增强 X 射线的光谱通量以解决超窄核跃迁问题

IF 8.1 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY
Elena Kuznetsova, Xiwen Zhang, Yuri Shvyd’ko, Marlan O. Scully, Olga Kocharovskaya
{"title":"增强 X 射线的光谱通量以解决超窄核跃迁问题","authors":"Elena Kuznetsova, Xiwen Zhang, Yuri Shvyd’ko, Marlan O. Scully, Olga Kocharovskaya","doi":"10.1103/physrevlett.133.193401","DOIUrl":null,"url":null,"abstract":"Recently, the 1.4 feV ultranarrow nuclear transition at 12.4 keV energy in <mjx-container ctxtmenu_counter=\"24\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(5 0 1 2 3 4)\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\"0,1,2,3,4\" data-semantic-collapsed=\"(5 0 1 2 3 4)\" data-semantic- data-semantic-owns=\"0 1 2 3 4\" data-semantic-role=\"unknown\" data-semantic-speech=\"Superscript 45 Baseline upper S c\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.645em;\">4</mjx-c><mjx-c style=\"padding-top: 0.645em;\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.634em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.669em;\">S</mjx-c><mjx-c style=\"padding-top: 0.669em;\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.643em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container> was resonantly excited for the first time using radiation from the self-seeded EuXFEL laser [Y. Shvyd’ko <i>et al.</i>, Resonant x-ray excitation of the nuclear clock isomer <mjx-container ctxtmenu_counter=\"25\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(5 0 1 2 3 4)\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\"0,1,2,3,4\" data-semantic-collapsed=\"(5 0 1 2 3 4)\" data-semantic- data-semantic-owns=\"0 1 2 3 4\" data-semantic-role=\"unknown\" data-semantic-speech=\"Superscript 45 Baseline upper S c\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.645em;\">4</mjx-c><mjx-c style=\"padding-top: 0.645em;\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.634em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.669em;\">S</mjx-c><mjx-c style=\"padding-top: 0.669em;\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.643em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container>, <span>Nature (London)</span> <b>622</b>, 471 (2023)], establishing <mjx-container ctxtmenu_counter=\"26\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(5 0 1 2 3 4)\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\"0,1,2,3,4\" data-semantic-collapsed=\"(5 0 1 2 3 4)\" data-semantic- data-semantic-owns=\"0 1 2 3 4\" data-semantic-role=\"unknown\" data-semantic-speech=\"Superscript 45 Baseline upper S c\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.645em;\">4</mjx-c><mjx-c style=\"padding-top: 0.645em;\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.634em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.669em;\">S</mjx-c><mjx-c style=\"padding-top: 0.669em;\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.643em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container> as a promising candidate for a future Mössbauer nuclear clock. While this experiment demonstrated a high potential of x-ray free-electron laser sources for resonantly exciting nuclear isomers in the hard x-ray range, it also highlighted a severe limitation in the achievable excitation level caused by their extremely large spectral bandwidth <mjx-container ctxtmenu_counter=\"27\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math breakable=\"true\" data-semantic-children=\"6,2,3,4\" data-semantic-collapsed=\"(10 (c 7 8 9) 6 2 3 4)\" data-semantic- data-semantic-owns=\"6 2 3 4\" data-semantic-role=\"text\" data-semantic-speech=\"tilde 1 e upper V\" data-semantic-structure=\"(10 (6 5 0 1) 2 3 4)\" data-semantic-type=\"punctuated\"><mjx-mrow data-semantic-added=\"true\" data-semantic-children=\"5,1\" data-semantic-content=\"0\" data-semantic- data-semantic-owns=\"5 0 1\" data-semantic-parent=\"10\" data-semantic-role=\"equality\" data-semantic-type=\"relseq\" inline-breaks=\"true\"><mjx-mrow data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"6\" data-semantic-role=\"unknown\" data-semantic-type=\"empty\"></mjx-mrow><mjx-break size=\"0\"></mjx-break><mjx-mo data-semantic- data-semantic-operator=\"relseq,∼\" data-semantic-parent=\"6\" data-semantic-role=\"equality\" data-semantic-type=\"relation\"><mjx-c>∼</mjx-c></mjx-mo><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"6\" data-semantic-role=\"integer\" data-semantic-type=\"number\" space=\"4\"><mjx-c>1</mjx-c></mjx-mn></mjx-mrow><mjx-mtext data-semantic-annotation=\"clearspeak:unit\" data-semantic- data-semantic-parent=\"10\" data-semantic-role=\"space\" data-semantic-type=\"text\" style='font-family: MJX-STX-ZERO, \"Helvetica Neue\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 3px;\" variant=\"-explicitFont\"> </mjx-utext></mjx-mtext><mjx-mtext data-semantic-annotation=\"clearspeak:unit\" data-semantic- data-semantic-parent=\"10\" data-semantic-role=\"space\" data-semantic-type=\"text\" style='font-family: MJX-STX-ZERO, \"Helvetica Neue\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 3px;\" variant=\"-explicitFont\"> </mjx-utext></mjx-mtext><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"10\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\" space=\"2\"><mjx-c noic=\"true\" style=\"padding-top: 0.657em;\">e</mjx-c><mjx-c style=\"padding-top: 0.657em;\">V</mjx-c></mjx-mi></mjx-math></mjx-container>. In this Letter, we propose a method to enhance the spectral flux of x-ray free-electron laser radiation using a resonant absorber with a longitudinal gradient in the nuclear transition frequency. A portion of the incident pulse can be absorbed into a nuclear collective excitation, and converted back into x-ray radiation by reversing the sign of the frequency gradient. Spectral narrowing and flux enhancement of this re-emitted x-ray field is achieved by using a reversed frequency gradient with a smaller magnitude than the initial one. About a hundredfold of such spectral flux enhancement is feasible in <mjx-container ctxtmenu_counter=\"28\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(12 (7 (5 0 1 2 3 4) 6) 11 (10 8 9))\"><mjx-mrow data-semantic-annotation=\"clearspeak:unit\" data-semantic-children=\"7,10\" data-semantic-content=\"11\" data-semantic- data-semantic-owns=\"7 11 10\" data-semantic-role=\"implicit\" data-semantic-speech=\"Superscript 45 Baseline upper S c Subscript 2 Baseline normal upper O 3\" data-semantic-type=\"infixop\"><mjx-msub data-semantic-children=\"5,6\" data-semantic- data-semantic-owns=\"5 6\" data-semantic-parent=\"12\" data-semantic-role=\"unknown\" data-semantic-type=\"subscript\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\"0,1,2,3,4\" data-semantic-collapsed=\"(5 0 1 2 3 4)\" data-semantic- data-semantic-owns=\"0 1 2 3 4\" data-semantic-parent=\"7\" data-semantic-role=\"unknown\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.645em;\">4</mjx-c><mjx-c style=\"padding-top: 0.645em;\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.634em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.669em;\">S</mjx-c><mjx-c style=\"padding-top: 0.669em;\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\"vertical-align: 0.396em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.643em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"5\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow><mjx-script style=\"vertical-align: -0.282em;\"><mjx-mrow size=\"s\"><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"7\" data-semantic-role=\"integer\" data-semantic-type=\"number\"><mjx-c>2</mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msub><mjx-mo data-semantic-added=\"true\" data-semantic- data-semantic-operator=\"infixop,⁢\" data-semantic-parent=\"12\" data-semantic-role=\"multiplication\" data-semantic-type=\"operator\"><mjx-c>⁢</mjx-c></mjx-mo><mjx-msub data-semantic-children=\"8,9\" data-semantic- data-semantic-owns=\"8 9\" data-semantic-parent=\"12\" data-semantic-role=\"latinletter\" data-semantic-type=\"subscript\"><mjx-mrow><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"10\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\"><mjx-c>O</mjx-c></mjx-mi></mjx-mrow><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mrow size=\"s\"><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"10\" data-semantic-role=\"integer\" data-semantic-type=\"number\"><mjx-c>3</mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msub></mjx-mrow></mjx-math></mjx-container> single crystal, rendering a more efficient source for nuclear excitation and facilitating the experimental observation of resonant fluorescence and coherent forward scattering at the 12.4 keV transition, both of which are essential for realizing a nuclear clock.","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"33 1","pages":""},"PeriodicalIF":8.1000,"publicationDate":"2024-11-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spectral Flux Enhancement of X Rays for Addressing Ultra Narrow Nuclear Transitions\",\"authors\":\"Elena Kuznetsova, Xiwen Zhang, Yuri Shvyd’ko, Marlan O. Scully, Olga Kocharovskaya\",\"doi\":\"10.1103/physrevlett.133.193401\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Recently, the 1.4 feV ultranarrow nuclear transition at 12.4 keV energy in <mjx-container ctxtmenu_counter=\\\"24\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math data-semantic-structure=\\\"(5 0 1 2 3 4)\\\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\\\"0,1,2,3,4\\\" data-semantic-collapsed=\\\"(5 0 1 2 3 4)\\\" data-semantic- data-semantic-owns=\\\"0 1 2 3 4\\\" data-semantic-role=\\\"unknown\\\" data-semantic-speech=\\\"Superscript 45 Baseline upper S c\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.645em;\\\">4</mjx-c><mjx-c style=\\\"padding-top: 0.645em;\\\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.634em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"identifier\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.669em;\\\">S</mjx-c><mjx-c style=\\\"padding-top: 0.669em;\\\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsuper\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.643em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container> was resonantly excited for the first time using radiation from the self-seeded EuXFEL laser [Y. Shvyd’ko <i>et al.</i>, Resonant x-ray excitation of the nuclear clock isomer <mjx-container ctxtmenu_counter=\\\"25\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math data-semantic-structure=\\\"(5 0 1 2 3 4)\\\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\\\"0,1,2,3,4\\\" data-semantic-collapsed=\\\"(5 0 1 2 3 4)\\\" data-semantic- data-semantic-owns=\\\"0 1 2 3 4\\\" data-semantic-role=\\\"unknown\\\" data-semantic-speech=\\\"Superscript 45 Baseline upper S c\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.645em;\\\">4</mjx-c><mjx-c style=\\\"padding-top: 0.645em;\\\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.634em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"identifier\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.669em;\\\">S</mjx-c><mjx-c style=\\\"padding-top: 0.669em;\\\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsuper\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.643em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container>, <span>Nature (London)</span> <b>622</b>, 471 (2023)], establishing <mjx-container ctxtmenu_counter=\\\"26\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math data-semantic-structure=\\\"(5 0 1 2 3 4)\\\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\\\"0,1,2,3,4\\\" data-semantic-collapsed=\\\"(5 0 1 2 3 4)\\\" data-semantic- data-semantic-owns=\\\"0 1 2 3 4\\\" data-semantic-role=\\\"unknown\\\" data-semantic-speech=\\\"Superscript 45 Baseline upper S c\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.645em;\\\">4</mjx-c><mjx-c style=\\\"padding-top: 0.645em;\\\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.634em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"identifier\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.669em;\\\">S</mjx-c><mjx-c style=\\\"padding-top: 0.669em;\\\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsuper\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.643em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container> as a promising candidate for a future Mössbauer nuclear clock. While this experiment demonstrated a high potential of x-ray free-electron laser sources for resonantly exciting nuclear isomers in the hard x-ray range, it also highlighted a severe limitation in the achievable excitation level caused by their extremely large spectral bandwidth <mjx-container ctxtmenu_counter=\\\"27\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math breakable=\\\"true\\\" data-semantic-children=\\\"6,2,3,4\\\" data-semantic-collapsed=\\\"(10 (c 7 8 9) 6 2 3 4)\\\" data-semantic- data-semantic-owns=\\\"6 2 3 4\\\" data-semantic-role=\\\"text\\\" data-semantic-speech=\\\"tilde 1 e upper V\\\" data-semantic-structure=\\\"(10 (6 5 0 1) 2 3 4)\\\" data-semantic-type=\\\"punctuated\\\"><mjx-mrow data-semantic-added=\\\"true\\\" data-semantic-children=\\\"5,1\\\" data-semantic-content=\\\"0\\\" data-semantic- data-semantic-owns=\\\"5 0 1\\\" data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"equality\\\" data-semantic-type=\\\"relseq\\\" inline-breaks=\\\"true\\\"><mjx-mrow data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"6\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"empty\\\"></mjx-mrow><mjx-break size=\\\"0\\\"></mjx-break><mjx-mo data-semantic- data-semantic-operator=\\\"relseq,∼\\\" data-semantic-parent=\\\"6\\\" data-semantic-role=\\\"equality\\\" data-semantic-type=\\\"relation\\\"><mjx-c>∼</mjx-c></mjx-mo><mjx-mn data-semantic-annotation=\\\"clearspeak:simple\\\" data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"6\\\" data-semantic-role=\\\"integer\\\" data-semantic-type=\\\"number\\\" space=\\\"4\\\"><mjx-c>1</mjx-c></mjx-mn></mjx-mrow><mjx-mtext data-semantic-annotation=\\\"clearspeak:unit\\\" data-semantic- data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"space\\\" data-semantic-type=\\\"text\\\" style='font-family: MJX-STX-ZERO, \\\"Helvetica Neue\\\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\\\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 3px;\\\" variant=\\\"-explicitFont\\\"> </mjx-utext></mjx-mtext><mjx-mtext data-semantic-annotation=\\\"clearspeak:unit\\\" data-semantic- data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"space\\\" data-semantic-type=\\\"text\\\" style='font-family: MJX-STX-ZERO, \\\"Helvetica Neue\\\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\\\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 3px;\\\" variant=\\\"-explicitFont\\\"> </mjx-utext></mjx-mtext><mjx-mi data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"identifier\\\" space=\\\"2\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.657em;\\\">e</mjx-c><mjx-c style=\\\"padding-top: 0.657em;\\\">V</mjx-c></mjx-mi></mjx-math></mjx-container>. In this Letter, we propose a method to enhance the spectral flux of x-ray free-electron laser radiation using a resonant absorber with a longitudinal gradient in the nuclear transition frequency. A portion of the incident pulse can be absorbed into a nuclear collective excitation, and converted back into x-ray radiation by reversing the sign of the frequency gradient. Spectral narrowing and flux enhancement of this re-emitted x-ray field is achieved by using a reversed frequency gradient with a smaller magnitude than the initial one. About a hundredfold of such spectral flux enhancement is feasible in <mjx-container ctxtmenu_counter=\\\"28\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math data-semantic-structure=\\\"(12 (7 (5 0 1 2 3 4) 6) 11 (10 8 9))\\\"><mjx-mrow data-semantic-annotation=\\\"clearspeak:unit\\\" data-semantic-children=\\\"7,10\\\" data-semantic-content=\\\"11\\\" data-semantic- data-semantic-owns=\\\"7 11 10\\\" data-semantic-role=\\\"implicit\\\" data-semantic-speech=\\\"Superscript 45 Baseline upper S c Subscript 2 Baseline normal upper O 3\\\" data-semantic-type=\\\"infixop\\\"><mjx-msub data-semantic-children=\\\"5,6\\\" data-semantic- data-semantic-owns=\\\"5 6\\\" data-semantic-parent=\\\"12\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"subscript\\\"><mjx-mrow><mjx-mmultiscripts data-semantic-children=\\\"0,1,2,3,4\\\" data-semantic-collapsed=\\\"(5 0 1 2 3 4)\\\" data-semantic- data-semantic-owns=\\\"0 1 2 3 4\\\" data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.645em;\\\">4</mjx-c><mjx-c style=\\\"padding-top: 0.645em;\\\">5</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.634em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-mi data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"identifier\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.669em;\\\">S</mjx-c><mjx-c style=\\\"padding-top: 0.669em;\\\">c</mjx-c></mjx-mi></mjx-mrow><mjx-scripts style=\\\"vertical-align: 0.396em;\\\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsuper\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.643em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"5\\\" data-semantic-role=\\\"rightsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow><mjx-script style=\\\"vertical-align: -0.282em;\\\"><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-annotation=\\\"clearspeak:simple\\\" data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"integer\\\" data-semantic-type=\\\"number\\\"><mjx-c>2</mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msub><mjx-mo data-semantic-added=\\\"true\\\" data-semantic- data-semantic-operator=\\\"infixop,⁢\\\" data-semantic-parent=\\\"12\\\" data-semantic-role=\\\"multiplication\\\" data-semantic-type=\\\"operator\\\"><mjx-c>⁢</mjx-c></mjx-mo><mjx-msub data-semantic-children=\\\"8,9\\\" data-semantic- data-semantic-owns=\\\"8 9\\\" data-semantic-parent=\\\"12\\\" data-semantic-role=\\\"latinletter\\\" data-semantic-type=\\\"subscript\\\"><mjx-mrow><mjx-mi data-semantic-annotation=\\\"clearspeak:simple\\\" data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"latinletter\\\" data-semantic-type=\\\"identifier\\\"><mjx-c>O</mjx-c></mjx-mi></mjx-mrow><mjx-script style=\\\"vertical-align: -0.15em;\\\"><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-annotation=\\\"clearspeak:simple\\\" data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"10\\\" data-semantic-role=\\\"integer\\\" data-semantic-type=\\\"number\\\"><mjx-c>3</mjx-c></mjx-mn></mjx-mrow></mjx-script></mjx-msub></mjx-mrow></mjx-math></mjx-container> single crystal, rendering a more efficient source for nuclear excitation and facilitating the experimental observation of resonant fluorescence and coherent forward scattering at the 12.4 keV transition, both of which are essential for realizing a nuclear clock.\",\"PeriodicalId\":20069,\"journal\":{\"name\":\"Physical review letters\",\"volume\":\"33 1\",\"pages\":\"\"},\"PeriodicalIF\":8.1000,\"publicationDate\":\"2024-11-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical review letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevlett.133.193401\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.133.193401","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

摘要

最近,利用自种子 EuXFEL 激光器的辐射,首次共振激发了 45Sc 中能量为 12.4 keV 的 1.4 feV 超宽核转变[Y. Shvyd'ko 等人,Resonant X-ray excitation of the nuclear clock isomer 45Sc,Nature (London) 622, 471 (2023)]。Shvyd'ko 等人,Resonant X-ray excitation of the nuclear clock isomer 45Sc,Nature (London) 622, 471 (2023)],将 45Sc 确立为未来莫斯鲍尔核时钟的候选者。该实验证明了 X 射线自由电子激光源在硬 X 射线范围内共振激发核同分异构体的巨大潜力,但同时也凸显了其超大光谱带宽 ∼ 1 eV 对可实现激发水平的严重限制。在这封信中,我们提出了一种利用核转变频率纵向梯度的谐振吸收器来增强 X 射线自由电子激光辐射光谱通量的方法。入射脉冲的一部分可以被吸收到核集体激发中,并通过反转频率梯度的符号将其转换回 X 射线辐射。通过使用幅度小于初始频率梯度的反向频率梯度,可以实现这种重新发射的 X 射线场的光谱收窄和通量增强。在 45Sc2O3 单晶体中,这种光谱通量增强约为原来的 100 倍,从而提供了更有效的核激发源,并促进了对 12.4 千伏跃迁的共振荧光和相干正向散射的实验观察,而这两者对于实现核时钟都是至关重要的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spectral Flux Enhancement of X Rays for Addressing Ultra Narrow Nuclear Transitions
Recently, the 1.4 feV ultranarrow nuclear transition at 12.4 keV energy in 45Sc was resonantly excited for the first time using radiation from the self-seeded EuXFEL laser [Y. Shvyd’ko et al., Resonant x-ray excitation of the nuclear clock isomer 45Sc, Nature (London) 622, 471 (2023)], establishing 45Sc as a promising candidate for a future Mössbauer nuclear clock. While this experiment demonstrated a high potential of x-ray free-electron laser sources for resonantly exciting nuclear isomers in the hard x-ray range, it also highlighted a severe limitation in the achievable excitation level caused by their extremely large spectral bandwidth 1eV. In this Letter, we propose a method to enhance the spectral flux of x-ray free-electron laser radiation using a resonant absorber with a longitudinal gradient in the nuclear transition frequency. A portion of the incident pulse can be absorbed into a nuclear collective excitation, and converted back into x-ray radiation by reversing the sign of the frequency gradient. Spectral narrowing and flux enhancement of this re-emitted x-ray field is achieved by using a reversed frequency gradient with a smaller magnitude than the initial one. About a hundredfold of such spectral flux enhancement is feasible in 45Sc2O3 single crystal, rendering a more efficient source for nuclear excitation and facilitating the experimental observation of resonant fluorescence and coherent forward scattering at the 12.4 keV transition, both of which are essential for realizing a nuclear clock.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Physical review letters
Physical review letters 物理-物理:综合
CiteScore
16.50
自引率
7.00%
发文量
2673
审稿时长
2.2 months
期刊介绍: Physical review letters(PRL)covers the full range of applied, fundamental, and interdisciplinary physics research topics: General physics, including statistical and quantum mechanics and quantum information Gravitation, astrophysics, and cosmology Elementary particles and fields Nuclear physics Atomic, molecular, and optical physics Nonlinear dynamics, fluid dynamics, and classical optics Plasma and beam physics Condensed matter and materials physics Polymers, soft matter, biological, climate and interdisciplinary physics, including networks
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信