Modelsim xe ii 5.7 g free#

Finally the RFDACT system is implemented on chip using 0.18 m Library, Synopsys Compiler and tools. The output waveforms from the FPGA are tested on the Tektronix Logic Analyzer for real time verification. The system has been successfully implemented in hardware using Field Programmable Grid Array (FPGA) VirtexII. The system is simulated using Modelsim and synthesized using Xilinx Synthesis Technology. The proposed system is designed using Verilog HDL. The PostFDACT will identify the tag by using the deterministic fast detection anti-collision technique.

Modelsim xe ii 5.7 g free#

Then, the identification bit (ID) of the error free packet will be fed to the next subsystem. The PreFDACT detects any error in the incoming messages. The RFDACT consists of two main subsystems PreFDACT and PostFDACT. Our proposed RFDACT is implemented on-chip using Application Specific Integrated Circuit (ASIC) technology. 2008, Johor, Malaysia Reliable Fast Detection Anti-collision Technique for RFID System Implemented on Chip Jahariah Sampe, Nonmember, IEEE and Masuri Othman, Member, IEEE Department of Electrical, Electronics and System Faculty of Engineering, Institute of Microengineering and Nanoelectronic, Universiti Kebangsaan Malaysia 43600 Bangi, Selangor, MALAYSIA Abstract The paper presented a proposed Reliable Fast Detection Anti-collision Technique (RFDACT) for Radio Frequency Identification (RFID) system. Interactions of 209 GeV muons in the Multimuon Spectrometer at Fermilab have yielded more than 8 x 10/sup 4/ events with two muons in the final state. Thesis Country of Publication: United States Language: English Subject: 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PSI RESONANCES PARTICLE PRODUCTION CROSS SECTIONS ELASTIC SCATTERING EXPERIMENTAL DATA FEYNMAN DIAGRAM GEV RANGE 100-1000 INELASTIC SCATTERING MUON PAIRS PARTICLE DECAY PERTURBATION THEORY QUANTUM CHROMODYNAMICS VECTOR MESONS BOSONS DATA DECAY DIAGRAMS ELEMENTARY PARTICLES ENERGY RANGE FIELD THEORIES GEV RANGE HADRONS INFORMATION MESON RESONANCES MESONS NUMERICAL DATA QUANTUM FIELD THEORY RESONANCE PARTICLES SCATTERING 645104* - High Energy Physics- Particle Interactions & Properties-Experimental- Strong Meson-Induced Interactions- = ) < 2.3 nb at 95% C.L. В«В lessДЄuthors: Markiewicz, T W Publication Date: Research Org.: Lawrence Berkeley Lab., CA (USA) OSTI Identifier: 5886241 Report Number(s): LBL-19287 ON: DE85009897 DOE Contract Number: AC03-76SF00098 Resource Type: Technical Report Resource Relation: Other Information: Portions of this document are illegible in microfiche products. = 3.0 +- 0.2 GeV, and the nu dependence is similar to that observed for elastic production. The Q/sup 2/ dependence of sigma/sub eff/ is that of P(.lambda.) with. The p/sub perpendicular//sup 2/ dependence is flatter than that of d sigma/dt for elastic events, with average p/sub perpendicular//sup 2/ slope b = 1.46 +- 0.10. The differential cross section d/sup 2/sigma/sub eff//dzdp/sub perpindicular//sup 2/ for inelastically produced psi's rises approximately linearly with elasticity z identical with E/sub psi//nu. psi) perturbative quantum chromodynamic model for psi production provides an excellent description of the nu dependence of sigma/sub eff/, but cannot simultaneously explain the observed cross section and value of. After correction for nuclear effects, d sigma/sub eff//dt is described by the sum of two exponential terms in t, with average t slope b = 2.56 (+0.35 or - moreВ В» 0.32). psiN conserves helicity in the s channel through natural-parity exchange in the t channel.

We find that W(theta,phi) is consistent with the form expected if the reaction. = (2.0 - 2.4) +- 0.15 GeV, where the spread in values arises from considering the possibility of a Q/sup 2/ dependence in the decay angular distribution W (theta,phi) and in the nuclear shadowing factor.

Its dependence on Q/sup 2/ fits the vector-meson dominance form P(.lambda.) = (1 + Q/sup 2//.lambda./sup 2/)/sup -2/, with. The cross section for elastic psi production by virtual photons, sigma/sub eff/(.gamma./sub V/N), rises with energy nu as log nu. These interactions are classified as either elastic (sigma = 0.36 +- 0.07 nb) or inelastic (sigma = 0.28 +- 0.06 nb) based primarily on the calorimetric determination of E/sub X/. mu./sup +/.mu./sup -/ pairs from J/psi decay, corresponding to the cross section sigma(.mu.N. Interactions of 209-GeV muons within an instrumented magnetized-steel calorimeter have produced 4374 +- 87.