Large gas inflow driven by a matured galactic bar in the early Universe

  • 1National Astronomical Observatory of Japan, Mitaka, Tokyo, Japan. shuohuang.version3@gmail.com.
  • 2Department of Physics, Graduate School of Science, Nagoya University, Nagoya, Japan. shuohuang.version3@gmail.com.
  • 3National Astronomical Observatory of Japan, Mitaka, Tokyo, Japan.
  • 4Department of Astronomy, School of Science, Graduate University for Advanced Studies (SOKENDAI), Mitaka, Tokyo, Japan.
  • 5Department of Physics, Graduate School of Science, Nagoya University, Nagoya, Japan.
  • 6Institute for Advanced Research, Nagoya University, Nagoya, Japan.
  • 7Institute of Astronomy, Graduate School of Science, University of Tokyo, Mitaka, Tokyo, Japan.
  • 8Research Center for the Early Universe, Graduate School of Science, University of Tokyo, Bunkyo-ku, Tokyo, Japan.
  • 9Faculty of Global Interdisciplinary Science and Innovation, Shizuoka University, Shizuoka, Japan.
+

|

Abstract

Bar structures are present in about half of local disk galaxies1 and play pivotal roles in secular galaxy evolution. Bars impose a non-axisymmetric perturbation on the rotating disk and transport gas inwards to feed the central starburst and, possibly, the activity of the nuclear supermassive black hole2. They are believed to be long-lived structures3,4 and are now identified at redshift z > 2 (refs. 5,6). However, little is known about the onset and effects of bars in the early cosmic epoch because the spectroscopy of distant bars at sufficient resolution is prohibitively expensive. Here we report on a kinematic study of a galactic bar at redshift 2.467, 2.6 billion years after the Big Bang. We observed the carbon monoxide and atomic carbon emission lines of the dusty star-forming galaxy J0107a and found the bar of J0107a has gas distribution and motion in a pattern identical to local bars7-9. At the same time, the bar drives large-scale non-circular motions that dominate over disk rotation, funnelling molecular gas into its centre at a rate of approximately 600 solar masses per year. Our results show that bar-driven dynamical processes and secular evolution were already at play 11.1 billion years ago, powering active star formation amid the gas-rich and far-infrared luminous growth phase in a massive disk galaxy.

Related Concept Videos

Detection of Black Holes 01:10

2.1K

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...

Excess Pressure Inside a Drop and a Bubble 01:13

1.6K

The shape of a small drop of liquid can be considered spherical, neglecting the effect of gravity. This drop can further be considered as two equal hemispherical drops put together due to surface tension. The forces acting on the spherical drop are due to the pressure of the liquid inside the drop, the pressure due to air outside the drop, and the force due to the surface tension acting on the two hemispherical drops.

where γ corresponds to the surface tension. Recalling that the force...

General External Flow Characteristics 01:26

61

The study of external flow is essential for creating structures and objects that interact efficiently and safely with moving fluids, such as air or water. When a body is immersed in a flowing fluid, it experiences two primary forces: drag, which opposes motion along the flow direction, and lift, which acts perpendicular to the flow. The shape, size, and orientation of the object influence these forces.Streamlined and Blunt Bodies in External FlowObjects in fluid flow are classified as...

Gravitation Between Spherically Symmetric Masses 01:14

820

The gravitational potential energy between two spherically symmetric bodies can be calculated from the masses and the distance between the bodies, assuming that the center of mass is concentrated at the respective centers of the bodies.

Consider that a spherically symmetric mass distribution comprises multiple concentric spherical shells. A point mass is placed at a distance 'r' from the center of mass of the spherical shell. All the particles in a given spherical ring on the surface...

Couette Flow 01:22

168

Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...

Turbulent Flow 01:24

108

Turbulent flow is characterized by unpredictable fluctuations in velocity and pressure, which result in a chaotic fluid movement distinct from the orderly patterns of laminar flow. While laminar flow is governed by smooth, parallel layers with minimal mixing, turbulent flow exhibits highly irregular, three-dimensional patterns. This behavior arises due to instabilities in the fluid's velocity profile, and amplifies as the flow velocity increases. Minor disturbances, known as turbulent...