{"id":233,"date":"2024-10-09T10:04:59","date_gmt":"2024-10-09T08:04:59","guid":{"rendered":"https:\/\/web.infn.it\/jlab12\/?page_id=233"},"modified":"2024-10-09T10:05:00","modified_gmt":"2024-10-09T08:05:00","slug":"search-for-dark-force-en","status":"publish","type":"page","link":"https:\/\/web.infn.it\/jlab12\/en\/search-for-dark-force-en\/","title":{"rendered":"Search for Dark Force (en)"},"content":{"rendered":"\n<h2 class=\"wp-block-heading\" id=\"imPgTitle\">Search for dark forces<\/h2>\n\n\n\n<p>The Heavy Photon Search (HPS) is an experiment proposed for Jefferson Laboratory to search for new heavy vector boson(s), aka &#8220;heavy photons&#8221; or &#8220;dark photons&#8221; or &#8220;hidden sector photons&#8221;, in the mass range of $20$ MeV\/c$^2$ to $1000$ MeV\/c$^2$. Such particles will arise if there are additional U(1) gauge bosons in nature, and they will couple, albeit weakly, to electric charge through kinetic mixing. Many Beyond-the-Standard-Model theories predict the existence of additional U(1)&#8217;s, and recent observations of high energy electrons and positrons &nbsp;in the cosmic rays may be the result of primordial dark matter annihilating into heavy photons. HPS searches for electro-produced heavy photons that decay in di-lepton pairs using both invariant mass and separated decay vertex signatures. With good mass resolution, heavy photons will appear as sharp resonances above the QED continuum. For &nbsp;suitable values of mass and coupling, heavy photons will have long lifetimes, resulting in discernible secondary decay vertex. The HPS employs a large acceptance forward magnetic spectrometer with precise momentum measurement and vertexing capability, followed by a highly segmented lead-tungstate crystal electromagnetic calorimeter for fast &nbsp;triggering and electron identification. Tracks position is detected by silicon microstrips while the state-of-the-art data acquisition system based on 250MHz fADCs allows for high ratetriggering to fully exploit CEBAF CW, high intensity, electron beam.<\/p>\n\n\n\n<p>A muon identification system, just downstream of the ECal, significantly boosts the experimental reach for heavy photon masses above the di-muon threshold and provides an independent trigger. HPSprobes a unique region of the mass-coupling parameter space where the heavy photon signal would be lost in the trident background without the vertex signature, and it simultaneously accesses a region at higher coupling strength by relying on bump hunting alone. HPS is sensitive to a region of parameter space favored by accounting for the discrepancy between measured and calculated values for the muon&#8217;s g-2 with the existence of a heavy photon, and probes an extensive region suggested by parameters which could account for dark matter annihilations into heavy photons. In broader terms, HPS searches for heavy photons in a region suggested on very general theoretical grounds. With the final approval from JLab management, and US-DOE approval and funding, the HPS &nbsp;Collaboration can design, build and commission the experiment and begin in earnest its search for spectacular new physics at the Intensity Frontier.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Search for dark forces The Heavy Photon Search (HPS) is an experiment proposed for Jefferson Laboratory to search for new heavy vector boson(s), aka &#8220;heavy photons&#8221; or &#8220;dark photons&#8221; or &#8220;hidden sector photons&#8221;, in the mass range of $20$ MeV\/c$^2$ to $1000$ MeV\/c$^2$. Such particles will arise if there are additional U(1) gauge bosons in [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"wp-custom-template-pagina-senza-titolo-en","meta":{"footnotes":""},"class_list":["post-233","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/pages\/233","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/comments?post=233"}],"version-history":[{"count":1,"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/pages\/233\/revisions"}],"predecessor-version":[{"id":234,"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/pages\/233\/revisions\/234"}],"wp:attachment":[{"href":"https:\/\/web.infn.it\/jlab12\/wp-json\/wp\/v2\/media?parent=233"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}