THE IMPROVED ARTEMIS–Jean Louis Steinberg (ARTEMIS-IV) MULTICHANNEL SOLAR RADIO SPECTROGRAPH  

OF THE UNIVERSITY OF ATHENS

 

 

Abstract. We present the lately (2002) improved solar radiospectrograph of the University of Athens operating at the Thermopylae Satellite Station since 1996. Observations now cover the whole frequency range from 20 to 650 MHz. The spectrograph has the old 7-meter moving parabolic antenna for 110 to 650MHz and a new stationary antenna for the 20 to 110 MHz. There are two receivers operating in parallel, one sweep frequency for the whole range (10 spectrums/sec, 630 channels/spectrum) and one acousto-optical receiver for the range 270 to 470 MHz (100 spectrums/sec, 128 channels/spectrum). The data acquisition system consists of two PCs (equipped with 12 bit, 225ksamples/sec DAC, one for every receiver) Windows operating system, connected through Ethernet. The daily operation is fully automated: pointing the antenna to the sun, starting and stopping the observations at preset times, data acquisition, and archiving on DVD. We can also control the whole system through modem or Internet. The instrument can be used either by itself to study the onset and evolution of solar radio bursts or in conjunction with other instruments including the Nancy Decametric Array, the WIND/WAVES, and the under construction STEREO/WAVES and LOFAR low frequency receivers to study associated interplanetary phenomena.

Introduction

Radio Spectrography of the solar corona, at decimeter meter and decameter wavelengths, provides basic information on the origin and early evolution of many phenomena which later extend through the interplanetary medium and some of them reach the Earth.

The Artemis IV solar radiospectrograph at Thermopylae is a complete system that receives and records the dynamic spectrum of solar radio bursts on a daily basis  figure1 .figure5. It consists of:

·       Two antennas figure4 (one stationary for the 20-110MHz band figure3 and one  pointing to the sun for the 110-650MHz figure2 ) and their cabin where there are amplifiers, filters, a combiner, the calibration circuit and the antenna movement circuit  figure5  figure6 

·       The control room where there is a rack with two spectrum analyzers one sweep for the whole range 20-650MHz and one acousto-optic for the range 270-450MHz, a GPS for receiving Universal Time, the control of the calibration and the antenna movement circuits  figure7. There are also two PCs equipped with A/D cards, network cards, modem, and DVD Writer figure8

The distance between the antennas with their cabin and the control room is 70m. An underground low loss 50 Ù coaxial line transmits the radio signal from the antenna cabin to the control room and a multi pair line transmits the various control and indication signals between the control room and the cabin figure6.

The output signal from every spectrum analyzer is driven to two PCs where it is digitized, real time mapped on the screen, storaged on the hard disk and at the end of the daily observation the data are transferred to a DVD.figure8

figure9

The two PCs are connected via Ethernet and via the OTE Lan they are connected to the Internet. We can also control the whole operation via the telephone modem.

Later we study the data and conclusions are derived for the solar events at the corona region figure10   figure11

 

The antennas and their cabin

The solar radiospectrograph has a parabolic and a dipole antenna.

A. The parabolic antenna has a diameter of 7m, an angular span 1200, focal length 3m and its reflective surface is made from a metal grid.figure12 On its axis, there two identical log period antennas perpendicular each other’s for the 100-1000MHz region. Each antenna has a length of 2.25m, apex angle 450 and consists of 13 dipoles. figure13 At the present we use only the one log-period and therefore we receive only the projection of the solar radio burst electric field on the antenna dipoles. This combination gives a mean gain of 21db, a mean half power beamwidth of 60 and 50Ù input resistance.figure14 In future we can use the two antennas to increase the sensitivity or to measure polarization characteristics. The antenna has a typical equatorial mounting. It can be rotated around two axes using motors and tracks the sun in declination and hour angle.figure2 After sunset the antenna moves automatically to the east. The antenna was designed in France and constructed by the Greek company PYRKAL.

After collection the signal goes to a 110 MHz high pass filter to reject strong FM radio broadcasting and a pre-amplifier (10db gain and 3db noise figure) which are on the antenna. Follows a compensation amplifier for the long transmission line. It is a three-stage amplifier (30db total gain) with a low pass 650MHz and a high pass 110 MHz filter between them.figure15

Every morning the system is self-calibrated. The antenna is disconnected from the system and a white noise generator (constant T=104 K) is connected. After this the noise level is increased from 102  to 108 K linearly with time. The whole process lasts about 1 min and the signal is storaged. So we know the whole system behavior figure10

In the cabin there is the antenna movement control circuit. Every morning the antenna starts its motion from hour angle –72.50. Its constant angular velocity is 150/houre (equal to the sun angular velocity) and at the end it reaches at 72.50 hour angle. The declination angle that changes 230/3 months is manually controlled by the position control system or remotely through the modem. We observe the antenna position at indicators on the rack and the sun position on the PC screen. The position control as the calibration control is performed through the PC serial port. figure7  figure9

B. The dipole antenna is a very fat inverted V dipole on the east-west plane. Every leg has an overall length 3.5 m and a width of 1m. It is constructed by 15mm diameter copper tube. The two legs form a 900 corner and its apex is 3.6m above ground.figure16 figure3 It has a resonance frequency at about 45 MHz with a very large bandwidth because it is very fat. figure17 The floating over ground input impedance is about 200Ù for frequencies from 20 to 100MHz. The antenna receives vertically polarized signals from low angles over the horizon from east-west and horizontally polarized signals from high angles over the horizon from south-north.figure18 figure34 figure35 figure36 So we can receive the sun signals during all the day and a lot of interfering signals. figure19 figure20 figure21 figure22  figure29  figure30

After collection the signal goes through a floating high pass and a low pass chebyshev ninth order filter (fH=20 MHz and fL=90MHz) to avoid interference from strong short wave and FM broadcasting. Follows an active balun –amplifier  constructed by two hybrid broadband amplifiers (  Motorola CA  2832.) whose output are combined with the primary coil of an rf transformer. The secondary coil drives a coaxial 50 Ù transmission line. The overall amplification is about 30db figure15

Follows a low pass filter (fL=90MHz) in order to protect the other antenna signal from possible harmonics generated by the active balun. A combiner combines the signals from the two antennas and drives them to the control room through the long transmission line .

 

 

The control room

A splitter divides the signal from the transmission line in two ways.figure8

First way. It includes a classical sweep frequency analyzer (Analyseur de Spectre Global or ASG) which covers the whole range from 20 to 650MHz at 10 sweeps/sec with instantaneous bandwidth 1MHz and logarithmic amplification with dynamic range of 70 db. A pulse from a timer on the ADC card triggers every sweep. figure23

The analog output from the ASG drives an ADC card (Kethley 3100) on a PC. A timer on the card generates a pulse every 100msec (frequency 10 Hz) which triggers the ASG to begin a new frequency sweep. In 63msec the ASG sweeps the range from 20 to 650 MHz with instantaneous bandwidth 1MHz and the ADC takes 6300 samples with a resolution of 12bit. figure24 The samples are averaged by ten so we have divide the whole spectrum to 630 channels with resolution bandwidth 1MHz. If in a channel (10 samples) some measurements correspond to the constant frequencies of strong FM radio or TV broadcasting we average by the number of the useful ‘un-infected’ measurements. If in a channel all the measurements are ‘infected’ we replace its intensity by the average of the two adjacent channels. This arrangement leads to a high signal to noise ratio.figure25 Every 5 sweeps the measurements are transferred to the hard disk with a universal time stamp. The 5 spectrums with the time stamp constitute a data block. Simultaneously we see the dynamic spectrum on the PC screen. At the end of the day or later we can take the daily activity and storage it on a DVD. The daily data are about 0.5Gbyte.

Every morning, before taking measurements, this PC receives the Universal Time from a GPS through one serial port to correct its clock. Also this PC controls the starting of the parabolic antenna movement (when the hour angle of the sun is –72.50) and the self-calibration procedure through the other serial port.

This PC is equipped with a telephone line modem so whenever we can watch, receive the daily activity, and if it is necessary we can control manually the system. Also there is an ethernet connection with the other PC

 

Second way: It includes a pass band filter 270-450 MHz, RF amplifier, and finally an acousto-optic frequency analyzer (Spectrograph Acousto-Optic, SAO) for the above frequency range with low dynamic linear range (20db), very good frequency resolution at 176kHz and very fast frame rate at 100Hz. The SAO output drives an ADC card at the second PC. figure8

The SAO output comes from the discharge of a linear CCD with 1024 pixel so that every pixel corresponds to a different frequency. A correct sampling demands synchronization between the SAO and the ADC card. For this reason the SAO pulses that trigger the pixel output (1024 pulses in 10msec) drive and the ADC sampling.figure26 Also these pulses drive a frequency divider (on the ADC card) which gives a pulse every 10msec. Every one of these pulses triggers a new frame of the SAO.

Finally every 10msec the SAO sweep the range from 270 to 450 MHz with instantaneous bandwidth 176kHz and the ADC takes 1024 samples with a resolution of 12bit. The samples are averaged by eight, so we have divide the whole spectrum to 128 channels with resolution bandwidth 1.4MHz.figure27 This arrangement leads to a high signal to noise ratio. Every 50 sweeps the measurements are transferred to the hard disk with a universal time stamp. The 50 spectrums with the time stamp constitute a data block. Simultaneously we see the dynamic spectrum on the PC screen.figure28 At the end of the day or later we can take the daily activity and storage it on a DVD. The daily data are about 1Gbyte. The Universal Time is received every morning from the other PC through the Ethernet.

 

Conclusions and perspectives

This instrument has a very high time and frequency resolution from decimeter to decameter wavelengths with a very good signal to noise ratio, so we can distinguish fine structure at solar radiobursts.figure31 figure32 figure33Future perspectives are the use of the old and construction of new antenna to make polarimetric measurements and extension of the SAO frequency range.

 

References

1.  C.Caroubalos, D. Maroulis, N. Patavalis, J.-l. Bougeret, G. Doumas, C. Perche, C. Alissandrakis, A. Hillaris, X. Moussas, P. Preka-Papadema, A. Kontogeorgos, P. Tsitsipis, G. Kanelakis: 2001 ”The new multichannel radiospectrograph ARTEMIS-IV/HECATE of the University of Athens”   Experimental Astronomy 11, 23-32

2.  William C. Erickson Professor at Utas University of Australia.private communication.

3.  http://www.lofar.org

4.  Kethley   KPCI   3100 ADC   manual.


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