Transcript Document
Spring 2007 PHYS 5830: Condensed Matter Physics
Course Code 2536
Instructor: Dr. Tom N. Oder
Physics 5830: Condensed Matter Physics Course Code 2536
• Dr. Tom N. Oder • WBSH 1016, E-mail: [email protected], • Phone (330) 941-7111 • Website: http://www.ysu.edu/physics/tnoder • Class Website:
www.ysu.edu/physics/tnoder/ S07-PHYS2536 /index.html
• Class Time: 2:00 pm – 3:00 pm MWF, WBSH 2009 • Office Hours: M, W, F 3:00 pm – 4:00 pm.
• Research: (Wide Band Gap) Semiconductors.
Required Texts:
1. R.F. Pierret:
Advanced Semiconductor Fundamentals
, (Second Edition) - Modular Series on Solid-State Devices, Volume VI, Addison-Wesley, 1988.
By
.
2. R. C. Jeager:
Introduction to Microelectronics Fabrication
( 2 nd Edition) - Modular Series on Solid-State Devices, Volume V, Addison-Wesley.
3. S upplemental reference materials will come from archival journal papers selected by the instructor
.
Prerequisite:
Phys. 3704 Modern Physics. [May be waived by instructor].
Course Structure:
Lecture sessions and hands-on laboratory activities.
Course Objectives:
1.
To develop a background knowledge of semiconductor theory sufficient to understand modern semiconductor devices.
2.
To provide students with practical experience in cutting-edge technology related to electronic device fabrication including lithography, thin film deposition and device characterization.
Major Areas to be covered
1. Semiconductor Physics 2. Device Physics 3. Processing and Characterization 1 + 2: Mondays, Wednesdays 3: Fridays
Semiconductor Physics
• Crystals: Structure and Growth.
• Energy Bands • Carriers in Semiconductors • Phonon Spectra and Optical Properties of Semiconductors • Basic Equations for Semiconductor Device Operation
Relevant References: http://ece-www.colorado.edu/~bart/book/book/contents.htm
1. Crystal Structure of Solids What is “Crystal” to the man on the street?
Significance of Semiconductors
•
Computers, palm pilots, laptops,
Silicon (Si) MOSFETs, ICs, CMOS
anything “intelligent”
•
Cell phones, pagers
Si ICs, GaAs FETs, BJTs •
CD players
AlGaAs and InGaP laser diodes, Si photodiodes •
TV remotes, mobile terminals
Light emitting diodes •
Satellite dishes
InGaAs MMICs •
Fiber networks
InGaAsP laser diodes, pin photodiodes •
Traffic signals, car
GaN LEDs ( green , blue )
Taillights
InGaAsP LEDs ( red , amber )
Fundamental Properties of matter
Matter
: - Has mass, occupies space
Mass
– measure of inertia - from Newton’s first law of motion. It is one of the fundamental physical properties.
States of Matter 1. Solids
– Definite volume, definite shape.
2. Liquids
– Definite volume, no fixed shape. Flows.
3. Gases
– No definite volume, no definite shape. Takes the volume and shape of its container.
4. Plasma:
•Regarded as fourth state of matter. No definite volume, no definite shape. Composed of electrically charged particles.
•Fully ionized gas at low density with equal amount of positive and negative charges – net electrically neutral.
•Affected by electric and magnetic fields.
•Plasma is the main state of matter in planetary objects such as stars.
5. Condensate:
•Regarded as fifth state of matter obtained when atoms/molecules are at very low temperature and their motion is halted. •They lose their individual identity and become a different entity.
•Bose-Einstein condensates – Formed by bosons.
•Fermionic condensates – By fermions.
Fermions and Bosons Fermions Bosons Spin Half integral Integral spin Occupancy Only one per state Many allowed Examples electrons, protons, neutrons, quarks, neutrinos photons, 4 He atoms, gluons
Element
– one type of atoms
Compound
– Two or more different atoms chemically joined. Constituent atoms (fixed ratios) can be separated only by chemical means.
Mixture
- Two or more different atoms combined. Constituent atoms (variable ratios) can be separated by physical means.
Solid-State Physics
– branch of physics dealing with solids.
Now replaced by a more general terminology -
Condensed Matter Physics
. To include fluids which in many cases share same concepts and analytical techniques.
STRUCTURE OF SOLIDS
•
Can be classified under several criteria based on atomic arrangements, electrical properties, thermal properties, chemical bonds etc.
•
Using electrical criterion: Conductors, Insulators, Semiconductors
•
Using atomic arrangements: Amorphous, Polycrystalline, Crystalline.
Under what categories could this class be grouped?
Amorphous Solids
•No regular long range order of arrangement in the atoms.
•Eg. Polymers, cotton candy, common window glass, ceramic. •Can be prepared by rapidly cooling molten material. •Rapid – minimizes time for atoms to pack into a more thermodynamically favorable crystalline state. •Two sub-states of amorphous solids: Rubbery and Glassy states. Glass transition temperature T g = temperature above which the solid transforms from glassy to rubbery state, becoming more viscous.
Amorphous Solids Continuous random network structure of atoms in an amorphous solid
Polycrystalline Solids
•
Atomic order present in sections (grains) of the solid.
•
Different order of arrangement from grain to grain. Grain sizes = hundreds of
m.
•
An aggregate of a large number of small crystals or grains in which the structure is regular, but the crystals or grains are arranged in a random fashion.
Polycrystalline Solids
Crystalline Solids Atoms arranged in a 3-D long range order. “Single crystals” emphasizes one type of crystal order that exists as opposed to polycrystals.
Single- Vs Poly- Crystal
• Properties of single crystalline materials vary with direction, ie anisotropic.
•Properties of polycrystalline materials may or may not vary with direction.
If the polycrystal grains are randomly oriented, properties will not vary with direction ie isotropic.
•If the polycrystal grains are textured, properties will vary with direction ie anisotropic
Single- Vs Poly- Crystal
Single- Vs Poly- Crystal
200
m -Properties may/may not vary with direction.
-If grains are randomly oriented: isotropic .
(E poly iron = 210 GPa) -If grains are textured , anisotropic.
Solid state devices employ semiconductor materials in all of the above forms.
Examples: Amorphous silicon (a-Si) used to make thin film transistors (TFTs) used as switching elements in LCDs.
Ploycrystalline Si – Gate materials in MOSFETS.
Active regions of most solid state devices are made of crystalline semiconductors.
Hard Sphere Model of Crystals
•
Assumes atoms are hard spheres with well defined diameters that touch.
•
Atoms are arranged on periodic array – or lattice
•
Repetitive pattern – unit cell defined by lattice parameters sides (
,
,
).
comprising lengths of the 3 sides (a, b, c) and angles between the
Lattice Parameters
a
c
b
Atoms in a Crystal
The Unit Cell Concept
•The simplest repeating unit in a crystal is called a
unit cell
. •Opposite faces of a unit cell are parallel.
•The edge of the unit cell connects equivalent points.
•Not unique. There can be several unit cells of a crystal.
•The smallest possible unit cell is called
primitive unit cell
of a particular crystal structure. •A primitive unit cell whose symmetry matches the lattice symmetry is called
Wigner-Seitz cell
.
• Each unit cell is defined in terms of
lattice points.
•Lattice point not necessarily at an atomic site.
• For each crystal structure, a conventional unit cell, is chosen to make the lattice as symmetric as possible. However, the conventional unit cell is not always the primitive unit cell. •A crystal's structure and symmetry play a role in determining many of its properties, such as cleavage (tendency to split along certain planes with smooth surfaces), electronic band structure and optical properties.
Unit cell
b a
•
Unit cell
: Simplest portion of the structure which is repeated and shows its full symmetry
.
•
Basis vectors a
and
b
defines relationship between a unit cell and (Bravais) lattice points of a crystal.
•Equivalent points of the lattice is defined by translation vector.
r
=
ha
+
kb
where h and k are integers. This constructs the entire lattice.
•
By repeated duplication, a unit cell should reproduce the whole crystal.
•
A Bravias lattice (unit cells) - a set of points constructed by translating a single point in discrete steps by a set of basis vectors.
•
In 3-D, there are 14 unique Bravais lattices. All crystalline materials fit in one of these arrangements.
In 3-D, the translation vector is
r
= ha + kb + lc
Crystal System
•The
crystal system:
Set of rotation and reflection symmetries which leave a lattice point fixed. •There are seven unique crystal systems: the cubic (isometric), hexagonal, tetragonal, rhombohedral (trigonal), orthorhombic, monoclinic and triclinic.
Bravais Lattice and Crystal System
Crystal structure: contains atoms at every lattice point.
•The symmetry of the crystal can be more complicated than the symmetry of the lattice.
•Bravais lattice points do not necessarily correspond to real atomic sites in a crystal. A Bravais lattice point may be used to represent a group of many atoms of a real crystal. This means more ways of arranging atoms in a crystal lattice.
1. Cubic (Isometric) System 3 Bravais lattices
Symmetry elements: Four 3-fold rotation axes along cube diagonals
a = b = c
= = = 90 o
a
c
b
By convention, the edge of a unit cell always connects equivalent points. Each of the eight corners of the unit cell therefore must contain an identical particle.
(1-a): Simple Cubic Structure (SC)
• Rare due to poor packing • Close-packed directions (only Po has this structure) are cube edges.
Coordination # = 6 (# nearest neighbors)
1 atom/unit cell
Coordination Number = Number of nearest neighbors
One atom per unit cell 1/8 x 8 = 1
Atomic Packing Factor
(1-b): Face Centered Cubic Structure (FCC) • Exhibited by Al, Cu, Au, Ag, Ni, Pt • Close packed directions are face diagonals.
• Coordination number = 12 • 4 atoms/unit cell All atoms are identical Adapted from Fig. 3.1(a), Callister 6e.
6 x (1/2 face) + 8 x 1/8 (corner) = 4 atoms/unit cell
FCC Coordination number = 12 3 mutually perpendicular planes.
4 nearest neighbors on each of the three planes.
How is a and R related for an FCC?
[a= unit cell dimension, R = atomic radius].
All atoms are identical
(1-c): Body Centered Cubic Structure (BCC) • Exhibited by Cr, Fe, Mo, Ta, W • Close packed directions are cube diagonals .
• Coordination number = 8 All atoms are identical
2 atoms/unit cell
How is a and R related for an BCC?
[a= unit cell dimension, R = atomic radius].
All atoms are identical
2 atoms/unit cell
Which one has most packing ?
Which one has most packing ?
For that reason, FCC is also referred to as cubic closed packed (CCP)
2. Hexagonal System Only one Bravais lattice
Symmetry element: One 6-fold rotation axis a = b = 120 o = c = 90 o
Hexagonal Closed Packed Structure (HCP) • Exhibited by …. • ABAB... Stacking Sequence • Coordination # = 12 3D Projection A sites B sites A sites Adapted from Fig. 3.3, Callister 6e.
2D Projection
3. Tetragonal System Two Bravais lattices
Symmetry element: One 4-fold rotation axis a = b = = c = 90 o
4. Trigonal (Rhombohedral) System One Bravais lattice
Symmetry element: One 3-fold rotation axis a = b = 120 o = c = 90 o
5. Orthorhombic System Four Bravais lattices
Symmetry element: Three mutually perpendicular 2 fold rotation axes
a
= b
= c
= 90 o
6. Monoclinic System Two Bravais lattices
Symmetry element: One 2-fold rotation axis
a
= b
c = 90 o ,
90 o
7. Triclinic System One Bravais lattice Symmetry element: None a
b
c
90 o
•The
crystal system:
Set of symmetries which leave a lattice point fixed. There are seven unique crystal systems.
• Some symmetries are identified by special name such as zincblende, wurtzite, zinc sulfide etc.
HCP Layer Stacking Sequence A sites B sites A sites = ABAB… = ABCABC..
FCC
FCC: Coordination number FCC Coordination number = 12 3 mutually perpendicular planes.
4 nearest neighbors on each of the three planes.
Diamond Lattice Structure
•
Exhibited by Carbon (C), Silicon (Si)
and
Germanium (Ge).
•Consists of two interpenetrating FCC lattices, displaced along the body diagonal of the cubic cell by 1/4 the length of the diagonal.
• Also regarded as an FCC lattice with two atoms per lattice site: one centered on the lattice site, and the other at a distance of a/4 along all axes, ie an FCC lattice with the two point basis.
Diamond Lattice Structure
a = lattice constant
Diamond Lattice Structure
Two merged FCC cells offset by a/4 in x, y and z.
Basic FCC Cell Merged FCC Cells Omit atoms outside Cell Bonding of Atoms
8 atoms at each corner, 6 atoms on each face, 4 atoms entirely inside the cell
Zinc Blende
•
Similar to the diamond cubic structure except that the two atoms at each lattice site are different.
•
Exhibited by many semiconductors
including ZnS, GaAs, ZnTe and CdTe.
•
GaN and SiC can also crystallize in this structure.
Zinc Blende
Each Zn bonded to 4 Sulfur - tetrahedral Equivalent if Zn and S are reversed Bonding often highly covalent
Zinc sulfide crystallizes in two different forms: Wurtzite and Zinc Blende.
GaAs
Red = Ga-atoms, Blue = As-atoms •
Equal numbers of Ga and As ions distributed on
•
a diamond lattice.
Each atom has 4 of the opposite kind as nearest neighbors.
Wurtzite (Hexagonal) Structure
•
This is the hexagonal analog of the zinc-blende lattice.
•
Can be considered as two interpenetrating close-packed lattices with half of the tetrahedral sites occupied by another kind of atoms.
•
F our equidistant nearest neighbors, similar to a zinc-blende structure.
•
Certain compound semiconductors (ZnS, CdS, SiC) can crystallize in both zinc-blende (cubic) and wurtzite (hexagonal) structure.
WURTZITE A sites B sites A sites
Wurtzite Gallium Nitride (GaN)
Miller Index For Cubic Structures
•
Miller index is used to describe directions and planes in a crystal.
• •
Directions - written as [u v w] where u, v, w.
Integers u, v, w represent coordinates of the vector in real space.
•
A family of directions which are equivalent due to symmetry operations is written as
•
Planes: Written as (h k l).
•
Integers h, k, and l represent the intercept of the
•
plane with x-, y-, and z- axes, respectively.
Equivalent planes represented by {h k l}.
Miller Indices: Directions z x
[1] Draw a vector and take components [2] Reduce to simplest integers [3] Enclose the number in square brackets x y z 0 2a 2a 0 1 1 [0 1 1]
y
Negative Directions
z x
[1] Draw a vector and take components [2] Reduce to simplest integers [3] Enclose the number in square brackets x y z 0 -a 2a 0 -1 2
y
Miller Indices: Equivalent Directions
Equivalent directions due to crystal symmetry:
z
1: 2: 3: [100] [010] [001]
3 y x 2 1
Notation <100> used to denote all directions equivalent to [100]
Directions
The intercepts of a crystal plane with the axis defined by a set of unit vectors are at 2a, -3b and 4c. Find the corresponding Miller indices of this and all other crystal planes parallel to this plane. The Miller indices are obtained in the following three steps: 1. Identify the intersections with the axis, namely 2, -3 and 4.
2. Calculate the inverse of each of those intercepts, resulting in 1/2, -1/3 and 1/4.
3. Find the smallest integers proportional to the inverse of the intercepts. Multiplying each fraction with the product of each of the intercepts (24 = 2 x 3 x 4) does result in integers, but not always the smallest integers. 4. These are obtained in this case by multiplying each fraction by 12.
5. Resulting Miller indices is 6 4 3 6. Negative index indicated by a bar on top.
Miller Indices of Planes
z= z x=a x y= y x y z [1] Determine intercept of plane with each axis a ∞ ∞ [2] Invert the intercept values 1/a 1/ ∞ 1/ ∞ [3] Convert to the smallest integers [4] Enclose the number in round brackets 1 0 0 (1 0 0)
Miller Indices of Planes z y x
x y z [1] Determine intercept of plane with each axis 2a 2a 2a [2] Invert the intercept values 1/2a 1/2a 1/ 2a [3] Convert to the smallest integers [4] Enclose the number in round brackets 1 1 1 (1 1 1)
Planes with Negative Indices z x
[2] Invert the intercept values x y z [1] Determine intercept of plane with each axis a -a a 1/a -1/ a 1/ a [3] Convert to the smallest integers [4] Enclose the number in round brackets 1 -1 -1
y
Equivalent Planes
(100) plane z (001) plane (010) plane y x
• Planes (100), (010), (001), (100), (010), (001) are equivalent planes. Denoted by {1 0 0}.
• Atomic density and arrangement as well as electrical, optical, physical properties are also equivalent.
In the cubic system the (hkl) plane and the vector [hkl] are normal to one another.
This characteristic is unique to the cubic crystal system and does not apply to crystal systems of lower symmetry.
The (110) surface
Assignment
Intercepts :
a
,
a
, Fractional intercepts : 1 , 1 , Miller Indices :
(110)
The (100), (110) and (111) surfaces considered above are the so-called low index surfaces of a cubic crystal system (the "low" refers to the Miller indices being small numbers 0 or 1 in this case).
Crystallographic Planes
Miller Indices (hkl) reciprocals
The (111) surface
Assignment
Intercepts :
a
,
a
,
a
Fractional intercepts : 1 , 1 , 1 Miller Indices :
(111)
The (210) surface
Assignment
Intercepts : ½
a
,
a
, Fractional intercepts : ½ , 1 , Miller Indices :
(210)
Symmetry-equivalent surfaces
the three highlighted surfaces are related by the symmetry elements of the cubic crystal they are entirely equivalent.
In fact there are a total of 6 faces related by the symmetry elements and equivalent to the (100) surface any surface belonging to this set of symmetry related surfaces may be denoted by the more general notation {100} where the Miller indices of one of the surfaces is instead enclosed in curly-brackets.
Angle Between Crystal Directions
Angle ( ) between directions [h 1 of a cubic crystal is: cos( ) (
h
1 2
h
1
h
2
k
1 2
k
1
k
2
l
1
l
2
l
1 2 )(
h
2 2 k
k
2 2 1 l 1 ] and [h
l
2 2 ) 2 k 2 l 2 ]
Miller Index for Hexagonal Crystal System
•Four principal axes used, leading to four Miller Indices: •Directions [h k i l]; Planes (h k i l), e.g. (0001) surface.
•First three axes/indices are related: h + k + i = 0 or i = -h-k.
•Indices
h
,
k
and
l
are identical to the Miller index.
• Rhombohedral crystal system can also be identified with four indices.
Miller Index for Hexagonal System