Saúl J.C. Salazar, Humberto G. Laguna, Robin P. Sagar
{"title":"Tuning Pair and Higher-Order Mutual Information Measures in Oscillator Systems with N-Dependent Frequencies","authors":"Saúl J.C. Salazar, Humberto G. Laguna, Robin P. Sagar","doi":"10.1002/adts.202400777","DOIUrl":null,"url":null,"abstract":"Analytical expressions for pair and higher-order mutual information measures in position and momentum space are examined for many-particle (<span data-altimg=\"/cms/asset/7a96fe85-1c08-4ed1-aa4e-e5cc85348515/adts202400777-math-0004.png\"></span><mjx-container ctxtmenu_counter=\"365\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0004.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0004\" display=\"inline\" location=\"graphic/adts202400777-math-0004.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\">N</mi>$N$</annotation></semantics></math></mjx-assistive-mml></mjx-container>) coupled oscillator systems in their ground states. These relations reveal that the magnitudes of the statistical correlations monotonically increase with the strength of the particle interaction for all particle numbers (<span data-altimg=\"/cms/asset/1df474c4-b958-4dda-961a-c98491554218/adts202400777-math-0005.png\"></span><mjx-container ctxtmenu_counter=\"366\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0005.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0005\" display=\"inline\" location=\"graphic/adts202400777-math-0005.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\">N</mi>$N$</annotation></semantics></math></mjx-assistive-mml></mjx-container>). On the other hand, the magnitudes of the measures monotonically decrease as <span data-altimg=\"/cms/asset/7ec68f81-bd35-4642-ac7d-7a9d437ce2bf/adts202400777-math-0006.png\"></span><mjx-container ctxtmenu_counter=\"367\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0006.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0006\" display=\"inline\" location=\"graphic/adts202400777-math-0006.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\">N</mi>$N$</annotation></semantics></math></mjx-assistive-mml></mjx-container> increases, when the intensities of the one- and two-body potentials are fixed. However, extremal points appear in the measures as <span data-altimg=\"/cms/asset/889c3488-e50d-4b78-813a-e7dc800d6af5/adts202400777-math-0007.png\"></span><mjx-container ctxtmenu_counter=\"368\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0007.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0007\" display=\"inline\" location=\"graphic/adts202400777-math-0007.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\">N</mi>$N$</annotation></semantics></math></mjx-assistive-mml></mjx-container> is varied, when the intensity of the one-body potential is <span data-altimg=\"/cms/asset/66a368db-36e5-492c-865e-415ce4b4b910/adts202400777-math-0008.png\"></span><mjx-container ctxtmenu_counter=\"369\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0008.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0008\" display=\"inline\" location=\"graphic/adts202400777-math-0008.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N\" data-semantic-type=\"identifier\">N</mi>$N$</annotation></semantics></math></mjx-assistive-mml></mjx-container>-dependent, and set at <span data-altimg=\"/cms/asset/9e1b650c-6a55-4a03-abce-7d571610c4f9/adts202400777-math-0009.png\"></span><mjx-container ctxtmenu_counter=\"370\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0009.png\"><mjx-semantics><mjx-msup data-semantic-children=\"0,3\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N Superscript negative alpha\" data-semantic-type=\"superscript\"><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: 0.363em; margin-left: 0.054em;\"><mjx-mrow data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic- data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\" size=\"s\"><mjx-mo data-semantic- data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" rspace=\"1\"><mjx-c></mjx-c></mjx-mo><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"3\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-mrow></mjx-script></mjx-msup></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0009\" display=\"inline\" location=\"graphic/adts202400777-math-0009.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msup data-semantic-=\"\" data-semantic-children=\"0,3\" data-semantic-role=\"latinletter\" data-semantic-speech=\"upper N Superscript negative alpha\" data-semantic-type=\"superscript\"><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"4\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\">N</mi><mrow data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-children=\"2\" data-semantic-content=\"1\" data-semantic-parent=\"4\" data-semantic-role=\"negative\" data-semantic-type=\"prefixop\"><mo data-semantic-=\"\" data-semantic-operator=\"prefixop,−\" data-semantic-parent=\"3\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\">−</mo><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"3\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\">α</mi></mrow></msup>$N^{-\\alpha }$</annotation></semantics></math></mjx-assistive-mml></mjx-container>. Fractional values of <span data-altimg=\"/cms/asset/95e6b672-a314-4bd4-b9f4-5c4526d80e03/adts202400777-math-0010.png\"></span><mjx-container ctxtmenu_counter=\"371\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400777-math-0010.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"greekletter\" data-semantic-speech=\"alpha\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400777:adts202400777-math-0010\" display=\"inline\" location=\"graphic/adts202400777-math-0010.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"greekletter\" data-semantic-speech=\"alpha\" data-semantic-type=\"identifier\">α</mi>$\\alpha$</annotation></semantics></math></mjx-assistive-mml></mjx-container> lead to the appearance of extremal points. These results illustrate how the intensity of the one-body potential can be used to tune the behavior of the statistical correlation measures in these systems.","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"49 1","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2024-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Theory and Simulations","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/adts.202400777","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MULTIDISCIPLINARY SCIENCES","Score":null,"Total":0}
引用次数: 0
Abstract
Analytical expressions for pair and higher-order mutual information measures in position and momentum space are examined for many-particle () coupled oscillator systems in their ground states. These relations reveal that the magnitudes of the statistical correlations monotonically increase with the strength of the particle interaction for all particle numbers (). On the other hand, the magnitudes of the measures monotonically decrease as increases, when the intensities of the one- and two-body potentials are fixed. However, extremal points appear in the measures as is varied, when the intensity of the one-body potential is -dependent, and set at . Fractional values of lead to the appearance of extremal points. These results illustrate how the intensity of the one-body potential can be used to tune the behavior of the statistical correlation measures in these systems.
期刊介绍:
Advanced Theory and Simulations is an interdisciplinary, international, English-language journal that publishes high-quality scientific results focusing on the development and application of theoretical methods, modeling and simulation approaches in all natural science and medicine areas, including:
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