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| 1 | 榆全爪螨在桑树和某些植物上的发育显示文摘榆全爪螨分布广泛。为落叶果树,尤以属于蔷薇科的重要害虫(van de vrie等,1972;Ehara,1973)。它的亲缘种柑桔全爪螨(Ehara,1984)同样广泛分布并为害多种植物。这两个种都有一些共同的宿主植物如日本梨树和桃树(Shinkaji,1961a)。而不属蔷薇科的桑树、三叶柑桔、萨摩柑桔和菜豆都是柑桔全爪螨的宿主植物(Ehara,1956 3 Shinkaji, | M.Osakabe S.Kobayashi W.Ashihara 陈劲伟 | 1991 | 国外农学(蚕业)1991，，1： | 0 |
| 2 | Magnetic Configuration Effects on Fast Ion Losses Induced by Fast Ion Driven Toroidal Alfvén Eigenmodes in the Large Helical Device显示文摘Beam-ion losses induced by fast-ion-driven toroidal Alfvén eigenmodes (TAE) were measured with a scintillator-based lost fast-ion probe (SLIP) in the large helical device (LHD). The SLIP gave simultaneously the energy E and the pitch angle χ=arccos(v // /v) distribution of the lost fast ions. The loss fluxes were investigated for three typical magnetic configurations of R ax vac =3.60 m, 3.75 m, and 3.90 m, where R ax vac is the magnetic axis position of the vacuum field. Dominant losses induced by TAEs in these three configurations were observed in the E/χ regions of 50~190 keV/40°, 40~170 keV/25°, and 30~190 keV/30°, respectively. Lost-ion fluxes induced by TAEs depend clearly on the amplitude of TAE magnetic fluctuations, R ax vac and the toroidal field strength Bt . The increment of the loss fluxes has the dependence of (bTAE /Bt ) s . The power s increases from s = 1 to 3 with the increase of the magnetic axis position in finite beta plasmas. | K.OGAWA M.ISOBE K.TOI F.WATANABE D.A.SPONG A.SHIMIZU M.OSAKABE D.S.DARROW S.OHDACHI S.SAKAKIBARA LHD Experiment Group | 2012 | Plasma Science and Technology2012，14，4： | 0 |
| 3 | High Power Neutral Beam Injection in LHD显示文摘The results on high power injection with the neutral beam injection(NBI)systemfor the Large Helical Device(LHD)are reported.The system consists of three beam-lines withtwo hydrogen negative ion(H^- ion)sources installed in each beam-line.In order to improvethe injection power,a new beam accelerator with a multi-slot grounded grid(MSGG)has beendeveloped and applied to one beam-line.Using the accelerator,a maximum power of 5.7 MW wasachieved in 2003 and 2004,and the maximum energy of 189 keV was reached.The power andenergy exceeded the design values of the individual beam-line for LHD.The other beam-lines alsoincreased their injection power up to about 4 MW,and the total injection power of 13.1 MW wasachieved with three beam-lines in 2003.Although the accelerator had an advantage in high powerbeam injection,extracted beams expand in the short side direction of the ground-grid slot.Thedisadvantage has been resolved by modifying the aperture shapes of the steering grid. | K.TSUMORI Y.TAKEIRI K.NAGAOKA K.IKEDA M.OSAKABE Y.OKA O.KANEKO M.SHIBUYA T.KONDO M.SATO E.ASANO | 2006 | Plasma Science and Technology2006，8，1： | 0 |
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