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The Behaviour of the XMM-Newton Background: From the beginning of the mission until May 2015 XMM-SOC-GEN-TN-0014 issue 3.8
R. Gonz´lez-Riestra and P.M. Rodr´ uez-Pascual a ig XMM-SOC User Support Group June 29, 2015

1

Intro duction

This do cument sup ersedes XMM-SOC-USR-TN-0014, issue 3.7 The sample includes now data obtained until 1st May 2015, while the previous version covered until May 2014. The aim of this document is to study the seasonal and long-term behaviour of the XMM-Newton background. For this purpose we have examined the background in RGS1 and EPIC-pn science observations taken from the beginning of the mission until May 2015. The first version of this document, issued in January 2007, fulfilled the recommendation made by the XMM-Newton Users Group "to reassess the EPIC background loading for a 1 year sample in order to investigate a seasonal dependence" (rec. 2006-05-19/34). The contributors to the EPIC and RGS background are detailed in the XMM Users Handbook and in the XMM-Newton Background Analysis page. This is a short summary of the most relevant features: The EPIC background has two components: a cosmic X-ray background, and an instrumental background. The latter can be further divided into a detector noise component (dominant below 200 eV) and a second component due to the interaction of particles with the structure surrounding the detectors and the detectors themselves. This component is particularly important above a few keV. The particle induced background has in turn two components: a stable internal component, due to the interaction of high-energy particles (energies above some 100 MeV) with the structure surrounding the detectors and possibly the detectors themselves, and an external "flaring" component, characterised by strong and rapid variability. This flaring component is attributed to soft protons (with energies below a few 100 keV), which are presumably funnelled towards the detectors by the X-ray mirrors. The RGS background has also several components, the dominant one being soft protons entering through the mirrors. The current understanding is that soft protons are most likely organised in clouds populating the Earth's magnetosphere. The number of such clouds encountered by XMM-Newton in its orbit depends upon many factors, such as the altitude of the satellite, its position with respect to the magnetosphere, and the amount of solar activity.

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Figure 1: Evolution of the background in RGS1 (left) and EPIC-pn (right) since the beginning of the mission until May 2015. The selection criteria in Mode/Filter makes EPIC-pn data to be more scarce than RGS. In addition, EPIC-pn science exposures are generally stopped earlier than RGS exposures when approaching perigee passage. 2


2

Data Sample and Metho dology
· RGS1 (9076 exposures) ­ RGS1 data since the beginning of the operational phase until 1st May 2015 ­ Spectroscopy mode ­ Background indicator: countrate in CCD9 off axis region (> 1 arcmin away from the on-axis position) (CCDNR==9 && (XDSP CORR < -0.0003 || XDSP CORR > 0.0003)) · EPIC-pn (6191 exposures) ­ EPIC-pn data since the beginning of the operational phase until 1st May 2015 ­ Full Frame or Extended Full Frame mode with THIN or MEDIUM filter. ­ Background indicators: high energy events (FLAG==0) && (PI>10000) && (PATTERN==0)

In this study we have used the following datasets:

3

Mission Planning constraints and Op erational Pro cedures

The Radiation Monitor (RM) on-board XMM-Newton is mainly used to detect the entry/exit to/from the Earth radiation belts. Whenever the RM flux is higher than a given threshold (Radiation Monitor Warning Flag Active) the MOS cameras are kept closed or commanded to SAFE-STANDBY mode, EPIC-pn is commanded to IDLE mode with the CLOSED filter, and RGS is commanded to SETUP mode. The RM Warning Flag can also be set to "active" during solar flares, leading to the interruption of science observations. Even before the limit for the RM Warning Flag goes to "active", high radiation (due either to proximity to perigee or to low-energy protons flares) can be identified with the information provided by the X-ray science instruments, basically the countrate in the MOS peripheral CCDs, in RGS CCD9 and the EPIC-pn Discarded Lines. In general, RGS is stopped at higher radiation levels than EPIC. For this reason RGS data have a more complete coverage of the end of the revolution. In April 2005, science observations started to be scheduled only in the part of the orbit predicted as "low-radiation" by the model by Casale and Fauste (2004). Currently, EPIC observations with the CALCLOSED filter are scheduled at the beginning of the revolution in the epoch of the year in which there are more than 3 ks between the start of the Science Window and the predicted end of the high radiation period (November-March). The last science observation in the revolution is scheduled to last until the end of the Science Window and it is stopped when the radiation reaches the critical level. EPIC exposures with the CALCLOSED filter are then performed, if there is enough time available

4

Overall Trend

Fig. 1 shows the evolution of the background in RGS1 (left) and EPIC-pn (right). EPIC-pn data are more scarce due to the selection of mode and filter. Also, RGS is usually on for a longer time at the end of the revolution. As shown below, within the intrinsic scatter in the data, there are not significant differences in the behaviour of the background in both instruments. In what follows, we have divided the revolution in six parts, from phase 0.125 to 0.875, of 6 hours each. We refer to the first two parts as the beginning of the revolution, to the next two as the apogee, and to the remaining two as the end of the revolution. 3


4 Figure 2: Evolution of the XMM-Newton background along the years in different parts of the revolution (left: since the beginning of the mission until 2009; right: since 2009 until May 2015). Data have been averaged in two months bins. RGS1 is shown in black and EPIC-pn in red. Units are RGS1 cts/s. EPIC-pn countrates have been arbitrarily scaled and slightly shifted in time for clarity. Note the different scales in each panel.


Figure 3: RGS1 background at apogee. As shown in the top panel, flares were larger and more frequent during the first years of the mission. The lower panel presents the same data with a different scale, to better show that the minimum background was lower during the period of high solar activity, increased during the solar minimum, and decreased again since 2009 until 2014.

5

Secular Variations

The evolution of the background along the mission is shown in Figs. 2 to 4. First thing to note is the agreement in the behaviour of the background in both instruments, which justifies that we base our results mainly in the RGS1 data, due to the poorer coverage of the EPIC-pn data. The overall level of background has decreased slightly since the start of the mission. Also, the strong annual periodicity observed in the first years is much less pronounced now. The strength of the maxima increased steadily from 2000 to 2003-2005 and started to decline afterwards, nearly disappearing in 2009. The RGS1 background at apogee is shown in Fig. 3. In periods of high solar activity, until approximately 2006, the number of flares was larger and the minimum background was at a level of 0.03 cts/s. The minimum background started to increase in 2006, reaching a maximum in 2009, at a level of 0.06 cts/s, and decreasing afterwards, with the start of the current solar cycle.

6

Seasonal and Orbital Variations

Figs. 5 and 6 show the behaviour of the background along the year. As shown in Casale and Fauste (2004), the observed seasonal dependence can be explained by the asymmetry of the Earth magnetic field along the sunward-antisun line. 5


Countrate at apogee Year 2000 2001 2002 2003 2004 2005 2006 2007 2008 2009 2010 2011 2012 2013 2014 Rate 0.17 0.13 0.11 0.13 0.09 0.10 0.09 0.09 0.10 0.09 0.09 0.09 0.07 0.06 0.08 ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± std 0.09 0.06 0.05 0.06 0.03 0.04 0.03 0.03 0.04 0.03 0.03 0.03 0.02 0.02 0.03

Figure 4: Similar to the left panel of Fig. 2, but showing the background in different parts of the revolution with the same scale. Data have been averaged in three months bins for clarity. The table on the right lists the average yearly countrate and its standard deviation near apogee, between phases 0.45 and 0.55. We have plotted in Fig. 5 separately two periods of time: before and after 2009, as we have found that in the last years the background, in addition of being slightly lower, shows a different, less marked, seasonal variation. a) The b eginning of the revolution Seasonal variations at the beginning of the revolution were more marked in the first years of the mission. In the last years the radiation is slightly lower from June to September. The level of the background in the first hours of the revolution vary by not more than a factor two along the year. The amplitude of this variation becomes smaller when approaching to apogee. b) The ap ogee Since 2009, the intensity of the background close to apogee has not shown significant seasonal changes, only being slightly higher from January to June. c) The end of the revolution The highest background levels and the largest seasonal variations are observed in the second half of the revolution. There is a maximum around March-April, when the background is on average four times higher than in November-December.

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7 Figure 5: Behaviour of the monthly background in different parts of the revolution (left: until end 2008; right: since 2009). RGS1 is shown in black and EPIC-pn in red. Units are RGS1 cts/s. EPIC-pn countrates have been arbitrarily scaled. Note the different scales in each panel.


Figure 6: Similar to Fig. 5, but showing the monthly background in different parts of the revolution with the same scale (left: until end 2008, right: since 2009, note the different scales).

7

Conclusions
monthly mission, (i.e. the indicate ehaviour

The results of this study are summarised in Table 1 and Figures 7 and 8. The table lists the average RGS1 background countrate in the different parts of the revolution for the whole and before and after 2009. Also listed are the standard deviations of each monthly average standard deviation of the monthly averages of the different years). Large standard deviations large year-to-year variations in the given month. The conclusions listed below refer to the b of the background in the last five years.

· The most remarkable characteristic is the change in the intensity of the background along the orbit. The distance to the Earth is the dominant factor (the background is lower close to apogee, as expected), but the asymmetry of the changes in the background when moving away from perigee and when approaching to it, indicates that other effects may play an important role. · The background is lower at the beginning of the revolution than at the end. The high background time does not extend beyond orbital phase 0.15 (i.e. eight hours after perigee). Around March the background starts to rise 10 hours after apogee, while it does it later during the rest of the year. · Seasonal variations are now much less background near apogee does not vary by factors up to three-four are observed conditions, the background at the end observed at apogee. pronounced than in the first years of the mission. The by more than a factor 1.5 along the year, but variations at the end of the revolution. Even in the most favourable of the revolution is much higher than the highest value

· Periods of high solar activity are characterised by frequent flares, but also by a lower background at apogee.

References
XMM-Newton Users Handbook Attempt of Modelling the XMM-Newton Radiation Environment, XMM-OPS-TN-004, Casale, M. and Fauste, J., 2004. 8


Table 1: Average monthly RGS1 Background Countrate Phase in Revolution [Hours after perigee] 0.250-0.375 0.375-0.625 0.625-0.750 [12-18] [18-30] [30-36] 2000 - 2015 0.08 (0.01) 0.07 (0.02) 0.08 (0.04) 0.16 (0.23) 0.10 (0.14) 0.17 (0.14) 0.16 (0.14) 0.13 (0.09) 0.34 (0.24) 0.13 (0.04) 0.12 (0.04) 0.33 (0.22) 0.14 (0.04) 0.12 (0.03) 0.18 (0.08) 0.14 (0.08) 0.10 (0.03) 0.12 (0.04) 0.13 (0.07) 0.11 (0.04) 0.13 (0.05) 0.11 (0.05) 0.10 (0.04) 0.12 (0.07) 0.14 (0.09) 0.11 (0.05) 0.14 (0.07) 0.11 (0.05) 0.11 (0.06) 0.13 (0.06) 0.07 (0.02) 0.08 (0.04) 0.10 (0.05) 0.06 (0.02) 0.06 (0.01) 0.07 (0.02) 2000 - 2008 0.08 (0.01) 0.06 (0.01) 0.09 (0.05) 0.20 (0.28) 0.12 (0.18) 0.22 (0.16) 0.20 (0.17) 0.15 (0.10) 0.49 (0.20) 0.16 (0.04) 0.13 (0.04) 0.47 (0.14) 0.15 (0.04) 0.12 (0.03) 0.21 (0.08) 0.17 (0.08) 0.11 (0.04) 0.14 (0.04) 0.16 (0.05) 0.13 (0.04) 0.14 (0.05) 0.14 (0.03) 0.12 (0.04) 0.15 (0.07) 0.18 (0.09) 0.13 (0.05) 0.16 (0.07) 0.12 (0.05) 0.13 (0.06) 0.16 (0.04) 0.08 (0.02) 0.09 (0.04) 0.12 (0.04) 0.06 (0.01) 0.06 (0.01) 0.07 (0.02) 2009 - 2015 0.09 (0.02) 0.08 (0.02) 0.08 (0.02) 0.09 (0.02) 0.09 (0.01) 0.10 (0.03) 0.10 (0.03) 0.11 (0.04) 0.12 (0.04) 0.09 (0.03) 0.09 (0.01) 0.09 (0.02) 0.12 (0.05) 0.11 (0.04) 0.10 (0.03) 0.07 (0.02) 0.08 (0.02) 0.09 (0.02) 0.06 (0.01) 0.07 (0.02) 0.09 (0.05) 0.06 (0.01) 0.06 (0.02) 0.07 (0.02) 0.07 (0.02) 0.07 (0.02) 0.11 (0.07) 0.10 (0.06) 0.07 (0.02) 0.06 (0.02) 0.07 (0.02) 0.07 (0.01) 0.06 (0.01) 0.08 (0.03) 0.09 (0.06) 0.07 (0.05)

Month January February March April May June July August September October November December January February March April May June July August September October November December January February March April May June July August September October November December


0.125-0.250 [6-12] 0.17 0.32 0.36 0.34 0.31 0.30 0.25 0.23 0.13 0.11 0.12 0.11 0.20 0.45 0.53 0.51 0.40 0.51 0.34 0.32 0.15 0.09 0.09 0.11 0.11 0.12 0.13 0.14 0.15 0.09 0.07 0.08 0.10 0.13 0.16 0.12 (0.06) (0.30) (0.29) (0.23) (0.20) (0.22) (0.21) (0.20) (0.12) (0.05) (0.05) (0.05) (0.06) (0.32) (0.28) (0.18) (0.18) (0.16) (0.21) (0.20) (0.15) (0.04) (0.02) (0.06) (0.02) (0.03) (0.04) (0.06) (0.07) (0.03) (0.02) (0.04) (0.02) (0.05) (0.05) (0.04)

0.750-0.875 [36-42] 0.58 0.81 1.11 1.43 1.22 0.76 0.55 0.40 0.39 0.50 0.63 0.51 0.79 1.04 1.47 1.98 1.56 0.90 0.64 0.44 0.44 0.65 0.93 0.72 0.25 0.48 0.64 0.69 0.52 0.43 0.34 0.28 0.28 0.22 0.14 0.13 (0.49) (0.60) (0.73) (0.81) (0.66) (0.33) (0.23) (0.17) (0.15) (0.31) (0.59) (0.46) (0.51) (0.64) (0.78) (0.63) (0.60) (0.32) (0.23) (0.17) (0.14) (0.24) (0.55) (0.45) (0.23) (0.32) (0.39) (0.38) (0.17) (0.17) (0.18) (0.17) (0.16) (0.21) (0.12) (0.07)

Numbers in parenthesis are the standard deviations of the monthly averages.

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Figure 7: Top: Three-dimensional representation of the RGS1 background by date and by phase in the revolution; Bottom: Pro jection of the above surface in the Year/Phase plane.

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11 Figure 8: Behaviour of the RGS1 background by month (left: from the beginning of the mission until end 2008; right: from January 2009 until May 2015). In both figures the top panel is a representation of the RGS1 background by month and by phase in the revolution, and the bottom panel is the pro jection of the above surface in the Month/Phase plane, showing the contours corresponding to 0.1, 0.2 and 1 cts/s, defining the regions of low (dark blue), medium (light blue-green) and high (yellow-red) background.