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73 Pith papers citing it
Method 53% of classified citations

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method 8 background 4 dataset 2 other 1

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  • other NGC 1068 094.B-0321(A) 64.6" x 63.8" 5.29 x 5.16 0.9" 2014-10-06 NGC 253 0102.B-0078(A) 87.4" x 87.2" 1.51 x 1.51 0.9" 2018-11-07 NGC 1320 108.229J.001 63.6" x 63.8" 12.51 x 12.55 0.7" 2022-01-07 13h25m30s 29s 28s 27s 26s 25s □43◦00′45′′ 01′00′′ 15′′ 30′′ RA DEC N 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 1" 200pc -17 -16.5 -16 -15.5 -15 log(F lux) [erg cm□2s□1] (a) Centaurus A, H α line map. 2h42m42s 41s 40s 39s □0◦00′15′′ 30′′ 45′′ 01′00′′ 15′′ RA DEC N 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17
  • method analysis, as described in the following. Since all sources but one (J103853.29+392151.12) show only narrow emission lines, we used the stellar velocity dispersion (σ∗) found through the fitting of the stellar kinematic component to estimate the BH mass. To do this, we used the relation from McConnell & Ma (2013): log10  MBH M⊙  =(8.32±0.05)+(5.64±0.32) log 10  σ∗ 200 km s−1  . (1) Using these mass estimates, we derived the corresponding Eddington (1916) luminosity (LEdd) of each AGN in the 2
  • method about these mechanisms in Appendix B. 1.3. Cluster relaxation and core-collapse Any gravitationally bound system undergoes dynamical relax- ation driven by the continuous dynamical interactions among its constituents. In a star cluster, this process occurs over a timescale (Spitzer 1969; Binney & Tremaine 2008): trel =4.2 Gyr 15 lnΛ c ! Rh,cl 4 pc ! s Mcl 107 M⊙ ,(1) called half-mass relaxation time, which depends on the cluster mass (Mcl) and the radius within which half of the cluster mass is
  • method the star-galaxy separation by selecting objects that have a half- light radius larger than 0 .′′09. At the same time we removed faint galaxies with very large (and often non-physical) size es- timates, which can occur for very noisy objects. The magnitude- dependent selection that we adopted for this keeps objects with a half-light radius less than [−0 .′′1875 (IE − 24) + 1 .′′85]. This se- lection excludes all objects with a half-light radius larger than 1 .′′85 at IE = 24, but this limit incre
  • method We follow the approach described by Leja et al. (2019a) with prior continuity. The continuity prior constrains the ratio of SFRs between the consecutive time-steps. This approach results in re- duced burstiness, that is, fewer rapid changes in SFR in time. The SFR changes follow the Student-t distribution, which is de- scribed by: PDF(x, ν)= Γ  ν+1 2  √νπΓ  ν 2  1+ (x/σt)2 ν !− ν+1 2 ,(1) whereΓis the Gamma function,νis the degree of freedom, and σt is the scale factor. Since with Student-t
  • background covering the wavelength of the H 2 line of interest is shown in Figure 1. This data is yet to be corrected for tellurics or blaze; as such it has arbitrary flux units and displays an upward trend with wavelength. Article number, page 3 of 16 A&A proofs:manuscript no. aanda Table 1: Stellar and Disk Parameters for HD 131488 and HD 110058. Parameter HD 131488 References HD 110058 References Spectral Type A1 V [1] A0 V [2] R.A. (J2000) 14 55 08.03 [1] 12 39 46.14 [2] Decl. (J2000) -41 07 13.3 [1] -

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representative citing papers

The hydrodynamical response of cold circumgalactic clouds to quasar radiation

astro-ph.GA · 2026-04-17 · accept · novelty 7.0

Cold CGM clouds under quasar radiation follow optically thin ionization, radiation-shielded, or rocket-effect paths, with the latter increasing Lyα luminosity up to 10x and bright quasars fully ionizing the cold gas while faint ones drive rocket effects.

Neutron star atmospheres composed of fusion ashes

astro-ph.HE · 2026-04-17 · unverdicted · novelty 6.0

Numerical models of neutron star atmospheres from fusion ashes show a radiation-pressure layer limiting flux and absorption edges tied to chemical composition, with fits to diluted blackbodies plus edges for X-ray burst interpretation.

Near-critical magnetic fields in Kepler red giants

astro-ph.SR · 2026-04-10 · unverdicted · novelty 6.0

Near-critical magnetic fields of 100-700 kG confined below the H-burning shell are inferred in eight Kepler red giants via non-perturbative modeling of mixed-mode frequencies, identifying components as m=0 and m=1 rather than m=±1.

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Showing 50 of 73 citing papers.