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ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University [email protected]

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Page 1: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

ECE 474:Principles of Electronic Devices

Prof. Virginia AyresElectrical & Computer EngineeringMichigan State [email protected]

Page 2: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example for VA Pr. 01 1.13: The {111} family of planes with the <111> family of directions. There are X = 8 of these.

Page 3: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Va Pr. 01 is: do likewise for the {110} family. You need only draw four out of the X possibilities.Hint: X is NOT equal to 8.

Page 4: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Lecture 08:

Lectures: Hexagonal nanosystems: graphene and carbon nanotubes

Introduction to graphene and CNTsThe Basis Vectors: a1 and a2Nearest neighbor distancesThe Chiral Vector: ChThe CNT diameter dtThe Translation Vector: TThe Unit Cell of a CNTNumber of hexagons NNumber of carbon atoms 2N (π electrons)Areal Density

Examples of each

Quantify physical structures of crystal systems that are important for devices:

Page 5: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Lecture 08:

Lectures: Hexagonal nanosystems: graphene and carbon nanotubes

Introduction to graphene and CNTsThe Basis Vectors: a1 and a2Nearest neighbor distancesThe Chiral Vector: ChThe CNT diameter dtThe Translation Vector: TThe Unit Cell of a CNTNumber of hexagons NNumber of carbon atoms 2N (π electrons)Areal Density

Examples of each

Quantify physical structures of crystal systems that are important for devices:

Page 6: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

The Unit Cell of a CNT (single wall)

Note that T and Ch are perpendicular.

Therefore T X Ch = the area of the CNT Unit Cell

= | T || Ch |sin(90o)

= | T || Ch |

Page 7: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the area of the Unit cell for a (10,10) CNT.

Page 8: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the area of the Unit cell for a (10,10) CNT.

From Lec 07:

|Ch| = 43.13 Ang

| T | = 2.49 Ang

Area of the Unit cell = | T || Ch | = 107.39 Ang2

Page 9: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the formula for the area of the Unit cell in terms of n, m and dR.

Page 10: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the formula for the area of the Unit cell in terms of n, m and dR.

Area of the Unit cell = | T || Ch |

Page 11: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Number of hexagons N in the Unit Cell:

Basic unit is the hexagon.

The number of hexagons in the Unit cell is called N

Therefore:the number of hexagons N per CNT Unit Cell is:

N = area of the Unit cellarea of one hexagon

Page 12: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Called: dividing by the Primitive Cell of a CNT:

a1 x a2 is the area of a single basic hexagon. This is also called the primitive cell.

Note: the area of the dotted rhombus is equal to the area of a single hexagon. The magnitude is:

Note the two inequivalent carbon atoms A and B inside the rhombus

23 2a

C C

Page 13: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Page 14: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

The number of hexagons N per CNT Unit Cell is:

N = | T X Ch || a1 x a2 |

= 2(m2 + n2+nm)/dR

How many carbon atoms per hexagon?

Number of hexagons N versus the number of carbon atoms in the Unit Cell:

Page 15: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

120o

120o

120o

Each C atom is 1/3 inside the hexagon.

Page 16: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

120o

120o

120o

Each C atom is 1/3 inside the hexagon.

6 X (1/3) = 2 atoms per hexagon

Page 17: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

The number of hexagons N per CNT Unit Cell is:

N = | T X Ch || a1 x a2 |

= 2(m2 + n2+nm)/dR

How many carbon atoms per hexagon?

Answer: 2

Number of hexagons N versus the number of carbon atoms in the Unit Cell:

Page 18: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

How many carbon atoms in the Unit cell?

Answer:First solve for the number of hexagons N.

The number of carbon atoms in the Unit cell = 2N.

Number of hexagons N versus the number of carbon atoms in the Unit Cell:

Page 19: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Each primitive cell contains two carbon atoms.

There is one pz-orbital per each carbon atom.

Therefore there are 2N pzorbitals available per CNT (or graphene) Unit Cell = cloud of electrons = greatconductivity.

The shared electrons from the pz orbitals are called πelectrons.

π electrons and electrical properties:

Page 20: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

a) Example:

Find the number of hexagons N in the unit cell of a (10, 10) CNT.Find the number of carbon atoms in the unit cell of a (10, 10) CNT.

Page 21: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Page 22: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the areal density of the unit cell of a (10, 10) CNT.

Page 23: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Page 24: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Example: find the general areal density formula and evaluate it.

This is the conclusion of the discussion we started on the board. The answer is obvious when you think about it!

Page 25: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Page 26: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

= the same number as for the (10,10) CNT. Of course! The density of a material doesn’t change when you cut it.The areal density on different faces within the cubic system changes but graphene has only one face.

Page 27: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

Interesting fact: there are Endcap restrictions on CNT diameter dt:

CNTs have closed endcapswhich are ½ a buckyball.

Armchair

Zigzag

Chiral

Page 28: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

C60

XZ Ke, et al, Physics Letters A 255 (1999) 294-300

C36

C60 mean ball diameter 6.83 Å

C60 ball outer diameter 10.18 Å

C60 ball inner diameter 3.48 Å

http://www.sesres.com/PhysicalProperties.asp

Buckyballs are ‘round CNTs’. They have some pentagons amongst their hexagons for curvature. C60 forms quite easily, C36 is a more strained structure.

Page 29: ECE 474: Principles of Electronic Devices · ECE 474: Principles of Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

V.M. Ayres, ECE474, Spring 2011

The smallest possible buckyball endcap is half of the dodecahedral C20, a shape consisting of 12 pentagonal faces and no hexagonal faces. So the smallest CNT diameter dt is about 4 Angstroms.

C20

~4 angstroms