低磁場ソフトガンマリピエーター
1Institut de Ciéncies de l'Espai, Consejo Superior de Investigaciones Científicas, Institut d'Estudis Espacials de Catalunya, Facultat de Ciéncies, Campus UAB, Torre C5-parell, 2a planta, 08193 Bellaterra (Barcelona), Spain. rea@ieec.uab.es
まとめ
マグネタール,または強烈な磁場によって駆動される中性子星は,非常に高い表面場を必要としない場合があります. この研究では,マグネタールのような爆発を持つ柔らかいガンマリピエーターが発見されたが,磁場は低かったため,既存の理論に異議を唱えた.
科学分野:
- 天体物理学 天体物理学
- 高エネルギー天体物理学
- 中性子星物理学 中性子星物理学
背景:
- ソフトガンマリピーター (SGR) と異常なX線パルサーは,散発的な爆発を持つX線源である.
- これらの源は,極限磁場 (10^1410^15ガウス) によって駆動される磁星であると仮定されています.
研究 の 目的:
- マグネタルのような活動を示す柔らかいガンマリピーターの磁場強さを調査するために.
- 非常に高い磁場がマグネタールのような行動に不可欠であるかどうかを判断する.
主な方法:
- 柔らかいガンマリピーターSGR 0418+5729.9のX線観測結果
- 磁場特性を推測するために,爆破放射の分析.
主要な成果:
- SGR 0418+5729はマグネターのような爆発を示しています.
- X線観測は,電波パルサーの典型である7.5 × 10^12ガウス未満の二極磁場を示しています.
- これは,これまで考えられていたよりも低い磁場で磁石のような活動が起こる可能性があることを示唆しています.
結論:
- 高表面二極磁場は,マグネタールのような活動のための前提条件ではありません.
- マグネタール集団は,磁場強度,年齢,進化状態のより広いスペクトルを包含している可能性があります.
- この発見は,中性子星の多様性と磁星形成に関する私たちの理解を広げています.
関連する概念動画
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
Atomic Nuclei: Nuclear Relaxation Processes
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis. This...
Atomic Nuclei: Magnetic Resonance
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
Generating Electromagnetic Radiations
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in the...
Atomic Nuclei: Larmor Precession Frequency
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession, and the angular frequency...
NMR Spectrometers: Resolution and Error Correction
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...


