Shapes of rotating normal fluid 3He versus superfluid 4He droplets in molecular beams
| Autor: | 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. |
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| Rok vydání: | 2020 |
| Předmět: | |
| Zdroj: | Phys. Rev. B 102, 014504 (2020) |
| Druh dokumentu: | Working Paper |
| DOI: | 10.1103/PhysRevB.102.014504 |
| Popis: | 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 ($\Lambda$) and reduced angular velocities ($\Omega$) similar to that of 4He droplets. Given the different physical nature of 3He and 4He, this similarity in $\Lambda$ and $\Omega$ 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. Comment: 29 pages, 6 figures |
| Databáze: | arXiv |
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