Shock waves in the Tamm problem and the possibility of their experimental observation
The position of the singular electromagnetic shock waves arising in the smooth Tamm problem is found. They consist of the Cherenkov shock wave and shock waves arising when the charge velocity coincides with the velocity of light in medium. In the limit of small intervals of accelerated and decelerat...
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Veröffentlicht in: | Journal of mathematical physics 2005-02, Vol.46 (2), p.P1 |
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description | The position of the singular electromagnetic shock waves arising in the smooth Tamm problem is found. They consist of the Cherenkov shock wave and shock waves arising when the charge velocity coincides with the velocity of light in medium. In the limit of small intervals of accelerated and decelerated motion they are not transformed into the singular electromagnetic shock waves of the original Tamm problem. The reasons for this and the relation of the arising electromagnetic shock waves to the experimental situation are discussed. |
doi_str_mv | 10.1063/1.1836013 |
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N. ; Shilov, V. M. ; Stepanovsky, Yu. P.</creator><creatorcontrib>Afanasiev, G. N. ; Shilov, V. M. ; Stepanovsky, Yu. P.</creatorcontrib><description>The position of the singular electromagnetic shock waves arising in the smooth Tamm problem is found. They consist of the Cherenkov shock wave and shock waves arising when the charge velocity coincides with the velocity of light in medium. In the limit of small intervals of accelerated and decelerated motion they are not transformed into the singular electromagnetic shock waves of the original Tamm problem. The reasons for this and the relation of the arising electromagnetic shock waves to the experimental situation are discussed.</description><identifier>ISSN: 0022-2488</identifier><identifier>EISSN: 1089-7658</identifier><identifier>DOI: 10.1063/1.1836013</identifier><identifier>CODEN: JMAPAQ</identifier><language>eng</language><publisher>New York: American Institute of Physics</publisher><subject>Electromagnetism ; Mathematics ; Physics ; Velocity</subject><ispartof>Journal of mathematical physics, 2005-02, Vol.46 (2), p.P1</ispartof><rights>American Institute of Physics</rights><rights>Copyright American Institute of Physics Feb 2005</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c286t-da4f64eba039cf98012a70efae41906a271b072b363baaae673fb586a5b1fd653</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jmp/article-lookup/doi/10.1063/1.1836013$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1559,4512,27924,27925,76384,76390</link.rule.ids></links><search><creatorcontrib>Afanasiev, G. N.</creatorcontrib><creatorcontrib>Shilov, V. M.</creatorcontrib><creatorcontrib>Stepanovsky, Yu. P.</creatorcontrib><title>Shock waves in the Tamm problem and the possibility of their experimental observation</title><title>Journal of mathematical physics</title><description>The position of the singular electromagnetic shock waves arising in the smooth Tamm problem is found. They consist of the Cherenkov shock wave and shock waves arising when the charge velocity coincides with the velocity of light in medium. In the limit of small intervals of accelerated and decelerated motion they are not transformed into the singular electromagnetic shock waves of the original Tamm problem. The reasons for this and the relation of the arising electromagnetic shock waves to the experimental situation are discussed.</description><subject>Electromagnetism</subject><subject>Mathematics</subject><subject>Physics</subject><subject>Velocity</subject><issn>0022-2488</issn><issn>1089-7658</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNp9kF1LwzAYhYMoOKcX_oPgnUJnPto0vZThFwy8cLsOb9qEZbZNTbrp_r3dJnohePXC4eG85xyELimZUCL4LZ1QyQWh_AiNKJFFkotMHqMRIYwlLJXyFJ3FuCKEUpmmI7R4XfryDX_AxkTsWtwvDZ5D0-AueF2bBkNb7cXOx-i0q12_xd7uJBew-exMcI1pe6ix19GEDfTOt-foxEIdzcX3HaPFw_18-pTMXh6fp3ezpGRS9EkFqRWp0UB4UdpCEsogJ8aCSWlBBLCcapIzzQXXAGBEzq3OpIBMU1uJjI_R1cF3SPu-NrFXK78O7fBSMZoJlmW5HKDrA1SGoUMwVnVDZghbRYnajaao-h5tYG8ObCxdv6_yA298-AVVV9n_4L_OX4Awez0</recordid><startdate>200502</startdate><enddate>200502</enddate><creator>Afanasiev, G. N.</creator><creator>Shilov, V. M.</creator><creator>Stepanovsky, Yu. 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P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Shock waves in the Tamm problem and the possibility of their experimental observation</atitle><jtitle>Journal of mathematical physics</jtitle><date>2005-02</date><risdate>2005</risdate><volume>46</volume><issue>2</issue><spage>P1</spage><pages>P1-</pages><issn>0022-2488</issn><eissn>1089-7658</eissn><coden>JMAPAQ</coden><abstract>The position of the singular electromagnetic shock waves arising in the smooth Tamm problem is found. They consist of the Cherenkov shock wave and shock waves arising when the charge velocity coincides with the velocity of light in medium. In the limit of small intervals of accelerated and decelerated motion they are not transformed into the singular electromagnetic shock waves of the original Tamm problem. The reasons for this and the relation of the arising electromagnetic shock waves to the experimental situation are discussed.</abstract><cop>New York</cop><pub>American Institute of Physics</pub><doi>10.1063/1.1836013</doi><tpages>14</tpages></addata></record> |
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title | Shock waves in the Tamm problem and the possibility of their experimental observation |
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