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Last updated September 29, 2024

Pulsar: A Beating Stellar Heart

Pulsar PSR B1509-58

Pulsars: Rotating Neutron Stars

A pulsar is a rapidly rotating neutron star, resulting from the gravitational collapse of a massive star at the end of its life. Its extremely dense core, consisting mainly of degenerate neutrons, generates an intense magnetic field and emits periodic electromagnetic radiation detected as pulses. These signals, often in the radio range, resemble a cosmic lighthouse rotating with remarkable precision.

N.B.: Under the extreme conditions of pressure and density in a pulsar, neutron matter becomes an extremely dense degenerate fluid. Strong nuclear interactions favor certain energy states, which can induce partial or global alignment of neutron spins, thus producing macroscopic magnetization.

Physical Structure of a Pulsar

A pulsar is a compact object with a typical mass between 1.4 and 2 solar masses, but reduced to a radius of about 10 to 15 km. Its average density exceeds \(10^{17} \, \mathrm{kg/m^3}\), comparable to nuclear density. Neutron pressure provides the force counterbalancing gravity, thus stabilizing the neutron star.

The magnetic field can reach \(10^8\) to \(10^{11}\) Tesla, billions of times more intense than Earth's. This magnetic field is inclined relative to the rotation axis, causing the pulsed emission perceived on Earth.

Emission Mechanism and Rotation

The standard model describes the pulsar as a source emitting electromagnetic beams at the magnetic poles. The rapid rotation, with periods ranging from a few milliseconds to a few seconds, induces periodicity in the reception of signals.

The conservation of angular momentum explains the rapid rotation: during the collapse of the initial star, its radius decreases drastically, and the angular velocity increases according to the relation \(\omega = \frac{L}{I}\) where \(L\) is the conserved angular momentum and \(I\) is the moment of inertia of the neutron star.

This rotation is gradually slowed by electromagnetic radiation and the particle wind, causing a slow but measurable increase in the rotation period.

Physical Parameters and Observations

Observations measure the period \(P\), its time derivative \(\dot{P}\), and allow the deduction of the rotational energy loss \(\dot{E}\) related to electromagnetic emission. These parameters provide information on the characteristic age of the pulsar and its surface magnetic field estimated by the classical formula: \( B \approx 3.2 \times 10^{15} \sqrt{P \dot{P}} \quad \mathrm{Tesla} \)

where \(P\) is in seconds and \(\dot{P}\) is dimensionless (variation per second).

Comparative Table of Physical Characteristics of Pulsars

Typical Physical Characteristics of Pulsars
ParameterOrder of MagnitudeUnitPhysical Description
Mass1.4 – 2Solar Masses (M☉)Compact gravitational mass of the neutron star
Radius10 – 15kmTypical radius of the neutron star
Average Density~ \(10^{17}\)kg/m³Density comparable to nuclear matter
Magnetic Field10^8 – 10^{11}TeslaIntensity of the surface magnetic field
Rotation Period1.4 ms – a few ssecondsTime between two detected pulses
Slowdown Rate \(\dot{P}\)10^{-21} – 10^{-12}s/sTemporal variation of the period due to braking

Source: NRAO - The Pulsar Handbook and Kaspi et al., Astrophysical Journal, 2004.

Pulsars: Natural Laboratories

Pulsars are unique natural laboratories for studying extreme physics: dense matter, intense magnetism, general relativity. Their periodic signal, with precision comparable to the best atomic clocks, allows fundamental tests in physics, including the detection of gravitational waves and the measurement of matter under conditions inaccessible in terrestrial laboratories.

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