}
 
A '''particle beam''' is a stream of [[charged particle|charged]] or [[neutral particle]]s. In [[Particle accelerator|particle accelerators]], inthese manyparticles casescan movingmove atwith neara velocity close to the [[speed of light]]. There is a difference between the creation and control of [[charged particle beam]]s and neutral particle beams, as only the first type can be manipulated to a sufficient extent by devices based on [[electromagnetism]]. The manipulation and diagnostics of charged particle beams at high kinetic energies using [[particle accelerator]]s are main topics of [[accelerator physics]].
 
==Sources==
There is a difference between the creation and control of [[charged particle beam]]s and neutral particle beams, as only the first type can be manipulated to a sufficient extent by devices based on [[electromagnetism]]. The manipulation and diagnostics of charged particle beams at high kinetic energies using [[particle accelerator]]s are main topics of [[accelerator physics]].
 
==Creation==
[[Charged particles]] such as [[electron]]s, [[positron]]s, and [[proton]]s may be separated from their common surrounding. This can be accomplished by e.g. [[thermionic emission]] or [[arc discharge]]. The following devices are commonly used as sources for particle beams:
* [[ionIon source]]
* [[cathode Cathode-ray tube]], or more specifically in one of its parts called [[electron gun]]. This is also part of traditional television and computer screens.
* [[photocathodePhotocathode]]s may also be built in as a part of an [[electron gun]], using the [[photoelectric effect]] to separate particles from their substrate.<ref>T. J. Kauppila et al. (1987), ''A pulsed electron injector using a metal photocathode irradiated by an excimer laser'', Proceedings of Particle Accelerator Conference 1987</ref>
* [[Neutron]] beams may be created by energetic [[proton beam]]s which impact on a target, e.g. of [[beryllium]] material. (see article [[Particle therapy]]).
* Bursting a Petawattpetawatt Laserlaser onto a [[Titaniumtitanium]] foil to produce a proton beams,beam<!-- and also water, and organic compose residue on the residual titanium foil. as a side effect -->.<ref>[https://www.nextbigfuture.com/2018/04/petawatt-proton-beams-at-lawrence-livermore.html Petawatt proton beams at Lawrence Livermore]</ref>
 
==AccelerationManipulation==
===Acceleration===
{{See also|Accelerator physics|Superconducting radio frequency}}
 
Charged beams may be further accelerated by use of high resonant, sometimes also [[superconducting]], [[microwave cavity|microwave cavities]]. These devices accelerate particles by interaction with an [[electromagnetic field]]. Since the [[wavelength]] of hollow macroscopic, conducting devices is in the [[radio frequency]] (RF) band, the design of such cavities and other RF devices is also a part of accelerator physics.
 
More recently, [[plasma acceleration]] has emerged as a possibility to accelerate particles in a [[plasma (physics)|plasma]] medium, using the [[Radiant energy|electromagnetic energy]] of pulsed high-power [[laser]] systems or the [[kinetic energy]] of other charged particles. This technique is under active development, but cannot provide reliable beams of sufficient quality at present.
 
==Usage=Guidance===
In all cases, the beam is steered with [[dipole magnet]]s and focused with [[quadrupole magnet]]s. With the end goal of reaching the desired position and beam spot size in the experiment.
 
==Applications==
===High-energy physics===
{{See also|Particle collider|Large Hadron Collider}}
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===Synchrotron radiation===
{{Main|Synchrotron light source|Synchrotron radiation}}
[[Electron beamsbeam]]s are employed in [[synchrotron light sourcessource]]s to produce electromagnetic[[X-ray|X-ray radiation]] with a continuous [[spectrum]] over a wide [[frequency]] band which is called [[synchrotron radiation]]. This X-ray radiation may beis used at [[beamline]]s of the synchrotron storagelight ringsources for a variety of experiments[[spectroscopy|spectroscopies]] ([[XAS]], [[XANES]], [[EXAFS]], [[X-ray fluorescence|''μ''-XRF]], [[X-ray crystallography|''μ''-XRD]]) in order to probe and to characterize the structure and the chemical speciation of solids and biological materials.
 
===Particle therapy===
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===Astrophysics===
Many phenomena in astrophysics are attributed to particle beams of various kinds.<ref>{{cite journal |author1=[[Anthony Peratt]] |title= The role of particle beams and electrical currents in the plasma universe |journal=Laser and Particle Beams |date=1988 |volume=6 |issue= 3 |pages=471–491 |doi= 10.1017/S0263034600005401 |bibcode= 1988LPB.....6..471P |url=https://plasmacosmology.info/downloads/Peratt_RolePartBeams.pdf |access-date=26 January 2023}}</ref> Solar Type III radio bursts, the most common impulsive radio signatures from the Sun, are used by scientists as a tool to better understand solar accelerated electron beams.<ref>{{cite journal |last1=Reid |first1=Hamish Andrew Sinclair |last2=Ratcliffe |first2=Heather |title=A review of solar type III radio bursts |journal=Research in Astronomy and Astrophysics |date=July 2014 |volume=14 |issue=7 |pages=773–804 |doi=10.1088/1674-4527/14/7/003 |arxiv=1404.6117 |bibcode=2014RAA....14..773R |s2cid=118446359 |url=https://iopscience.iop.org/article/10.1088/1674-4527/14/7/003 |issn=1674-4527}}</ref>
Many phenomena in astrophysics are attributed to particle beams of various kinds.
Perhaps of these the most iconic is the solar [[Type III radio burst]], due to a mildly relativistic electron beam.
 
===Military===
Though particle beams are perhaps most famously employed as weapon systems in [[science fiction]], theThe U.S. [[Defense Advanced Research Projects Agency|Advanced Research Projects Agency]] started work on [[particle beam weapon]]s in 1958.<ref name=roberds84>{{cite journal | last=Roberds | first=Richard M. | year=1984 | title=Introducing the Particle-Beam Weapon | journal=Air University Review | volume=July–August | url=http://www.airpower.maxwell.af.mil/airchronicles/aureview/1984/jul-aug/roberds.html | access-date=2005-01-03 | archive-url=https://web.archive.org/web/20120417021903/http://www.airpower.maxwell.af.mil/airchronicles/aureview/1984/jul-aug/roberds.html | archive-date=2012-04-17 | url-status=dead }}</ref> The general idea of such weaponry is to hit a target object with a stream of accelerated particles with high [[kinetic energy]], which is then transferred to the atoms, or molecules, of the target. The power needed to project a high-powered beam of this kind surpasses the production capabilities of any standard battlefield powerplant,<ref name=roberds84/> thus such weapons are not anticipated to be produced in the foreseeable future.
 
===Mars Colonization===
 
Proton beams such as "Laser-generated proton beams"<ref>[https://www.nextbigfuture.com/2018/04/petawatt-proton-beams-at-lawrence-livermore.html Petawatt proton beams at Lawrence Livermore]</ref> maybe used as way to generate Hydrogen for the production of Water on planets such as Mars where Hydrogen is scare and Oxygen is relative rich in the Atmosphere in the form of C2O. By analogy, a high energy proton beam is nothing more than a stream of fast baseballs that have been hit really hard, once its caught with a "baseball glove", and kinetic energy has been transferred to the glove, the proton becomes a regular hydrogen ION, ready for binding with Oxygen to produce water.
 
==See also==
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* [[Ion beam]]
* [[Polar_jet|Jet]]
* [[Atomic beam]]
 
* [[Accelerator neutrino]]
 
==References==