Electrochemical biocomputing: a new class of molecular-electronic logic devices

Soft Matter ◽  
2013 ◽  
Vol 9 (29) ◽  
pp. 6571 ◽  
Author(s):  
Yongmei Jia ◽  
Ruixue Duan ◽  
Fan Hong ◽  
Boya Wang ◽  
Nannan Liu ◽  
...  
Keyword(s):  
Molecular Electronic ◽  
Logic Devices ◽  
New Class ◽  
Electronic Logic

scholarly journals Label-Free, Dual-Analyte Electrochemical Biosensors: A New Class of Molecular-Electronic Logic Gates

2010 ◽  
Vol 132 (25) ◽  
pp. 8557-8559 ◽  
Author(s):  
Fan Xia ◽  
Xiaolei Zuo ◽  
Renqiang Yang ◽  
Ryan J. White ◽  
Yi Xiao ◽  
...  
Keyword(s):  
Logic Gates ◽  
Electrochemical Biosensors ◽  
Label Free ◽  
Molecular Electronic ◽  
New Class ◽  
Electronic Logic

Hard Limiting Opto-electronic Logic Devices

1988 ◽  
pp. 69-72 ◽  
Author(s):  
P. Wheatley ◽  
M. Whitehead ◽  
P. J. Bradley ◽  
G. Parry ◽  
J. E. Midwinter ◽  
...  
Keyword(s):  
Logic Devices ◽  
Electronic Logic

Graphenylene-based nanoribbons for novel molecular electronic devices

2020 ◽  
Vol 22 (48) ◽  
pp. 28365-28375
Author(s):  
Leonardo Villegas-Lelovsky ◽  
Ricardo Paupitz
Keyword(s):  
Electronic Devices ◽  
Molecular Devices ◽  
Two Dimensional ◽  
Molecular Electronic ◽  
New Class ◽  
Low Dimensional ◽  
Molecular Electronic Devices

A new class of two-dimensional molecular devices is proposed and investigated theoretically. Doped graphenylene could be used to obtain 2-dimensional p–n junctions suitable for low dimensional electronic devices.

A New Class of Chaotic Sources in Programmable Logic Devices

2020 ◽  
Author(s):  
Tommaso Addabbo ◽  
Ada Fort ◽  
Riccardo Moretti ◽  
Marco Mugnaini ◽  
Hadis Takaloo ◽  
...  
Keyword(s):  
Programmable Logic ◽  
Logic Devices ◽  
New Class ◽  
Programmable Logic Devices

Semiconductor MQWs Photo-Electronic Logic Devices

2018 ◽  
pp. 35-68
Author(s):  
Xiujian Li ◽  
Zhengzheng Shao ◽  
Mengjun Zhu ◽  
Junbo Yang
Keyword(s):  
Logic Devices ◽  
Electronic Logic

In Situ microscopy of the anodic etching of silicon

1995 ◽  
Vol 53 ◽  
pp. 232-233
Author(s):  
Frances M. Ross ◽  
Peter C. Searson
Keyword(s):  
Composite Structures ◽  
High Surface ◽  
High Surface Area ◽  
Chemical Properties ◽  
Selective Etching ◽  
Silicon On Insulator ◽  
Second Phase ◽  
Porous Layers ◽  
New Class ◽  
Porous Semiconductors

Porous semiconductors represent a relatively new class of materials formed by the selective etching of a single or polycrystalline substrate. Although porous silicon has received considerable attention due to its novel optical properties1, porous layers can be formed in other semiconductors such as GaAs and GaP. These materials are characterised by very high surface area and by electrical, optical and chemical properties that may differ considerably from bulk. The properties depend on the pore morphology, which can be controlled by adjusting the processing conditions and the dopant concentration. A number of novel structures can be fabricated using selective etching. For example, self-supporting membranes can be made by growing pores through a wafer, films with modulated pore structure can be fabricated by varying the applied potential during growth, composite structures can be prepared by depositing a second phase into the pores and silicon-on-insulator structures can be formed by oxidising a buried porous layer. In all these applications the ability to grow nanostructures controllably is critical.

The microtubule associated protein (MAP) tau forms a new class of triple-stranded left-hand helical fibrous protein polymer

1992 ◽  
Vol 50 (1) ◽  
pp. 540-541
Author(s):  
G. C. Ruben ◽  
K. Iqbal ◽  
I. Grundke-Iqbal ◽  
H. Wisniewski ◽  
T. L. Ciardelli ◽  
...  
Keyword(s):  
Axial Ratio ◽  
Normal Structure ◽  
Paired Helical Filaments ◽  
Left Hand ◽  
New Class ◽  
Protein Polymer ◽  
Fibrous Protein ◽  
Protein Map ◽  
Neurotransmitter Transport ◽  
Alzheimer Neurofibrillary Tangles

In neurons, the microtubule associated protein, tau, is found in the axons. Tau stabilizes the microtubules required for neurotransmitter transport to the axonal terminal. Since tau has been found in both Alzheimer neurofibrillary tangles (NFT) and in paired helical filaments (PHF), the study of tau's normal structure had to preceed TEM studies of NFT and PHF. The structure of tau was first studied by ultracentrifugation. This work suggested that it was a rod shaped molecule with an axial ratio of 20:1. More recently, paraciystals of phosphorylated and nonphosphoiylated tau have been reported. Phosphorylated tau was 90-95 nm in length and 3-6 nm in diameter where as nonphosphorylated tau was 69-75 nm in length. A shorter length of 30 nm was reported for undamaged tau indicating that it is an extremely flexible molecule. Tau was also studied in relation to microtubules, and its length was found to be 56.1±14.1 nm.

Study of segregation in La1.8Sr0.2CuO4 superconductor by STEM-EDS microanalysis

1987 ◽  
Vol 45 ◽  
pp. 54-55
Author(s):  
T. F. Kelly ◽  
P. J. Lee ◽  
E. E. Hellstrom ◽  
D. C. Larbalestier
Keyword(s):  
Rare Earth ◽  
High Field ◽  
Transport Current ◽  
Total Thickness ◽  
New Class ◽  
Ceramic Superconductors ◽  
Current Densities ◽  
Group Ii ◽  
Eds Microanalysis

Recently there has been much excitement over a new class of high Tc (>30 K) ceramic superconductors of the form A1-xBxCuO4-x, where A is a rare earth and B is from Group II. Unfortunately these materials have only been able to support small transport current densities 1-10 A/cm2. It is very desirable to increase these values by 2 to 3 orders of magnitude for useful high field applications. The reason for these small transport currents is as yet unknown. Evidence has, however, been presented for superconducting clusters on a 50-100 nm scale and on a 1-3 μm scale. We therefore planned a detailed TEM and STEM microanalysis study in order to see whether any evidence for the clusters could be seen.A La1.8Sr0.2Cu04 pellet was cut into 1 mm thick slices from which 3 mm discs were cut. The discs were subsequently mechanically ground to 100 μm total thickness and dimpled to 20 μm thickness at the center.

Electronic structure studies of conducting polymers by electron energy-loss spectroscopy

1996 ◽  
Vol 54 ◽  
pp. 160-161
Author(s):  
J. Fink
Keyword(s):  
Electronic Structure ◽  
Conducting Polymers ◽  
Conjugated Polymers ◽  
Electron Acceptors ◽  
Electron Donors ◽  
Light Emitting ◽  
One Dimensional ◽  
New Class ◽  
Electrical Conductivities ◽  
Electron Energy Loss

Conducting polymers comprises a new class of materials achieving electrical conductivities which rival those of the best metals. The parent compounds (conjugated polymers) are quasi-one-dimensional semiconductors. These polymers can be doped by electron acceptors or electron donors. The prototype of these materials is polyacetylene (PA). There are various other conjugated polymers such as polyparaphenylene, polyphenylenevinylene, polypoyrrole or polythiophene. The doped systems, i.e. the conducting polymers, have intersting potential technological applications such as replacement of conventional metals in electronic shielding and antistatic equipment, rechargable batteries, and flexible light emitting diodes.Although these systems have been investigated almost 20 years, the electronic structure of the doped metallic systems is not clear and even the reason for the gap in undoped semiconducting systems is under discussion.

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