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PSR J1311−3430

PSR J1311−3430 is a science topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand PSR J1311−3430 rather than just read about it. In short: PSR J1311−3430 is a pulsar with a spin period of 2.5603 milliseconds and is characteristic age of 1.94 billion years old. It is the first millisecond pulsar found via gamma-ray pulsations.

PSR J1311−3430 — main illustration
PSR J1311−3430 — illustration

Key takeaways

  • PSR J1311−3430 belongs to science; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect PSR J1311−3430 to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of PSR J1311−3430 from memory before moving on to harder problems.

Reference excerpt

PSR J1311−3430 is a pulsar with a spin period of 2.5603 milliseconds and is characteristic age of 1.94 billion years old. It is the first millisecond pulsar found via gamma-ray pulsations. The source was originally identified by the Energetic Gamma Ray Experiment Telescope as a bright gamma ray source, but was not recognized as a pulsar until observations with the Fermi Gamma-ray Space Telescope discovered pulsed gamma ray emission. The pulsar has a helium-dominated companion much less massive than itself, and the two are in an orbit with a period of 93.8 minutes. The system is explained by a model where mass from the low mass companion was transferred on to the pulsar, increasing the mass of the pulsar and decreasing its period. These systems are known as Black Widow Pulsars, named after the original such system discovered, PSR B1957+20, and may eventually lead to the companion being completely vaporized. Among systems like these, the orbital period of PSR J1311−3430 is the shortest ever found. Spectroscopic observations of the companion suggest that the mass of the pulsar is 2.7 M ⊙ {\displaystyle M_{\odot }} (solar masses). Though there is considerable uncertainty in this estimate, the minimum mass for the pulsar that the authors find adequately fits the data is 2.15 M ⊙ {\displaystyle M_{\odot }} , which is still more massive than PSR J1614−2230, the previous record holder for most massive known pulsar.

Discovery and observations The Energetic Gamma Ray Experiment Telescope (EGRET) and the Fermi Gamma-ray Space Telescope (Fermi), the successor to EGRET, both performed surveys of the sky for gamma ray emission. The telescopes observed emission on large scales in the sky, associated with emission from the Milky Way, as well as "point" sources, so named because they are smaller than the angular resolution of the telescopes. Some point sources detected by EGRET and Fermi were at the same locations as previously known objects from observations at other wavelengths, and included astrophysical sources such as pulsars and active galactic nuclei. Other point sources, however, remained a mystery, as they had no known counterpart at other wavelengths. One such unidentified source was 2FGL J1317.7−3429 (so named because it was in a catalog of Fermi sources, with the J1317.7−3429 designating its position in the sky in right ascension and declination). In an effort to detect a new origin of gamma-ray emission, Roger Romani performed a deep search for counterparts of the brightest unidentified gamma-ray sources. His search uncovered optical and X-ray emission at the same location as 2FGL J1317.7−3429 that changed amplitude with a period of roughly 1.5 hours, and suggested that the origin could be a millisecond pulsar in a black-widow-type system, but also noted that this would need to be confirmed by the discovery of pulsations in the gamma-ray data or at radio wavelengths. Within a few months, this conjecture was confirmed. A blind search of more than four years of Fermi data, led by Holger Pletsch, revealed that 2FGL J1317.7−3429 was a millisecond pulsar with a 2.5603 millisecond period, the first example of a millisecond pulsar detected via gamma-ray pulsations. With the discovery of the pulsations, it was named PSR J1311−3430, with "PSR" denoting pulsar. Follow-up radio observations were able to also detect intermittent radio pulsations with the Green Bank Telescope that were only visible for <10% of the time the source was observed. The authors suggested that the pulses could be eclipsed or scattered by material in the system.

Characteristics The detection and timing of the gamma ray pulsations was used to determine the spin period of the pulsar to be 2.5603 milliseconds. The presence of the companion to the pulsar causes very slight variations in the time at which these pulses appear to be emitted, meaning precise timing allows the minimum mass of the companion to be determined using Kepler's third law. The minimum mass found with this method is 8.2×10−3 M☉, or roughly 8 times the mass of Jupiter. Optical spectroscopy of this companion reveal that it is composed primarily of helium, with no hydrogen detected. Variations in the optical brightness reveal large temperature variations in the companion. Modeling of the variations indicate strong heating of the companion by the pulsar, and that the companion nearly fills its Roche lobe. An object that overflows its Roche lobe will lose mass to its more massive companion. Such a scenario is used to explain how the companion in this system, once likely a star, lost so much mass to become a planet massed object. The accretion of this material also explains the "spin-up" of the millisecond pulsar, so that it can have such a short rotational period. It is possible that PSR J1311−3430 will eventually completely vaporize its companion, and become a solitary millisecond pulsar.

Significance The identification of a millisecond pulsar via a blind search of gamma-ray data alone provides hope that other gamma-ray sources with unknown origin can be identified as millisecond pulsars, especially given that radio pulses from PSR J1311−3430 were detected less than 10% of the time observed. Among known black-widow-type binary pulsar systems, PSR J1311−3430 has the shortest orbital period, and a mass constrained to be larger than 2.1 M ⊙ {\displaystyle M_{\odot }} . This mass determination for the pulsar supports the existing notion that these systems are hosts to pulsars with large masses, and also provides constraints on the equation of state for neutron stars, strongly favoring "stiff" equations of state.

Notes

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Worked examples

Example 1 — a first encounter with PSR J1311−3430

Start with the simplest possible case. Write down what PSR J1311−3430 claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In science, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to PSR J1311−3430 before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about PSR J1311−3430 ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of PSR J1311−3430

In research
PSR J1311−3430 appears in science research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses PSR J1311−3430 in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
PSR J1311−3430 is common in secondary-school and first-year university syllabi. It links to neighbouring topics Centaurus, Millisecond pulsars, so understanding it makes those chapters shorter.
In everyday life
Look for PSR J1311−3430 outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study PSR J1311−3430 in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what PSR J1311−3430 means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain PSR J1311−3430 out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is PSR J1311−3430 in simple terms?

PSR J1311−3430 is a pulsar with a spin period of 2.5603 milliseconds and is characteristic age of 1.94 billion years old. It is the first millisecond pulsar found via gamma-ray pulsations.

Why does PSR J1311−3430 matter?

Because it connects several science ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study PSR J1311−3430?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on PSR J1311−3430.

Tags

  • Centaurus
  • Millisecond pulsars

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