A minimum gradient algorithm for phased-array null formation
Formation of the null at the phased‐array beam pattern pointed toward the source of a radio frequency interference (RFI) can serve to mitigate the effects of that RFI. Several algorithms for creating a null at the phased‐array beam pattern have been designed. On the basis of an array side lobe minim...
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| Published in | Radio science Vol. 40; no. 2 |
|---|---|
| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
Blackwell Publishing Ltd
01.04.2005
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| Subjects | |
| Online Access | Get full text |
| ISSN | 0048-6604 1944-799X 1944-799X |
| DOI | 10.1029/2004RS003140 |
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| Abstract | Formation of the null at the phased‐array beam pattern pointed toward the source of a radio frequency interference (RFI) can serve to mitigate the effects of that RFI. Several algorithms for creating a null at the phased‐array beam pattern have been designed. On the basis of an array side lobe minimization algorithm (Kogan, 2000), a new method for creating a null at the phased‐array beam pattern is described here. The algorithm is a straightforward one and can have an advantage in creating wide‐area nulls, especially for phased arrays with a small number of antennas. We have tested this algorithm for a possible Square Kilometre Array antenna station configured as a phased array of 19 antennas and for the Very Large Array configuration D (VLA‐D), working as a phased array for very long baseline interferometry experiments. The null is created at the given area around the given direction. The narrow null (∼0.1 ) deeper than 100 dB level can be achieved at the cost of a 2% decrease in the signal‐to‐noise ratio in the main direction. The creation of such a deep null can be impractical for many reasons, however, first and foremost because the phases and weights would have to be specified with impractical precision. Rounding the phase and weights to 1° and 0.01, respectively raises the null up to ∼50 dB. |
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| AbstractList | Formation of the null at the phased‐array beam pattern pointed toward the source of a radio frequency interference (RFI) can serve to mitigate the effects of that RFI. Several algorithms for creating a null at the phased‐array beam pattern have been designed. On the basis of an array side lobe minimization algorithm (Kogan, 2000), a new method for creating a null at the phased‐array beam pattern is described here. The algorithm is a straightforward one and can have an advantage in creating wide‐area nulls, especially for phased arrays with a small number of antennas. We have tested this algorithm for a possible Square Kilometre Array antenna station configured as a phased array of 19 antennas and for the Very Large Array configuration D (VLA‐D), working as a phased array for very long baseline interferometry experiments. The null is created at the given area around the given direction. The narrow null (∼0.1 ) deeper than 100 dB level can be achieved at the cost of a 2% decrease in the signal‐to‐noise ratio in the main direction. The creation of such a deep null can be impractical for many reasons, however, first and foremost because the phases and weights would have to be specified with impractical precision. Rounding the phase and weights to 1° and 0.01, respectively raises the null up to ∼50 dB. Formation of the null at the phased‐array beam pattern pointed toward the source of a radio frequency interference (RFI) can serve to mitigate the effects of that RFI. Several algorithms for creating a null at the phased‐array beam pattern have been designed. On the basis of an array side lobe minimization algorithm (Kogan, 2000), a new method for creating a null at the phased‐array beam pattern is described here. The algorithm is a straightforward one and can have an advantage in creating wide‐area nulls, especially for phased arrays with a small number of antennas. We have tested this algorithm for a possible Square Kilometre Array antenna station configured as a phased array of 19 antennas and for the Very Large Array configuration D (VLA‐D), working as a phased array for very long baseline interferometry experiments. The null is created at the given area around the given direction. The narrow null (∼0.1 ) deeper than 100 dB level can be achieved at the cost of a 2% decrease in the signal‐to‐noise ratio in the main direction. The creation of such a deep null can be impractical for many reasons, however, first and foremost because the phases and weights would have to be specified with impractical precision. Rounding the phase and weights to 1° and 0.01, respectively raises the null up to ∼50 dB. |
| Author | Kogan, Leonid |
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| References | Smolders, B., and G. Hampson (2002), Deterministic nulling in phased arrays for the next generation of radio telescopes, IEEE Trans. Antennas Propag., 44(4), 13-22. Ellingson, S. W., and G. A. Hampson (2002), A subspace tracking approach to interference nulling for phased array based radio telescopes, IEEE Trans. Antennas Propag., 50(1), 25-30. Kogan, L. (2000), Optimising a large array configuration to minimize the side lobes, IEEE Trans. Antennas Propag., 48(7), 1075-1078. Ellingson, S. W., and W. Cazemier (2003), Efficient multibeam synthesis with interference nulling for large arrays, IEEE Trans. Antennas Propag., 51(3), 503-511. Godara, L. C. (1997), Application of antenna arrays to mobile communications, part II: Beam-forming and direction-of-arrival considerations, Proc. IEEE, 85, 1195-1245. 2003 2002 2001 2000; 48 2003; 51 2002; 50 1997; 85 2002; 44 e_1_2_7_6_1 e_1_2_7_11_1 e_1_2_7_5_1 e_1_2_7_10_1 e_1_2_7_4_1 e_1_2_7_3_1 e_1_2_7_9_1 e_1_2_7_8_1 e_1_2_7_7_1 e_1_2_7_2_1 |
| References_xml | – reference: Godara, L. C. (1997), Application of antenna arrays to mobile communications, part II: Beam-forming and direction-of-arrival considerations, Proc. IEEE, 85, 1195-1245. – reference: Kogan, L. (2000), Optimising a large array configuration to minimize the side lobes, IEEE Trans. Antennas Propag., 48(7), 1075-1078. – reference: Ellingson, S. W., and W. Cazemier (2003), Efficient multibeam synthesis with interference nulling for large arrays, IEEE Trans. Antennas Propag., 51(3), 503-511. – reference: Smolders, B., and G. Hampson (2002), Deterministic nulling in phased arrays for the next generation of radio telescopes, IEEE Trans. Antennas Propag., 44(4), 13-22. – reference: Ellingson, S. W., and G. A. Hampson (2002), A subspace tracking approach to interference nulling for phased array based radio telescopes, IEEE Trans. Antennas Propag., 50(1), 25-30. – volume: 51 start-page: 503 issue: 3 year: 2003 end-page: 511 article-title: Efficient multibeam synthesis with interference nulling for large arrays publication-title: IEEE Trans. Antennas Propag. – volume: 48 start-page: 1075 issue: 7 year: 2000 end-page: 1078 article-title: Optimising a large array configuration to minimize the side lobes publication-title: IEEE Trans. Antennas Propag. – volume: 44 start-page: 13 issue: 4 year: 2002 end-page: 22 article-title: Deterministic nulling in phased arrays for the next generation of radio telescopes publication-title: IEEE Trans. Antennas Propag. – volume: 50 start-page: 25 issue: 1 year: 2002 end-page: 30 article-title: A subspace tracking approach to interference nulling for phased array based radio telescopes publication-title: IEEE Trans. Antennas Propag. – volume: 85 start-page: 1195 year: 1997 end-page: 1245 article-title: Application of antenna arrays to mobile communications, part II: Beam‐forming and direction‐of‐arrival considerations publication-title: Proc. IEEE – start-page: 109 year: 2003 end-page: 125 – year: 2002 – year: 2001 – year: 2003 – ident: e_1_2_7_4_1 doi: 10.1109/8.992558 – ident: e_1_2_7_8_1 doi: 10.1109/8.876326 – ident: e_1_2_7_2_1 – ident: e_1_2_7_6_1 doi: 10.1007/0-306-48080-8_7 – ident: e_1_2_7_7_1 – ident: e_1_2_7_9_1 – ident: e_1_2_7_10_1 doi: 10.1109/MAP.2002.1043143 – ident: e_1_2_7_3_1 doi: 10.1109/TAP.2003.809840 – ident: e_1_2_7_5_1 doi: 10.1109/5.622504 – ident: e_1_2_7_11_1 |
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| Title | A minimum gradient algorithm for phased-array null formation |
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