{"id":198,"date":"2020-06-16T00:26:48","date_gmt":"2020-06-16T00:26:48","guid":{"rendered":"http:\/\/www.physics.lbl.gov\/qiscom\/?page_id=198"},"modified":"2026-03-27T16:36:02","modified_gmt":"2026-03-27T16:36:02","slug":"qis-for-hep","status":"publish","type":"page","link":"https:\/\/www.physics.lbl.gov\/qiscom\/qis-for-hep\/","title":{"rendered":"QIS For HEP"},"content":{"rendered":"<h1 style=\"text-align: center\">Quantum Sensors for Dark Matter Detection<\/h1>\n<p>&nbsp;<\/p>\n<div style=\"margin:auto;\">\n<h2>Superconducting Sensors<\/h2>\n<p>Our Superconducting quantum sensor work focuses on understanding and pushing the limits of phonon energy resolution. This includes investigating the origin of the Low Energy Excess (LEE) background in superconducting devices, from transition edge sensors to qubits. We collaborate with LBNL and UC Berkeley materials scientists to understand he connections between materials and processing and performance. Examples of this work can be found at phononics.lbl.gov. We also collaborate closely with the TESSERACT collaboration for device testing and LEE characterization (see for example https:\/\/doi.org\/10.1063\/5.0247343)<\/p>\n<p>we have developed a process for low Tc kinetic microwave inductance detectors (MKID) using hafnium (arXiv:2502.19818). This was a necessary step towards the development of quasiparticle trapping MKIDs, which would enable RF readout of future dark matter search experiments. We are also applying this to Josephson Johnson (JJ) devices, such as SQUATs using JJ fabrication at foundry.lbl.gov<\/p>\n<p><figure id=\"attachment_314\" aria-describedby=\"caption-attachment-314\" style=\"width: 1280px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03.png\" alt=\"Superconducting resonator fabricated on a suspended membrane to investigate phonon coupling effects on quality factor\" width=\"1280\" height=\"775\" class=\"size-full wp-image-314\" srcset=\"https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03.png 1280w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-300x182.png 300w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-1024x620.png 1024w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-768x465.png 768w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-100x61.png 100w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-150x91.png 150w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-200x121.png 200w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-450x272.png 450w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-600x363.png 600w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Sensor03-900x545.png 900w\" sizes=\"(max-width: 1280px) 100vw, 1280px\" \/><figcaption id=\"caption-attachment-314\" class=\"wp-caption-text\">Superconducting resonator fabricated on a suspended membrane to investigate phonon coupling effects on quality factor<\/figcaption><\/figure><br \/>\n<figure id=\"attachment_309\" aria-describedby=\"caption-attachment-309\" style=\"width: 1155px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team.png\" alt=\"Superconducting Sensors Group\" width=\"1155\" height=\"873\" class=\"size-full wp-image-309\" srcset=\"https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team.png 1155w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-300x227.png 300w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-1024x774.png 1024w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-768x580.png 768w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-100x76.png 100w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-150x113.png 150w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-200x151.png 200w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-450x340.png 450w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-600x454.png 600w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Superconducting_Sensors_Team-900x680.png 900w\" sizes=\"(max-width: 1155px) 100vw, 1155px\" \/><figcaption id=\"caption-attachment-309\" class=\"wp-caption-text\">Superconducting Sensors @ LBNL<\/figcaption><\/figure><\/p>\n<h2>Optomechanical Sensors<\/h2>\n<p>Our program has given rise to two new experiments exploiting optomechanical quantum measurement:<\/p>\n<div style=\"padding-left:40px;padding-right:60px;\">\n<ul>\n<li>Use of levitated superconducting devices to search for gravitational waves, in particular those with frequencies in the 10 kHz-10 MHz range, which is above LIGO&#8217;s detection band (arXiv:2408.01583)<\/li>\n<li>Quantum Invisible Particle Sensor (QuIPS), in collaboration with Yale U.,  uses optically levitated nanospheres, loaded with beta emitters, together with conventional electron particle detectors to fully reconstruct the 4 momentum of emitted invisible particles, such as (sterile) neutrinos ((PRX Quantum 4 (2023) 1, 010315).  We aim to use squeezed light to make boost the sensitivity   (arXiv:2502.05168). In addition to the quantum techniques for measuring levitated particle recoil, this project involves challenges of low momentum electron track reconstruction and loading nanoparticles with radioactive isotopes.<\/li>\n<\/ul>\n<\/div>\n<p>At a more theoretical level, we produced important results related to experimental tests<br \/>\nof quantum gravity. One, arXiv: 2409.03894, settled a long-standing debate about the size of vacuum fluctuations in the gravitational field and their effect on a gravitational wave detector. The other, arXiv:2502.17575, proposes a concrete model of Verlinde&#8217;s &#8220;entropic gravity&#8221; and a number of experimental tests. This work strongly motivated a Heising-Simons funded experiment with UC Berkeley,  which looks for anomalous noise in the gravitational interaction.<\/p>\n<p><figure id=\"attachment_310\" aria-describedby=\"caption-attachment-310\" style=\"width: 677px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors.png\" alt=\"Detector to measure momentum vector if beta electrons emitted from optically levitated nanospheres (QuIPS experiment)\" width=\"677\" height=\"909\" class=\"size-full wp-image-310\" srcset=\"https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors.png 677w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-223x300.png 223w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-100x134.png 100w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-150x201.png 150w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-200x269.png 200w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-300x403.png 300w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-450x604.png 450w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/Optomechanical_Sensors-600x806.png 600w\" sizes=\"(max-width: 677px) 100vw, 677px\" \/><figcaption id=\"caption-attachment-310\" class=\"wp-caption-text\">Detector to measure momentum vector if beta electrons emitted from optically levitated nanospheres (QuIPS experiment)<\/figcaption><\/figure><br \/>\n<figure id=\"attachment_311\" aria-describedby=\"caption-attachment-311\" style=\"width: 1000px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS.png\" alt=\"QuIPS Group\" width=\"1000\" height=\"726\" class=\"size-full wp-image-311\" srcset=\"https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS.png 1000w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-300x218.png 300w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-768x558.png 768w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-100x73.png 100w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-150x109.png 150w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-200x145.png 200w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-450x327.png 450w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-600x436.png 600w, https:\/\/www.physics.lbl.gov\/qiscom\/wp-content\/uploads\/sites\/51\/2026\/03\/QiPS-900x653.png 900w\" sizes=\"(max-width: 1000px) 100vw, 1000px\" \/><figcaption id=\"caption-attachment-311\" class=\"wp-caption-text\">QuIPS @ LBNL<\/figcaption><\/figure>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Quantum Sensors for Dark Matter Detection &nbsp; Superconducting Sensors Our Superconducting quantum sensor work focuses on understanding and pushing the limits of phonon energy resolution. This includes investigating the origin of the Low Energy Excess (LEE) background in superconducting devices, &hellip;<\/p>\n<p class=\"read-more\"> <a class=\"more-link\" href=\"https:\/\/www.physics.lbl.gov\/qiscom\/qis-for-hep\/\"> <span class=\"screen-reader-text\">QIS For HEP<\/span> Read More &raquo;<\/a><\/p>\n","protected":false},"author":7,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"_links":{"self":[{"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/pages\/198"}],"collection":[{"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/users\/7"}],"replies":[{"embeddable":true,"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/comments?post=198"}],"version-history":[{"count":14,"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/pages\/198\/revisions"}],"predecessor-version":[{"id":316,"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/pages\/198\/revisions\/316"}],"wp:attachment":[{"href":"https:\/\/www.physics.lbl.gov\/qiscom\/wp-json\/wp\/v2\/media?parent=198"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}