Zobrazeno 1 - 4
of 4
pro vyhledávání: '"HamidReza Uoosefian"'
Publikováno v:
ACM Journal on Emerging Technologies in Computing Systems. 18:1-20
In this paper, a novel and highly efficient inexact Full Adder cell by exploiting two logic styles including conventional CMOS (C-COMS) and pass transistor logic (PTL) are presented. The so-called carbon nanotube field-effect transistor (CNFET) techn
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::9607ba669b33517405c1332628a038b9
https://doi.org/10.1145/3524061
https://doi.org/10.1145/3524061
Publikováno v:
Circuit World. 46:285-299
PurposeThe high demand for fast, energy-efficient, compact computational blocks in digital electronics has led the researchers to use approximate computing in applications where inaccuracy of outputs is tolerable. The purpose of this paper is to pres
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::cfda32695c00509c8e33e508ee785c93
https://doi.org/10.1108/cw-12-2018-0106
https://doi.org/10.1108/cw-12-2018-0106
Publikováno v:
Circuit World.
Purpose Full adder cells are building blocks of arithmetic circuits and affect the performance of the entire digital system. The purpose of this study is to provide a low-power and high-performance full adder cell. Design/methodology/approach Approxi
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::1be615be3b162c6b493a7aa7efd3c3b7
https://doi.org/10.1108/cw-05-2021-0128
https://doi.org/10.1108/cw-05-2021-0128
Publikováno v:
Journal of Circuits, Systems and Computers. 30:2150101
This paper presents two novel current-mode Full Adders based on Carbon Nanotube FET (CNFET). They comprise of three main parts: current-to-voltage converter, threshold detector and voltage-to-current converter. While other designs in the literature u
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::dd0d9ee4bbb88b96bfaa1c0fc1f00362
https://doi.org/10.1142/s0218126621501012
https://doi.org/10.1142/s0218126621501012