{"id":37187,"date":"2025-05-19T17:35:50","date_gmt":"2025-05-19T10:35:50","guid":{"rendered":"https:\/\/1dddev.com\/physicssci\/?post_type=ku-personnel&#038;p=37187"},"modified":"2025-05-19T17:36:16","modified_gmt":"2025-05-19T10:36:16","slug":"%e0%b8%9c%e0%b8%a8-%e0%b8%94%e0%b8%a3-%e0%b8%aa%e0%b8%a1%e0%b8%b2%e0%b8%99-%e0%b8%a1%e0%b8%87%e0%b8%84%e0%b8%87%e0%b8%aa%e0%b8%81%e0%b8%b8%e0%b8%a5%e0%b8%a7%e0%b8%87%e0%b8%a8%e0%b9%8c","status":"publish","type":"ku-personnel","link":"https:\/\/1dddev.com\/physicssci\/ku-personnel\/%e0%b8%9c%e0%b8%a8-%e0%b8%94%e0%b8%a3-%e0%b8%aa%e0%b8%a1%e0%b8%b2%e0%b8%99-%e0%b8%a1%e0%b8%87%e0%b8%84%e0%b8%87%e0%b8%aa%e0%b8%81%e0%b8%b8%e0%b8%a5%e0%b8%a7%e0%b8%87%e0%b8%a8%e0%b9%8c\/","title":{"rendered":"\u0e1c\u0e28.\u0e14\u0e23.\u0e2a\u0e21\u0e32\u0e19 \u0e21\u0e07\u0e04\u0e07\u0e2a\u0e01\u0e38\u0e25\u0e27\u0e07\u0e28\u0e4c"},"content":{"rendered":"\n<p><strong>\u0e2b\u0e49\u0e2d\u0e07:<\/strong> SC45-677<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">\u0e1b\u0e23\u0e30\u0e27\u0e31\u0e15\u0e34\u0e2a\u0e48\u0e27\u0e19\u0e15\u0e31\u0e27<\/h2>\n\n\n\n<p><strong>\u0e01\u0e32\u0e23\u0e28\u0e36\u0e01\u0e29\u0e32<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>2548\u00a0\u00a0 \u0e1b\u0e23.\u0e14.(\u0e04\u0e13\u0e34\u0e15\u0e28\u0e32\u0e2a\u0e15\u0e23\u0e4c) \u0e21.\u0e21\u0e2b\u0e34\u0e14\u0e25 \u0e01\u0e31\u0e1a Prof. I. Ming Tang<\/li>\n\n\n\n<li>\u0e27\u0e17.\u0e21.(\u0e1f\u0e34\u0e2a\u0e34\u0e01\u0e2a\u0e4c) \u0e08\u0e38\u0e2c\u0e32\u0e25\u0e07\u0e01\u0e23\u0e13\u0e4c\u0e21\u0e2b\u0e32\u0e27\u0e34\u0e17\u0e22\u0e32\u0e25\u0e31\u0e22<\/li>\n\n\n\n<li>\u0e01\u0e28.\u0e1a.(\u0e27\u0e34\u0e17\u0e22\u0e4c-\u0e1f\u0e34\u0e2a\u0e34\u0e01\u0e2a\u0e4c)<\/li>\n<\/ul>\n\n\n\n<p><strong>\u0e1b\u0e23\u0e30\u0e2a\u0e1a\u0e01\u0e32\u0e23\u0e13\u0e4c\u0e01\u0e32\u0e23\u0e17\u0e33\u0e07\u0e32\u0e19<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>2535 &#8211; \u0e1b\u0e31\u0e08\u0e08\u0e38\u0e1a\u0e31\u0e19 \u0e2d\u0e32\u0e08\u0e32\u0e23\u0e22\u0e4c\u0e1b\u0e23\u0e30\u0e08\u0e33\u0e20\u0e32\u0e04\u0e27\u0e34\u0e0a\u0e32\u0e1f\u0e34\u0e2a\u0e34\u0e01\u0e2a\u0e4c\u00a0\u0e04\u0e13\u0e30\u0e27\u0e34\u0e17\u0e22\u0e32\u0e28\u0e32\u0e2a\u0e15\u0e23\u0e4c \u0e21\u0e2b\u0e32\u0e27\u0e34\u0e17\u0e22\u0e32\u0e25\u0e31\u0e22\u0e40\u0e01\u0e29\u0e15\u0e23\u0e28\u0e32\u0e2a\u0e15\u0e23\u0e4c<\/li>\n<\/ul>\n\n\n\n<p><strong>\u0e07\u0e32\u0e19\u0e27\u0e34\u0e08\u0e31\u0e22<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>\u0e01\u0e32\u0e23\u0e27\u0e34\u0e40\u0e04\u0e23\u0e32\u0e30\u0e2b\u0e4c\u0e1b\u0e31\u0e0d\u0e2b\u0e32\u0e01\u0e32\u0e23\u0e40\u0e04\u0e25\u0e37\u0e48\u0e2d\u0e19\u0e17\u0e35\u0e48\u0e02\u0e2d\u0e07\u0e08\u0e38\u0e14\u0e28\u0e39\u0e19\u0e22\u0e4c\u0e01\u0e25\u0e32\u0e07\u0e21\u0e27\u0e25\u0e02\u0e2d\u0e07\u0e04\u0e19\u0e42\u0e14\u0e1a\u0e2a\u0e23\u0e49\u0e32\u0e07\u0e41\u0e1a\u0e1a\u0e08\u0e33\u0e25\u0e2d\u0e07\u0e1f\u0e34\u0e2a\u0e34\u0e01\u0e04\u0e31\u0e25\u0e40\u0e1e\u0e19\u0e14\u0e39\u0e25\u0e31\u0e21\u0e41\u0e1a\u0e1a\u0e01\u0e25\u0e31\u0e1a<\/li>\n\n\n\n<li>\u0e01\u0e32\u0e23\u0e41\u0e01\u0e49\u0e1b\u0e31\u0e0d\u0e2b\u0e32\u0e41\u0e1a\u0e1a\u0e44\u0e21\u0e48\u0e40\u0e1b\u0e47\u0e19\u0e40\u0e0a\u0e34\u0e07\u0e40\u0e2a\u0e49\u0e19\u0e14\u0e49\u0e27\u0e22\u0e27\u0e34\u0e18\u0e35 Parametric solution \u0e1b\u0e23\u0e30\u0e01\u0e2d\u0e1a\u0e14\u0e49\u0e27\u0e22 self-consistency equations \u0e41\u0e25\u0e30 order parameter equations \u0e42\u0e14\u0e22\u0e2b\u0e32\u0e17\u0e35\u0e48\u0e21\u0e32\u0e08\u0e32\u0e01 nonlinear Fokker-Planck equations<\/li>\n\n\n\n<li>\u0e01\u0e32\u0e23\u0e04\u0e04\u0e32\u0e19\u0e27\u0e13\u0e1b\u0e31\u0e0d\u0e2b\u0e32\u0e02\u0e2d\u0e07\u0e01\u0e25\u0e38\u0e48\u0e21\u0e2d\u0e19\u0e38\u0e20\u0e32\u0e04\u0e17\u0e35\u0e48\u0e01\u0e33\u0e25\u0e31\u0e07\u0e40\u0e04\u0e25\u0e37\u0e48\u0e2d\u0e19\u0e17\u0e35\u0e48\u0e43\u0e19\u0e40\u0e04\u0e23\u0e37\u0e48\u0e2d\u0e07\u0e40\u0e23\u0e48\u0e07\u0e2d\u0e19\u0e38\u0e20\u0e32\u0e04 \u0e42\u0e14\u0e22\u0e43\u0e0a\u0e49\u0e17\u0e24\u0e29\u0e0e\u0e35\u0e02\u0e2d\u0e07 Haissinski \u0e43\u0e19\u0e01\u0e23\u0e13\u0e35\u0e02\u0e2d\u0e07 nonextensive thermostatistical<\/li>\n<\/ul>\n\n\n\n<p><strong>\u0e1c\u0e25\u0e07\u0e32\u0e19\u0e27\u0e34\u0e08\u0e31\u0e22\u0e15\u0e35\u0e1e\u0e34\u0e21\u0e1e\u0e4c<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Frank, TD, SAMAN MONGKOLSAKULVONG, &#8220;Parametric solution method for self -consistency equations and order parameter equations derived from nonlinear Fokker-Planck equations&#8221;, PHYSICA D-NONLINEAR PHENOMENA 238 (14) (2009) 1186 -1196<\/li>\n\n\n\n<li>Frank, TD, SAMAN MONGKOLSAKULVONG, &#8220;A nonextensive thermostatistical approach to the Haissinski theory of accelerator beams&#8221;, PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS 387 (19 -20) (2008) 4828-4838<\/li>\n\n\n\n<li>SAMAN MONGKOLSAKULVONG, &#8220;Extension of Mean Field Theory and General Form of Order Parameter&#8221;, Kasetsart Journal (Natural Science) 41 (1) (2007) 192 -197<\/li>\n\n\n\n<li>SAMAN MONGKOLSAKULVONG, Frank, TD, Tang, IM, &#8220;On a leveraging effect of weak azimuthal inhomogeneities explaining the nonuniqueness ofcritical Maier-Saupe order parameters&#8221;, PHASE TRANSITIONS 80 (9) (2007) 967 -9807<\/li>\n<\/ul>\n\n\n\n<p><strong>\u0e07\u0e32\u0e19\u0e2a\u0e2d\u0e19<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Special Problems<\/li>\n\n\n\n<li>General Physics I<\/li>\n\n\n\n<li>General Physics II<\/li>\n\n\n\n<li>Laboratory in Abridged Physics<\/li>\n\n\n\n<li>Laboratory in Physics I<\/li>\n\n\n\n<li>Methods of Theoretical Physics I<\/li>\n\n\n\n<li>Physics of Waves<\/li>\n<\/ul>\n","protected":false},"featured_media":37188,"parent":0,"template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-37187","ku-personnel","type-ku-personnel","status-publish","has-post-thumbnail","hentry"],"acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v26.3 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>\u0e1c\u0e28.\u0e14\u0e23.\u0e2a\u0e21\u0e32\u0e19 \u0e21\u0e07\u0e04\u0e07\u0e2a\u0e01\u0e38\u0e25\u0e27\u0e07\u0e28\u0e4c - \u0e20\u0e32\u0e04\u0e27\u0e34\u0e0a\u0e32\u0e1f\u0e34\u0e2a\u0e34\u0e01\u0e2a\u0e4c \u0e04\u0e13\u0e30\u0e27\u0e34\u0e17\u0e22\u0e32\u0e28\u0e32\u0e2a\u0e15\u0e23\u0e4c 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