@misc{oai:repo.qst.go.jp:00074593,
 author = {西内, 満美子 and 榊, 泰直 and 桐山, 博光 and ドーバー, ニコラス ピーター and コーガ, ジェームズ and 近藤, 康太郎 and 渡辺, 幸信 and 神門, 正城 and 近藤, 公伯 and 畑, 昌育 and 岩田, 夏弥 and 千徳, 靖彦 and 西内 満美子 and 榊 泰直 and 桐山 博光 and ドーバー ニコラス ピーター and コーガ ジェームズ and 近藤 康太郎 and 渡辺 幸信 and 神門 正城 and 近藤 公伯 and 千徳 靖彦},
 month = {Sep},
 note = {Recently short-pulse petawatt-class high peak power laser systems are able to deliver laser pulses with intensities of ~1022Wcm-2 for real experiments. For such a high intensity laser pulse interaction especially with solid density targets, the real laser matter interaction is not as simple as an idealized high peak power laser pulse with a Gaussian-like temporal and spatial distribution solely interacting with an idealized solid density target. In particular, the temporal distribution of the laser pulse alters the target condition significantly. The J-KAREN-P laser system at the Kansai Photon Science Institute can , uncommonly for high power laser systems[1-5], provide real high intensity laser pulses on target of ~1022Wcm-2 with good laser contrast conditions and an almost diffraction limited spatial distribution. By the interaction between J-KAREN-P laser pulses and solid density target,  we have achieved extra-ordinary strong electric field [3,4-7].  We describe how under appropriate conditions an extremely large electrostatic field can be established., ICUIL 2018},
 title = {Extra-ordinary macroscopic strong electric field established by the high-peak high-contrast laser pulse interaction with a solid density target},
 year = {2018}
}