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6. Performances

6.1. Hypothesis

The purpose of this section is to evaluate the performance of the proposed detector. The number of samples, N, and the size Q of the vector tex2html_wrap_inline1415 have been fixed respectively at 10000 and 30. Under the tex2html_wrap_inline1427 hypothesis, the noise is Gaussian and its spectral shape is given in Fig. 4 (click here). All the numerical processing, including the quantized autocorrelation, has been simulated numerically. The quantization parameters are those given in Table 1 (click here). The tests were made, first on synthetic data and, then, on actual data acquired by the Nançay Decimetric Radio Telescope (NRT).

  figure524
Figure 4: Spectrum of the noise under the tex2html_wrap_inline1427 hypothesis. This typical shape has been measured from the NRT receiver

  figure530
Figure 5: Spectra of the spread spectrum RFI. They are extracted from spectra similar to those generated by Global Positioning System (GPS) or Global Navigation Satellite System (GLONASS): a) spectrum of a spread spectrum signal, b) spectrum of the tested narrow band filtered spread spectrum RFI (NSP), c) spectrum of the tested large band filtered spread spectrum RFI (LSP)

  figure537
Figure 6: tex2html_wrap_inline1734 against tex2html_wrap_inline1736 for the three types of RFI retained: a sine wave (SW), a narrow band filtered spread spectrum RFI (NSP), a large band filtered spread spectrum RFI (LSP). N = 10000 samples are used for each one of the 800 trials. Q is the size of the test vector tex2html_wrap_inline1415

  figure544
Figure 7: Experimental spectra resulting from the NRT receiver. They are measured over 10 s on a 100 kHz band without (thin lines) and with time-blanking (thick lines) processing. Detection time = 50 ms (equivalent to N=10000 samples), tex2html_wrap_inline1748, Q=30, tex2html_wrap_inline1752: a) 12 sine waves RFI (SW), b) 2 large band spread spectrum RFI (LSP)

6.2. Tests with synthetic data

Three typical RFI were chosen for the tests : a sine wave (SW), and two filtered spread spectrum signals with two kinds of band limitation (see Fig. 5 (click here)). The performance analysis is based on hypothesis testing. Two cases are possible, whether the RFI is present (tex2html_wrap_inline1762 hypothesis) or not (tex2html_wrap_inline1427 hypothesis). In order to obtain the needed probabilities of detection tex2html_wrap_inline1736 and probabilities of false alarm tex2html_wrap_inline1734, it is necessary to generate many sample paths of the involved data. For the results presented here, 800 sample paths for each hypothesis were generated. Figure 6 (click here) shows the plots of tex2html_wrap_inline1734 against tex2html_wrap_inline1736 (ROC curvesgif) for the three types of RFI retained. The aim was to find the smallest INR (tex2html_wrap_inline1776) which yields at least a tex2html_wrap_inline1736 superior to tex2html_wrap_inline1780 with a tex2html_wrap_inline1734 inferior to tex2html_wrap_inline1784.

This objective is outperformed in the sine wave case, since an INR of tex2html_wrap_inline1786 is reached. For the spread spectrum cases, the performance decreases. The large band spread spectrum (LSP) case is still detected well with a level of tex2html_wrap_inline1788 but the narrow band spread spectrum (NSP) case does not reach the limit of tex2html_wrap_inline1790. These performance differences are related to the spectral appearance of the RFI when they are observed through a resolution of 1/Q (see Sect. 5.2 (click here)). With Q=30, the NSP case appears spectrally as a white noise, thereby diminishing the detection capabilities. By increasing the resolution, the detection is improved (see Fig. 6 (click here) with Q=70).

6.3. Tests with real data

To validate the results obtained with simulated data and verify the likelihood of the tex2html_wrap_inline1427 hypothesis, the noise delivered by the receiver was sampled at a rate of 200 kHz during 10 s. A dedicated RFI generator (see images available on the electronic version of the paper) was used to emit the retained three types of RFI.

Firstly, the measured ROC curves were similar to those obtained with synthetic data. This comparison has validated the hypothesis made on the noise under the tex2html_wrap_inline1427 hypothesis. Secondly, a practical test was made. The RFI generator was turned on and off manually at random times and for random durations. The power of RFI was adjusted to deliver an INR of tex2html_wrap_inline1790. The same algorithm (defined in Sect. 5 (click here)) was applied to the stored data, the detection threshold being chosen to guarantee a tex2html_wrap_inline1734 of tex2html_wrap_inline1784. The detection window was fixed at 50 ms (N=10000 samples). When an RFI was detected, the corresponding data were discarded from the final integration. The resulting spectra are shown in Fig. 7 (click here). In both cases, the final spectrum shows significant improvement.

6.4. Asymptotic performances

In this section, the asymptotic performance is evaluated as a function of INR and N. As shown in Sect. 5.2 (click here), the dependance on Q is strongly linked with the RFI spectral appearance and is not included in this analysis. Equation (6 (click here)) shows that tex2html_wrap_inline1557 is proportional to N. When INR is low (tex2html_wrap_inline1776) the quantized correlator can be considered as linear. Consequently, the term tex2html_wrap_inline1820 of Eq. (3 (click here)) is proportional to INR. Thus, the criterion tex2html_wrap_inline1443 is proportional to tex2html_wrap_inline1824. For example, if the detection time is increased by a factor 100, a sine wave with an INR of tex2html_wrap_inline1826 can be detected with a tex2html_wrap_inline1736 of tex2html_wrap_inline1780 and a tex2html_wrap_inline1734 of tex2html_wrap_inline1784.

6.5. Test with higher order moments

In the application presented here, only the second order statistics of s(t) are tested. Nevertheless, it is also possible to exploit higher order statistics of s(t) through the correlator. In this case, some channels of the correlator must be devoted to the computation of these higher order tests. For example, tests on the tex2html_wrap_inline1840 or tex2html_wrap_inline1842 order statistics can be performed by feeding the correlator with s(t) and its square version s2(t). Then, the non-linear functions are:


 equation592

where tex2html_wrap_inline1848 and tex2html_wrap_inline1850 are parameters used to center and to normalize s2(t) in relation to the quantization levels. Unfortunately, simulations for low INR (tex2html_wrap_inline1776) have shown that performance is not improved compared with the second order case given by Eq. (4 (click here)). In fact, such modifications of tex2html_wrap_inline1415 increase its variance without increasing the difference between itself and the reference vector tex2html_wrap_inline1431.


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