nanoelectronics final

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Presented by:- Shikha Gupta (UE6558)

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Page 1: Nanoelectronics Final

Presented by:- Shikha Gupta (UE6558)

Page 2: Nanoelectronics Final

NANOELECTRONICS Branch of Engineering which uses

nanometer scale elements in design of integrated circuits such that one of the three dimensions of the electronic component is in nm.

Generally, Nanometer scale refers to electronic circuits less than 100nm.

1 nm= 10-9 metres

Page 3: Nanoelectronics Final

MOORE’S LAW

According to Moore’s Law, the number of transistors that will fit on a silicon chip doubles every eighteen months. Presently, microprocessors have

more than forty million transistors By the year 2020, the trend line of

Moore’s law states that there should be a one nanometer feature size. .

Page 4: Nanoelectronics Final

SCALING PRINCIPLES

For designing nano FET apart from channel length, other parameters like doping, voltages etc. are to be also scaled.

Page 5: Nanoelectronics Final

Original Device

Scaled Device

Page 6: Nanoelectronics Final

EJ MOSFET (Electrically variable shallow junction MOSFET)

NANO MOSFET

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SCALING LIMITS OF MOSFET

Technical problem: For channel length<30nm , insulating SiO2 is expected to be less than 2nm thick. This thin layer causes gate dielectric tunneling

Physical problem: For channel length<10nm, direct source-drain tunneling occurs.

Page 8: Nanoelectronics Final

Schematic representation of Gate –dielectric tunneling and Direct source-drain tunneling

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EJ- MOSFET

Construction

It consists of 2 gates :Upper gate and a lower gate. Gates are insulated from each other by an integrate oxide layer

Page 10: Nanoelectronics Final

Working

Upper layer electrically induces the inversion layers that are self aligned to the lower gate and the lower gate controls the current between the inversion layer.

Presence of two gates helps in suppressing short channel effects

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QUANTUM EFFECTS IN ULTRASHORT CHANNEL MOSFET Mobility enhancement due to

decrease in scattering Threshold voltage increases with

decrease in channel width

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THRESHOLD VOLTAGE ADJUSTMENT USING QUANTUM EFFECTS

For <110> oriented device n type has greater VT shift than p type

For <100> oriented device p type has greater VT shift than n type

To keep VT same for both square scaling i.e. width = height is used.

Page 13: Nanoelectronics Final

BASIC PHENOMENON OBSERVED IN NANO

DEVICES

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BALLISTIC TRANSPORT IN NANO STRUCTURES

At room temperature mean free path of electron is around 10nm.So, at ultrashort channel length electron scattering decreases considerably.

At channel length less than 10nm,scattering approaches zero. It is called ballistic transport.

With decrease in temperature mean free path can be increased & ballistic transport can be obtained at larger channel length.

Page 15: Nanoelectronics Final

RESONANT TUNNELING IN NANO DEVICES RT is observed in hetero-structure

semiconductor devices made from pairs of different alloys III-V alloys..

Eg. AlGaAs/GaAs/AlGaAs diodes

Page 16: Nanoelectronics Final

MISCELLANEOUSNANO-STRUCTURES

Carbon nanotubes & nanowires

Page 17: Nanoelectronics Final

CARBON NANOTUBES

Single-wall carbon nanotubes are a new form of carbon made by rolling up a single graphite sheet to a narrow but long tube closed at both sides by fullerene-like end caps..

Page 18: Nanoelectronics Final

PROPERTIES

Exhibit electrical conductivity as high as copper, thermal conductivity as high as diamond

Strength 100 times greater than steel at one sixth the weight

Electrical conductivity depends on their helicity.

Page 19: Nanoelectronics Final

CURRENT APPLICATIONS

In field of electronics & communication

In solar cells to trap electrons Touch screens and flexible displays nanoradio, a radio receiver consisting

of a single nanotube, was demonstrated in 2007

In fabrication of ultracapacitors (which have high energy density)

Page 20: Nanoelectronics Final

NANOWIRES

Electrons in nanowires are quantum confined laterally and thus occupy energy levels that are different from that in bulk materials.

Aspect ratios (length-to-width ratio) of 1000 or more

Poor conductivity (edge effect)

Page 21: Nanoelectronics Final

APPLICATIONSCurrent Create active electronic devices like logic gates etc.Potential use As photon ballistic waveguides For connecting molecular-scale

entities in a molecular computer For flexible flat-screen displays

Page 22: Nanoelectronics Final

RECENT DEVELOPMENTS IN

FIELD OF NANOELECTRONICS

Page 23: Nanoelectronics Final

WORLD’S SMALLEST TRANSISTOR

Graphene Transistor

Page 24: Nanoelectronics Final

WORLD’S smallest transistor

quantum dot with a tiny circular cage at the center known as the central island. Voltage can change the conductivity of thesequantum dots, allowing them to store logic states

Ability to retain conductivity when only one atom thick.a small sheet of graphene is taken & channels are carved into it using electron beam lithography. What remains is a

Graphene Sheets

Page 25: Nanoelectronics Final

Schematic diagram of graphene transistor

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NANO RADIO

First Radio at nano-scale

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NANO RADIO

A nanoradio is a radio receiver or transmitter constructed on a nanometer scale.

Currently only receivers have been

developed( October 2007)

Page 28: Nanoelectronics Final

WORKING The nanotube, is contained in a

vacuum and one of its ends is connected to an electrode of a battery. The other electrode is placed a short distance from the nanotube's other end. The tube will vibrate in tune with any external electromagnetic signal, effectively acting as an antenna. The vibration frequency can be adjusted by changing the applied voltage.

Page 29: Nanoelectronics Final

NANO RADIO

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NANO EMISSIVE DISPLAY

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NANO EMISSIVE DISPLAY Launched in May,2005 by motorola

Works by moving electrons through its driver electronics and into the nanotubes, which then direct the electrons at groups of phosphors (pixels) on the interior surface of the display. When the phosphors are bombarded with electrons, they glow, giving off color—similar to the operation of a traditional CRT

Page 32: Nanoelectronics Final

ADVANTAGES

Light in weight and more slim

Saves 20% to 30% more power than other flat panel displays

Manufacturing cost is estimated to be a half to a third the cost of LCD and plasma displays

Page 33: Nanoelectronics Final

APPLICATION

Laptop screen due to better power saving & size

Screens in fighter planes due to better brightness & resolution

Automotive and aeronautical purposes

TV displays

Page 34: Nanoelectronics Final