2025ApJ...989..228T


Query : 2025ApJ...989..228T

2025ApJ...989..228T - Astrophys. J., 989, 228 (2025/August-3)

Pulsar Cyclic Spectroscopy in the Partial-deconvolution Regime: Benefits and Limitations.

TURNER J.E., DOLCH T., DEMOREST P.B., LYNCH R.S., STINEBRING D.R., JESSUP C., JONES N. and SCHEITHAUER C.

Abstract (from CDS):

We explore possible advantages of cyclic spectroscopy for observations of pulsars in instances where full cyclic deconvolution is not possible. We compute cyclic merits and full-deconvolution regime boundaries for pulsars observed by NANOGrav and discuss which sources stand to benefit the most from using cyclic spectroscopy when observed with the Green Bank Telescope and DSA-2000 in a given frequency range. We compare data products, namely the wavefield, in both full-deconvolution and partial-deconvolution regimes to demonstrate what can be accomplished with incomplete phase retrieval. Additionally, we show how some phase retrieval can still be achieved in the partial-deconvolution regime and how this allows for additional information in scintillation-based data products, like the dynamic wavefield power, compared to what can be found in traditional dynamic spectra. An examination of dynamic wavefield phase as a function of observing frequency reveals more complete phase retrieval is achieved the closer one gets to the full-deconvolution regime, agreeing with the expectations of cyclic merit. While we demonstrate that fragmentary recovery of the secondary wavefield can be accomplished in the partial-deconvolution regime, we advocate for a synergistic approach with phase retrieval methods like the θ-θ transform, although we also provide discussion about shortcomings of this strategy. Finally, we use the combination of modest cyclic merit and lack of discernible results for PSR J1903+0327 to motivate the creation of an updated “cyclic merit 2.0,” which relies on scintillation bandwidth instead of observing bandwidth.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Millisecond pulsars - Pulsars - Pulsar timing method - Interstellar medium

Simbad objects: 47

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Number of rows : 47
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0023+0923 Psr 00 23 16.890 +09 23 24.18           ~ 137 0
2 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
3 PSR J0340+41 Psr 03 40 23.2887 +41 30 45.300           ~ 91 0
4 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
5 PSR J0636+5129 Psr 06 36 04.84645 +51 28 59.9625           ~ 101 0
6 PSR J0645+5158 Psr 06 45 59.08191 +51 58 14.9210           ~ 65 0
7 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
8 PSR J0922-52 Psr 09 21 59.8785 -52 02 38.470           ~ 9 0
9 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
10 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
11 PSR J1125+7819 Psr 11 25 59.851 +78 19 48.70           ~ 36 0
12 PSR J1453+1902 Psr 14 53 45.7175 +19 02 12.224           ~ 41 1
13 PSR J1455-3300 Psr 14 55 47.976991 -33 30 46.40280           ~ 165 1
14 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
15 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
16 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
17 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
18 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
19 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
20 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
21 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
22 PSR J1747-4036 Psr 17 47 48.715690 -40 36 54.79950           ~ 83 0
23 PSR J1832-0836 Psr 18 32 27.589497 -08 36 55.14540           ~ 86 0
24 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
25 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
26 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
27 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
28 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
29 PSR J1911+1347 Psr 19 11 55.204694 +13 47 34.38383           ~ 72 0
30 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
31 PSR J1923+2515 Psr 19 23 22.494560 +25 15 40.64360           ~ 53 0
32 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
33 PSR J1944+0907 Psr 19 44 09.32 +09 07 23.2           ~ 65 1
34 PSR J1946+3417 Psr 19 46 25.13182 +34 17 14.6770           ~ 64 0
35 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
36 PSR J2010-1323 Psr 20 10 45.922635 -13 23 56.13270           ~ 93 0
37 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 120 1
38 PSR J2033+1736 Psr 20 33 16.9140266736 +17 37 48.047177388   11.59 10.50     ~ 76 0
39 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
40 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
41 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 136 0
42 PSR J2229+26 Psr 22 29 50.883815 +26 43 57.61393           ~ 121 1
43 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0
44 PSR J2234+0944 Psr 22 34 46.856913 +09 44 30.04150           ~ 82 0
45 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0
46 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1
47 PSR J2322+2057 Psr 23 22 22.320041 +20 57 02.50080           ~ 129 1

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