<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJDM</journal-id><journal-title-group><journal-title>Open Journal of Discrete Mathematics</journal-title></journal-title-group><issn pub-type="epub">2161-7635</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojdm.2012.21001</article-id><article-id pub-id-type="publisher-id">OJDM-17152</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Code of the Symmetric Net with m = 4 and μ = 2
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hmad</surname><given-names>N. Al-Kenani</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>aalkenani10@hotmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>01</month><year>2012</year></pub-date><volume>02</volume><issue>01</issue><fpage>1</fpage><lpage>4</lpage><history><date date-type="received"><day>September</day>	<month>29,</month>	<year>2011</year></date><date date-type="rev-recd"><day>November</day>	<month>1,</month>	<year>2011</year>	</date><date date-type="accepted"><day>November</day>	<month>12,</month>	<year>2011</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we investigated the code over GF(2) which is generated by the incidence matrix of the symmetric (2,4) - net D. By computer search, we found that this binary code of D has rank 13 and the minimum distance is 8.
 
</p></abstract><kwd-group><kwd>Symmetric Nets; Codes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A <img src="1-1200035\deb28018-55a6-466c-937a-d1a0a9aecf02.jpg" /> design <img src="1-1200035\f65dade8-2bb6-44f3-a8b7-145dce78ed2f.jpg" /> is an incidence structure with <img src="1-1200035\32e91420-d6df-4032-96e2-b488613601e0.jpg" /> points, <img src="1-1200035\4353c536-7fec-4c19-8927-efd8946e081f.jpg" />points on each block and any subset of <img src="1-1200035\e0610714-b9dc-4cad-bae4-3197ecb8693c.jpg" /> points is contained in exactly <img src="1-1200035\cca51839-50a4-47b6-905e-687541930bcb.jpg" /> blocks, where<img src="1-1200035\545039d6-8c84-4a24-ae9e-94a3ffec163b.jpg" />. the number of blocks is <img src="1-1200035\cef918c8-8257-47a1-86c7-1c91429eec6a.jpg" /> and the number of blocks on a point is<img src="1-1200035\f64f59e1-9c0c-44ca-90bd-4c2450abc4a3.jpg" />.</p><p>The design <img src="1-1200035\cf337dd6-d570-4cf7-b8b6-8f98d50dd2c1.jpg" /> is resolvable if its blocks can be partitioned into <img src="1-1200035\9cd9e6e8-00c2-464d-8572-9943c5627dee.jpg" /> parallel classes, such that each parallel class partitions the point set of<img src="1-1200035\aad13943-b693-4012-b7ff-cef6be422d53.jpg" />. Blocks in the same parallel class are parallel. Clearly each parallel class has <img src="1-1200035\637e86f6-371a-4210-9acf-e7bcb058ce66.jpg" /> blocks. <img src="1-1200035\d5403ecd-57d0-4346-b79e-401cdb753947.jpg" />is affine resolvable, or simply affine, if it can be resolved so that any two nonparallel blocks meet in <img src="1-1200035\90c238e9-ff3e-4720-9dfa-d7ed3f42ba4e.jpg" /> points, where <img src="1-1200035\9e69f986-dd1d-4837-8a04-97601066ec44.jpg" /> is constant. Affine 1-designs are also called nets. The dual design of a design <img src="1-1200035\1a1adc66-af72-4ce1-a844-9c5e143efc48.jpg" /> is denoted by<img src="1-1200035\e0b9ad83-fac0-4530-aef9-5d8e62b4bdaf.jpg" />. If <img src="1-1200035\7024f616-38ed-4ee4-82ca-181f709a8646.jpg" /> and <img src="1-1200035\58c81f32-644b-4517-b696-991da78c0bed.jpg" /> are both affine, we call <img src="1-1200035\572118ca-8599-458a-b710-bbec28cfd1f3.jpg" /> a &#160;symmetric net. We use the terminology of Jungnickel [<xref ref-type="bibr" rid="scirp.17152-ref1">1</xref>] (see also [2-5]). In this case <img src="1-1200035\0e8ab555-b6db-42f7-b803-f85b5b5abd5e.jpg" /> and <img src="1-1200035\9b0ec89f-53b9-48de-8ed5-350061b7ec46.jpg" />. That is, <img src="1-1200035\a71f0063-fc89-4113-8cea-64245e208ef2.jpg" />is an affine <img src="1-1200035\f1d9b374-9889-463a-a572-5a361809f870.jpg" /> design whose dual <img src="1-1200035\05c7b5c4-f29a-48e7-b5b9-f513018d17d2.jpg" /> is also affine with the same parameters. For short we call such a symmetric net a <img src="1-1200035\b451160c-4351-4171-946e-49516ac9e526.jpg" />-net.</p><p>If <img src="1-1200035\e6978fc9-cb41-4c57-99ca-56c8fe124fb4.jpg" /> is a symmetric net we shall refer to the parallel classes of <img src="1-1200035\0c57dce5-59a9-445b-9166-e2cb993b1e8c.jpg" /> as block classes of <img src="1-1200035\91e9e8ab-223a-46ed-b6db-1f04b4562af1.jpg" /> and to the parallel classes of <img src="1-1200035\ce1655e0-062f-469e-8656-6aa7cd469acf.jpg" /> as point classes of<img src="1-1200035\1aceaac0-e555-449f-8e42-85fd627a1896.jpg" />.</p><p>For any finite structure <img src="1-1200035\6990cabe-85c2-4772-9f9d-f7be738b2e71.jpg" /> with point set <img src="1-1200035\f2f20a02-dd0d-414d-9f40-039ea587bfa8.jpg" /> and block set<img src="1-1200035\15815a7d-ee4a-43e2-9d69-d235355e80d8.jpg" />, the code <img src="1-1200035\07e2af12-f8d4-472a-ae34-360479585f2a.jpg" /> of <img src="1-1200035\49c3e252-ef13-4744-ba7c-0b168560e81a.jpg" /> over prime field <img src="1-1200035\b36f9b07-b833-43af-ac84-0dd1d6836de4.jpg" /> is the subspace of the space <img src="1-1200035\af02a0bb-639f-4e5b-9dca-cc015705bdcd.jpg" /> of all functions from <img src="1-1200035\d603542b-8d1c-4fe7-b2d4-d0932715f9f1.jpg" /> to <img src="1-1200035\a8e4a6f3-e6bc-4d17-87c7-4968a9d0f5b4.jpg" /> that is spanned by the incidence vectors of the blocks of<img src="1-1200035\266b75b3-e743-4280-8cde-1b089fa458c5.jpg" />. This code is equivalent to the code given by the column space of any incidence matrix of the incidence structure, where we use the blocks to index the columns (and the points the rows) of the incidence matrix.</p></sec><sec id="s2"><title>2. The Symmetric Net with <img src="1-1200035\f4356a4d-42c0-4156-ad0a-2eeef92af252.jpg" /> and <img src="1-1200035\5251e9c6-4a07-4303-a44e-2fb7097769d9.jpg" /></title><p>The symmetric net that we shall be concerned with in this paper is the one with <img src="1-1200035\b95ab46a-dd3a-472b-9c75-91c2c787e453.jpg" /> and <img src="1-1200035\9542ac3c-4942-46fd-ab29-946dff6b7ef3.jpg" /> As a design it has parameters</p><p><img src="1-1200035\61809961-d362-4bcc-a58d-9d2206d44693.jpg" /></p><p>Its incidence matrix is (1).</p><p>A computer search has shown that to within isomorphism there is only one symmetric net with these parameters. We denote this symmetric net by<img src="1-1200035\3ff44782-b1d7-48fd-abc0-365623ca79bc.jpg" />.</p><p>Butson [<xref ref-type="bibr" rid="scirp.17152-ref6">6</xref>] showed that there exist symmetric nets with <img src="1-1200035\73df902f-688c-4573-b161-54cb7ad9de61.jpg" /> any prime and <img src="1-1200035\9c14ccc4-105a-44f8-866d-6d70c62bfbe0.jpg" /> This was extended to <img src="1-1200035\24fbdc1a-2f9b-45ab-8d92-441d80a0d992.jpg" /> any prime power by Jungnickel [<xref ref-type="bibr" rid="scirp.17152-ref7">7</xref>]. Therefore <img src="1-1200035\b1ca57fc-4bc5-4124-813f-25ad39d8a8a7.jpg" /> is one of the family of symmetric nets constructed by Jungnickel.</p></sec><sec id="s3"><title>3. The Codes</title><p>The columns of the incidence matrix of <img src="1-1200035\91c94d1d-b70a-4868-aed5-8d78632d71d5.jpg" /> can be considered as vectors of the 32-dimensional vector space over any finite prime field <img src="1-1200035\4c7e9d03-09f9-4364-ba64-96f730d15129.jpg" /> The subspace they generate is the code of the net <img src="1-1200035\09fe7a6d-7932-4660-b025-52ebbec09cbb.jpg" /> over <img src="1-1200035\87d19c1e-6b68-4f5d-801f-d05318e26878.jpg" /> By computer we found that the binary code (that is, the code over the field of order 2) of <img src="1-1200035\d27bcb32-0a27-4a03-933d-8d755ef5191b.jpg" /> has rank 13. The weight distribution of its codewords is given below. The all one vector is in the code since it is obtained as the sum of the 4 columns corresponding to the blocks of any parallel class in the incidence matrix. Therefore the code is self-complementary in that the complement of a codeword is also a codeword, see [<xref ref-type="bibr" rid="scirp.17152-ref8">8</xref>] or [<xref ref-type="bibr" rid="scirp.17152-ref9">9</xref>]. Hence we only list the number of codewords of weight up to 16.</p><p><img src="1-1200035\4f935d49-697f-4436-b96e-8705d8c5c10b.jpg" /></p><p>Since the minimum distance is 8, the binary code is 3-error correcting.</p><p>There doesn’t seem to be an easy proof that the dimension of the code is 13 over the binary field. The dimension of the code of <img src="1-1200035\16673445-4e0a-4318-a7d2-43c81c37e67e.jpg" /> for odd characteristic is 25. This we prove in this paper.</p><p>The incidence matrix of <img src="1-1200035\7668815c-e7e7-4c18-815a-48ca971a8ed0.jpg" /> may be put in the form:</p><p><img src="1-1200035\65aace98-286a-4f36-91b7-1e08439ffd20.jpg" /></p><p>where</p><p><img src="1-1200035\affef92b-5a2c-4081-8c2a-bc4f47c18369.jpg" /></p><p><img src="1-1200035\b700ed7f-adcf-4890-8c94-bba2bdef186c.jpg" /></p><p><img src="1-1200035\769f5138-a60a-4f25-bc54-2036473c3998.jpg" />is an elementary abelian group of order 4.</p><p>First suppose that the characteristic of the field is not 2.</p><p>The matrices in <img src="1-1200035\042dfc1e-9025-4675-b46a-c863ea1f0bac.jpg" /> can be simultaneously diagonalised by</p><p><img src="1-1200035\f287058a-1de3-449f-8939-2af426b6a96b.jpg" /></p><p>Conjugating by diagonal <img src="1-1200035\b2e13dbb-bb18-40af-930a-f94a8e150aa0.jpg" /> and then by<img src="1-1200035\37d8dde1-6171-4b8d-a0c4-d2d82c00df4b.jpg" />, the permutation matrix which moves rows (and columns) <img src="1-1200035\0a2cd9a4-8e10-4798-91f8-31081c6c62db.jpg" />to the first eight positions, rows (and columns) <img src="1-1200035\85ea22fe-bf30-4b03-b3c6-e8bb739a34a0.jpg" />to the next eight positions, rows (and columns) <img src="1-1200035\bd167485-f71a-4f45-b0c3-eb191fab2055.jpg" /> to the next eight positions, rows (and columns) <img src="1-1200035\4339f1a5-0b81-4d93-8d8f-22f5921ab25c.jpg" />to the last eight positions, we get <img src="1-1200035\91412dec-e614-4fa8-869f-363c34c36aa3.jpg" /> conjugate to</p><p><img src="1-1200035\0f7ded17-a020-4843-8942-f279ff4d588b.jpg" /></p><p>have determinant 4096. In fact they are Hadamard matrices. Hence the rank of <img src="1-1200035\c431b442-3e88-4326-a382-c99398751412.jpg" /> is<img src="1-1200035\4ab7622c-df57-4e15-a1d4-c1740ee57b8d.jpg" />, if the characteristic is not 2.</p></sec><sec id="s4"><title>4. Acknowledgements</title><p>The author would like to thank the Deanship of Scientific Research at King Abdulaziz University for supporting a project no. 169/428, where this paper is a part of that project.</p></sec><sec id="s5"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.17152-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">T. Beth, D. Jungnickel and H. Lenz, “Design Theory,” Cambridge University Press, Cambridge, 1999. </mixed-citation></ref><ref id="scirp.17152-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">C. J. Colbourn and J. H. Dinitz, “The CRC Handbook of Combinatorial Designs,” CRC Press, Boca Raton, New York, London, Tokyo, 1996. </mixed-citation></ref><ref id="scirp.17152-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Y. J. Ionin and M. S. Shrikhande, “Combinatorics of Symmetric Designs,” Cambridge University Press, Cambridge, 2006. </mixed-citation></ref><ref id="scirp.17152-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">A. N. Al-Kenani and V. C. Mavron, “Non-Tactical Symmetric Nets,” Journal of the London Mathematical Society, Vol. 67, No. 2, 2003, pp. 273-288.  
doi:10.1112/S0024610702004052</mixed-citation></ref><ref id="scirp.17152-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">V. C. Mavron and V. D. Tonchev, “On Symmetric Nets and Generalised Hadamard Matrices from Affine Designs,” Journal of Geometry, Vol. 67, No. 1-2, 2000, pp. 180-187.  doi:10.1007/BF01220309</mixed-citation></ref><ref id="scirp.17152-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">A. T. Butson, “Generalized Hadamard Matrices,” Proceedings of the American Mathematical Society, Vol. 13, 1962, pp. 894-898.  
doi:10.1090/S0002-9939-1962-0142557-0</mixed-citation></ref><ref id="scirp.17152-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">D. Jungnickel, “On Difference Matrices, Resolvable Transversal Designs and Generalised Hadamard Matrices,” Mathematische Zeitschrift, Vol. 167, No. 1, 1979, pp. 49-60. doi:10.1007/BF01215243</mixed-citation></ref><ref id="scirp.17152-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">E. F. Assmus Jr. and J. D. Key, “Designs and Their Codes,” Cambridge Tracts in Mathematics, Vol. 103, Cambridge University Press, 1992. </mixed-citation></ref><ref id="scirp.17152-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">V. D. Tonchev, “Quasi-Symmetric Designs, Codes, Quadrics, and Hyperplane Sections,” Geometriae Dedicata, Vol. 48, No. 3, 1993, pp. 295-308.   
doi:10.1007/BF01264073</mixed-citation></ref></ref-list></back></article>