๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

FREQUENCY AND TIME DOMAIN CHARACTERISTIC OF A NOVEL NOTCH FREQUENCY UWB ANTENNA

โœ Scribed by Akhoondzadeh-Asl, Lida; Fardis, Masum; Abolghasemi, Ali; Dadashzadeh, Gholamreza R.


Book ID
117994019
Publisher
The Electromagnetics Academy (EMW Publishing)
Year
2008
Tongue
English
Weight
436 KB
Volume
80
Category
Article
ISSN
1559-8985

No coin nor oath required. For personal study only.


๐Ÿ“œ SIMILAR VOLUMES


Design of a compact frequency-notched UW
โœ Jung N. Lee; Jong K. Park; Sang S. Choi ๐Ÿ“‚ Article ๐Ÿ“… 2005 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 160 KB ๐Ÿ‘ 1 views

In this paper, we propose a frequency-notched ultrawideband (UWB) slot antenna. The proposed antenna can cover the entire UWB band and the IEEE 802.11a frequency band can be notched out by inserting a hat-shaped slot into the antenna. The path loss อ‰S 21 อ‰ and group delay are measured and discussed.

Planar ultra-wideband antenna with a fre
โœ Chih-Yu Huang; Wei-Chun Hsia ๐Ÿ“‚ Article ๐Ÿ“… 2006 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 405 KB ๐Ÿ‘ 1 views

## Abstract A novel and simple design of a printed circular patch antenna for ultraโ€wideband application with a bandโ€notched characteristic is presented. By cutting a pieโ€shaped slot on the circular radiating patch, a frequency band notch will be created. The cutting pie depth contributes to the no

A novel ultra-wideband frequency planar
โœ C. Gรณmez-Calero; B. TahaAhmed; R. Martรญnez ๐Ÿ“‚ Article ๐Ÿ“… 2009 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 466 KB

## Abstract Many research works have emerged for ultraโ€wideband (UWB) systems. One important issue is the antenna design to cover all frequency bands (3.1โ€“10.6 GHz). In most applications, a reduced compact antenna is needed but with several requirements. In this paper, a novel triangleโ€“semicircular

Frequency-domain measurement of indoor U
โœ A. Bayram; A. M. Attiya; A. Safaai-Jazi ๐Ÿ“‚ Article ๐Ÿ“… 2004 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 142 KB

between the two degenerate modes is characterized by the coupling coefficient [15] and is dependent on the structure of the perturbation [16]: where f H and f L are the respective peak-resonance frequencies. Moreover, the three attenuation poles coincide exactly with those of the simulated results.