B. Albertazzi1、a), P. Mabey2, Th. Michel1, G. Rigon1, J. R. Marquès1, S. Pikuz3、4, S. Ryazantsev3、4, E. Falize5, L. Van Box Som5, J. Meinecke6, N. Ozaki7、8, G. Gregori6, and M. Koenig1、7
Author Affiliations
1LULI–CNRS, CEA, Sorbonne Universités, École Polytechnique, Institut Polytechnique de Paris, F-91120 Palaiseau cedex, France2Department of Physics, Freie Universität Berlin, 14195 Berlin, Germany3JIHT-RAS, 13-2 Izhorskaya st., Moscow 125412, Russia4National Research Nuclear University “MEPhI,” Moscow 115409, Russia5CEA-DAM-DIF, F-91297 Arpajon, France6Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom7Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan8Institute of Laser Engineering, Osaka University, Suita, Osaka 565-0871, Japanshow less
DOI: 10.1063/5.0068689
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B. Albertazzi, P. Mabey, Th. Michel, G. Rigon, J. R. Marquès, S. Pikuz, S. Ryazantsev, E. Falize, L. Van Box Som, J. Meinecke, N. Ozaki, G. Gregori, M. Koenig. Triggering star formation: Experimental compression of a foam ball induced by Taylor–Sedov blast waves[J]. Matter and Radiation at Extremes, 2022, 7(3): 036902
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Fig. 1. Illustration of the evolution of a massive molecular cloud, indicating the importance of SNR propagation in forming new stars.
Fig. 2. Experimental setup for N2 at 11.4 mbar. Not to scale.
Fig. 3. Experimental results in N2 at 11.4 mbar. (a) Expansion of a single BW, taken 100 ns after the main pulse, toward the obstacle located 7.07 mm from the carbon rod. (b) Expansion of a single BW, taken at 450 ns, toward the obstacle located 11 mm from the carbon rod. (c) Zoom of (b) showing the deviation of the morphology of the BW from spherical to nonspherical when interacting with the foam ball. (d) Interferogram corresponding to (a). (e) Simulated interferogram. (f) Electron density profile corresponding to (f). (g) Experimental BW radius R vs time taken as illustrated in (a), i.e., parallel to the rod orientation. (h) Instantaneous velocity deduced from radius measurements vs time.
Fig. 4. Comparison between PrismSPECT simulations and experimental data averaged between 138 and 162 ns, corresponding to the time of impact with the obstacle. The simulations were performed with an initial mass density ρ = 5 × 10−5 g/cm3. The best agreement is found for a temperature in the range of 4.5–4.9 eV.
Fig. 5. X-ray radiographs of the 150 mg/cm3 foam ball: (a) without the influence of a BW, for reference; (b) at t = 500 ns after the beginning of the main laser pulse.
Fig. 6. (a) Schlieren data showing the expansion of both BWs toward the obstacle t = 100 ns after the beginning of the interaction. The thin red arrow indicates the expansion of the interaction zone formed by the collision of the two BWs. (b)–(g) Corresponding x-ray radiographs of the 150 mg/cm3 foam ball at different times during the interaction: (b) without the influence of a BW; (c) at 300 ns; (d) at 500 ns; (e) at 700 ns; (f) at 1000 ns; (g) at 1500 ns. The green arrows in (c) show the trajectories of the two BWs.
Fig. 7. (a) Deformation of the foam. The inset shows the different ways measurements were performed. (b) Mass density retrieved from the data shown in Fig. 6 (here 0 corresponds to the middle of the foam).
| Parameter | Symbol | LULI experiment | Astrophysical system |
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Propagation medium | Nature of gas | | N2 | | Initial density | ρi,i | 1.34 × 10−5 g/cm3 | 0.1–105 cm−3 | Density ratio | χ | ∼1 × 104 | 10–105 | Blast wave | Shock velocity at impact | vb,sh | 21 km/s | 10–3000 km/s | Shock front density at impact | ρb,i | 5 × 10−5 g/cm3 | | Mach number | M | 1–10 | 1–100 | Postshock intercloud temperature | Tb,sh | ∼4–5 eV | 1 up to ∼2000 eV | Cloud | Cloud radius | Rc | 475 µm | 0.01–200 pc | Preshock cloud density | ρc,i | (60–500) × 10−3 g/cm3 | 1–500 cm−3 | Shock cloud velocity | vc,sh | 0.2 km/s | 0.03–1000 km/s | Characteristic timescales | Cloud crushing timescale | τcc | 2375 ns | 1 × 104–1 × 105 yr | Pressure variation timescale | τp | 30 ns | 1 × 103–1 × 104 yr | Cooling timescale | τcool | ≥1000 ns | 100–1000 yr | Comparison of characteristic timescales | τcc vs τcool | | τcc ≥ τcool | τcc ≫ τcool (radiative) | τcc vs τp | | τcc ≫ τp | τcc ≪ τp |
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Table 1. Summary of experimental and astrophysical parameters. Astrophysical data for the SNRs are taken from Ref. 32.