Calibration Activities the MOS perspective

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Transcription:

Calibration Activities the perspective Changing the Quantum Efficiency Calibration: Motivation and Justification.

Flux comparison using a sample (17) of AGN observations: as presented at MPE (May 2006) Band (kev) (1-PN)/PN (2-PN)/PN 0.54-0.85 0.85-1.50 1.50-4.0 4.0-10.0-5.4% +2.4% +6.8% +11.4% -1.6% +4.1% +7.3% +7.4%

v PN effective area discrepancy: 3C 273 comparison

Investigating additional transmission layers H2O 0.12 µm SiO2 0.068 Si3N4 0.059 Si 0.12

3C 273: What the PN sees Model: phabs*(po+po) N H = 1.79x10 20 cm -2 χ 2 = 1.08

Comparison: PN Model with 1 data and various QEs ICE 0.12 µm

Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO2 0.068 µm

Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO2 0.068 µm Si3N4 0.059 µm

Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO2 0.068 µm Si3N4 0.059 µm Si 0.12 µm

Constraint on Si edge also precludes strong Si absorber Edge depth known Within ~2-3%

QE17 Adjustment of edges at C, N, O, only

Comparison with Orsay CCD1 1 CCD1 2

Comparison with Orsay CCD1 1

Model: phabs*(po+po) χ 2 = 1.19

All Const = 1.0 Model: const*phabs*(po+po): const(m1) = 1.03 const(m2) =1.06 χ 2 = 1.11 (with global renormalisation, c.f. 1.19 before without)

PN soft/hard slopes: Γ 1 =3.20(0.11) Γ 2 =1.63(0.01) M1 M2 qe16 M1 M2 qe17 Γ 1 =4.71(0.15) Γ 1 =4.65(0.15) Γ 1 =3.73(0.15) Γ 1 =3.76(0.15) Γ 2 =1.64(0.02) Γ 2 =1.69(0.02) Γ 2 =1.61(0.02) Γ 2 =1.65(0.02)

M1 M1 0065 0981 1ES0102 M2 M2 0065 0981

1 v RGS model, 1ES0102 Rev 0065 N H =5.36x10 20 cm -2 Const x (RGS model) 0.3-1.5 kev 1 χ 2 = 3.65 -> 1.78 Const. 0.51 -> 0.80 2 χ 2 = 3.70 -> 2.30 Const. 0.58 -> 0.90

1 v RGS model, 1ES0102 Rev 0981 N H =5.36x10 20 cm -2 Const x (RGS model) 0.3-1.5 kev 1 χ 2 = 5.47 -> 2.16 Const. 0.39 -> 0.74 2 χ 2 = 7.46 -> 2.62 Const. 0.33 -> 0.70

N H =5.36x10 20 cm -2 N H =8.00x10 20 cm -2

Zoom showing resolution adjustment required for later Revs

Comparison with Zeta Puppis On-axis Point Source Const x (RGS model) 0.3-1.5 kev 1 χ 2 = 1.69 -> 1.49 Const. 1.05 -> 1.12 2 χ 2 = 1.76 -> 1.51 Const. 1.07 -> 1.15

Independent astrophysical evidence? Spectral fitting to relatively high column density BL Lac N H ~ 4.4x10 20 cm -2 TBABS * PO Wilms abund 0.15-5.0 kev 1 χ 2 = 1.13 -> 1.06 2 χ 2 = 1.16 -> 1.08

(1-PN)/PN Thin Medium (2-PN)/PN

Problem with the psf? See talk by Andy later 3c 273: Flux Comparison, 7.5-40 v 15-40 extraction radii pn 1 2

Problem with the psf? See talk by Andy later MCG-6-30-15: 0, 7.5, 11.25, 15 inner extraction radii, 40 outer pn 1 2

Band (kev) 0.54-0.85 0.85-1.50 1.50-4.0 4.0-10.0 (1-PN)/PN -5.4% +2.4% +6.8% +11.4% (2-PN)/PN -1.6% +4.1% +7.3% +7.4%

Quantum Efficiency measurements from Orsay 1 Central CCD

Quantum Efficiency measurements from Orsay 2 Central CCD

Surface Pixel Geometry in Monte Carlo model

SEM Pictures Side View Top View

(1-PN)/PN +12% +2%

(2-PN)/PN +12% +2%

H 2 O = 0.08 µm

H 2 O = 0.08 µm SiO 2 = 0.05 µm

Summary: Shape of the /PN discrepancy suggests problem lies with the quantum efficiency Adjustment of the QE would be consistent with Orsay measurements and probable uncertainties in model Adjusting the QE would leave a residual normalisation offset of about 5-7% between and PN Would need to increase global effective area or decrease PN global effective area to achieve absolute consistency low energy rmf would need re-calibration for consistency with any change in the QE

Comparison Count Rate/Effective of high energy Area portion normalised of the spectra to Rev from 156795 Datum and 903 Rate down 8% Eff. Area down 3% Flux down 5%