{"id":106,"date":"2021-09-10T10:04:10","date_gmt":"2021-09-10T10:04:10","guid":{"rendered":"https:\/\/ultracoldtest.quantumlah.org\/?page_id=106"},"modified":"2025-09-26T16:41:48","modified_gmt":"2025-09-26T08:41:48","slug":"non-abelian-gauge-field","status":"publish","type":"page","link":"https:\/\/ultracold.quantumlah.org\/?page_id=106","title":{"rendered":"Non-Abelian Gauge Field"},"content":{"rendered":"\n<h1 class=\"wp-block-heading\">Introducing more symmetries by dressing an ultracold gas with lasers<\/h1>\n\n\n\n<p class=\"wp-block-paragraph\">We explore quantum simulations mimicking Hamiltonians with an artificial gauge field. While most research in the ultracold atoms community focuses on lattices, to address Hubbard-like Hamiltonians for condensed-matter problems, we followed an alternative path generating gauge fields for bulk systems. Apart from its simplicity, this approach gives more diversity in gauge field structures and symmetries and allows for addressing problems ranging from quantum information to high-energy physics. The first experiment was dedicated to\u00a0non-Abelian transformations to create geometrical qubits, which are known to be less prone to errors than normal qubits\u00a0[1]. We then explored the matter-wave dynamic in SU(2) symmetry and found that it is governed by a non-inertial force leading to the spin-Hall effect and generalization of the\u00a0Zitterbewegung\u00a0relativistic effect in a two-dimensional non-Abelian gauge field [2], [3]. To create our artificial SU(2) gauge field, we suggested the so-called tripod scheme: a generalization of the celebrated \u039b-scheme, used in electromagnetic-induced transparency. We extended the application domain of the tripod scheme, created an atomic Datta-Das transistor for atomtronic circuits\u00a0[4], and proposed a new test of the Born rules\u00a0[5]. We proposed a further extension of the tripod scheme to address SU(3) symmetry problems\u00a0[6]\u00a0that we are currently implementing in one of our experiments.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img fetchpriority=\"high\" decoding=\"async\" width=\"1560\" height=\"904\" src=\"https:\/\/ultracoldtest.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup.jpeg\" alt=\"\" class=\"wp-image-217\" style=\"width:507px;height:294px\" srcset=\"https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup.jpeg 1560w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup-300x174.jpeg 300w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup-1024x593.jpeg 1024w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup-768x445.jpeg 768w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup-1536x890.jpeg 1536w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Setup-496x287.jpeg 496w\" sizes=\"(max-width: 1560px) 100vw, 1560px\" \/><figcaption class=\"wp-element-caption\"><em>Figure: (a) Tripod scheme. Black arrow indicates tripod beams, red arrows indicate spin-sensitive imaging system and purple arrows indicate doppler cooling in the far-off resonant trap. (b) Arrangement of the tripod beam.<\/em><\/figcaption><\/figure>\n<\/div>\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img decoding=\"async\" width=\"1024\" height=\"631\" src=\"https:\/\/ultracoldtest.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature-1024x631.jpeg\" alt=\"\" class=\"wp-image-218\" style=\"width:447px;height:275px\" srcset=\"https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature-1024x631.jpeg 1024w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature-300x185.jpeg 300w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature-768x473.jpeg 768w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature-487x300.jpeg 487w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2021\/09\/Geometric_Temperature.jpeg 1188w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\"><em>Ground state population evolution during Ballistic expansion of a cold gas in presence of the non-Abelian gauge field<\/em>.<\/figcaption><\/figure>\n<\/div>\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img decoding=\"async\" width=\"844\" height=\"646\" src=\"https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2023\/02\/QM.jpg\" alt=\"\" class=\"wp-image-567\" style=\"width:422px;height:323px\" srcset=\"https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2023\/02\/QM.jpg 844w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2023\/02\/QM-300x230.jpg 300w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2023\/02\/QM-768x588.jpg 768w, https:\/\/ultracold.quantumlah.org\/wp-content\/uploads\/2023\/02\/QM-392x300.jpg 392w\" sizes=\"(max-width: 844px) 100vw, 844px\" \/><figcaption class=\"wp-element-caption\"><em>Figure: (a) Oscillation of an atomic wave-packet in a homogenous non-Abelian gauge field. (b) the discrete velocity distribution, obtained after time of flight, indicates the quantum nature of the phenomenon. (c) Spin texture showing non-zero winding number.<\/em><\/figcaption><\/figure>\n<\/div>\n\n\n<div style=\"height:40px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p class=\"wp-block-paragraph\">[1]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; F. Leroux, K. Pandey, R. Rebhi, F. Chevy, C. Miniatura, B. Gremaud, and D. Wilkowski,&nbsp;<em>Non-Abelian and adiabatic geometric transformation in a cold atomic gas<\/em>,&nbsp;Nature Communications&nbsp;<strong>9<\/strong>, 3580 (2018). <a rel=\"noreferrer noopener\" href=\"https:\/\/www.nature.com\/articles\/s41467-018-05865-3\" data-type=\"URL\" data-id=\"https:\/\/www.nature.com\/articles\/s41467-018-05865-3\" target=\"_blank\">doi: 10.1038\/s41467-018-05865-3<\/a>.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[2]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; M. Hasan&nbsp; C. Madasu, K. Rathod, C. C. Kwong, C. Miniatura, F. Chevy and D. Wilkowski, <em>Wave-packet Dynamics in Synthetic Non-Abelian Gauge Fields<\/em>, Phys. Rev. Lett.,&nbsp;<strong>129<\/strong>, 130402 (2022). <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.129.130402\" data-type=\"URL\" target=\"_blank\" rel=\"noreferrer noopener\">doi.org\/10.1103\/PhysRevLett.129.130402<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[3]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; M. Hasan, C. S. Madasu, K. D. Rathod, C. C. Kwong, D. Wilkowski,&nbsp;<em>Evolution of an ultracold gas in a non-Abelian gauge fields: Finite temperature effect<\/em>, Q. Elec&nbsp;<strong>52<\/strong>, 532 (2022). <a href=\"https:\/\/iopscience.iop.org\/article\/10.1070\/QEL18071\" data-type=\"URL\" data-id=\"https:\/\/iopscience.iop.org\/article\/10.1070\/QEL18071\" target=\"_blank\" rel=\"noreferrer noopener\">doi: 10.1070\/QEL18071<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[4]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; C. S. Madasu, M. Hasan, K. D. Rathod, C. C. Kwong, D. Wilkowski,&nbsp;<em>Datta-Das transistor for atomtronic circuits using artificial gauge fields,&nbsp;<\/em>Phys. Rev. R&nbsp;<strong>4<\/strong>, 033180 (2022). <a href=\"https:\/\/link.aps.org\/doi\/10.1103\/PhysRevResearch.4.033180\" data-type=\"URL\" data-id=\"https:\/\/link.aps.org\/doi\/10.1103\/PhysRevResearch.4.033180\" target=\"_blank\" rel=\"noreferrer noopener\">doi: 10.1103\/PhysRevResearch.4.033180<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[5]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; K. S. Lee, Z. Zhuo, C. Couteau, D. Wilkowski, and T. Paterek, <em>An atomic test of higher-order interference<\/em>, Phys. Rev. A&nbsp;<strong>101<\/strong>, 183101 (2020). <a rel=\"noreferrer noopener\" href=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.101.052111\" data-type=\"URL\" data-id=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.101.052111\" target=\"_blank\">doi: 10.1103\/PhysRevA.101.052111<\/a>.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[6]&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Y.-X. Hu, C. Miniatura, D. Wilkowski, and B. Gr\u00e9maud, <em>U(3) artificial gauge fields for cold atoms<\/em>, Phys. Rev. A&nbsp;<strong>90<\/strong>, 023601 (2014). <a rel=\"noreferrer noopener\" href=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.90.023601\" data-type=\"URL\" data-id=\"https:\/\/journals.aps.org\/pra\/abstract\/10.1103\/PhysRevA.90.023601\" target=\"_blank\">doi: 10.1103\/PhysRevA.90.023601<\/a>.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Introducing more symmetries by dressing an ultracold gas with lasers We explore quantum simulations mimicking Hamiltonians with an artificial gauge field. 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