Formation of supernova-origin presolar SiC grains

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Presentation transcript:

Formation of supernova-origin presolar SiC grains 2018/05/31 Formation of supernova-origin presolar SiC grains Takaya Nozawa (National Astronomical Observatory of Japan) Collaborators: Sachiko Amari, Takashi Yoshida (U. of Tokyo), Shigeru Wakita (ELSI), Yasuhiro Hasegawa (JPL), Kyoko, K. Tanaka, Hidekazu Tanaka (Tohoku Univ.), Yuki Kimura (Hokkaido Univ.)

1-1. Presolar grains ○ Presolar grains ➜ offering key information on ‐ discovered in primitive meteorites ‐ showing peculiar isotopic compositions (different from the solar system’s materials) ‐ thought to have formed in stars before the Sun was formed ➜ offering key information on   ・ nuclear processes in the parent stars   ・ physical conditions in which they formed ‐ abundance (volume fraction): ~100-500 ppm (~0.1-0.5 %) ‐ mineral composition graphite, SiC, TiC, Si3N4, Al2O3, MgAl2O4, Mg2SiO4, MgSiO3 … http://presolargrains.net/

1-2. Presolar Type X SiC grains Nittler 2003 ○ Presolar SiC grains (~10 ppm) Nittler & Hoppe 2005 〇 Type X SiC grains (~0.1 ppm, size: 0.1-20 µm) ‐ 12C/28Si rich, with excesses in 44Ca (44Ti), 49Ti (49V) ➜ originated from core-collapse supernovae

1-3. Long-lasting questions 〇 Fact A fraction of presolar SiC grains is highly likely SN-origin 〇 Question How do these SiC grains form in the ejecta of core-collapse supernovae? ## Any theoretical studies have not yet realized the ## formation of SiC grains in supernovae

2-1. Elemental abundances in the SN ejecta Si isotopes 44Ti 28Si rich 12C rich C (N) isotopes Yoshida 2007; 4 Msun He-core model (Mstar ~ 18 Msun) O-rich (O/C >> 1) 29, 30Si rich 29, 30Si solar 14N rich Needed unrealistic mixing of the ejecta

2-2. Possible formation site of SiC grains in SNe 4He ○ Moderately energetic SNe Ekin = (3-5)x1051 erg (normal SNe : Ekin ~ 1x1051 erg) explosive burning happens at the boundary between O-rich region and He-rich region ➜ producing 12C-rich, 28Si-rich, (44Ti-rich) region ## 3(4He)  12C ## 12C + n(4He) ➜ α-elements 12C 28Si Pignatari+2013

2-3. No formation of SiC in the calculations 〇 Condensation temperature ‐C grains : Tcon = 1700-2200 K ‐SiC grains: Tcon = 1300-1800 K ➜ In C/Si-rich gas, C grains first condense to use up the gas- phase C atoms 〇 Formation path of grains cool down More efficient destruction of C grains (clusters)? UV radiation, high-energy e, chemical reaction, … ➜ this may not do a good job

2-4. Formation of SiC grains via molecules 〇 Previous works ➜ accretion of Si/C atoms 〇 This work ‐accretion of SiC molecules ‐coagulation rate coefficients of radiative association of molecules ki,j Rate coefficients; ki,j Andreazza+2009 300 K Temperature; T 104 K

3-1. Formation of SiC molecules Element # abundance He 0.3 C O 0.001 Ne Mg 0.002 Si 0.2 S 0.19 Ar 0.006 Pignatari+2013

3-2. Equation of dust formation 〇 Master equations of dust growth taking account of nucleation and grain growth through gas accretion and coagulation between grains simultaneously!

3-3. Can SiC grains form in the SN ejecta? behavior of dust formation size distribution of dust Yes, the formation of SiC grains is possible !

3-4. Formation process of SiC grains 〇 Formation of SiC grains is possible !! ‐ Condensation temperature is higher for higher gas density ‐ Dust growth proceeds on a short timescale through rapid accretion of molecules ‐ Coagulation makes the average radius by about a factor of 2

3-5. Size distribution of SiC grains formed ‐ Radius of newly formed grains is larger for higher gas density ‐ In the most dense gas considered in this study, grain radius is as large as ones (> 0.1 µm) observed in presolar SiC grains

4. Summary of this talk We investigate the formation of SiC grains in the ejecta of supernovae, self-consistently treating ‐formation of SiC molecules ‐growth of SiC grains via accretion of molecules ‐growth of SiC grains via grain-grain coagulation We have realized, for the first time, the formation of SiC grains in the ejecta of supernovae ➜ Large presolar Type-X SiC grains above 0.1 µm could form only in significantly dense clumps