A Fundamental Plane for Gamma-Ray Pulsars. (arXiv:1904.01765v1 [astro-ph.HE])
A Fundamental Plane for Gamma-Ray Pulsars. (arXiv:1904.01765v1 [astro-ph.HE]) <a href="http://arxiv.org/find/astro-ph/1/au:+Kalapotharakos_C/0/1/0/all/0/1">Constantinos Kalapotharakos</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Harding_A/0/1/0/all/0/1">Alice K. Harding</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Kazanas_D/0/1/0/all/0/1">Demosthenes Kazanas</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Wadiasingh_Z/0/1/0/all/0/1">Zorawar Wadiasingh</a> We show that the $gamma$-ray pulsar observables, i.e., their total $gamma$-ray luminosity, $L_{gamma}$, spectrum cut-off energy, $epsilon_{rm cut}$, stellar surface magnetic field, $B_{star}$, and spin-down power $dot{mathcal{E}}$, obey a relation of the form $L_{gamma}=f(epsilon_{rm cut},B_{star},dot{mathcal{E}})$, which represents a 3D plane in their 4D log-space. Fitting the data of the 88 pulsars of the second Fermi pulsar catalog, we show this relation to be $L_{gamma}propto epsilon_{rm cut}^{1.18pm 0.24}B_{star}^{0.17pm 0.05}dot{mathcal{E}}^{0.41pm 0.08}$, a pulsar fundamental plane (FP). We show that the observed FP is remarkably close toRead More →