赤道偏移5〜6の銀河は,一貫して塵の含有量が低く,[C II]の放出量が高い
P L Capak1, C Carilli2, G Jones3
11] Infrared Processing and Analysis Center (IPAC), 1200 East California Boulevard, Pasadena, California 91125, USA [2] California Institute of Technology, 1200 East California Boulevard, Pasadena, California 91125, USA.
Nature
|June 26, 2015
まとめ
初期の銀河 (赤道偏移 z > 4) は,後の宇宙時代と比較して,塵がかなり少なく,二酸化炭素の放出が増加しています. これは,若い宇宙に急速に進化する星間媒体が存在していたことを示唆している.
科学分野:
- 宇宙の進化とは,宇宙の進化である.
- 銀河の形成と進化について
- 星間媒体の特性
背景:
- 赤道偏移 z > 4 時の銀河の紫外線の性質は,急速な塵の遮蔽の進化を示唆しています.
- 初期の銀河における星間媒体の以前の測定は,仮定と検出能力によって制限されていました.
研究 の 目的:
- 初期の恒星形成銀河の恒星間媒体の特性を直接測定するために.
- ビッグバン (z ≈ 5−6) から約10億年後の銀河の塵とガスの含有量を調査する.
主な方法:
- ガスから測定された禁止炭素II ([CII]) 排出量.
- z ≈ 5-6の9つの典型的な恒星形成銀河の塵からの遠赤外線放射を測定しました.
主要な成果:
- これらの初期の銀河は,後の時期 (z < 3) の類似の銀河の1 / 12未満の熱放出を示しています.
- 遠赤外線連続体に対する強化された[C II]放射は,異なるガスと塵の比率を示している.
- ガスは,様々なダイナミクスを持つ1〜8キロパーセックに分布しています.
結論:
- 初期の銀河の星間介質は大きく進化し,z < 3の銀河よりも塵がかなり少なくなった.
- これらの初期の銀河の塵の含有量は,局所的な低金属性のシステムに匹敵する.
- これらの発見は,初期の銀河の構成と進化に関する以前の仮定に異議を唱える.
関連する概念動画
Emission Spectra
78.9K
When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
78.9K
Detection of Black Holes
2.6K
Although black holes were theoretically postulated in the 1920s, they remained outside the domain of observational astronomy until the 1970s.
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
2.6K
Atomic Emission Spectroscopy: Overview
4.3K
Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
4.3K
Atomic Emission Spectroscopy: Lab
818
AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...
818
Flame Photometry: Lab
1.2K
In a flame photometer, when a solution like potassium chloride is aspirated into the flame, the solvent evaporates, leaving behind dehydrated salt. This salt dissociates into free gaseous atoms in their ground state. Some of these atoms absorb energy from the flame, leading to their excitation. The excited atoms return to the ground state, emitting photons at characteristic wavelengths. Because only electronic transitions are involved, the resulting emission lines are very narrow. The intensity...
1.2K
Atomic Emission Spectroscopy: Instrumentation
1.6K
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
1.6K


