“Diffuse ionized gas”的版本间差异
跳到导航
跳到搜索
无编辑摘要 |
|||
(未显示同一用户的1个中间版本) | |||
第1行: | 第1行: | ||
[[electron temperature|电子温度]] |
[[electron temperature|电子温度]] |
||
==IFS观测== |
==[[IFS观测]]== |
||
*DIG可以用Ha的等值宽度来做判据,EW(Ha)双峰分布 |
*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 |
*arXiv1907.08635:讨论了DIG对金属丰度测量的影响 |
||
第8行: | 第8行: | ||
*Referred to as the Reynolds layer, or warm ionized medium (WIM); |
*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). |
*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 |
:*[[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. |
*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. |
||
*[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.
- [1]