{"created":"2023-06-20T15:08:04.908392+00:00","id":329,"links":{},"metadata":{"_buckets":{"deposit":"526a4c6e-ed82-4dff-a1f0-45ed481dce13"},"_deposit":{"created_by":3,"id":"329","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"329"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00000329","sets":["6:7"]},"author_link":["122945","122655","122950","66595","122956","122954","122966","122975","66644","66902","67531","122963","122946","66803","66578","122968","66600","122952","122951","66909","122960","122958","122972","122942","66555","122973","122962","66739","66899","122965","122970","66587","122967","122961","122953","66558","122944","66611","66580","122943","122964","66545","122955","67644","122949","122971","122941","66608","122969","122959","66541","122947","123644","122974","66609","122948","122728","66610","66594","122957","122588","66906","66787","67585"],"item_2_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2002-01-01","bibliographicIssueDateType":"Issued"},"bibliographicPageStart":"pp.201-204","bibliographicVolumeNumber":"Vol.5","bibliographic_titles":[{"bibliographic_title":"Journal of Plasma and Fusion Research SERIES"},{"bibliographic_title":"Journal of Plasma and Fusion Research SERIES","bibliographic_titleLang":"en"}]}]},"item_2_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"The spatial resolved energy spectra can be observed during a long discharge of NBI plasma by\ncontinuously scanning the neutral particle analyzer. In these discharges, the plasmas are initiated by the ECH heating, after that NBI#2 (Co-injection) sustains the plasma during 40-60 seconds. The scanned pitch angle is from 44 degrees to 74 degrees. The injected neutral beam (hydrogen) energy of NBI#2 is only 130 keV because the original ion source polarity is negative. The shape of spectra is almost similar from 44 degrees to 53 degrees. However the spectra from 55 degrees are strongly varied. It reflects the injection pitch angle of the beam according to the simulation (53 degrees ot R* = 3.75 m in simulation). The beam keeps the pitch angle at incidence until the beam energy becomes to the energy, which the pitch angle scattering is occurred by the energy loss due to the electron collision. The low flux region can be observed around 10-15 keV, which is 15 times of the electron temperature. The energy region may be equal to the energy at which the pitch angle scattering is occurred. At the energy, the particle is scattered by the collision with the plasma ions and some of particles may run away from the plasma because they have a possibility to enter the loss cone. According to the simulation, the loss cone can be expected at the 10 keV with the small angular dependence. The depth of the loss cone is deep at the small pitch angle. The hollow in the spectrum may be concluded to be the loss cone as the tendency is almost agreed with the experimental result.","subitem_description_type":"Abstract"}]},"item_2_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"The Japan Society of Plasma Science and Nuclear Fusion Research"}]},"item_2_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_name":[{"subitem_relation_name_text":"Publisher version"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"http://www.jspf.or.jp/JPFRS/index_vol5-2.html","subitem_relation_type_select":"URI"}}]},"item_2_rights_15":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"@20O2 by The Japan Society of Plasma Science and Nuclear Fusion 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