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Area and Energy
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Effective Area and
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Line Flux Density
Effective Area and Energy Resolution
vs. Grade Selection; Pre-launch Results
The HRMA/ACIS effective area and energy resolution were calculated for
the ASCA grade selections g0, g01, g012, g0123, g01234, g012345, g02346.6.1
We also considered the special case of including all grades except ACIS
grade 255. ACIS 255 (which corresponds to all eight neighbors of the central
pixel being above the Split Event Threshold) is considered to contain mostly
events that result from interactions of cosmic ray particles with ACIS
(and not X-ray photons). Figure 6.1
and figure
6.2 show the dependence
of effective area with grade selection for ACIS CCD's I1 and S3. Tables
6.8 and 6.9
provide numerical forms of the results.
Figure 6.1: Effective Area vs. Energy and Grade Selection
for ACIS CCD I1 calculated for grade selections of g0, g01, g02, g023,
g01234, g012345, g02346, all grades - ACIS255
Table 6.8: Effective Area vs. Energy
and Grade Selection for CCD I1
| Energy keV |
Effective Area |
| g0 |
g01 |
g02 |
g023 |
g01234 |
g012345 |
g02346 |
all - ACIS(255) |
| cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
| 0.277 |
2.33 |
2.33 |
2.37 |
2.37 |
2.38 |
2.38 |
2.38 |
2.38 |
| 0.525 |
96.82 |
101.15 |
106.49 |
109.60 |
117.11 |
118.37 |
118.87 |
118.96 |
| 0.93 |
283.51 |
289.22 |
309.47 |
317.53 |
330.60 |
333.30 |
334.75 |
335.31 |
| 1.4867 |
412.15 |
426.40 |
480.60 |
506.20 |
545.22 |
558.62 |
570.06 |
572.62 |
| 3 |
213.56 |
217.10 |
248.15 |
260.79 |
276.30 |
279.77 |
286.28 |
287.23 |
| 4 |
204.53 |
216.40 |
260.17 |
280.58 |
312.61 |
326.90 |
345.91 |
351.00 |
| 5 |
136.17 |
151.35 |
193.68 |
215.76 |
253.12 |
277.71 |
320.80 |
341.08 |
| 6 |
51.96 |
60.69 |
81.09 |
92.91 |
112.95 |
130.95 |
168.88 |
207.70 |
| 7 |
21.77 |
25.13 |
35.76 |
40.97 |
49.48 |
56.26 |
79.82 |
109.90 |
| 8 |
8.93 |
9.98 |
14.83 |
17.05 |
20.28 |
22.62 |
34.23 |
52.95 |
| 9 |
3.60 |
4.03 |
6.00 |
6.96 |
8.34 |
9.00 |
14.44 |
23.77 |
The effective area values listed in this table apply for CCD
ID = 1, a HRMA Pitch angle of 5 arcmin, a HRMA Yaw angle of -3.7 arcmin,
and a split event threshold of 13 adu. Events within the entire CCD were
considered.
Figure 6.2: Effective Area vs.
Energy for ACIS CCD S3 calculated for grade selections of g0, g01, g02,
g023, g01234, g012345, g02346, all grades - ACIS255
Table 6.9: Effective Area vs. Energy for
CCD S3
| Energy keV |
Effective Area |
| g0 |
g01 |
g02 |
g023 |
g01234 |
g012345 |
g02346 |
all - ACIS(255) |
| cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
cm2 |
| 0.277 |
109.09 |
113.72 |
137.46 |
149.75 |
166.9 |
167.65 |
168.43 |
168.49 |
| 0.522 |
141.25 |
147.66 |
236.67 |
279.46 |
330.76 |
354.62 |
394.43 |
405.34 |
| 1.4867 |
154.10 |
160.54 |
305.89 |
373.49 |
451.76 |
480.94 |
591.09 |
611.30 |
| 3 |
39.15 |
40.90 |
119.42 |
155.51 |
196.07 |
209.37 |
348.93 |
380.83 |
| 4 |
32.02 |
35.22 |
92.73 |
115.54 |
148.12 |
170.75 |
307.53 |
387.58 |
| 5 |
26.06 |
29.64 |
67.36 |
80.18 |
104.11 |
125.00 |
224.27 |
322.95 |
| 6 |
15.96 |
18.27 |
39.48 |
46.06 |
59.37 |
73.77 |
129.18 |
204.34 |
| 7 |
12.68 |
14.15 |
29.06 |
33.79 |
43.54 |
51.44 |
87.31 |
125.03 |
| 8 |
5.98 |
6.42 |
13.10 |
14.90 |
19.23 |
22.23 |
37.13 |
51.08 |
| 9 |
3.50 |
3.77 |
8.14 |
9.22 |
12.11 |
14.01 |
24.54 |
32.72 |
The effective area values listed in this table apply for CCD
ID = 7, a HRMA Pitch angle of 0 arcmin, a HRMA Yaw angle of 0 arcmin, and
a split event threshold of 13 adu. Events within the entire CCD were considered.
The effective area measurements for the FI and BI devices presented
here were made with HRMA (Pitch,Yaw) values of (5',-3.7') and (0,0) respectively.
For the purpose of comparing FI with BI performance we present in Table
6.10
a list of HRMA effective area correction factors for converting the off-axis
(5',-3.7') FI effective areas to on-axis ones.
Table 6.10: HRMA Effective Area (EA) Correction Factors
for a HRMA Pitch Angle of 5 arcmin and a HRMA Yaw Angle of -3.7 arcmin.
Energy
keV |
HRMA EA |
HRMA EA |
Correction Factor |
| off-axis |
on-axis |
| cm2 |
cm2 |
| 0.277 |
766.71863 |
812.18695 |
0.9440 |
| 0.525 |
737.62781 |
781.42084 |
0.9440 |
| 0.93 |
740.83380 |
784.86621 |
0.9439 |
| 1.4867 |
732.67267 |
776.44696 |
0.9436 |
| 3 |
418.14990 |
445.54376 |
0.9385 |
| 4 |
432.86209 |
465.34161 |
0.9302 |
| 5 |
379.03247 |
417.80930 |
0.9072 |
| 6 |
251.41301 |
295.91565 |
0.8496 |
| 7 |
144.60548 |
190.16235 |
0.7604 |
|
The HRMA effective area off-axis correction factor is defined as the
ratio of the off-axis effective area to the on-axis value.
The first significant result is that the HRMA/ACIS effective area varies
considerably with grade selection for both front illuminated (FI) and back
illuminated (BI) CCD's. A possible use of this effect is in the analysis
of grating observations of faint objects where CCD energy resolution only
influences the separation of overlapping spectral orders. The exclusion
of only ACIS grade 255 will result in a relatively high effective area
and a higher signal to noise spectrum of the faint object.
Figure 6.3 and figure 6.4
show the dependence of energy resolution with grade selection for ACIS
CCD's I1 and S3. (Tables
6.11
and 6.12 give numeric
values of this data.) The energy resolution for FI chips is fairly insensitive
to grade selection in the 3-6 keV range. For energies above 6 keV the exclusion
of grades begins to improve energy resolution for FI chips. In the energy
range of 3-9 keV investigated so far, the energy resolution for back sided
CCD's improves significantly with the exclusion of grades.
A possible astrophysical observation in which this effect may be exploited
is ACIS imaging of a bright source with the BI chip. For bright sources
imaged on a BI chip it may be desirable to sacrifice source counts for
spectral resolution by selecting only single events.
Figure 6.3: Energy Resolution
(FWHM) vs. Energy for ACIS CCD I1 calculated for grade selections of g0,
g01, g012, g0123, g01234, g012345, g02346, all grades - ACIS255
Table 6.11: The energy resolution
(FWHM) values listed in this table apply for
CCD ID = 1, a HRMA
Pitch angle of 5 arcmin, a HRMA Yaw angle of -3.7 arcmin, and a split event
threshold of 13 adu. Events within the entire CCD were considered.
| Energy keV |
Energy Resolution |
| g0 |
g01 |
g012 |
g0123 |
g01234 |
g012345 |
g02346 |
all - ACIS(255) |
| eV |
eV |
eV |
eV |
eV |
eV |
eV |
eV |
| 3 |
89.40 |
89.86 |
90.10 |
90.08 |
89.78 |
90.03 |
90.59 |
90.19 |
| 4 |
100.80 |
101.57 |
103.14 |
103.17 |
103.00 |
102.81 |
103.59 |
103.67 |
| 5 |
115.21 |
114.78 |
115.44 |
115.92 |
116.01 |
116.19 |
116.50 |
116.52 |
| 6 |
126.29 |
126.06 |
129.75 |
130.70 |
132.07 |
133.08 |
134.67 |
134.44 |
| 7 |
137.47 |
138.59 |
141.74 |
142.48 |
143.12 |
146.60 |
151.75 |
151.84 |
| 8 |
139.43 |
141.91 |
146.13 |
148.93 |
152.01 |
154.79 |
164.02 |
165.79 |
| 9 |
158.36 |
154.01 |
165.58 |
167.14 |
168.19 |
175.50 |
188.22 |
196.76 |
Figure 6.4: Energy Resolution (FWHM) vs. Energy for ACIS
CCD S3 calculated for grade selections of g0, g01, g02, g023, g01234, g012345,
g02346, all grades - ACIS255
Table 6.12: The energy resolution
(FWHM) values listed in this table apply for
CCD ID = 7, a HRMA
Pitch angle of 0 arcmin, a HRMA Yaw angle of 0 arcmin, and a split event
threshold of 13 adu. Events within the entire CCD were considered.
| Energy keV |
Energy Resolution |
| g0 |
g01 |
g02 |
g023 |
g01234 |
g012345 |
g02346 |
all - ACIS(255) |
| eV |
eV |
eV |
eV |
eV |
eV |
eV |
eV |
| 0.277 |
77.18 |
77.22 |
73.07 |
71.20 |
69.84 |
69.89 |
70.07 |
69.96 |
| 0.525 |
90.86 |
90.86 |
92.83 |
93.11 |
93.12 |
93.20 |
92.34 |
92.70 |
| 1.4867 |
98.11 |
97.41 |
99.14 |
98.0 |
99.66 |
99.93 |
102.10 |
102.43 |
| 3 |
119.18 |
120.74 |
133.01 |
128.95 |
133.87 |
134.82 |
137.55 |
139.11 |
| 4 |
130.11 |
131.13 |
139.07 |
140.48 |
142.43 |
143.16 |
149.48 |
151.17 |
| 5 |
142.36 |
142.98 |
161.41 |
159.14 |
163.89 |
165.92 |
173.58 |
177.65 |
| 6 |
148.95 |
149.94 |
171.94 |
169.68 |
172.56 |
174.57 |
184.27 |
190.27 |
| 7 |
157.89 |
157.48 |
182.49 |
180.67 |
183.12 |
184.56 |
193.79 |
197.96 |
| 8 |
180.15 |
178.86 |
203.08 |
200.06 |
200.22 |
200.50 |
205.97 |
211.79 |
| 9 |
192.39 |
191.20 |
204.37 |
202.54 |
200.05 |
200.75 |
207.44 |
216.57 |



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Area and Energy
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Effective Area and
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Line Flux Density
Please address comments and questions to Dr. John Nousek ( nousek@astro.psu.edu
)