Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna

The maximum number of elements of a nonredundant configuration on a square array antenna is estimated empirically employing the investigated structure of differences between the elements of the configuration mapping onto the scan. Отримано емпіричну оцінку максимальної кількості елементів безнадлишк...

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Datum:2009
1. Verfasser: Kopilovich, L.E.
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Veröffentlicht: O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine, 2009
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Zitieren:O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine, / L. E. Kopilovich // Радиофизика и радиоастрономия. — 2009. — Т. 14, № 3. — С. 183–187. — Бібліогр.: 10 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Kopilovich, L.E.
author_facet Kopilovich, L.E.
citation_txt O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine, / L. E. Kopilovich // Радиофизика и радиоастрономия. — 2009. — Т. 14, № 3. — С. 183–187. — Бібліогр.: 10 назв. — англ.
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description The maximum number of elements of a nonredundant configuration on a square array antenna is estimated empirically employing the investigated structure of differences between the elements of the configuration mapping onto the scan. Отримано емпіричну оцінку максимальної кількості елементів безнадлишкової конфігурації на квадратній антенній решітці, що грунтується на вивченні структури різниць між елементами її відображення на розгортці. Получена эмпирическая оценка максимального числа элементов безызбыточной конфигурации на квадратной антенной решетке, основанная на изучении структуры разностей между элементами ее отображения на развертке.
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fulltext Радиофизика и радиоастрономия, 2009, т. 14, №2, с. 183-187 © L. E. Kopilovich, 2009 Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna L. E. Kopilovich O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine, 12, Acad. Proskury St., Kharkiv, 61085, Ukraine E-mail: kopil@ire.kharkov.ua Received August 18, 2008 The maximum number of elements of a nonredundant configuration on a square array antenna is estimated empirically employing the investigated structure of differences between the elements of the configuration mapping onto the scan. Introduction The problem of constructing a nonredundant configuration (NRC) of elements is of urgent necessity for radio interferometry. Here, a mo- mentous problem is how to build the NRC with the maximum number of elements to obtain the maximum number of interferometer baselines. Such NRCs on square n n× grids (so called “Golomb squares” [1]) with the maximum possi- ble elements are found at 22n ≤ in a number of papers [1-7]. At the same time, the size of modern array antenna, as well as the number of its elements, can substantially exceed these values [8] that requires the elaboration of meth- ods for building NRCs on large grids. Such NRCs were obtained in [4] with using combinatorial constructions – cyclic difference sets (see also [9]). However, it remains unclari- fied to what degree the element number of the NRC thus found is close to a maximum. The rigorous estimates for the NRC element number on a square grid were obtained in [1, 3], however, the former is too overrated, while for applying the latter the information on NRCs on linear grids of large lengths, unavailable to date, is required. In this connection, the obtainment of the upper estimate based on available empirical data is of interest. Analysis of the mapping structure of the NRC on the square grid scan Consider an arbitrary k-element NRC on the n n× grid and analyze the system of vector differ- ences between its elements (see Fig. 1). Number the cells of the first grid row from 1 to n, of the second one – from 1n + to 2n, and so on. Fig. 1. An example of a nonredundant configuration (NRC) on the square grid. The NRC elements are denoted with bold dots. The vectors connecting the elements are pointed rigthwards or strictly downwards (type I) or leftwards (type II) L. E. Kopilovich 184 Радиофизика и радиоастрономия, 2009, т. 14, №2 The vector connecting the cells can be pointed rightwards or strictly downwards (type I), or left- wards (type II). When scanning the grid, the NRC on it passes to a point system on the segment, and the differences between these points can be either one-fold (i. e. non-repeated) or two-fold ones. Obviously, vector differences on a 2-D grid be- longing to the same type cannot pass to equal dif- ferences on the scan, while only some part of these belonging to the opposite types passes to the equal ones. Thus, the share of the one-fold differences on the scan can be expected to exceed half of their total number ( 1) 2.K k k= − Besides, it should be taken into account that the NRC placed on a square grid, the latter being rotated through 90 ,° would give an alternative point system on the scan (see Fig. 2). In addition, for most of n values, at least, several different NRCs with a maximum number of elements can be built [7]. This allows suggestion that for almost all values of n a maxi- mum-element NRC on the n n× grid can be built for which the share (α) of the non-repeated differ- ences on the scan exceeds 50 % of their total number, 50 %.α > (1) These qualitative considerations were verified by using the available data. The n n× grids at 3 22n≤ ≤ with the NRCs found in [4, 6, 7] placed on them were scanned in two variants (as in Fig. 2), and it was found out that for all n in this range, except for 7,n = this suggestion was validated at least in one of such variants (see Table 1). Now we will seek the upper estimate for the NRC element number under the assumption that for 7n > a maximum-element NRC can be found for which condition (1) is fulfilled. Upper estimate of the NRC element number Consider a k-element NRC placed on the n n× grid. When scanning the grid, the NRC elements pass to a point sequence 1 2 ... ka a a< < < (2) on the scan. Here, we apply the approach suggested for the linear case [10]. The order of differences Fig. 2. A grid with an NRC placed on it, and its scan (a). The same grid rotated through 90°, and its scan (b). The share of non-repeated differences between the points on the scan is denoted with α (%) Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna 185Радиофизика и радиоастрономия, 2009, т. 14, №2 between elements ja and ia of sequence (2), ,j i> is the difference ,j i− at this point, the sum of differences of the first order is 2 2 1 1( ) ... ( ) ,k ka a a a n−− + + − < and similarly, the sum of differences of order ν is 2 1 1( ) ... ( ) .k ka a a a nν+ −ν− + + − < ν It follows that the sum of differences of orders up to t is 2 ( 1) 2.tS n t t< + (3) On the other hand, the number of these differen- ces is ( 1) ... ( ) ( 1) 2 ,k k t kt t t ts− + + − = − + = (4) where ( 1) 2, 1 .s k t t k= − + ≤ ≤ Should the differences between the elements on the scan be all distinct then one might write 1 ... ,tS ts≥ + + and comparing the last inequality with (3) find the estimate of the maximum element number. Vir- tually, in such a way the estimate for the maxi- mum element number of an NRC on a linear grid can be obtained [10]. In our case, some part of differences on the scan are two-fold, but using condition (1) and with the Eq. (4) considered, we may write ( ) ( )2 1 ... [ / 4] [ / 4] 1 ... [3 / 4],tS ts ts ts≥ + + + + + + (5) where [c] means integer part of c. If one writes 4 ,ts r= + β with the r integer and 0, 1, 2β = or 3, inequality (5) can be rewritten in the form 2(1 ... ) ( 1) ... (4 ).tS r r r r≥ + + + + + + + β − When performing here the summation opera- tions and returning again to the ts one obtains 2 2 25 1 1 5( ) ( ) . 16 8 2 16 16tS ts ts tsβ⎛ ⎞≥ + + + β >⎜ ⎟⎝ ⎠ Further, one correlates the last inequality with (3) and obtains: 2 25 ( 1)( ) , 16 2 t t nts +< whence n k m K a (%) 3 5 6 10 60.0 4 6 11 15 73.3 5 8 16 28 57.4 6 9 24 36 66.7 7 11 27 55 49.1 8 12 34 66 51.5 9 13 45 78 56.7 10 15 53 105 50.5 11 16 64 120 53.3 12 17 82 136 60.3 13 18 87 153 56.9 14 19 101 171 59.1 15 21 112 210 53.3 16 22 125 231 54.1 17 23 149 253 58.9 18 24 168 276 60.9 19 25 184 300 61.3 20 26 198 325 60.9 22 29 244 406 60.1 Table 1. The characteristics of the maximum-element NRCs and point sequences obtained from them when scanning the location grids. Here, n is the grid side- length, k is the number of the NRC elements, m is the number of non-repeated differences between points on the scan, and α is their share in the total number of differences equal to K k( k 1) 2−= L. E. Kopilovich 186 Радиофизика и радиоастрономия, 2009, т. 14, №2 ( )1 1 1 1 (2 ) ,s nb t nb t< + ≅ + with 8 5 1.265,b = = and ( )( 1) 2 1 1 (2 ) ( ).k t nb t f t< + + + = Function ( )f t has its minimum at ,t nb= thus 1.265 1.124 0.5k n n< + + (6) or ,ek k≤ where ek is the integer part of the expression in the right-hand side of (6). Results Table 2 shows the maximal found element numbers of NRCs placed on n n× grids at 7n > taken from [7], in comparison with their estimates as obtained by (6) and those known from litera- ture. It can be seen that the values of ek are smaller than the estimates given in [1]; as for the estimates in [3], obtained only for 11,n ≤ in this range they roughly equal to ours. As is seen from Table 2, there is a “reserve” kept in the discrepancy between ek and the cor- responding value of k. Apparently, owing to this estimate (6) is valid also for the case of a possible value of n when condition (1) is not fulfilled. The comparison of the estimates for large arrays given by (6) with the results obtained in [4] (see Table 3) shows that the number of NRC elements given by the suggested method, though not maximum, is nevertheless wholly acceptable for feasible purposes. Conclusion The upper estimate obtained for the element number of an NRC on a square grid is more ef- ficient than those earlier known. It can serve a guiding line when building a large size array an- tenna with the maximum NRC element number. References 1. J. P. Robinson, “Golomb rectangles”, IEEE Trans, Vol. IT-31, No. 6, pp. 781-787, 1985. 2. J. B. Shearer, “Some new Golomb rectangles”, Elect- ron. J. Comb., Vol. 2, No. R12, 1995. 3. J. P. Robinson, “Golomb rectangles as folded rulers”, IEEE Trans, Vol. IT-43, No. 1, pp. 290-293, 1997. 4. L. E. Kopilovich, “Nonredundant apertures for opti- cal interferometric systems: maximization of the num- Table 3. The element numbers in the NRCs on large grids [6], and their estimates with (6) n k ek 25 30 37 30 35 44 40 47 58 50 58 71 Table 2. The estimates of the maximum number of the NRC elements on square grids. Here, n and k are the same as in Fig. 1, ek is estimated with (6), rk and r1k are the estimates of k taken from [1] and [3], respectively n k ek rk 1rk 8 12 13 13 13 9 13 15 15 14 10 15 16 17 16 11 16 18 19 18 12 17 19 21 – 13 18 21 23 – 14 19 22 25 – 15 21 23 27 – 16 22 25 28 – 17 23 26 29 – 18 24 28 31 – 19 25 29 33 – 20 26 30 34 – 21 27 32 – – 22 29 33 – – Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna 187Радиофизика и радиоастрономия, 2009, т. 14, №2 ber of elements”, J. Mod. Opt., Vol. 45, No. 11, pp. 2417-2424, 1998. 5. J. P. Robinson, “Genetic search for Golomb ar- rays”, IEEE Trans, Vol. IT-46, No. 6, pp. 781-787, 2000. 6. Yu. V. Kornienko, “Construction of nonredundant antenna configurations on square grids by a ran- dom search technique”, Telecommunications and Radio Engineering, Vol. 57, Nos. 2&3, pp. 23-30, 2002. 7. J. B. Shearer “Symmetric Golomb squares”, IEEE Trans, Vol. IT-50, No. 8, pp. 1846-1847, 2004. 8. R. Schultz, “Radio astronomy antennas by the Thou- sands”, Experimental Astronomy, Vol. 17, pp. 119-139, 2004. 9. L. E. Kopilovich and L. G. Sodin, “Multielement System Design in Astronomy and Radio Science”, vol. 268, Dordrecht/Boston/London: Kluwer Acade- mic Publishers, Astrophysics and Space Science Library, 2001, 190 p. 10. B. Lindström, “On inequality for B-sequences”, J. Combin. Theory, Vol. A6, No. 2, pp. 211-212, 1969. Эмпирическая оценка максимального числа элементов безызбыточной конфигурации на квадратной антенной решетке Л. Е. Копилович Получена эмпирическая оценка максималь- ного числа элементов безызбыточной конфигу- рации на квадратной антенной решетке, осно- ванная на изучении структуры разностей между элементами ее отображения на развертке. Емпірична оцінка максимальної кількості елементів безнадлишкової конфігурації на квадратній антенній решітці Л. Ю. Копилович Отримано емпіричну оцінку максимальної кількості елементів безнадлишкової конфігу- рації на квадратній антенній решітці, що грун- тується на вивченні структури різниць між елементами її відображення на розгортці.
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
language English
last_indexed 2025-12-07T17:00:42Z
publishDate 2009
publisher O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine,
record_format dspace
spelling Kopilovich, L.E.
2014-04-09T15:34:37Z
2014-04-09T15:34:37Z
2009
O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine, / L. E. Kopilovich // Радиофизика и радиоастрономия. — 2009. — Т. 14, № 3. — С. 183–187. — Бібліогр.: 10 назв. — англ.
https://nasplib.isofts.kiev.ua/handle/123456789/59641
The maximum number of elements of a nonredundant configuration on a square array antenna is estimated empirically employing the investigated structure of differences between the elements of the configuration mapping onto the scan.
Отримано емпіричну оцінку максимальної кількості елементів безнадлишкової конфігурації на квадратній антенній решітці, що грунтується на вивченні структури різниць між елементами її відображення на розгортці.
Получена эмпирическая оценка максимального числа элементов безызбыточной конфигурации на квадратной антенной решетке, основанная на изучении структуры разностей между элементами ее отображения на развертке.
en
O. Ya. Usikov Institute for Radiophysics and Electronics of NAS of Ukraine,
Антенны, волноводная и квазиоптическая техника
Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
Емпірична оцінка максимальної кількості елементів безнадлишкової конфігурації на квадратній антенній решітці
Эмпирическая оценка максимального числа элементов безызбыточной конфигурации на квадратной антенной решетке
Article
published earlier
spellingShingle Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
Kopilovich, L.E.
Антенны, волноводная и квазиоптическая техника
title Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
title_alt Емпірична оцінка максимальної кількості елементів безнадлишкової конфігурації на квадратній антенній решітці
Эмпирическая оценка максимального числа элементов безызбыточной конфигурации на квадратной антенной решетке
title_full Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
title_fullStr Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
title_full_unstemmed Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
title_short Empirical Estimate for the Maximum Element Number of a Nonredundant Configuration on Square Array Antenna
title_sort empirical estimate for the maximum element number of a nonredundant configuration on square array antenna
topic Антенны, волноводная и квазиоптическая техника
topic_facet Антенны, волноводная и квазиоптическая техника
url https://nasplib.isofts.kiev.ua/handle/123456789/59641
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