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Structure of localized plasma produced by pulsed discharges in pressurized superfluid liquid helium

机译:加压超流体氦气中脉冲放电产生的局部等离子体的结构

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Summary form only given. At a temperature below 2.17 K, liquid helium (LHe) at 1 atm includes a superfluid component (Bose-Einstein condensate) that has no viscosity against impurity ions, namely, electron bubbles and He cluster ions. To produce a distributed ion mixture, i.e., transient cryogenic plasma with rare collisions between ions we apply high voltage pulsed discharges in superfluid LHe (LHeII). LHe has weak affinity to be a solvent of impurity materials, and our current effort is concentrated on how to implant a large amount of ions into LHe. Our preliminary measurement by time-resolved spectroscopy revealed the presence of high-density plasmas just after pulsed discharges (20 kV, 50 A, I /spl mu/s) between a pair of needle electrodes with small separation in LHeII. The measurements of Stark broadening and intensity ratios of spectral lines of neutral He atoms revealed spatial structure of the localized afterglow plasma in a large gaseous He bubble surrounded by LHe. The plasma is characterized by density above 1018 cm/sup -3/ and electron temperature of a few eV. Stark broadening of line 587.6 nm indicates the shape of the plasma to be a flat ellipsoid. The half widths of the ellipsoid are 0.6 and 1.2 mm at the time 0.4 /spl mu/s after the discharge. The spatial structure of the localized afterglow plasma is estimated to have a central part, where rapidly decreasing high-density plasma in gas He is formed, and a peripheral region surrounded by cool LHe, where a large amount of clusters survive for longer time than the core plasma. It is emphasized that the cryogenic plasma in the present study involves various unknown phenomena to be studied in future such as cluster formation, multi-electron bubbles, strongly coupled plasmas in LHeII.
机译:仅提供摘要表格。在低于2.17 K的温度下,在1个大气压下的液氦(LHe)包含对杂质离子(即电子气泡和He团簇离子)没有粘度的超流体组分(玻色-爱因斯坦缩合物)。为了产生分布的离子混合物,即离子之间发生罕见碰撞的瞬态低温等离子体,我们在超流体LHe(LHeII)中施加了高压脉冲放电。 LHe作为杂质材料的溶剂的亲和力很弱,我们目前的工作集中在如何将大量离子注入LHe中。我们通过时间分辨光谱法进行的初步测量表明,在一对针电极之间的脉冲放电(20 kV,50 A,I / spl mu / s)刚好发生脉冲放电(20 kV,50 A,I / spl mu / s)之后,就存在了高密度等离子体。对中性He原子的谱线的Stark加宽和强度比的测量揭示了在被LHe包围的大的气态He气泡中局部余辉等离子体的空间结构。等离子体的特征在于高于1018 cm / sup -3 /的密度和几eV的电子温度。线587.6 nm的明显加宽表示等离子体的形状为扁平椭圆形。放电后的时间为0.4 / spl mu / s时,椭圆形的半宽度分别为0.6和1.2 mm。据估计,局部余辉等离子体的空间结构具有中心部分,在该中心部分中迅速形成了气体He中高密度等离子体的下降,而外围区域则被冷LHe包围,在该外围区域中,大量团簇的存活时间长于LHe。核心血浆。要强调的是,本研究中的低温等离子体涉及各种未知现象,将来有待研究,例如团簇形成,多电子气泡,LHeII中的强耦合等离子体。

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