Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>)
The QCD effective charge <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><...
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2022-05-01
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author | Alexandre Deur Volker Burkert Jian-Ping Chen Wolfgang Korsch |
author_facet | Alexandre Deur Volker Burkert Jian-Ping Chen Wolfgang Korsch |
author_sort | Alexandre Deur |
collection | DOAJ |
description | The QCD effective charge <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> is an observable that characterizes the magnitude of the strong interaction. At high momentum <i>Q</i>, it coincides with the QCD running coupling <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><mi mathvariant="normal">s</mi></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula>. At low <i>Q</i>, it offers a nonperturbative definition of the running coupling. We have extracted <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> from measurements carried out at Jefferson Lab that span the very low to moderately high <i>Q</i> domain, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mn>0.14</mn><mo>≤</mo><mi>Q</mi><mo>≤</mo><mn>2.18</mn></mrow></semantics></math></inline-formula> GeV. The precision of the new results is much improved over the previous extractions and the reach in <i>Q</i> at the lower end is significantly expanded. The data show that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> becomes <i>Q</i>-independent at very low <i>Q</i>. They compare well with two recent predictions of the QCD effective charge based on Dyson–Schwinger equations and on the AdS/CFT duality. |
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spelling | doaj.art-4f9081638cfc48eab8f21eeff65696b72023-11-23T18:23:56ZengMDPI AGParticles2571-712X2022-05-015217117910.3390/particles5020015Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>)Alexandre Deur0Volker Burkert1Jian-Ping Chen2Wolfgang Korsch3Thomas Jefferson National Accelerator Facility, Physics Division, Newport News, VA 23606, USAThomas Jefferson National Accelerator Facility, Physics Division, Newport News, VA 23606, USAThomas Jefferson National Accelerator Facility, Physics Division, Newport News, VA 23606, USADepartment of Physics & Astronomy, University of Kentucky, Lexington, KY 40506, USAThe QCD effective charge <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> is an observable that characterizes the magnitude of the strong interaction. At high momentum <i>Q</i>, it coincides with the QCD running coupling <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><mi mathvariant="normal">s</mi></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula>. At low <i>Q</i>, it offers a nonperturbative definition of the running coupling. We have extracted <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> from measurements carried out at Jefferson Lab that span the very low to moderately high <i>Q</i> domain, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mn>0.14</mn><mo>≤</mo><mi>Q</mi><mo>≤</mo><mn>2.18</mn></mrow></semantics></math></inline-formula> GeV. The precision of the new results is much improved over the previous extractions and the reach in <i>Q</i> at the lower end is significantly expanded. The data show that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>α</mi><msub><mi>g</mi><mn>1</mn></msub></msub><mrow><mo>(</mo><mi>Q</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> becomes <i>Q</i>-independent at very low <i>Q</i>. They compare well with two recent predictions of the QCD effective charge based on Dyson–Schwinger equations and on the AdS/CFT duality.https://www.mdpi.com/2571-712X/5/2/15strong interactionQCDnonperturbativerunning coupling constanthadronsnucleon |
spellingShingle | Alexandre Deur Volker Burkert Jian-Ping Chen Wolfgang Korsch Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) Particles strong interaction QCD nonperturbative running coupling constant hadrons nucleon |
title | Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) |
title_full | Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) |
title_fullStr | Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) |
title_full_unstemmed | Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) |
title_short | Experimental Determination of the QCD Effective Charge <i>α</i><sub><i>g</i>1</sub>(<i>Q</i>) |
title_sort | experimental determination of the qcd effective charge i α i sub i g i 1 sub i q i |
topic | strong interaction QCD nonperturbative running coupling constant hadrons nucleon |
url | https://www.mdpi.com/2571-712X/5/2/15 |
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