{"id":14,"date":"2026-01-30T18:32:15","date_gmt":"2026-01-30T18:32:15","guid":{"rendered":"https:\/\/web110siwa.mydcts.org\/?page_id=14"},"modified":"2026-02-11T19:50:36","modified_gmt":"2026-02-11T19:50:36","slug":"particle-physics","status":"publish","type":"page","link":"https:\/\/web110siwa.mydcts.org\/index.php\/particle-physics\/","title":{"rendered":"Particle Physics"},"content":{"rendered":"\n
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Basic Inquiries<\/h2>\n\n\n\n

For basic inquiries into the dynamics and structure of matter, space, and time, physicists seek the simplest kinds of interactions at the highest possible energies. These typically entail particle energies of many GeV<\/a>, and interactions of the simplest kinds of particles: leptons<\/a> (e.g. electrons<\/a> and positrons<\/a>) and quarks<\/a> for the matter, or photons<\/a> and gluons<\/a> for the field quanta<\/a>. Since isolated quarks are experimentally unavailable due to color confinement<\/a>, the simplest available experiments involve the interactions of, first, leptons with each other, and second, of leptons with nucleons<\/a>, which are composed of quarks and gluons. To study the collisions of quarks with each other, scientists resort to collisions of nucleons, which at high energy may be usefully considered as essentially 2-body interactions<\/a> of the quarks and gluons of which they are composed. This elementary particle physicists tend to use machines creating beams of electrons<\/a>, positrons<\/a>, protons<\/a>, and antiprotons<\/a>, interacting with each other or with the simplest nuclei (e.g., hydrogen<\/a> or deuterium<\/a>) at the highest possible energies, generally hundreds of GeV<\/a> or more.<\/p>\n\n\n\n

The largest and highest-energy particle accelerator used for elementary particle physics<\/a> is the Large Hadron Collider<\/a> (LHC) at CERN<\/a>, operating since 2009.[13]<\/a><\/sup><\/p>\n\n\n\n

\"Animation
Animation illustrating how a linear particle accelerator works.<\/figcaption><\/figure>\n\n\n\n

Nuclear physics and isotope production<\/h3>\n\n\n\n

Nuclear physicists<\/a> and cosmologists<\/a> may use beams of bare atomic nuclei<\/a>, stripped of electrons, to investigate the structure, interactions, and properties of the nuclei themselves, and of condensed matter<\/a> at extremely high temperatures and densities, such as might have occurred in the first moments of the Big Bang<\/a>. These investigations often involve collisions of heavy nuclei \u2013 of atoms like iron<\/a> or gold<\/a> \u2013 at energies of several GeV per nucleon<\/a>. The largest such particle accelerator is the Relativistic Heavy Ion Collider<\/a> (RHIC) at Brookhaven National Laboratory<\/a>.<\/p>\n\n\n\n

Particle accelerators can also produce proton beams, which can produce proton-rich medical or research isotopes<\/a> as opposed to the neutron-rich ones made in fission reactors<\/a>; however, recent work has shown how to make 99<\/sup>Mo<\/a>, usually made in reactors, by accelerating isotopes of hydrogen,[14]<\/a><\/sup> although this method still requires a reactor to produce tritium<\/a>. An example of this type of machine is LANSCE<\/a> at Los Alamos National Laboratory<\/a>.<\/p>\n","protected":false},"excerpt":{"rendered":"

Basic Inquiries For basic inquiries into the dynamics and structure of matter, space, and time, physicists seek the simplest kinds of interactions at the highest possible energies. These typically entail particle energies of many GeV, and interactions of the simplest kinds of particles: leptons (e.g. electrons and positrons) and quarks for the matter, or photons and gluons for the field quanta. Since isolated quarks are experimentally unavailable due […]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-14","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/pages\/14","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/comments?post=14"}],"version-history":[{"count":12,"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/pages\/14\/revisions"}],"predecessor-version":[{"id":127,"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/pages\/14\/revisions\/127"}],"wp:attachment":[{"href":"https:\/\/web110siwa.mydcts.org\/index.php\/wp-json\/wp\/v2\/media?parent=14"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}