Millisecond Pulsars, Their Evolution and Applications
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Exploring Pulsars
High-energy astrophysics Explore the PUL SAR menagerie Astronomers are discovering many strange properties of compact stellar objects called pulsars. Here’s how they fit together. by Victoria M. Kaspi f you browse through an astronomy book published 25 years ago, you’d likely assume that astronomers understood extremely dense objects called neutron stars fairly well. The spectacular Crab Nebula’s central body has been a “poster child” for these objects for years. This specific neutron star is a pulsar that I rotates roughly 30 times per second, emitting regular appar- ent pulsations in Earth’s direction through a sort of “light- house” effect as the star rotates. While these textbook descriptions aren’t incorrect, research over roughly the past decade has shown that the picture they portray is fundamentally incomplete. Astrono- mers know that the simple scenario where neutron stars are all born “Crab-like” is not true. Experts in the field could not have imagined the variety of neutron stars they’ve recently observed. We’ve found that bizarre objects repre- sent a significant fraction of the neutron star population. With names like magnetars, anomalous X-ray pulsars, soft gamma repeaters, rotating radio transients, and compact Long the pulsar poster child, central objects, these bodies bear properties radically differ- the Crab Nebula’s central object is a fast-spinning neutron star ent from those of the Crab pulsar. Just how large a fraction that emits jets of radiation at its they represent is still hotly debated, but it’s at least 10 per- magnetic axis. Astronomers cent and maybe even the majority. -
This Work Is Protected by Copyright and Other Intellectual Property Rights
This work is protected by copyright and other intellectual property rights and duplication or sale of all or part is not permitted, except that material may be duplicated by you for research, private study, criticism/review or educational purposes. Electronic or print copies are for your own personal, non- commercial use and shall not be passed to any other individual. No quotation may be published without proper acknowledgement. For any other use, or to quote extensively from the work, permission must be obtained from the copyright holder/s. Fundamental properties of M-dwarfs in eclipsing binary star systems Samuel Gill Doctor of Philosophy Department of Physics, Keele University March 2019 i Abstract The absolute parameters of M-dwarfs in eclipsing binary systems provide important tests for evolutionary models. Those that have been measured reveal significant discrepancies with evolutionary models. There are two problems with M-dwarfs: 1. M-dwarfs generally appear bigger and cooler than models predict (such that their luminosity agrees with models) and 2. some M-dwarfs in eclipsing binaries are measured to be hotter than expected for their mass. The exact cause of this is unclear and a variety of conjectures have been put forward including enhanced magnetic activity and spotted surfaces. There is a lack of M-dwarfs with absolute parameters and so the exact causes of these disparities are unclear. As the interest in low-mass stars rises from the ever increasing number of exoplanets found around them, it is important that a considerable effort is made to understand why this is so. A solution to the problem lies with low-mass eclipsing binary systems discovered by the WASP (Wide Angle Search for Planets) project. -
Chapter 22 Neutron Stars and Black Holes Units of Chapter 22 22.1 Neutron Stars 22.2 Pulsars 22.3 Xxneutron-Star Binaries: X-Ray Bursters
Chapter 22 Neutron Stars and Black Holes Units of Chapter 22 22.1 Neutron Stars 22.2 Pulsars 22.3 XXNeutron-Star Binaries: X-ray bursters [Look at the slides and the pictures in your book, but I won’t test you on this in detail, and we may skip altogether in class.] 22.4 Gamma-Ray Bursts 22.5 Black Holes 22.6 XXEinstein’s Theories of Relativity Special Relativity 22.7 Space Travel Near Black Holes 22.8 Observational Evidence for Black Holes Tests of General Relativity Gravity Waves: A New Window on the Universe Neutron Stars and Pulsars (sec. 22.1, 2 in textbook) 22.1 Neutron Stars According to models for stellar explosions: After a carbon detonation supernova (white dwarf in binary), little or nothing remains of the original star. After a core collapse supernova, part of the core may survive. It is very dense—as dense as an atomic nucleus—and is called a neutron star. [Recall that during core collapse the iron core (ashes of previous fusion reactions) is disintegrated into protons and neutrons, the protons combine with the surrounding electrons to make more neutrons, so the core becomes pure neutron matter. Because of this, core collapse can be halted if the core’s mass is between 1.4 (the Chandrasekhar limit) and about 3-4 solar masses, by neutron degeneracy.] What do you get if the core mass is less than 1.4 solar masses? Greater than 3-4 solar masses? 22.1 Neutron Stars Neutron stars, although they have 1–3 solar masses, are so dense that they are very small. -
Mode Changing and Giant Pulses Found in a Millisecond Pulsar 17 July 2018, by Tomasz Nowakowski
Mode changing and giant pulses found in a millisecond pulsar 17 July 2018, by Tomasz Nowakowski between two or more quasi-stable modes of emission. To date, mode changing has been only observed in normal pulsars. However, a recent study conducted by a team of astronomers led by Nikhil Mahajan of the University of Toronto in Canada, shows the mode changing process could be also present in millisecond pulsars, as they observed that the pulse profile of pulsar PSR B1957+20 switches between two modes. Discovered in 1988, PSR B1957+20, also known as the "Black Widow Pulsar", is a 1.6 ms eclipsing binary millisecond pulsar in the constellation Sagitta. It orbits with a brown dwarf companion with a period of 9.2 hours with an eclipse duration of approximately 20 minutes. Mahajan's team observed this pulsar for over nine hours in four daily sessions between June 13 and 16, 2014 at the Arecibo Observatory in Puerto Rico, what Chandra image of PSR B1957+20. The blue and green resulted in uncovering new insights into its are optical images of the field in which the pulsar is behavior. found, the green indicating the H-alpha bow shock. The red and white are secondary shock structures "Here, we show that the millisecond pulsar PSR discovered in x-ray by the Chandra X-ray Observatory. B1957+20 shows mode changing, and that the Credit: X-ray: NASA/CXC/ASTRON/B.Stappers et al.; properties of the giant pulses that we found earlier Optical: AAO/J.Bland-Hawthorn & H.Jones (in the same data; Main et al. -
HOW FAST IS RF? by RON HRANAC
Originally appeared in the September 2008 issue of Communications Technology. HOW FAST IS RF? By RON HRANAC Maybe a better question is, "What's the speed of an electromagnetic signal in a vacuum?" After all, what we call RF refers to signals in the lower frequency or longer wavelength part of the electromagnetic spectrum. Light is an electromagnetic signal, too, existing in the higher frequency or shorter wavelength part of the electromagnetic spectrum. One way to look at it is to assume that RF is nothing more than really, really low frequency light, or that light is really, really high frequency RF. As you might imagine, the numbers involved in describing RF and light can be very large or very small. For more on this, see my June 2007 CT column, "Big Numbers, Small Numbers" (www.cable360.net/ct/operations/techtalk/23783.html). According to the National Institute of Standards and Technology, the speed of light in a vacuum, c0, is 299,792,458 meters per second (http://physics.nist.gov/cgi-bin/cuu/Value?c). The designation c0 is one that NIST uses to reference the speed of light in a vacuum, while c is occasionally used to reference the speed of light in some other medium. Most of the time the subscript zero is dropped, with c being a generic designation for the speed of light. Let's put c0 in terms that may be more familiar. You probably recall from junior high or high school science class that the speed of light is 186,000 miles per second. -
Constraining the Neutron Star Equation of State with Astrophysical Observables
CONSTRAINING THE NEUTRON STAR EQUATION OF STATE WITH ASTROPHYSICAL OBSERVABLES by Carolyn A. Raithel Copyright © Carolyn A. Raithel 2020 A Dissertation Submitted to the Faculty of the DEPARTMENT OF ASTRONOMY In Partial Fulfillment of the Requirements For the Degree of DOCTOR OF PHILOSOPHY WITH A MAJOR IN ASTRONOMY AND ASTROPHYSICS In the Graduate College THE UNIVERSITY OF ARIZONA 2020 3 ACKNOWLEDGEMENTS Looking back over the last five years, this dissertation would not have been possible with the support of many people. First and foremost, I would like to thank my advisor, Feryal Ozel,¨ from whom I have learned so much { about not only the science I want to do, but about the type of scientist I want to be. I am grateful as well for the support and mentorship of Dimitrios Psaltis and Vasileios Paschalidis { I have so enjoyed working with and learning from you both. To Joel Weisberg, my undergraduate research advisor who first got me started on this journey and who has continued to support me throughout, thank you. I believe a scientist is shaped by the mentors she has early in her career, and I am grateful to have had so many excellent ones. I am deeply thankful for my friends, near and far, who have supported me, encouraged me, and helped preserve my sanity over the last five years. To our astronomy crafting group Lia, Ekta, Samantha, and Allie; to my office mates David, Gabrielle, Tyler, Kaushik, and Michi; to Sarah, Marina, Tanner, Charlie, and Lina{ thank you. I will be forever grateful to my family for their continual support { espe- cially my parents, Don and Kathy, who instilled in me a love for learning from a very young age and who have encouraged me ever since. -
A Short Walk Through the Physics of Neutron Stars
A short walk through the physics of neutron stars Isaac Vidaña, INFN Catania ASTRA: Advanced and open problems in low-energy nuclear and hadronic STRAngeness physics October 23rd-27th 2017, Trento (Italy) This short talk is just a brush-stroke on the physics of neutron stars. Three excellent monographs on this topic for interested readers are: Neutron stars are different things for different people ² For astronomers are very little stars “visible” as radio pulsars or sources of X- and γ-rays. ² For particle physicists are neutrino sources (when they born) and probably the only places in the Universe where deconfined quark matter may be abundant. ² For cosmologists are “almost” black holes. ² For nuclear physicists & the participants of this workshop are the biggest neutron-rich (hyper)nuclei of the Universe (A ~ 1056-1057, R ~ 10 km, M ~ 1-2 M ). ¤ But everybody agrees that … Neutron stars are a type of stellar compact remnant that can result from the gravitational collapse of a massive star (8 M¤< M < 25 M¤) during a Type II, Ib or Ic supernova event. 50 years of the discovery of the first radio pulsar ² radio pulsar at 81.5 MHz ² pulse period P=1.337 s Most NS are observed as pulsars. In 1967 Jocelyn Bell & Anthony Hewish discover the first radio pulsar, soon identified as a rotating neutron star (1974 Nobel Prize for Hewish but not for Jocelyn) Nowadays more than 2000 pulsars are known (~ 1900 Radio PSRs (141 in binary systems), ~ 40 X-ray PSRs & ~ 60 γ-ray PSRs) Observables § Period (P, dP/dt) § Masses § Luminosity § Temperature http://www.phys.ncku.edu.tw/~astrolab/mirrors/apod_e/ap090709.html -
Low Latency – How Low Can You Go?
WHITE PAPER Low Latency – How Low Can You Go? Low latency has always been an important consideration in telecom networks for voice, video, and data, but recent changes in applications within many industry sectors have brought low latency right to the forefront of the industry. The finance industry and algorithmic trading in particular, or algo-trading as it is known, is a commonly quoted example. Here latency is critical, and to quote Information Week magazine, “A 1-millisecond advantage in trading applications can be worth $100 million a year to a major brokerage firm.” This drives a huge focus on all aspects of latency, including the communications systems between the brokerage firm and the exchange. However, while the finance industry is spending a lot of money on low- latency services between key locations such as New York and Chicago or London and Frankfurt, this is actually only a small part of the wider telecom industry. Many other industries are also now driving lower and lower latency in their networks, such as for cloud computing and video services. Also, as mobile operators start to roll out 5G services, latency in the xHaul mobile transport network, especially the demanding fronthaul domain, becomes more and more important in order to reach the stringent 5G requirements required for the new class of ultra-reliable low-latency services. This white paper will address the drivers behind the recent rush to low- latency solutions and networks and will consider how network operators can remove as much latency as possible from their networks as they also race to zero latency. -
Timestamp Precision
Timestamp Precision Kevin Bross 15 April 2016 15 April 2016 IEEE 1904 Access Networks Working Group, San Jose, CA USA 1 Timestamp Packets The orderInfo field can be used as a 32-bit timestamp, down to ¼ ns granularity: 1 s 30 bits of nanoseconds 2 ¼ ms µs ns ns Two main uses of timestamp: – Indicating start or end time of flow – Indicating presentation time of packets for flows with non-constant data rates s = second ms = millisecond µs = microsecond ns = nanosecond 15 April 2016 IEEE 1904 Access Networks Working Group, San Jose, CA USA 2 Presentation Time To reduce bandwidth during idle periods, some protocols will have variable rates – Fronthaul may be variable, even if rate to radio unit itself is a constant rate Presentation times allows RoE to handle variable data rates – Data may experience jitter in network – Egress buffer compensates for network jitter – Presentation time is when the data is to exit the RoE node • Jitter cleaners ensure data comes out cleanly, and on the right bit period 15 April 2016 IEEE 1904 Access Networks Working Group, San Jose, CA USA 3 Jitter vs. Synchronization Synchronization requirements for LTE are only down to ~±65 ns accuracy – Each RoE node may be off from TAI by up to 65 ns (or more in some circumstances) – Starting and ending a stream may be off by this amount …but jitter from packet to packet must be much tighter – RoE nodes should be able to output data at precise relative times if timestamp is used for a given packet – Relative bit time within a flow is important 15 April 2016 IEEE 1904 Access -
Origin and Binary Evolution of Millisecond Pulsars
Origin and binary evolution of millisecond pulsars Francesca D’Antona and Marco Tailo Abstract We summarize the channels formation of neutron stars (NS) in single or binary evolution and the classic recycling scenario by which mass accretion by a donor companion accelerates old NS to millisecond pulsars (MSP). We consider the possible explanations and requirements for the high frequency of the MSP population in Globular Clusters. Basics of binary evolution are given, and the key concepts of systemic angular momentum losses are first discussed in the framework of the secular evolution of Cataclysmic Binaries. MSP binaries with compact companions represent end-points of previous evolution. In the class of systems characterized by short orbital period %orb and low companion mass we may instead be catching the recycling phase ‘in the act’. These systems are in fact either MSP, or low mass X–ray binaries (LMXB), some of which accreting X–ray MSP (AMXP), or even ‘transitional’ systems from the accreting to the radio MSP stage. The donor structure is affected by irradiation due to X–rays from the accreting NS, or by the high fraction of MSP rotational energy loss emitted in the W rays range of the energy spectrum. X– ray irradiation leads to cyclic LMXB stages, causing super–Eddington mass transfer rates during the first phases of the companion evolution, and, possibly coupled with the angular momentum carried away by the non–accreted matter, helps to explain ¤ the high positive %orb’s of some LMXB systems and account for the (apparently) different birthrates of LMXB and MSP. Irradiation by the MSP may be able to drive the donor to a stage in which either radio-ejection (in the redbacks) or mass loss due to the companion expansion, and ‘evaporation’ may govern the evolution to the black widow stage and to the final disruption of the companion. -
Discovery of Frequency-Sweeping Millisecond Solar Radio Bursts Near 1400 Mhz with a Small Interferometer Physics Department Senior Honors Thesis 2006 Eric R
Discovery of frequency-sweeping millisecond solar radio bursts near 1400 MHz with a small interferometer Physics Department Senior Honors Thesis 2006 Eric R. Evarts Brandeis University Abstract While testing the Small Radio Telescope Interferometer at Haystack Observatory, we noticed occasional strong fringes on the Sun. Upon closer study of this activity, I find that each significant burst corresponds to an X-ray solar flare and corresponds to data observed by RSTN. At very short integrations (512 µs), most bursts disappear in the noise, but a few still show very strong fringes. Studying these <25 events at 512 µs integration reveals 2 types of burst: one with frequency structure and one without. Bursts with frequency structure have a brightness temperature ~1013K, while bursts without frequency structure have a brightness temperature ~108K. These bursts are studied at higher frequency resolution than any previous solar study revealing a very distinct structure that is not currently understood. 1 Table of Contents Abstract ..........................................................................................................................1 Table of Contents...........................................................................................................3 Introduction ...................................................................................................................5 Interferometry Crash Course ........................................................................................5 The Small Radio Telescope -
X-Ray Observations of Black Widow Pulsars
UvA-DARE (Digital Academic Repository) X-Ray Observations of Black Widow Pulsars Gentile, P.A.; Roberts, M.S.E.; McLaughlin, M.A.; Camilo, F.; Hessels, J.W.T.; Kerr, M.; Ransom, S.M.; Ray, P.S.; Stairs, I.H. DOI 10.1088/0004-637X/783/2/69 Publication date 2014 Document Version Final published version Published in Astrophysical Journal Link to publication Citation for published version (APA): Gentile, P. A., Roberts, M. S. E., McLaughlin, M. A., Camilo, F., Hessels, J. W. T., Kerr, M., Ransom, S. M., Ray, P. S., & Stairs, I. H. (2014). X-Ray Observations of Black Widow Pulsars. Astrophysical Journal, 783(2), 69. https://doi.org/10.1088/0004-637X/783/2/69 General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:27 Sep 2021 The Astrophysical Journal, 783:69 (8pp), 2014 March 10 doi:10.1088/0004-637X/783/2/69 C 2014.