《半導(dǎo)體簡(jiǎn)介》PPT課件.ppt

1、Technical English,2020/9/15,Introduction to Semiconductors,New words,conductor導(dǎo)體 insulator絕緣體 crystalline晶體的 valency化合價(jià) bond結(jié)合 covalent共價(jià)的 DNA 脫氧核糖核酸 deoxyribonucleic acid,2,molecule 分子 solder焊料, 焊接 polymorphic form 多晶型物 atom 原子 intrinsic固有的, 本質(zhì)的 doping (半導(dǎo)體)摻雜(質(zhì)) dopant 摻雜物, 摻雜劑 minuscule極小的 hole 空

2、穴,3,本節(jié)中用到的幾種化學(xué)元素（物質(zhì)）名稱：,germanium 鍺 silicon硅 tin 錫 boron 硼 selenium 硒 arsenic 砷 tellurium 碲 antimony 銻 arsenide 砷化物 gallium鎵,4,Text part 1,Semiconductors are materials that exhibit properties that are between a metal and a non-metal. Their electrical properties are part way between a conductor and a

3、n insulatorthus they are called “semi-conductors”. (Actually they are much closer to insulators than conductors.) A number of materials have these properties: The crystalline forms of most elements of Group IV (valency 4) (silicon1, germanium, tin).,5, Some forms of specific elementsboron (Group III

4、), arsenic and antimony (Group V), selenium and tellurium (Group VI). Crystalline alloys of elements in Group III (valency 3) with elements of group V (valency 5). Gallium arsenide (a compound or alloy of gallium and arsenic) is a good example here. Some compounds of elements of Group VI with elemen

5、ts of Group II.,6,Probably the most versatile elements are those with four electrons in their outer shell (Group IV: carbon, silicon, germanium, tin, lead). Because of the fact that they can have four bonds to four other elements, covalent compounds of endless complexity can be formed. (Indeed DNA i

6、s a single carbon-based molecule.) All of these elements can exist in multiple physical forms. Carbon can take many forms such as graphite (a form a bit like a classical metal) which conducts electricity very well or diamond (a crystalline form) which is an insulator.,7,Almost anyone who has ever so

7、ldered an electrical connection knows the difference between a good soldered joint (where the metal solidifies in a polymorphic form) and a “dry joint” where the solder crystallizes.2 Polymorphic solder is a very good electrical conductor. Solder (an alloy of lead and tin) in its crystalline form is

8、 a semiconductor!,8,In fact carbon is not classified by chemists as a semiconductor even though diamond does semiconduct at relatively high temperatures (well above room temperature). The technical reason is that carbon has very strong molecular bonds which do not break down very easily (the energy

9、“gap” between the valence band and the conduction band is greater than that provided by ambient heat at room temperature.) It would be somewhat difficult in practice to use carbon as a basis for semiconductor electronics since it is hard to grow large, extremely pure diamonds to cut up and use as ch

10、ips!,9,A major difference between semiconductors and conductors is their electrical behavior at different temperatures. In general, when you heat up a semiconductor its resistance to the flow of electricity decreases (or its conductance increases). In metals the opposite happens. As the tempe- ratur

11、e of a metal increases then its resistance also increases (or conductance decreases).,10,Today silicon is the most commonly used semiconductor although germanium was used almost exclusively in early (1950s) solid state devices. Silicon (like most elements) can take a number of physical forms. It res

12、embles a metal in its electrical conductivity properties. Crystalline silicon is the base for almost all semiconductors today.,11,12,Figure 1 Silicon crystal lattice,A silicon crystal lattice is illustrated in Figure 1. Each silicon atom is bonded to four other silicon atoms with covalent bonds. Not

13、e that although the picture is two-dimensional the crystal structure is (of course) three dimensional. A perfect silicon crystal (at a temperature near absolute zero) has no free electrons and thus cannot conduct electricity. A pure silicon crystal at any tempe- rature above absolute zero will have

14、some bonds broken by the random action of heat and so there will be some free electrons in the structure and you will get some conduction.,13,In addition to using pure silicon or germanium you can also use crystals made of almost any alloy of elements in Group III (with three electrons in their oute

15、r shell) with elements in Group V (with five electrons in their outer shell). The best known material used in this way is gallium arsenide although there are many others.,14,Electrical Conduction in an Intrinsic Semiconductor An “intrinsic” semiconductor is a uniform material that can act as a semic

16、onductor without the need to introduce anomalies in the structure by doping. Pure crystals of silicon, germanium and gallium arsenide are intrinsic semiconductors at room temperature.,15,Dopants,Semiconductors dont get very interesting (or useful) until you introduce dopants. A dopant is a very smal

17、l (indeed minuscule) amount of a controlled impurity introduced into the crystalline structure. The presence of the dopant is responsible for the properties of the semiconductor. Figure 2(left) shows a silicon crystal lattice doped with boron. Boron has three electrons in its outer shell. The regula

18、r crystalline structure remains but now there is a “hole” in it. A boron atom takes the place of a silicon atom in the structure. The structure is too strong to be changed by the single impurity atom and thus we have a missing bond in the structure.,16,Figure 2(right) shows a silicon crystal doped with phosphorus. Phosphorus has five electrons in its outer shell. Here the same thing happens as with boron except that we now have an electron too many rather than an electron too few as far as the lattice is concerned. The crystal structure is too s