1. Spring 2007 PHYS 5830: Condensed Matter Physics Course Code 2536 Instructor: Dr. Tom N. Oder

2. Dr. Tom N. Oder WBSH 1016, E-mail: tnoder@ysu.edu, 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. Physics 5830: Condensed Matter Physics Course Code 2536

3. 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].

4. 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.

5. 1.Semiconductor Physics 2.Device Physics 3.Processing and Characterization 1 + 2: Mondays, Wednesdays 3: Fridays Major Areas to be covered

6. Crystals: Structure and Growth. Energy Bands Carriers in Semiconductors Phonon Spectra and Optical Properties of Semiconductors Basic Equations for Semiconductor Device Operation Semiconductor Physics

7. Relevant References: http://ece-www.colorado.edu/~bart/book/book/contents.htm

8. 1.Crystal Structure of Solids What is “Crystal” to the man on the street?

9. 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) Significance of Semiconductors

10. Fundamental Properties of matter 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. Matter: - Has mass, occupies space Mass – measure of inertia - from Newton’s first law of motion. It is one of the fundamental physical properties.

11. 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. 4. Plasma:

12. 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. 5. Condensate:

13. SpinOccupancyExamples FermionsHalf integral Only one per state electrons, protons, neutrons, quarks, neutrinos BosonsIntegral spin Many allowed photons, 4 He atoms, gluons Fermions and Bosons

14. 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.

15. 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.

16. Under what categories could this class be grouped?

17. 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

18. Continuous random network structure of atoms in an amorphous solid Amorphous Solids

19. 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

21. Atoms arranged in a 3-D long range order. “Single crystals” emphasizes one type of crystal order that exists as opposed to polycrystals. Crystalline Solids

22. 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

24. -Properties may/may not vary with direction. -If grains are randomly oriented: isotropic. (E poly iron = 210 GPa) -If grains are textured, anisotropic. 200  m Single- Vs Poly- Crystal

25. 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.

26. 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 comprising lengths of the 3 sides (a, b, c) and angles between the sides ( , ,  ). Hard Sphere Model of Crystals

27. a b c    Lattice Parameters

28. Atoms in a Crystal

29. 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.

30. 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.

31. Unit cell

32. 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. a b

33. 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

34. 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. Crystal System

35. 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.

37. 1. Cubic (Isometric) System Symmetry elements: Four 3-fold rotation axes along cube diagonals a = b = c  =  =  = 90 o 3 Bravais lattices a b c   

38. 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.

39. Rare due to poor packing (only Po has this structure) Close-packed directions are cube edges. Coordination # = 6 (# nearest neighbors) 1 atom/unit cell (1-a): Simple Cubic Structure (SC)

40. Coordination Number = Number of nearest neighbors

41. One atom per unit cell 1/8 x 8 = 1

42. Atomic Packing Factor

43. Adapted from Fig. 3.1(a), Callister 6e. Exhibited by Al, Cu, Au, Ag, Ni, Pt Close packed directions are face diagonals. Coordination number = 12 4 atoms/unit cell 6 x (1/2 face) + 8 x 1/8 (corner) = 4 atoms/unit cell (1-b): Face Centered Cubic Structure (FCC) All atoms are identical

44. FCC Coordination number = 12 3 mutually perpendicular planes. 4 nearest neighbors on each of the three planes.

45. How is a and R related for an FCC? [a= unit cell dimension, R = atomic radius]. All atoms are identical

46. Exhibited by Cr, Fe, Mo, Ta, W Close packed directions are cube diagonals. Coordination number = 8 2 atoms/unit cell (1-c): Body Centered Cubic Structure (BCC) All atoms are identical

47. 2 atoms/unit cell All atoms are identical How is a and R related for an BCC? [a= unit cell dimension, R = atomic radius].

48. Which one has most packing ?

49. For that reason, FCC is also referred to as cubic closed packed (CCP)

50. Symmetry element: One 6-fold rotation axis a = b  c  = 120 o  =  = 90 o 2. Hexagonal System Only one Bravais lattice

51. Exhibited by …. ABAB... Stacking Sequence Coordination # = 12 3D Projection 2D Projection Adapted from Fig. 3.3, Callister 6e. Hexagonal Closed Packed Structure (HCP)

52. Symmetry element: One 4-fold rotation axis a = b  c  =  =  = 90 o 3. Tetragonal System Two Bravais lattices

53. Symmetry element: One 3-fold rotation axis a = b  c  = 120 o  =  = 90 o 4. Trigonal (Rhombohedral) System One Bravais lattice

54. 5. Orthorhombic System Symmetry element: Three mutually perpendicular 2- fold rotation axes a  b  c  =  =  = 90 o Four Bravais lattices

55. 6. Monoclinic System Symmetry element: One 2-fold rotation axis a  b  c  =  = 90 o,   90 o Two Bravais lattices

56. 7. Triclinic System Symmetry element: None a  b  c       90 o One Bravais lattice

57. 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.

58. HCP FCC Layer Stacking Sequence = ABCABC.. = ABAB…

59. FCC Coordination number = 12 3 mutually perpendicular planes. 4 nearest neighbors on each of the three planes. FCC: Coordination number

60. 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

61. a = lattice constant Diamond Lattice Structure

63. 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

64. 8 atoms at each corner, 6 atoms on each face, 4 atoms entirely inside the cell

65. 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

66. Each Zn bonded to 4 Sulfur - tetrahedral Equivalent if Zn and S are reversed Bonding often highly covalent

67. Zinc sulfide crystallizes in two different forms: Wurtzite and Zinc Blende.

68. GaAs Equal numbers of Ga and As ions distributed on a diamond lattice. Each atom has 4 of the opposite kind as nearest neighbors. Red = Ga-atoms, Blue = As-atoms

69. 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. Four 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.

70. WURTZITE

71. Wurtzite Gallium Nitride (GaN)

72. 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 Index For Cubic Structures

73. x y z [1] Draw a vector and take components0 2a 2a [2] Reduce to simplest integers0 1 1 [3] Enclose the number in square brackets [0 1 1] z y x Miller Indices: Directions

74. z y x x y z [1] Draw a vector and take components0 -a 2a [2] Reduce to simplest integers0 -1 2 [3] Enclose the number in square brackets Negative Directions

75. Miller Indices: Equivalent Directions z y x 1 2 3 1:[100] 2:[010] 3:[001] Equivalent directions due to crystal symmetry: Notation used to denote all directions equivalent to [100]

76. Directions

77. 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.Negative index indicated by a bar on top.

78. z y x z=  y=  x=a 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 integers1 0 0 [4] Enclose the number in round brackets (1 0 0) Miller Indices of Planes

79. 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 integers1 1 1 [4] Enclose the number in round brackets (1 1 1) Miller Indices of Planes

80. z y x Planes with Negative Indices x y z [1] Determine intercept of plane with each axis a -a a [2] Invert the intercept values 1/a -1/ a 1/ a [3] Convert to the smallest integers1 -1 -1 [4] Enclose the number in round brackets

81. 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. z y x (100) plane (010) plane (001) plane Equivalent Planes

83. 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.

84. 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).

85. Miller Indices (hkl) reciprocals Crystallographic Planes

86. 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)

87. 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.

88. Angle (  ) between directions [h 1 k 1 l 1 ] and [h 2 k 2 l 2 ] of a cubic crystal is: Angle Between Crystal Directions

89. 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 Crystal System

90. Miller Index for Hexagonal System