“Diffuse ionized gas”的版本间差异
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[[electron temperature|电子温度]] |
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==[[IFS观测]]== |
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*DIG可以用Ha的等值宽度来做判据,EW(Ha)双峰分布 |
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*arXiv1907.08635:讨论了DIG对金属丰度测量的影响 |
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==银河系中的DIG== |
==银河系中的DIG== |
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*Referred to as the Reynolds layer, or warm ionized medium (WIM); |
*Referred to as the Reynolds layer, or warm ionized medium (WIM); |
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*This warm (10^4 K), diffuse (n ~ 0.2 cm~3) gas fills 20% of the disk volume and accounts for most of the mass of ionized gas(90 percent). |
*This warm (10^4 K), diffuse (n ~ 0.2 cm~3) gas fills 20% of the disk volume and accounts for most of the mass of ionized gas(90 percent). |
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:*电子密度比hot gas要高一点( Typical values of the central electron density, central cooling time and total mass for the ETGs are ~ 0.1cm−3, ~ 5 x |
:*[[电子密度]]比 hot gas要高一点( Typical values of the central electron density, central cooling time and total mass for the ETGs are ~ 0.1cm−3, ~ 5 x 10^6 yr and 5 x 1O^9 M⊙) |
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*In terms of energetics, the Galactic WIM requires at least 10^42 ergs s~1 to remain ionized. This power is more than can be comfortably supplied by supernova shocks, but significantly less than the Lyman continuum luminosity of massive stars. |
*In terms of energetics, the Galactic WIM requires at least 10^42 ergs s~1 to remain ionized. This power is more than can be comfortably supplied by supernova shocks, but significantly less than the [[Lyman continuum]] luminosity of massive stars. |
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*[http://iopscience.iop.org/article/10.1086/306232/meta] |
*[http://iopscience.iop.org/article/10.1086/306232/meta] |
2024年7月22日 (一) 01:26的最新版本
IFS观测
- DIG可以用Ha的等值宽度来做判据,EW(Ha)双峰分布
- arXiv1907.08635:讨论了DIG对金属丰度测量的影响
银河系中的DIG
- Referred to as the Reynolds layer, or warm ionized medium (WIM);
- This warm (10^4 K), diffuse (n ~ 0.2 cm~3) gas fills 20% of the disk volume and accounts for most of the mass of ionized gas(90 percent).
- 电子密度比 hot gas要高一点( Typical values of the central electron density, central cooling time and total mass for the ETGs are ~ 0.1cm−3, ~ 5 x 10^6 yr and 5 x 1O^9 M⊙)
- In terms of energetics, the Galactic WIM requires at least 10^42 ergs s~1 to remain ionized. This power is more than can be comfortably supplied by supernova shocks, but significantly less than the Lyman continuum luminosity of massive stars.
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