ζ Pup: XMM RGS line-profile analysis

N VII at 20.910 A

There is almost no RGS2 data for this line, so we will use only the RGS1 data.

First we repeat the non-porous fit shown on the main page.

Non-porous: RGS1

N VII 20.910: non-porous: RGS1 fit, shift zero [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.05e-4   +/- (7.33e-4:1.13e-3)
q = 0
hinf = 0
taustar = 4.93   +/- (3.90:5.59)
Ro = 1.41   +/- (1.01:2.03)
shift = 0
norm = 1.66e-4   +/- (1.56e-4:1.73e-3)
chisq = 40.52 for N = 36

The fit is quite good (though mostly, I assume, because these data are relatively low S/N). The taustar value is high, as would be expected.

Next, we'll fit models with anisotropic porosity assuming flattened, radially oriented clumps. We use the "stretch" porosity length distribution, h(r), parameterized by hinf. We will fit first with hinf a free parameter, and then at fixed values of hinf = 0.5, 1, 2, and 5 R*.

aniso-porous: RGS1, hinf free

N VII 20.910: aniso-porous, h free: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.26e-4   +/- (:)
q = 0
hinf = 0.00   +/- (0.00:0.03)
taustar = 4.88   +/- (4.00:5.89)
Ro = 1.32   +/- (1.01:2.03)
shift = 0
norm = 1.65e-4   +/- (1.56e-4:1.75e-4)
chisq = 40.52 for N = 36

Note that despite the fact that the terminal porosity length's best-fit value is found to be zero (1e-7 or so, actually), the best-fit model parameters are not identical to the non-porous fit. They are very close, of course, but the small differences are probably due to the numerical integration that's required in the aniso case. Note that the 68% upper confidence limit on hinf is 0.03, and that enables slightly larger confidence limits on taustar.

Now, a sequence of fits with fixed hinf values of 0.5, 1, 2, and 5.

aniso-porous: RGS1, hinf = 0.5

N VII 20.910: aniso-porous, h = 0.5: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 7.61e-4   +/- (5.26e-4:9.96e-4)
q = 0
hinf = 0.5
taustar = 7.96   +/- (6.15:10.16)
Ro = 1.60   +/- (1.24:2.01)
shift = 0
norm = 1.69e-4   +/- (1.59e-4:1.80e-4)
chisq = 52.92 for N = 36

aniso-porous: RGS1, hinf = 1

N VII 20.910: aniso-porous, h = 1: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 6.20e-4   +/- (3.75e-4:8.79e-4)
q = 0
hinf = 1
taustar = 12.95   +/- (9.61:17.46)
Ro = 1.70   +/- (1.36:2.14)
shift = 0
norm = 1.75e-4   +/- (1.63e-4:1.86e-4)
chisq = 62.38 for N = 36

aniso-porous: RGS1, hinf = 2

N VII 20.910: aniso-porous, h = 2: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 3.53e-4   +/- (:)
q = 0
hinf = 2
taustar = 34.11   +/- (:)
Ro = 1.62   +/- (:)
shift = 0
norm = 1.86e-4   +/- (:)
chisq = 73.45 for N = 36

aniso-porous: RGS1, hinf = 5

N VII 20.910: aniso-porous, h = 5: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 3.53e-4   +/- (:)
q = 0
hinf = 5
taustar = 100   +/- (:)
Ro = 1.73   +/- (:)
shift = 0
norm = 1.91e-4   +/- (:)
chisq =84.35 for N = 36

Summarizing

The effect of porosity and the tradeoff between porosity length and optical depth can be summarized by looking at the joint parameter confidence limits. We show the 68%, 95%, and 99% limits below. The best-fit model is the filled circle.

N VII 20.910: aniso-porous h vs taustar confidence limits: RGS1

Now, we'll look at models with isotropic porosity.

iso-porous: RGS1, hinf free

N VII 20.910: iso-porous, h free: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.11e-4   +/- (6.94e-4:1.14e-3)
q = 0
hinf = 0.22   +/- (0.00:1.34)
taustar = 5.55   +/- (3.90:9.18)
Ro = 1.49   +/- (1.01:2.08)
shift = 0
norm = 1.66e-4   +/- (1.56e-4:1.76e-4)
chisq = 40.45 for N = 36

iso-porous: RGS1, hinf = 0.5

N VII 20.910: iso-porous, h = 0.5: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.19e-4   +/- (6.96e-4:1.11e-3)
q = 0
hinf = 0.5
taustar = 6.18   +/- (4.72:8.07)
Ro = 1.65   +/- (1.14:2.11)
shift = 0
norm = 1.66e-4   +/- (1.56e-4:1.76e-4)
chisq = 40.55 for N = 36

iso-porous: RGS1, hinf = 1

N VII 20.910: iso-porous, h = 1: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.19e-4   +/- (7.10e-4:1.15e-3)
q = 0
hinf = 1
taustar = 7.42   +/- (5.51:10.09)
Ro = 1.79   +/- (1.43:2.15)
shift = 0
norm = 1.66e-4   +/- (1.56e-4:1.76e-4)
chisq = 41.01 for N = 36

Note: with hinf = 1, taustar has increased by 51 percent.

iso-porous: RGS1, hinf = 2

N VII 20.910: iso-porous, h = 2: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 9.40e-4   +/- (7.26e-4:1.16e-3)
q = 0
hinf = 2
taustar = 10.16   +/- (7.40:14.42)
Ro = 1.95   +/- (1.65:2.28)
shift = 0
norm = 1.66e-4   +/- (1.56e-4:1.76e-4)
chisq = 42.40 for N = 36

iso-porous: RGS1, hinf = 5

N VII 20.910: iso-porous, h = 5: RGS1 [20.70:21.07]
vinf = 2250
β = 1
powerlaw continuum, n = 2
norm = 8.39e-4   +/- (6.23e-4:1.06e-3)
q = 0
hinf = 5
taustar = 26.09   +/- (18.13:38.53)
Ro = 2.14   +/- (1.85:2.52)
shift = 0
norm = 1.69e-4   +/- (1.60e-4:1.79e-4)
chisq = 49.02 for N = 36

Summarizing

We show the 68%, 95%, and 99% limits below. The best-fit model is the filled circle.

N VII 20.910: iso-porous h vs taustar confidence limits: RGS1

And here is an extensive log of all these xspec fits.

 

Back to the top


last modified: 18 May 2012