{"id":224,"date":"2010-05-10T12:32:39","date_gmt":"2010-05-10T17:32:39","guid":{"rendered":"http:\/\/people.williams.edu\/pmajumde\/?page_id=224"},"modified":"2014-06-25T14:38:46","modified_gmt":"2014-06-25T19:38:46","slug":"indium-hfs","status":"publish","type":"page","link":"https:\/\/sites.williams.edu\/pmajumde\/current-experiments-and-apparatus\/indium-hfs\/","title":{"rendered":"Indium and Thallium HFS measurements"},"content":{"rendered":"

First measurement of 115<\/sup>In HFS in the 6P3\/2 excited state.<\/strong><\/h3>\n

In 2009, with the help of several Williams honors thesis students (Jared Strait ’07, Paul Hess ’08, Charles Cao ’09) as well as postdoctoral associate Dr. Mevan Gunawardena, we completed a diode laser \/ vapor cell spectroscopy experiment in indium. \u00a0Here is the 2009\u00a0Phys. Rev. A<\/a> <\/span><\/em>article describing this work.<\/p>\n

This experiment used two lasers — the 410 nm GaN diode laser system described above, as well as an InGaAs diode laser system operating at 1291 nm. \u00a0By overlapping the blue and IR lasers in a heated quartz indium cell, we perform two-step spectroscopy. \u00a0Here is a relevant energy level diagram<\/a>. <\/span><\/p>\n

The blue laser selects one velocity class of atoms for first-step excitation, so that the second step spectrum is nearly Doppler-free. \u00a0 We thus need to lock the blue laser to the first-step transition, and scan the IR laser, searching for the small absorption induced by the latter. Since only of order 1% of the atoms are selected by the blue laser, we detect the very weak IR absorption signal using lock-in detection. \u00a0We chop the blue light and detect the IR transmission in a photodiode phase-sensitively, giving us high signal-to-noise, background free hyperfine spectra of the excited 6P3\/2<\/sub> state. \u00a0Here is a layout of the blue laser locking, and two-laser spectroscopy setup.<\/a><\/span><\/span><\/p>\n

Quantum mechanical selection rules imply that the IR laser can drive only three of the four hyperfine transitions at a time. \u00a0We produce both 3-peak spectra, and, with the aid of an electro-optic modulator (EOM) to produce first-order FM sidebands to the laser, we also produce “9-peak spectra”, which are then fit to a sum of Lorentzians to obtain frequency splittings. \u00a0The EOM technique allows convenient calibration and linearization information for the scans, since we drive this device with an RF synthesizer of exactly known frequency.<\/span><\/span><\/p>\n

Three-peak spectra<\/a> <\/span><\/p>\n

[top scan is F=3,4,5 driven from the intermediate F’=4 state; \u00a0bottom scan is F=4,5,6 driven from F’=5]<\/em><\/span><\/p>\n

Nine-peak spectra<\/a><\/span><\/p>\n

We obtained the three hyperfine splittings of the F=3,4,5,6 manifold of the 6P3\/2 state with uncertainties of roughly 0.5 MHz. \u00a0This allows us to extract dipole, quadrupole, and octupole hyperfine constants for this state of indium for the first time. \u00a0The dipole constant agrees well (within 2%) with recent Safranova group calculations. \u00a0With additional atomic theory work, our precise measurement of the quadrupole hyperfine constant would allow the most precise determination to date of the Indium-115 nuclear quadrupole moment.<\/p>\n

Two-step spectroscopy in thallium for HFS \/ IS measurement<\/strong><\/p>\n

With a very similar two-step spectroscopy scheme, a GaN diode laser system operating at 377.7 nm in our lab, and the same IR laser system used for indium (now tuned to 1301 nm) we explored the thallium 7p1\/2-state hyperfine splitting, as well as the Tl-205 \/ Tl-203 isotope shift (see energy levels and schematic below). \u00a0By locking the laser in between the two isotopic resonances, we can excite both isotopes, and by controlling the relative propagation direction of UV and IR lasers, we can then distinguish the true isotope shift from the relative Doppler shift of the isotopic components. \u00a0Details of this work can be found both in this Physical Review article<\/a>, as well as in the theses of David Kealhofer ’13 and Gabby Vukasin ’14 (see home page).<\/p>\n

\"\"<\/a>\u00a0 \u00a0 \u00a0 \u00a0\"\"<\/a>\u00a0 \u00a0 \u00a0\"Tl_HFS_spectrum\"<\/a><\/p>\n

HFS \/ IS structure \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0Basic two-color setup \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 205Tl spectrum <\/span><\/p>\n","protected":false},"excerpt":{"rendered":"

First measurement of 115In HFS in the 6P3\/2 excited state. In 2009, with the help of several Williams honors thesis students (Jared Strait ’07, Paul Hess ’08, Charles Cao ’09) as well as postdoctoral associate Dr. Mevan Gunawardena, we completed … Continue reading →<\/span><\/a><\/p>\n","protected":false},"author":93,"featured_media":0,"parent":143,"menu_order":2,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-224","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/pages\/224","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/users\/93"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/comments?post=224"}],"version-history":[{"count":25,"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/pages\/224\/revisions"}],"predecessor-version":[{"id":466,"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/pages\/224\/revisions\/466"}],"up":[{"embeddable":true,"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/pages\/143"}],"wp:attachment":[{"href":"https:\/\/sites.williams.edu\/pmajumde\/wp-json\/wp\/v2\/media?parent=224"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}