{"title":"封面图片:投稿。等离子体物理学报。02/2025","authors":"","doi":"10.1002/ctpp.202590003","DOIUrl":null,"url":null,"abstract":"<p>Normalized vector potential (<i>a<sub>y</sub></i>), the produced wakefield (<i>E<sub>x</sub></i>), the momentum (<i>p<sub>x</sub></i>) and the electron density (<i>n<sub>x</sub></i>) for hydrogen atoms density/pre-ionized plasma density <i>n</i><sub>0</sub> = 0.01<i>n<sub>cr</sub></i> at time 810 fs for the field-ionized plasma (panel a) and the pre-ionized plasma (panel b) and normalized vector potential variation <i>a</i><sub>0</sub> = 1 (in panels a1 and b1), <i>a</i><sub>0</sub> = 2 (in panels a2 and b2), and <i>a</i><sub>0</sub> = 3 (in panels a3 and b3). Fig. 4 of the paper by Elnaz Khalilzadeh et al. https://doi.org/10.1002/ctpp.202400022\n \n <figure>\n <div><picture>\n <source></source></picture><p></p>\n </div>\n </figure></p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"65 2","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2025-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202590003","citationCount":"0","resultStr":"{\"title\":\"Cover Picture: Contrib. Plasma Phys. 02/2025\",\"authors\":\"\",\"doi\":\"10.1002/ctpp.202590003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Normalized vector potential (<i>a<sub>y</sub></i>), the produced wakefield (<i>E<sub>x</sub></i>), the momentum (<i>p<sub>x</sub></i>) and the electron density (<i>n<sub>x</sub></i>) for hydrogen atoms density/pre-ionized plasma density <i>n</i><sub>0</sub> = 0.01<i>n<sub>cr</sub></i> at time 810 fs for the field-ionized plasma (panel a) and the pre-ionized plasma (panel b) and normalized vector potential variation <i>a</i><sub>0</sub> = 1 (in panels a1 and b1), <i>a</i><sub>0</sub> = 2 (in panels a2 and b2), and <i>a</i><sub>0</sub> = 3 (in panels a3 and b3). Fig. 4 of the paper by Elnaz Khalilzadeh et al. https://doi.org/10.1002/ctpp.202400022\\n \\n <figure>\\n <div><picture>\\n <source></source></picture><p></p>\\n </div>\\n </figure></p>\",\"PeriodicalId\":10700,\"journal\":{\"name\":\"Contributions to Plasma Physics\",\"volume\":\"65 2\",\"pages\":\"\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2025-02-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202590003\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Contributions to Plasma Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202590003\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, FLUIDS & PLASMAS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Contributions to Plasma Physics","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202590003","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
Normalized vector potential (ay), the produced wakefield (Ex), the momentum (px) and the electron density (nx) for hydrogen atoms density/pre-ionized plasma density n0 = 0.01ncr at time 810 fs for the field-ionized plasma (panel a) and the pre-ionized plasma (panel b) and normalized vector potential variation a0 = 1 (in panels a1 and b1), a0 = 2 (in panels a2 and b2), and a0 = 3 (in panels a3 and b3). Fig. 4 of the paper by Elnaz Khalilzadeh et al. https://doi.org/10.1002/ctpp.202400022