SpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913WEIGHTED STATISTICAL CONVERGENCE219223221710.22099/ijsts.2009.2217ENV.KARAKAYADepartment of Mathematical Engineering, Yildiz Technical University, Davutpasa
Campus, Esenler, 34750 Istanbul, TurkeyT. A.CHISHTICenter of Distance Education, University of Kashmir, Srinagar, IndiaJournal Article20090820In this paper, the notion of N, pn - summability to generalize the concept of statistical<br />convergence is used. We call this new method weighted statistically convergence. We also establish its<br />relationship with statistical convergence, C,1-summability and strong n N, p -summability.http://ijsts.shirazu.ac.ir/article_2217_176bc8128ea526368e2bcc429ae97a23.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913ESTIMATION OF GALAXY AGE BY MODIFIED MEYER AND SHRAMM NUCLEOSYNTHESIS MODEL225233221810.22099/ijsts.2009.2218ENM. R.ESKANDARIIslamic Azad University, Shiraz Branch, I. R. of IranM.BAHADORANIslamic Azad University, Shiraz Branch, I. R. of IranJournal Article20090119The independent model used by Meyer and Schramm (here after M&S) for determining the age of<br />elements (chemical evolution) is extended. Using new and extended definitions and including parameters<br />ignored by M&S, the galactic evolution equations are solved to determine the total duration of<br />nucleosynthesis,T. To be able to calculate the t T (mean age time for formation of elements to total duration of nucleosynthesis ratio), one event age, max ij , and r(i, j) are determined using approximation relating r(i, j) to the former value r(i, j). For Th/U pair, constraint on t T becomes 0.43 t T 0.61 and the age of the galaxy is obtained as 12.5 23.0 Gal Gyr T Gyr , reducing the variation considerably<br />compared to M&S formalism ( 8.7Gyr TGal 28.1 Gyr ). The range of constraints for the age of the<br />universe is shorter than the M&S and our modifications on the model have reduced the interval for galaxy age 83% and close to being concordant with other available methods.http://ijsts.shirazu.ac.ir/article_2218_4aecaa13eb3d2693ffdecfc3801786e7.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913A GENERALIZED SUMMABILITY FACTOR THEOREM FOR ABSOLUTE SUMMABILITY AND QUASI POWER INCREASING SEQUENCES235240221910.22099/ijsts.2009.2219ENE.SAVASDepartment of Mathematics, Istanbul Commerce University, Uskudar, Istanbul, TurkeyJournal Article20090215The object of this paper is to establish a summability factor theorem for summability<br />A, , k 1 k where A is the lower triangular matrix with non-negative entries satisfying certain conditions.http://ijsts.shirazu.ac.ir/article_2219_e0f8a4bf5159dc19e91050cd5e68a032.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913FINSLER METRICS WITH SPECIAL LANDSBERG CURVATURE241248222010.22099/ijsts.2009.2220ENA.TAYEBIDepartment of Mathematics and Computer Science, Qom University, Qom, I. R. of IranE.PEYGHANDepartment of Mathematics and Computer Science, Arak University, Arak, I. R. of IranJournal Article20090622In this paper, we study a class of Finsler metrics which contains the class of P-reducible and<br />general relatively isotropic Landsberg metrics, as special cases. We prove that on a compact Finsler manifold,<br />this class of metrics is nothing other than Randers metrics. Finally, we study this class of Finsler metrics with<br />scalar flag curvature and find a condition under which these metrics reduce to Randers metric.http://ijsts.shirazu.ac.ir/article_2220_7bbea45db2071e12f2c72620d637da2f.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913COMMON FIXED POINTS OF TWO NONEXPANSIVE MAPPINGS BY A NEW ONE-STEP ITERATION PROCESS249257222110.22099/ijsts.2009.2221ENS. H.KHANDepartment of Mathematics, Statistics and Physics, Qatar University, Doha 2713, QatarM.ABBASDepartment of Mathematics, Lahore University of Management
Sciences, 54792, Lahore, PakistanA. R.KHANKing Fahd University of Petroleum and Minerals, Department of Mathematics and Statistics,
Dhahran 31261, Saudi ArabiaJournal Article20080901We introduce a new one-step iteration process to approximate common fixed points of two<br />nonexpansive mappings in Banach spaces and prove weak convergence of the iterative sequence using (i)<br />Opial’s condition and (ii) Kadec-Klee property. Strong convergence theorems are also established in Banach<br />spaces and uniformly convex Banach spaces under the so-called Condition ( A ), which is weaker than<br />compactness.http://ijsts.shirazu.ac.ir/article_2221_9404272f263e0e8a6524fc174aec85fd.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913DESIGN AND CONSTRUCTION OF AN ACCURATE TIMING SINGLE CHANNEL ANALYZER259267222210.22099/ijsts.2009.2222ENA.EZZATPANAH LATIFIRadiation Application Group, Faculty of Nuclear Engineering,
Shahid Beheshti University, Tehran, I. R. of IranF.ABBASI DAVANIRadiation Application Group, Faculty of Nuclear Engineering,
Shahid Beheshti University, Tehran, I. R. of IranM.SHAHRIARIRadiation Application Group, Faculty of Nuclear Engineering,
Shahid Beheshti University, Tehran, I. R. of IranA.SHARGHI IDOIncubator Center of Technology Units of Shahid Beheshti University
P.O. Box: 1983963113, Tehran, I. R. of IranJournal Article20090519In this paper we discuss an approach to the design and construction of an accurate timing single<br />channel analyzer (TSCA) for the timing of pulses over a wide dynamic range. A brief overview of the timing<br />methods and uncertainty factors as "walk and jitter" and a detailed description of the TSCA circuit are given<br />together with some insight into the application and reasons that led us to the design and construction of<br />constructed TSCA. The advantages of this instrument are then highlighted and the experimental results are<br />presented.http://ijsts.shirazu.ac.ir/article_2222_bd6af23bc81fcd9e0c8344e7af691c5f.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913ANALYSIS AND OPTIMIZATION OF A FISSION CHAMBER DETECTOR USING MCNP4C AND SRIM MONTE CARLO CODES269276222310.22099/ijsts.2009.2223ENK.HADADSchool of Mechanical Engineering, Shiraz University, Shiraz, I. R. of IranM.HASHEMIIslamic Azad University, Science and Research Division, Tehran, I. R. of IranJournal Article20080109In this study, a general theoretical model to foresee and calculate the current-voltage<br />characteristics in a plateau zone and the associated efficiency of the neutron detector (sensitivity) is presented. This study is to complete the previous studies in this field. The model also considers electric field distortion resulting from the charge collection effect. The characteristics curve is obtained as a function of fission rate, chamber geometry, and filling gas pressure. The output current at the saturation domain is calculated. The applied voltages about two phenomena, recombination and avalanche, for working the chamber in an ionization zone are an important part of the calculation. In developing the theoretical model, the MCNP code for fission rate, the SRIM code for electron-ion pair and GEANT4 for gamma sensitivity calculations were used.http://ijsts.shirazu.ac.ir/article_2223_44c462083c6af7fbd79868c8191c0ac6.pdfSpringerIranian Journal of Science and Technology (Sciences)1028-627633320090913STUDY OF NEUTRON YIELD FOR THE 241Am9Be SOURCE277280222410.22099/ijsts.2009.2224ENT.KAKAVANDPhysics Department, Zanjan University, Zanjan, I. R. of IranM.HAJI-SHAFEIEHAIslamic Azad university of Qazvin, Qazvin, I. R. of IranH.GHAFOURIANAtomic Energy Organization of Iran, Tehran, I. R. of IranJournal Article20080517Beryllium chemical combination has a considerable effect on the design and fabrication of the<br />241Am9Be neutron source. In this investigation the beryllium combinations were studied as a generator of<br />neutrons with various mass percentage, and the neutron yields were also calculated using the results of the<br />ALICE and SRIM codes calculations per unit incident charge. The neutron yields of Beryllium Hydride,<br />Beryllium Carbide, Beryllium Hydroxide, Beryllium Oxide, Beryllium Acetate, Beryllium Acetylacetonate<br />and Beryllium Sulfate were calculated as 4397.992107 , 1511.184107 , 976.609107 , 595.299 107 , 336.163107 , 169.62107 and 149.053107 respectively. Our calculations indicate that, the Beryllium Hydride is a proper material for use in the 241Am9Be neutron source.http://ijsts.shirazu.ac.ir/article_2224_2386c79e3599fa454583916ce1f0b2bc.pdf