Long-term monitoring of PSR J2021+4026 in the heart of the Cygnus region with the Fermi Large Area Telescope unveiled a sudden decrease in flux above 100 MeV over a timescale shorter than a week. The "jump" was near MJD 55850 (2011 October 16), with the flux decreasing from (8.33 ± 0.08) × 10–10 erg cm–2 s–1 to (6.86 ± 0.13) × 10–10 erg cm–2 s–1. Simultaneously, the frequency spindown rate increased from (7.8 ± 0.1) × 10–13 Hz s–1 to (8.1 ± 0.1) × 10–13 Hz s–1. Significant (>5σ) changes in the pulse profile and marginal (<3σ) changes in the emission spectrum occurred at the same time. There is also evidence for a small, steady flux increase over the 3 yr preceding MJD 55850. This is the first observation at γ-ray energies of mode changes and intermittent behavior, observed at radio wavelengths for other pulsars. We argue that the change in pulsed γ-ray emission is due to a change in emission beaming and we speculate that it is precipitated by a shift in the magnetic field structure, leading to a change of either effective magnetic inclination or effective current.

PSR J2021+4026 IN THE GAMMA CYGNI REGION: THE FIRST VARIABLE γ-RAY PULSAR SEEN BY THE Fermi LAT

BALDINI, LUCA;RAZZANO, MASSIMILIANO;TINIVELLA, MARCO;
2013-01-01

Abstract

Long-term monitoring of PSR J2021+4026 in the heart of the Cygnus region with the Fermi Large Area Telescope unveiled a sudden decrease in flux above 100 MeV over a timescale shorter than a week. The "jump" was near MJD 55850 (2011 October 16), with the flux decreasing from (8.33 ± 0.08) × 10–10 erg cm–2 s–1 to (6.86 ± 0.13) × 10–10 erg cm–2 s–1. Simultaneously, the frequency spindown rate increased from (7.8 ± 0.1) × 10–13 Hz s–1 to (8.1 ± 0.1) × 10–13 Hz s–1. Significant (>5σ) changes in the pulse profile and marginal (<3σ) changes in the emission spectrum occurred at the same time. There is also evidence for a small, steady flux increase over the 3 yr preceding MJD 55850. This is the first observation at γ-ray energies of mode changes and intermittent behavior, observed at radio wavelengths for other pulsars. We argue that the change in pulsed γ-ray emission is due to a change in emission beaming and we speculate that it is precipitated by a shift in the magnetic field structure, leading to a change of either effective magnetic inclination or effective current.
2013
A., Allafort; Baldini, Luca; J., Ballet; G., Barbiellini; M. G., Baring; D., Bastieri; R., Bellazzini; E., Bonamente; E., Bottacini; T. J., Brandt; J., Bregeon; P., Bruel; R., Buehler; S., Buson; G. A., Caliandro; R. A., Cameron; P. A., Caraveo; C., Cecchi; R. C. G., Chaves; A., Chekhtman; J., Chiang; G., Chiaro; S., Ciprini; R., Claus; F., D'Ammando; F., de Palma; S. W., Digel; L., Di Venere; P. S., Drell; C., Favuzzi; E. C., Ferrara; A., Franckowiak; P., Fusco; F., Gargano; D., Gasparrini; N., Giglietto; M., Giroletti; T., Glanzman; G., Godfrey; I. A., Grenier; S., Guiriec; D., Hadasch; A. K., Harding; M., Hayashida; K., Hayashi; E., Hays; J., Hewitt; A. B., Hill; D., Horan; X., Hou; T., Jogler; A. S., Johnson; T. J., Johnson; M., Kerr; J., Knödlseder; M., Kuss; J., Lande; S., Larsson; L., Latronico; M., Lemoine Goumard; F., Longo; F., Loparco; P., Lubrano; D., Malyshev; M., Marelli; M., Mayer; M. N., Mazziotta; J., Mehault; T., Mizuno; M. E., Monzani; A., Morselli; S., Murgia; R., Nemmen; E., Nuss; T., Ohsugi; N., Omodei; M., Orienti; E., Orlando; D., Paneque; M., Pesce Rollins; M., Pierbattista; F., Piron; G., Pivato; T. A., Porter; S., Rainò; R., Rando; P. S., Ray; Razzano, Massimiliano; O., Reimer; T., Reposeur; R. W., Romani; A., Sartori; P. M., Saz Parkinson; C., Sgrò; E. J., Siskind; D. A., Smith; P., Spinelli; A. W., Strong; H., Takahashi; J. B., Thayer; D. J., Thompson; L., Tibaldo; Tinivella, Marco; D. F., Torres; G., Tosti; Y., Uchiyama; T. L., Usher; J., Vandenbroucke; V., Vasileiou; C., Venter; G., Vianello; V., Vitale; B. L., Winer; K. S., Wood
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/335668
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