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Display device basic microfabrication techniques

Категория: Информатика

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Microfabrication is the process of fabricating miniature structures of micrometre scales and smaller. Historically, the earliest microfabrication processes were used for integrated circuit fabrication, also known as "semiconductor manufacturing" or "semiconductor device fabrication". In the last two decades microelectromechanical systems (MEMS), microsystems (European usage), micromachines (Japanese terminology) and their subfields, microfluidics/lab-on-a-chip, optical MEMS (also called MOEMS), RF MEMS, PowerMEMS, BioMEMS and their extension into nanoscale (for example NEMS, for nano electro mechanical systems) have re-used, adapted or extended microfabrication methods. Flat-panel displays and solar cells are also using similar techniques.

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«Display device basic microfabrication techniques»

Lecture7  Basic Fabrication Techniques Author of presentation Ivanova Elvira

Lecture7 Basic Fabrication Techniques

Author of presentation

Ivanova Elvira

Basic Fabrication Techniques

Basic Fabrication Techniques

 Doping  In  semiconductor  production,  doping  intentionally introduces impurities into an extremely pure  intrinsic  semiconductor  for the purpose of modulating its electrical properties. The impurities are dependent upon the type of semiconductor and the properties that it needs to have for its intended purpose. Lightly and moderately doped semiconductors are referred to as  extrinsic  semiconductors .

Doping

In  semiconductor  production,  doping  intentionally introduces impurities into an extremely pure  intrinsic semiconductor  for the purpose of modulating its electrical properties. The impurities are dependent upon the type of semiconductor and the properties that it needs to have for its intended purpose. Lightly and moderately doped semiconductors are referred to as  extrinsic semiconductors .

 Doping  A semiconductor doped to such high levels that it acts more like a  conductor  than a semiconductor is referred to as a  degenerate  semiconductor . In the context of  phosphors  and  scintillators , doping is better known as  activation .

Doping

A semiconductor doped to such high levels that it acts more like a  conductor  than a semiconductor is referred to as a  degenerate semiconductor .

  • In the context of  phosphors  and  scintillators , doping is better known as  activation .
 Doping The techniques used to make all the semiconductor devices have many features in common, whether these be diodes, transistors, four-layer controlled rectifiers, or other devices. For this reason, the processes employed to fabricate transistors are of general application.  To achieve as large a current gain as possible within a transistor, the lifetime of the majority-charge carrier, in the base region, must be relatively long before recombination of a hole-electron pair takes place. This requires that the transistor be made from a single crystal of high quality. At the same time, to obtain other desirable transistor properties, the impurity content of the crystal must be accurately controlled. This is best achieved by refining the semiconductor material to maximum possible purity, and then adding impurities under carefully specified conditions through one of the available doping techniques.

Doping

  • The techniques used to make all the semiconductor devices have many features in common, whether these be diodes, transistors, four-layer controlled rectifiers, or other devices. For this reason, the processes employed to fabricate transistors are of general application.
  • To achieve as large a current gain as possible within a transistor, the lifetime of the majority-charge carrier, in the base region, must be relatively long before recombination of a hole-electron pair takes place. This requires that the transistor be made from a single crystal of high quality. At the same time, to obtain other desirable transistor properties, the impurity content of the crystal must be accurately controlled. This is best achieved by refining the semiconductor material to maximum possible purity, and then adding impurities under carefully specified conditions through one of the available doping techniques.
 Alloying An  alloy  is a mixture of  metals  or a mixture of a metal and another  element . Alloys are defined by metallic bonding character. In the manufacture of a germanium-alloyed transistor, an n-type crystal is usually cut into small wafers two millimetres square and 0.1mm thick. When the indium melts, it dissolves a small amount of the germanium base and then, as the structure cools, the germanium recrystallizes, but it now contains some indium in the crystal structure, giving a p-type region.

Alloying

  • An  alloy  is a mixture of  metals  or a mixture of a metal and another element . Alloys are defined by metallic bonding character.
  • In the manufacture of a germanium-alloyed transistor, an n-type crystal is usually cut into small wafers two millimetres square and 0.1mm thick. When the indium melts, it dissolves a small amount of the germanium base and then, as the structure cools, the germanium recrystallizes, but it now contains some indium in the crystal structure, giving a p-type region.
 Alloying The alloying process is repeated on the other side of the base crystal to obtain the required two-junction structure. Contacts are soldered to the n-type base region and to the collector and emitter pellets. To minimize the base resistance the base contact is often in the form of a ring around the emitter. Since most of the power is developed at the collector, this part of the transistor is made physically larger than the emitter. It is difficult to alloy into a wafer of a thickness of less than 0.05mm and extremely difficult to make alloyed-junction transistors with a base width narrower than 0.025mm consistently. Also, the alloying process produces only a poorly defined boundary for the p-n junction. This results in a usable upper frequency limit of about ten megahertz for germanium-alloyed transistors. This technique has been superseded for the most part by other doping methods.

Alloying

  • The alloying process is repeated on the other side of the base crystal to obtain the required two-junction structure. Contacts are soldered to the n-type base region and to the collector and emitter pellets. To minimize the base resistance the base contact is often in the form of a ring around the emitter. Since most of the power is developed at the collector, this part of the transistor is made physically larger than the emitter.
  • It is difficult to alloy into a wafer of a thickness of less than 0.05mm and extremely difficult to make alloyed-junction transistors with a base width narrower than 0.025mm consistently. Also, the alloying process produces only a poorly defined boundary for the p-n junction. This results in a usable upper frequency limit of about ten megahertz for germanium-alloyed transistors. This technique has been superseded for the most part by other doping methods.
 Diffusion Diffusion  is the net movement of molecules or atoms from a region of high concentration to a region of low concentration. This is also referred to as the movement of a substance down a  concentration  gradient . A gradient  is the change in the value of a quantity (e.g., concentration, pressure ,  temperature ) with the change in another variable (usually distance ). For example, a change in concentration over a distance is called a concentration gradient, a change in pressure over a distance is called a  pressure  gradient , and a change in temperature over a distance is a called a  temperature  gradient .

Diffusion

  • Diffusion  is the net movement of molecules or atoms from a region of high concentration to a region of low concentration. This is also referred to as the movement of a substance down a  concentration gradient . A gradient  is the change in the value of a quantity (e.g., concentration, pressure ,  temperature ) with the change in another variable (usually distance ). For example, a change in concentration over a distance is called a concentration gradient, a change in pressure over a distance is called a  pressure gradient , and a change in temperature over a distance is a called a  temperature gradient .
 Ion implantation   Ion implantation  is a  materials  engineering  process by which  ions  of a material are accelerated in an electrical field and impacted into a solid. This process is used to change the physical, chemical, or electrical properties of the solid. Ion implantation is used in semiconductor  device  fabrication  and in metal finishing, as well as various applications in  materials  science  research. The ions alter the elemental composition of the target (if the ions differ in composition from the target), stopping in the target and staying there. 

Ion implantation

  • Ion implantation  is a  materials engineering  process by which  ions  of a material are accelerated in an electrical field and impacted into a solid. This process is used to change the physical, chemical, or electrical properties of the solid. Ion implantation is used in semiconductor device fabrication  and in metal finishing, as well as various applications in  materials science  research. The ions alter the elemental composition of the target (if the ions differ in composition from the target), stopping in the target and staying there. 
 Ion implantation They also cause many chemical and physical changes in the target by transferring their energy and momentum to the electrons and atomic nuclei of the target material. This causes a structural change, in that the  crystal  structure  of the target can be damaged or even destroyed by the energetic  collision  cascades . Because the  ions  have masses comparable to those of the target atoms, they knock the target atoms out of place more than electron beams do. If the ion energy is sufficiently high (usually tens of MeV) to overcome the  coulomb  barrier , there can even be a small amount of nuclear transmutation.

Ion implantation

  • They also cause many chemical and physical changes in the target by transferring their energy and momentum to the electrons and atomic nuclei of the target material. This causes a structural change, in that the  crystal structure  of the target can be damaged or even destroyed by the energetic  collision cascades . Because the  ions  have masses comparable to those of the target atoms, they knock the target atoms out of place more than electron beams do. If the ion energy is sufficiently high (usually tens of MeV) to overcome the  coulomb barrier , there can even be a small amount of nuclear transmutation.
 Etching   Etching  is used in microfabrication to chemically remove layers from the surface of a  wafer  during manufacturing. Etching is a critically important process module, and every wafer undergoes many etching steps before it is complete. For many etch steps, part of the wafer is protected from the etchant by a

Etching

  • Etching  is used in microfabrication to chemically remove layers from the surface of a  wafer  during manufacturing. Etching is a critically important process module, and every wafer undergoes many etching steps before it is complete.
  • For many etch steps, part of the wafer is protected from the etchant by a "masking" material which resists etching. In some cases, the masking material is a photoresist which has been patterned usingphotolithography. Other situations require a more durable mask, such as silicon nitride.


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