相关实验视频
Updated: Aug 22, 2025

16:20
Hyperpolarized Xenon for NMR and MRI Applications
Published on: September 6, 2012
19.6K
极化X射线限制了黑洞X射线双星Cygnus X-1中的磁盘喷射几何
Henric Krawczynski1, Fabio Muleri2, Michal Dovčiak3
1Department of Physics and McDonnell Center for the Space Sciences, Washington University in St. Louis, St. Louis, MO 63130, USA.
概括
对黑洞X射线二进制星 (BHXB) Cygnus X-1的极度观测显示其射线与电场对齐. 这表明喷射源于内部X射线发射区域,与喷射轴垂直的延伸等离子体.
科学领域:
- 天体物理学
- 高能天体物理学
- 黑洞物理
背景情况:
- 黑洞X射线二进制星系 (BHXB) 是一个正常恒星的气体聚集到黑洞上,产生X射线的系统.
- 了解BHXB的几何和发射机制对于黑洞物理学至关重要.
研究的目的:
- 研究黑洞X射线双星 (BHXB) Cygnus X-1中的喷气的结构和起源.
- 确定热的X射线发射等离子体与喷气相对的空间分布.
主要方法:
- 使用成像X射线极度测量探测器 (IXPE) 对天X-1进行极度测量观测.
- 分析了X射线发射的电场位置角度和极化程度.
主要成果:
- 发现电场位置的角度与外流喷气线对齐.
- 在2到8千电子伏特之间测定了4.01±0.20%的极化度.
- 收缩盘可能比二进制轨道更接近边缘.
- 热的X射线发射等离子体在垂直于喷射轴的平面上空间延伸.
结论:
- 在Cygnus X-1中发射的喷气机来自内部的X射线发射区域.
- 积累盘的方向受到极化测量的限制.
- 热等离子体的几何形状是平面的, 垂直于喷气流.
相关概念视频
Potential Due to a Polarized Object
459
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
459
Detection of Black Holes
2.3K
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...
2.3K
X-ray Imaging
5.8K
German physicist Wilhelm Röntgen (1845–1923) was experimenting with electrical current when he discovered that a mysterious and invisible "ray" would pass through his flesh but leave an outline of his bones on a screen coated with a metal compound. In 1895, Röntgen made the first durable record of the internal parts of a living human: an "X-ray" image (as it came to be called) of his wife’s hand. Scientists worldwide quickly began their own experiments with...
5.8K
Gauss's Law: Cylindrical Symmetry
7.8K
A charge distribution has cylindrical symmetry if the charge density depends only upon the distance from the axis of the cylinder and does not vary along the axis or with the direction about the axis. In other words, if a system varies if it is rotated around the axis or shifted along the axis, it does not have cylindrical symmetry. In real systems, we do not have infinite cylinders; however, if the cylindrical object is considerably longer than the radius from it that we are interested in,...
7.8K
Schwarzschild Radius and Event Horizon
2.1K
No object with a finite mass can travel faster than the speed of light in a vacuum. This fact has an interesting consequence in the domain of extremely high gravitational fields.
The minimum speed required to launch a projectile from the surface of an object to which it is gravitationally bound so that it eventually escapes the object’s gravitational field is called the escape velocity. The escape velocity is independent of the mass of the object. Merging the idea of escape...
The minimum speed required to launch a projectile from the surface of an object to which it is gravitationally bound so that it eventually escapes the object’s gravitational field is called the escape velocity. The escape velocity is independent of the mass of the object. Merging the idea of escape...
2.1K
Electric Field of a Charged Disk
2.3K
The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
2.3K

