Matches in SemOpenAlex for { <https://semopenalex.org/work/W2536145767> ?p ?o ?g. }
- W2536145767 abstract "To put new constraints on the r-mode instability window, we analyse the formation of millisecond pulsars (MSPs) within the recycling scenario, making use of three sets of observations: (a) X-ray observations of neutron stars (NSs) in low-mass X-ray binaries; (b) timing of millisecond pulsars; and (c) X-ray and UV observations of MSPs. As shown in previous works, r-mode dissipation by shear viscosity is not sufficient to explain observational set (a), and enhanced r-mode dissipation at the red-shifted internal temperatures $T^inftysim 10^8$ K is required to stabilize the observed NSs. Here, we argue that models with enhanced bulk viscosity can hardly lead to a self-consistent explanation of observational set (a) due to strong neutrino emission, which is typical for these models (unrealistically powerful energy source is required to keep NSs at the observed temperatures). We also demonstrate that the observational set (b), combined with the theory of internal heating and NS cooling, provides evidence of enhanced r-mode dissipation at low temperatures, $T^inftysim 2times 10^7$ K. Observational set (c) allows us to set an upper limit on the internal temperatures of MSPs, $T^infty<2times 10^7$ K (assuming a canonical NS with the accreted crust). Recycling scenario can produce MSPs at these temperatures only if r-mode instability is suppressed in the whole MSP spin frequency range ($nulesssim 750$ Hz) at temperatures $2times 10^7lesssim T^inftylesssim 3 times 10^7$ K, providing thus a new constraint on the r-mode instability window. These observational constraints are analysed in more details in application to the resonance uplift scenario of Gusakov et al. [Phys. Rev. Lett., 112 (2014), 151101]." @default.
- W2536145767 created "2016-10-28" @default.
- W2536145767 creator A5007493982 @default.
- W2536145767 creator A5080032811 @default.
- W2536145767 creator A5084364549 @default.
- W2536145767 date "2017-02-16" @default.
- W2536145767 modified "2023-09-24" @default.
- W2536145767 title "R modes and neutron star recycling scenario" @default.
- W2536145767 cites W1819980193 @default.
- W2536145767 cites W1828825141 @default.
- W2536145767 cites W1860224658 @default.
- W2536145767 cites W1891879171 @default.
- W2536145767 cites W1895337021 @default.
- W2536145767 cites W1897104638 @default.
- W2536145767 cites W1937636621 @default.
- W2536145767 cites W1958239481 @default.
- W2536145767 cites W1967206153 @default.
- W2536145767 cites W1973820399 @default.
- W2536145767 cites W1975569559 @default.
- W2536145767 cites W1981177599 @default.
- W2536145767 cites W1987498268 @default.
- W2536145767 cites W1990382791 @default.
- W2536145767 cites W1992589084 @default.
- W2536145767 cites W1992707378 @default.
- W2536145767 cites W2001733457 @default.
- W2536145767 cites W2007049136 @default.
- W2536145767 cites W2011591061 @default.
- W2536145767 cites W2013079526 @default.
- W2536145767 cites W2013863497 @default.
- W2536145767 cites W2016762929 @default.
- W2536145767 cites W2020706287 @default.
- W2536145767 cites W2020860529 @default.
- W2536145767 cites W2022044745 @default.
- W2536145767 cites W2024184076 @default.
- W2536145767 cites W2034698434 @default.
- W2536145767 cites W2036056653 @default.
- W2536145767 cites W2038683553 @default.
- W2536145767 cites W2041194733 @default.
- W2536145767 cites W2045694681 @default.
- W2536145767 cites W2047136101 @default.
- W2536145767 cites W2047479827 @default.
- W2536145767 cites W2051368651 @default.
- W2536145767 cites W2054790748 @default.
- W2536145767 cites W2055817049 @default.
- W2536145767 cites W2056344596 @default.
- W2536145767 cites W2056543278 @default.
- W2536145767 cites W2057439225 @default.
- W2536145767 cites W2065450909 @default.
- W2536145767 cites W2065621451 @default.
- W2536145767 cites W2066573965 @default.
- W2536145767 cites W2070559138 @default.
- W2536145767 cites W2076222864 @default.
- W2536145767 cites W2081454720 @default.
- W2536145767 cites W2081545524 @default.
- W2536145767 cites W2082540985 @default.
- W2536145767 cites W2091459372 @default.
- W2536145767 cites W2092747576 @default.
- W2536145767 cites W2093261654 @default.
- W2536145767 cites W2101916493 @default.
- W2536145767 cites W2104339931 @default.
- W2536145767 cites W2111556607 @default.
- W2536145767 cites W2122383486 @default.
- W2536145767 cites W2140778314 @default.
- W2536145767 cites W2144732123 @default.
- W2536145767 cites W2147534440 @default.
- W2536145767 cites W2150450660 @default.
- W2536145767 cites W2171539518 @default.
- W2536145767 cites W2217627322 @default.
- W2536145767 cites W2241183286 @default.
- W2536145767 cites W2264236015 @default.
- W2536145767 cites W2288741738 @default.
- W2536145767 cites W2569502108 @default.
- W2536145767 cites W2594385597 @default.
- W2536145767 cites W2950667339 @default.
- W2536145767 cites W2963319749 @default.
- W2536145767 cites W3098295454 @default.
- W2536145767 cites W3098517639 @default.
- W2536145767 cites W3098562513 @default.
- W2536145767 cites W3098960446 @default.
- W2536145767 cites W3099003725 @default.
- W2536145767 cites W3099207879 @default.
- W2536145767 cites W3099506839 @default.
- W2536145767 cites W3099662046 @default.
- W2536145767 cites W3099702782 @default.
- W2536145767 cites W3099899127 @default.
- W2536145767 cites W3100196934 @default.
- W2536145767 cites W3100253665 @default.
- W2536145767 cites W3100346910 @default.
- W2536145767 cites W3101274556 @default.
- W2536145767 cites W3101623799 @default.
- W2536145767 cites W3101727583 @default.
- W2536145767 cites W3102725444 @default.
- W2536145767 cites W3103695714 @default.
- W2536145767 cites W3103706077 @default.
- W2536145767 cites W3103993031 @default.
- W2536145767 cites W3104965572 @default.
- W2536145767 cites W3105146501 @default.
- W2536145767 cites W3105804236 @default.
- W2536145767 cites W3106263174 @default.
- W2536145767 cites W3106415219 @default.