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Radio Frequency Interference Mitigation and Statistics in the Spectral Observations of FAST

2022-05-23 08:45:18ChuanPengZhangJinLongXuJieWangYingjieJingZimingLiuMingZhuandPengJiang

Chuan-Peng Zhang ,Jin-Long Xu,Jie Wang,Yingjie Jing,Ziming Liu,3,Ming Zhu,and Peng Jiang

1 National Astronomical Observatories,Chinese Academy of Sciences,Beijing 100101,China;cpzhang@nao.cas.cn

2 CAS Key Laboratory of FAST,NAOC,Chinese Academy of Sciences,Beijing 100101,China

3 College of Astronomy and Space Sciences,University of Chinese Academy of Sciences,Beijing 100049,China

Received 2021 September 22;revised 2021 November 10;accepted 2021 December 1;published 2022 February 2

Abstract In radio astronomy,radio frequency interference(RFI)becomes more and more serious for radio observational facilities.The RFI always in fluences the search and study of the interesting astronomical objects.Mitigating the RFI becomes an essential procedure in any survey data processing.The Five-hundred-meter Aperture Spherical radio Telescope(FAST)is an extremely sensitive radio telescope.It is necessary to find out an effective and precise RFI mitigation method for FAST data processing.In this work,we introduce a method to mitigate the RFI in FAST spectral observation and make a statistic for the RFI using~300 h FAST data.The details are as follows.First,according to the characteristics of FAST spectra,we propose to use the Asymmetrically Reweighted Penalized Least Squares algorithm for baseline fitting.Our test results show that it has a good performance.Second,we flag the RFI with four strategies,which are to flag extremely strong RFI,flag long-lasting RFI,flag polarized RFI,and flag beam-combined RFI,respectively.The test results show that all the RFI above a preset threshold could be flagged.Third,we make a statistic for the probabilities of polarized XX and YY RFI in FAST observations.The statistical results could tell us which frequencies are relatively quiescent.With such statistical data,we are able to avoid using such frequencies in our spectral observations.Finally,based on the~300 h FAST data,we obtained an RFI table,which is the most complete database currently for FAST.

Key words:telescopes–methods:statistical–site testing

1.Introduction

In radio astronomy,radio frequency interference(RFI)becomes more and more serious for radio observational facilities(Kesteven 2005;An et al.2017;Zeng et al.2021).The days of interference-free observations in radio astronomy are long gone.Substantial pressures are coming from commercial,defense,and other interests for greater access to the radio-frequency spectrum.This means that radio astronomers can no longer rely on the regulatory authorities for an environment free from interference,and must look seriously at mitigation strategies(Fridman&Baan 2001;Boonstra 2005;Baan 2011).

Mitigating the RFI becomes an essential procedure in pulsar survey and other spectral data processing.RFI can occur in impulse type bursts persistently,variable in time or in a transient manner.The RFI properties in the integrated postcorrelated data can be studied in terms of their morphology,consisting of broad band,narrow band roughly horizontal and vertical envelopes,mainly caused by the earlier described terrestrial sources,and unknown blob RFI(An et al.2017;Zeng et al.2021).The RFI amplitudes are typically much higher than the underlying astronomical signal and random noise,but some weak RFI signals are almost identical to the intensity of real celestial signals,such as pulsars and molecular spectra(An et al.2017;Zhang et al.2020).This will easily lead to misidenti fication and seriously in fluence the searching and analysis of the interesting astronomical objects.An important distinguishing feature for the separation of terrestrial sources of RFI from the astronomical signal relates to the amount of dispersion in the“time-frequency”domain of the received data(An et al.2017).

FAST is located at a site position of the protected radio-quiet zone in Guizhou of China.However,some strong RFIs from for example,broadcast radio and TV,communication satellites and navigation satellites are extremely hard to be shielded.In addition,FAST is very susceptible to RFI from the electronic instruments integrated with the telescope and active radio services around the FAST site,due to its high sensitivity(Zhang et al.2020).Therefore,we must look for other strategies to mitigate the RFI in FAST observations.

The aim of this work is to flag and mitigate the RFI from the FAST observations,and then give a probability and statistics for the FAST RFI showing up.Section 2 introduces the features of astronomical emission lines and terrestrial RFI in FAST observations.Section 3 presents our proposed scheme for RFI mitigation in FAST spectral observations.Section 4 shows the RFI statistical results using our proposed strategies.Section 5 gives a summary.

2.Astronomical Emission Lines and Terrestrial RFI in FAST

2.1.The Characteristics of the Spectral Data

FAST has a 19-beam receiver for simultaneously covering multiple observational areas,thus it is a good tool to carry out drift scan observations for searching for extra-galactic point sources.The data are recorded in the spectral-line backend using a dual linear polarization(XX and YY)mode with a relatively high time-resolution.The full wideband(500 MHz)in the spectral-line backend has a frequency coverage from 1000 to 1500 MHz(see Figure 1).The high and low frequency resolution modes have a number of 1 M and 64 k channels,respectively.The frequency resolution for the high and low resolution modes is 476.84 Hz and 7630 Hz,respectively.The sampling time is 1 s for each spectral line in this work.Generally,2048 s observation spectra for the 64 k channels are packaged into a data cube that has a size of around 2.1 GB.The aperture of the FAST is 500 m and the effective aperture is about 300 m corresponding to an HPBW of 2 9 at 1.4 GHz(Nan et al.2011;Jiang et al.2019,2020;Qian et al.2020;Han et al.2021).

Figure 1.Two full widebands of FAST spectra(polarizations:XX and YY;integration time:1 s)covering a frequency range from 1000 to 1500 MHz.All the visible emission lines except H I at~1420.5 MHz are RFI from terrestrial sources.

In Figure 1,we present a FAST 500 MHz-bandwidth spectrum with 1 s integration time.Each spectrum in the mode of low frequency resolution has 65,536(64 k)channels in total.This leads to that the computing resources are time-consuming in reducing the FAST spectral data.We could first choose one out of every 100 channels,and then fit the baseline only for the selected channels.Finally,we could use interpolation technique to promote and estimate the baseline for the whole 65,536 channels.

2.2.The General RFI Distribution

Figure 1 shows a full wideband of FAST spectrum covering a frequency range from 1000 to 1500 MHz.All the visible emission lines except H I at~1420.5 MHz in Figure 1 are RFI that comes from terrestrial sources.The RFI,including broadcast radio and TV,cell phones,communication satellites,navigation satellites,as well as all the wireless control and monitoring systems(Zhang et al.2020;Wang et al.2021),have the potential to affect radio-astronomical observations.The RFI pollution makes the background against what radio astronomers concern be noisy(Boonstra 2005).

Figure 2.Upper two panels:two FAST spectra(polarization:XX and YY;integration time:1 s)after removing the long-lasting(>128 s)RFI above a threshold of 3σ(σ≈108 mK).Lower two panels:two 2048 s waterfall images after removing the long-lasting RFI.

3.The Proposed Scheme for RFI Mitigation

A number of RFI mitigation methods(e.g.,Fridman&Baan 2001;Ford&Buch 2014;Baek et al.2015;Hu et al.2021;Wang et al.2021;Zhang et al.2021b)could be used at different stages in the data acquisition process.After collecting astronomical data,however,the only thing that astronomers can do for RFI mitigation is to flag and eliminate the effects of known and unknown sources of RFI.In the FAST astronomical spectral data,flagging RFI is seriously affected by the baseline distribution,due to the fact that the baseline is not flat enough.Therefore,we have to first choose an ef ficient method,which is the ArPLS-based method(Baek et al.2015),to remove the baseline,and then we could flag different types of RFI by experimentally setting a credible threshold for each spectrum.

3.1.The Ar PLS for Baseline Correction

For FAST spectrum data,we propose a baseline fitting method based on an Asymmetrically Reweighted Penalized Least Squares algorithm(ArPLS;Baek et al.2015).The baseline correction methods based on penalized least squares have been successfully applied to various spectral analysis(e.g.,Zeng et al.2021;Zhang et al.2021a).The methods could change a parameter“weight”iteratively to estimate a baseline.If a signal is below a previously fitted baseline,a large weight is given.On the other hand,no weight or a small weight is given when a signal is above a fitted baseline as it could be assumed to be a part of spectral peak.A preset coef ficientλ will control the balance between fitness and smoothness(see FAST spectrum with baseline correction in Figure 1).To decrease computing resources,we choose the fitted spectral channels with one out of every 100 channels.In this case,we experimentally setλto be 100,a constant,which could obtain satisfactory results for all of the available FAST data.This method could estimate the noise level iteratively and adjust the weights correspondingly(Baek et al.2015).

Figure 3.Upper two panels:two FAST spectra(polarization:XX and YY;integration time:1 s)after removing the polarized RFI above a threshold of 3σ(σ≈108 mK).Lower two panels:two 2048 s waterfall images after removing the polarized RFI.

The penalized constraint in this method makes the baseline fitting more robust and accurate than traditional methods by mitigating the negative in fluences from instrumental response(Baek et al.2015).After removing the estimated baseline using the ArPLS(see Figure 1),several novel strategies were proposed for flagging different types of RFI(see Section 3.2).

Figure 4.Upper two panels:two FAST spectra(polarization:XX and YY;integration time:1 s)after removing the beam-combined RFI above a threshold of 3σ(σ≈108 mK).Lower two panels:two 2048 s waterfall images after removing the beam-combined RFI.

3.2.Flag Different Types of RFI

The RFI-flagging method mentioned above mainly targets at the FAST drift scan observations for searching for extragalactic point sources.In this work,the used test data are from a blind drift scan survey.4https://fastwww.china-vo.org/cms/article/122/This project is blindly mapping the sky using the idle time of the FAST observation.The project numbers are N2020_3 and N2021_4,respectively.The observation dates for our used data5At the end of 2021 July,a strong standing wave(>1.0 K)with a period of~8 MHz has been removed from hardware.are from 2021 July 29 to September 11.The observation time is around~300 h for our used test data in total.Based on the characteristics of the RFI in FAST after baseline correction,we adopt several strategies to flag them as follows.

3.2.1.Flag Extremely Strong RFI

In FAST observations,there indeed exist many extremely strong and evident RFI,for example those from communication satellites and navigation satellites(Wang et al.2021)at around 1175,1207,1270,and 1480 MHz(see the emission line in Figure 1).These strong RFI have a serious effect on the FAST data reduction.These RFIs could be easily removed by setting a reasonable threshold in the baseline fitted spectrum.For example,we could remove the spectral channels above power=2×1011(see the lower panel of Figure 1).However,if we could not make sure whether they are RFIs,we could skip this strategy.

3.2.2.Flag Long-lasting RFI

In the FAST drift scan survey,generally these long-lasting(e.g.,>128 s in this work)emissions should be RFIs except the H I line at around 1420.5 MHz.The reason is that almost all the distant extragalactic galaxies are close to point sources relatively to the beam size of FAST,leading to that the signals cannot be lasting for long time.6In a tracking mode or toward the relatively extended sources,this strategy is not applicable.Therefore,we could first average some spectra(e.g.,averaging the neighborhood 8 s spectra for polarized XX and YY data,respectively,in this test work)that are close in time sequence(aim to improve signalto-noise ratio),and then set a reasonable threshold to remove this kind of RFI(see Figure 2).Those still existing strong emissions(power>0.5×1011;see Figure 3)cannot be lasting longer than 128 s,thus they are not flagged as such kind of RFI,for example the blob RFIs at 1255,1280,and 1380 MHz.These blob RFIs could be found using the strategy of flagging beam-combined RFIs(see Section 3.2.4).

Figure 5.Upper two panels:two FAST spectra(polarization:XX and YY;integration time:1 s)after removing all the flagged RFI.Lower two panels:two 2048 s waterfall images after removing all the flagged RFI.

3.2.3.Flag Polarized RFI

For FAST observation,a dual polarization receiver is equipped in the frontend,thus we could get two different polarized(XX and YY)emissions simultaneously(Jiang et al.2019,2020).A key fact is that the signals from the extragalactic galaxies are almost non-polarized,but most of the terrestrial RFIs are polarized.Therefore,we could first average some spectra(e.g.,averaging the neighborhood 8 s spectra for polarized XX and YY data,respectively,in this test work)that are close in time sequence(aim to improve signalto-noise ratio).With their discrepancy,we then set a reasonable threshold to flag those polarized RFIs from the terrestrial(see Figure 3).Those still existing strong emissions(power>0.5×1011;see Figure 3)after this strategy are non-polarized RFIs.

Figure 6.Probabilities of RFI(XX,YY)showing up in FAST spectral observations.The corresponding data are listed in Table 1.The used statistical data have a span of 45 days,which amount to around~300 hr of observation time in total.Currently we only flagged the RFI above a threshold of~324 mK.The emission at~1420.5 MHz is H I line from the Milky Way as background.

3.2.4.Flag Beam-combined RFI

The FAST has a powerful 19-beam receiver,which could simultaneously cover 19 different beam size areas(Jiang et al.2019,2020).In FAST drift scan survey,almost all the distant extragalactic galaxies are close to point sources relatively to the beam size of FAST.This leads to that the true extragalactic signals could not simultaneously go into any two of the 19-beam receiver in a high probability.However,the observed terrestrial RFI by all the 19 receivers should get the same emission,except the occasionally and extremely straight RFI in direction.Therefore,we assume that the received RFI have no discrepancy in different beam receivers.We could first average some spectra(e.g.,averaging the neighborhood 8 s spectra for polarized XX and YY data,respectively,in this test work)that are close in time sequence(aim to improve signal-to-noise ratio).Based on this advantage,we could then set a reasonable threshold to flag the beam-combined RFI(see Figure 4).After flagging the beam-combined RFI,there exist several strong RFIs,indicating this strategy is effective.In particular,most of the blob RFIs at 1255,1280,and 1380 MHz have been well flagged out using this strategy.Those still existing strong RFIs in Figure 4 could be occasional RFIs coming into the receivers.

3.2.5.Remove all the Flagged RFI

The upper panel of Figure 5 shows a FAST spectrum after removing all the flagged RFI.We can see that those obvious RFIs,compared with the spectrum in Figure 1,have been removed from the whole wideband.The 2048 s waterfall image in the lower panel of Figure 5 shows that the spectral data become very flat already.However,there still exist several RFIs un flagged,for example at 1170,1210,1260,and 1480 MHz.Currently in this work,we only flagged the RFI above 3σ≈324 mK.The existing RFI could be further flagged by lowering down the flagging threshold.This also means that the threshold is sensitive to the number of the found RFI.Thus,the flagging threshold could be determined by the expected sensitivity or other requirements for each observation.

4.RFI Statistics

Based on the RFI flagging process,we find that there are indeed many RFIs in the FAST spectral observation(Jiang et al.2020;Hu et al.2021;Wang et al.2021;Zhang et al.2021b).We also find that some RFIs are random and occasional,others are fixed at some frequencies.7See also the test results from RFI monitoring in website:https://fastwww.china-vo.org/cms/category/r f i_monitoring_en/.Because we already have a method which is able to flag the RFI above an expected threshold,it deserves to make a statistics for the probabilities of the RFI showing up in FAST spectral observations.The RFI statistical results have been shown in Figure 6 and Table 1.The used statistical data are the blind drift scan survey with project numbers being N2020_3 and N2021_4.All the data spanned 45 days from 2021 July 29 to September 11.The total observation time reach to~300 h for our used FAST data.Currently we only flagged the RFI above a threshold of 3σ≈324 mK for each spectrum.The~300 h statistical results would tell us which frequencies are relatively quiescent and which are noise.To do it,first we evenly bin the 500 MHz wideband into 5000 channels.8It can be easily binned into more channels if needed.Each channel will have a bandwidth of 0.1 MHz.With our RFI flagging procedure,we could find each RFI in every spectrum from long enough time observations.Then,we could compute theprobability for each RFI showing up in each channel(0.1 MHz bandwidth)and each polarization(XX or YY).

Figure 7.Ratios between the flagged RFI(XX,YY)probabilities derived from 30,100,200,and 300 h.The RFI probabilities derived by 300 h observations are shown in Figure 6 and Table 1.The red lines indicate the values with ratio=1.

Table 1 Probabilities and Intensities for FAST RFI Showing up in Spectral Observations

From Figure 6,we find that the RFI with different polarizations(XX or YY)have obvious discrepancies at some frequencies.This further suggests that the terrestrial RFI are mostly polarized.In addition,the probabilities for the flagged RFI in most wideband are lower than 10%,except the frequency range at 1155–1295 MHz and 1465–1500 MHz,where the RFI pollution is very serious withP>60%.Even some RFI linewidths achieve to 20 MHz.For the convenience of query,the full online table9http://www.doi.org/10.11922/sciencedb.j00001.00313of Table 1 lists the detailed RFI probabilities and antenna temperatures from 1000 to 1500 MHz with a step of 0.1 MHz.With the RFI statistical data,we are able to selectablely use some frequencies in the FAST observations.

Figure 8.Upper two panels:RFI(XX,YY)intensities from averaging the flagged RFI within~300 h spectra.The intensities are listed in Table 1.Lower two panels:RFI(XX,YY)intensities from averaging all~300 h spectra.

Figure 7 shows ratios between the flagged RFI(XX,YY)probabilities derived from 30,100,200,and 300 h.The ratios in different time tell us that:first,with increasing time the probability ratios become more and more stable,exampleratioat most frequencies;second,although~300 h of observation time have been used for the statistics,every different observation may still meet different RFIs possibly,especially for the small probability event(<0.1%).This is because that some RFIs are always occasionally appeared in some frequencies.Thus,the discrepancies will be much different,if the two observations are carried out in different days(or spanning many days).

In Figure 8,the upper two and lower two panels show RFI(XX,YY)intensities from averaging only the flagged RFI within~300 h spectra,and those from averaging all~300 h spectra,respectively.From the intensity discrepancies of RFI in Figure 8,we know that although some RFIs are very bright,their probabilities showing up are very low,for example at around 1060,1370,and 1450 MHz.These frequencies are safe for observations in our opinion.Furthermore,in our strategies we only flag the RFI with intensity above some threshold.This will lead to that some relatively weak RFIs cannot be flagged below the used threshold.Therefore,current flagged RFIs are still uncompleted,but the RFI probabilities showing up in~300 h data could be a good reference for FAST users.

5.Summary and Future Work

In FAST spectral observations,the RFI always in fluences the identi fication of the interesting astronomical objects.Mitigating the RFI becomes an essential procedure in the data reduction.Thus,we provide a method to mitigate the RFI in FAST spectral observation and give a statistical result for the flagged RFI as follows.

First,considering that the FAST spectra have a very wide bandwidth with 500 MHz,but its baseline is not flat enough.According to the characteristics of FAST spectra,we propose to use the ArPLS algorithm to do baseline fitting.The test results show that the ArPLS has a really good performance in the baseline correction of the FAST spectral data reduction.

Second,we flag the RFI in FAST spectra in four strategies,which are flagging extremely strong RFI,flagging long-lasting RFI,flagging polarized RFI,and flagging beam-combined RFI,respectively.The test results(see Figure 5)show that all the RFI above the preset threshold could be removed from the whole wideband ef ficiently.Furthermore,this also means that if lowering down the threshold,more RFI could be found.Thus,the threshold is sensitive to the number of the found RFI.The derived RFI table is the most complete database currently for FAST.

Third,we make a statistic for the probability and intensity of the RFI(including the polarized XX and YY)showing up in FAST spectral observations(see Figure 6 and Table 1).The statistical results could tell us which frequencies are relatively quiescent.With such statistical data,the astronomers could try to avoid using such frequencies in the spectral observations,and our FAST staff will also try to mitigate the RFI.

In future work,first,the standing wave,for example the 1 MHz wide standing wave,also seriously interferes the FAST observations,especially in extragalaxy survey.If this standing wave could be removed,the sensitivity will be improved several times.We are trying to remove it.Second,currently we do not know whether the RFI showing up is regular or not in different azimuth and zenith at different time(day or night).With our introduced strategies and using the huge FAST archival data,we will make a detailed statistical work to answer this question and tell FAST users how to avoid the terrible RFI.Third,we are considering to equip the script into the FAST observing or data reduction system,to real-time monitor RFI,and to provide FAST users for an RFI database for reference.

Acknowledgments

This work is supported by the National Key R&D Program of China(2018YFE0202900).FAST is a Chinese national mega-science facility,operated by the National Astronomical Observatories,Chinese Academy of Sciences(NAOC).C.-P.Z.and Y.J.acknowledge support by the NAOC Nebula Talents Program and the Cultivation Project for FAST Scienti fic Payoff and Research Achievement of CAMS-CAS.We also wish to thank the anonymous referee for comments that improved the clarity of the paper.

ORCID iDs

Chuan-Peng Zhang https://orcid.org/0000-0002-4428-3183

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