论文标题

旋转正常流体的形状3HE与分子束中的超氟4he液滴

Shapes of rotating normal fluid 3He versus superfluid 4He droplets in molecular beams

论文作者

Verma, Deepak, Connell, Sean M. O. O, Feinberg, Alexandra J., Erukala, Swetha, Tanyag, Rico M., Bernando, Charles, Pang, Weiwu, Saladrigas, Catherine A., Toulson, Benjamin W., Borgwardt, Mario, Shivaram, Niranjan, Lin, Ming-Fu, Haddad, Andre Al, Jäger, Wolfgang, Bostedt, Christoph, Walter, Peter, Gessner, Oliver, Vilesov, Andrey F.

论文摘要

以前的单脉冲极端紫外线和X射线相干衍射研究表明,在自由喷射膨胀中获得的超氟4he液滴​​可获得相当大的角动量,从而导致明显的离心失真。与正常流体3HE液滴进行的类似实验可能有助于阐明大量旋转激发的起源,并突出正常和超流液液滴中的动态相似性和动力学差异。在这里,我们介绍了在低至〜2 k的高温下真空中相应流体膨胀后,分离的3HE和4HE液滴的形状的首次比较。大于3He和4he液滴​​,平均半径分别为〜160 nm和〜350 nm。我们发现,梁中的大多数液滴中的大多数与旋转的面积相对应减少平均角动量($λ$)和与4HE液滴相似的角速度($ω$)的球体。鉴于3HE和4HE的物理性质不同,$λ$和$ω$的相似性可能令人惊讶,这表明相似的机制会导致旋转,而不论同位素如何。我们假设观察到的液滴大小和角动量的分布源于靠近喷嘴的密集区域的过程。在该区域中,液滴之间的显着速度扩散和碰撞会诱导过度旋转,然后降低液滴裂变。该过程可能会在液滴进入碰撞 - 费用高真空区域之前重复几次。

Previous single-pulse extreme ultraviolet and X-ray coherent diffraction studies revealed that superfluid 4He droplets obtained in free jet expansion acquire sizable angular momentum, resulting in significant centrifugal distortion. Similar experiments with normal fluid 3He droplets may help elucidating the origin of the of the large degree of rotational excitation and highlight similarities and differences of dynamics in normal and superfluid droplets. Here, we present the first comparison of the shapes of isolated 3He and 4He droplets following expansion of the corresponding fluids in vacuum at temperatures as low as ~ 2 K. Large 3He and 4He droplets with average radii of ~160 nm and ~350 nm, respectively, were produced. We find that the majority of the 3He droplets in the beam correspond to rotating oblate spheroids with reduced average angular momentum ($Λ$) and reduced angular velocities ($Ω$) similar to that of 4He droplets. Given the different physical nature of 3He and 4He, this similarity in $Λ$ and $Ω$ may be surprising and suggest that similar mechanisms induce rotation regardless of the isotope. We hypothesized that the observed distribution of droplet sizes and angular momenta stem from processes in the dense region close to the nozzle. In this region, the significant velocity spread and collisions between the droplets induce excessive rotation followed by droplet fission. The process may repeat itself several times before the droplets enter the collision-fee high vacuum region further downstream.

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