The correlations and anticorrelations in QPO data
| dc.creator | Abramowicz, M. A. | |
| dc.creator | Barret, D. | |
| dc.creator | Bursa, M. | |
| dc.creator | Horak, J. | |
| dc.creator | Kluzniak, W. | |
| dc.creator | Rebusco, P. | |
| dc.creator | Torok, G. | |
| dc.date | 2005-10-15 | |
| dc.date.accessioned | 2026-07-07T06:43:54Z | |
| dc.date.available | 2026-07-07T06:43:54Z | |
| dc.description | Double peak kHz QPO frequencies in neutron star sources varies in time by a factor of hundreds Hz while in microquasar sources the frequencies are fixed and located at the line ν_2 = 1.5 ν_1 in the frequency-frequency plot. The crucial question in the theory of twin HFQPOs is whether or not those observed in neutron-star systems are essentially different from those observed in black holes. In black hole systems the twin HFQPOs are known to be in a 3:2 ratio for each source. At first sight, this seems not to be the case for neutron stars. For each individual neutron star, the upper and lower kHz QPO frequencies, ν_2 and ν_1, are linearly correlated, ν_2=A ν_1 + B, with the slope A < 1.5, i.e., the frequencies definitely are not in a 1.5 ratio. In this contribution we show that when considered jointly on a frequency-frequency plot, the data for the twin kHz QPO frequencies in several (as opposed to one) neutron stars uniquely pick out a certain preferred frequency ratio that is equal to 1.5 for the six sources examined so far. | |
| dc.description | 3 pages, 1 figure, Astronomische Nachrichten, in press | |
| dc.identifier | https://arxiv.org/abs/astro-ph/0510462 | |
| dc.identifier | http://arxiv.org/abs/astro-ph/0510462 | |
| dc.identifier | Astron.Nachr. 326 (2005) 864-866 | |
| dc.identifier | doi:10.1002/asna.200510428 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/102594 | |
| dc.subject | Astrophysics | |
| dc.title | The correlations and anticorrelations in QPO data | |
| dc.type | text |