Lecture #10 Electrons, Atoms, and Materials Reading: Malvino chapter 2 (semiconductors) 9/22/2004 EE 42 fall 2004 lecture 10 1 Electrons • Electrons are not point particles • Can think of them like a vibrating jelly • Electrons take spatial shapes sometime known as orbitals—would have been better to call them states or modes • Only one electron of each of two types can be in the same mode (the types are called spin up and spin down) • This is called Fermi exclusion 9/22/2004 EE 42 fall 2004 lecture 10 2 Here is what some of the orbitals look like: 9/22/2004 EE 42 fall 2004 lecture 10 3 Occupation • Atomic nuclei have varying numbers of protons in them, which have a positive charge which has the same magnitude as that on the electron. • A nuclei will attract electrons to it until it becomes neutral, filling the electronic states around it, making an atom. 9/22/2004 EE 42 fall 2004 lecture 10 4 • Since only two electrons can be in each spatial state, they fill up the orbitals in order. • Lowest energy state first: 1S (spherical) • One proton→one electron Hydrogen • Two protons→two electrons Helium 9/22/2004 EE 42 fall 2004 lecture 10 5 Chemistry • Interactions of electrons in orbitals is what we call chemistry • The chemical reactions which a atom takes part in are determined by the outer orbitals. • Because the inner orbitals are all full, and that keeps out other electrons like a shield. 9/22/2004 EE 42 fall 2004 lecture 10 6 Filling of orbitals 1s 2s 2p 3s 3p 3d 4s 4p 4d 4f 5s 5p 5d 5f 6s 6p 6d 9/22/2004 The orbitals fill up in the order shown (simplified a bit) Since the p, d, f orbitals have similar shapes and they get filled up in sequence, we get a periodicity in the chemical properties, giving us the periodic table EE 42 fall 2004 lecture 10 7 Periodic table The number in each element’s box is the atomic number, which is the number of protons, and consequently the number of electrons needed for neutrality 9/22/2004 EE 42 fall 2004 lecture 10 8 Bonding • “Bonding” is due to the fact that when two atoms are close together, the outer orbitals are wrapped around both of the nuclei, and the electons are in these “shared” orbitals. • These orbitals can have lower energy than those of the two atoms would have if they were farther away from each other. • Since the energy decreases as the atoms get close together, this provides a bonding force • The shared electrons act like glue! 9/22/2004 EE 42 fall 2004 lecture 10 9 Column 4 of the periodic table IV 9/22/2004 EE 42 fall 2004 lecture 10 10 Orbitals • The periodic table can be understood by the following • The single S orbital can hold 2 electrons • The three P orbitals can hold 6 electrons • If the orbitals are all full, the atom does not share and play well with friends. (Neon) • While the other orbitals are filling, we get a whole bunch of different metals. 9/22/2004 EE 42 fall 2004 lecture 10 11 Silicon • The elements of column four of the periodic table can bond with each other in a regular structure (crystallize) • each atom bonded to the four nearest neighbors 9/22/2004 EE 42 fall 2004 lecture 10 12 Silicon structure and bonding • There are four nearest neighbors, four orbitals to share, and 4 electrons to contribute • Since each neighbor contributes one electron for each orbital, the orbitals are all full and the lattice is strong and stable • Carbon in this form is called Diamond 9/22/2004 EE 42 fall 2004 lecture 10 13 TEM picture of silicon 9/22/2004 EE 42 fall 2004 lecture 10 14 Semiconductor • Interestingly enough, even though this electronic glue is everywhere in the crystal, they can not contribute to current because they are locked into this pattern. • These electrons are said to be in the “valence band” • If there were a few extra electrons, they could wander about. • How do we get extra electrons into our crystal? 9/22/2004 EE 42 fall 2004 lecture 10 15 Column 5 of the periodic table V If we look at column 5 of the periodic table, we can see that these elements are very similar to silicon, except that they have one extra proton—an extra quantum of positive charge. 9/22/2004 EE 42 fall 2004 lecture 10 16 • So a column 5 element substituted for a silicon atom results in what looks like a silicon crystal but which has a fixed postive charge. • This is called “doping” the silicon with Arsenic or phosphorus. • If the crystal is to be electrically neutral, then there will be a mobile electron, called a conduction band electron, hanging around. 9/22/2004 EE 42 fall 2004 lecture 10 17 N type silicon • So if we take a silicon crystal, and add a very small amount of atoms of arsenic or phosphorous to it, then it will have extra electrons which can wander around. • Since these extra electrons can move, they can conduct a current • This is called N type because the carriers that can move are negative. • They are at a higher energy than they could have if they could fall down into a bond • Electrons which can wander around above a full set of orbitals are said to be in the “conduction band” 9/22/2004 EE 42 fall 2004 lecture 10 18 P type But wait a minute: the electrons are always what moves through a crystal, and they are always negative! • Lets look at what happens if we put a few atoms from column 3 of the periodic table into the crystal 9/22/2004 EE 42 fall 2004 lecture 10 19 Column 3 of the periodic table III If we look at column 3 of the periodic table, we can see that these elements are very similar to silicon, except that they have one fewer protons—one less quantum of positive charge. 9/22/2004 EE 42 fall 2004 lecture 10 20 P type semiconductors • If we have a silicon crystal with a few Boron, Aluminum, or Gallium atoms in it, then a few orbitals will be missing an electron. • Other electrons can hop into that orbital • Since the electrons can now move, the crystal can conduct an electrical current • Since it is an unoccupied orbital that is moving, it is called a “Hole” • It moves like a positively charged particle would. 9/22/2004 EE 42 fall 2004 lecture 10 21 Electrons and Holes • If you were to have both electrons and holes in the crystal, the electrons could fill up the holes until one or the other was depleted. • Silicon crystals with quite a few extra electrons running around are called N-type, and they only have a few holes in the valence band. • Silicon crystals with many holes running around are called P-type, and they only have a few electrons in the conduction band. 9/22/2004 EE 42 fall 2004 lecture 10 22 Applications • We can take silicon wafers and put patterns of doping on their surface, and control its conductivity. • We can further control the conductivity by applying electric fields • We can make use of the difference between P and N type carriers moving through the crystal. • This ability to control the conduction of silicon is the basis for the function of transistors, the foundation of the entire electronics industry 9/22/2004 EE 42 fall 2004 lecture 10 23