Types of Semiconductor Materials | Intrinsic & Extrinsic Semiconductor | Engineering Funda

Engineering Funda
10 Aug 202312:23

Summary

TLDRThis engineering video delves into semiconductor materials, distinguishing between intrinsic and extrinsic types. Intrinsic semiconductors, like pure silicon, have low conductivity due to a lack of free charge carriers, but their conductivity increases with temperature as electron-hole pairs are generated. Extrinsic semiconductors, in contrast, have higher conductivity due to added impurities. N-type materials are doped with pentavalent impurities, introducing extra electrons, while P-type materials incorporate trivalent impurities, creating holes. The video explains how these impurities define the number of free electrons and holes, affecting the material's conductivity and temperature coefficient.

Takeaways

  • πŸ˜€ Semiconductor materials are categorized into intrinsic and extrinsic types, with the former being pure and the latter having added impurities.
  • πŸ” Intrinsic semiconductors, such as pure silicon, have lower conductivity due to the absence of free charge carriers, as all electrons are involved in covalent bonds.
  • 🌑️ The conductivity of intrinsic semiconductors increases with temperature because thermal energy can break covalent bonds, generating electron-hole pairs.
  • ⬇️ Intrinsic semiconductors exhibit a negative temperature coefficient, meaning their resistivity decreases as temperature increases due to the generation of more free charge carriers.
  • πŸ”‹ Examples of intrinsic semiconductor materials include silicon and germanium, which are widely used in electronic devices like chips.
  • πŸ“ˆ Extrinsic semiconductors have higher conductivity than intrinsic ones because impurities introduce additional free charge carriers.
  • πŸ”¬ N-type semiconductors are created by adding pentavalent impurities like phosphorus, which donate free electrons, increasing conductivity.
  • πŸ”§ P-type semiconductors are formed by introducing trivalent impurities like aluminum, which create vacancies or holes that act as free charge carriers.
  • 🏭 Both n-type and p-type semiconductors are used in various electronic applications, with n-type materials having electrons as majority carriers and p-type having holes as majority carriers.
  • βš™οΈ Covalent bonds in semiconductors can be broken not only by increasing temperature but also by applying a high potential difference or a strong electric field, leading to the generation of electron-hole pairs.

Q & A

  • What are the three categories of solid materials mentioned in the script?

    -The three categories of solid materials mentioned are conductors, semiconductors, and insulators.

  • What is an intrinsic semiconductor material?

    -An intrinsic semiconductor material is a pure semiconductor material with no impurities added, such as pure silicon or germanium.

  • How does the conductivity of intrinsic semiconductor materials compare to extrinsic semiconductor materials?

    -Intrinsic semiconductor materials have lower conductivity compared to extrinsic semiconductor materials because they do not have additional free charge carriers.

  • What happens to the conductivity of intrinsic semiconductors when the temperature increases?

    -As the temperature increases, electron-hole pairs are generated, which increases the number of free charge carriers and thus increases the conductivity.

  • What is the term for the phenomenon where resistivity decreases with an increase in temperature in intrinsic semiconductors?

    -The phenomenon where resistivity decreases with an increase in temperature is called a negative temperature coefficient.

  • What are the two basic types of extrinsic semiconductor materials?

    -The two basic types of extrinsic semiconductor materials are n-type and p-type.

  • Which impurities are added to create n-type semiconductor material, and why?

    -Pentavalent impurities, such as phosphorus or arsenic, are added to create n-type semiconductor material because they have five electrons in their outer orbit, which results in an extra free electron and thus increases conductivity.

  • How do trivalent impurities contribute to the formation of p-type semiconductor material?

    -Trivalent impurities, such as aluminum or boron, contribute to the formation of p-type semiconductor material by creating vacancies or holes in the electron structure, which increases the number of free holes and conductivity.

  • What is the term for impurities that add free electrons in n-type semiconductors?

    -The term for impurities that add free electrons in n-type semiconductors is 'donor impurities' because they donate an extra electron.

  • What is the term for impurities that add free holes in p-type semiconductors?

    -The term for impurities that add free holes in p-type semiconductors is 'acceptor impurities' because they accept an electron, creating a hole.

  • What are the three ways mentioned in the script to generate electron-hole pairs in semiconductor materials?

    -The three ways to generate electron-hole pairs in semiconductor materials are by increasing temperature, applying a higher potential difference across the material, or applying a higher electric field through the material.

Outlines

00:00

πŸ”¬ Introduction to Semiconductor Materials

The paragraph introduces the topic of semiconductor materials, contrasting them with conductors and insulators. It explains that semiconductors can be classified into intrinsic and extrinsic types. Intrinsic semiconductors are pure, without added impurities, and have lower conductivity compared to extrinsic semiconductors, which have impurities added to increase their conductivity. The concept of energy bands in materials is referenced, and the role of temperature in generating free charge carriers in intrinsic semiconductors is discussed. Silicon is given as an example of an intrinsic semiconductor material, with its four electrons in the outer orbit forming covalent bonds with neighboring atoms, resulting in no free charge carriers at 0 Kelvin. As temperature increases, electron-hole pairs are generated, which can increase conductivity. The negative temperature coefficient of intrinsic semiconductors is highlighted, meaning that as temperature rises, resistivity decreases due to the generation of more free charge carriers.

05:02

🌐 Extrinsic Semiconductor Materials and Conductivity

This paragraph delves into extrinsic semiconductor materials, which are created by adding impurities to pure semiconductors, resulting in higher conductivity. The unit of measurement for impurities, parts per million (PPM), is introduced. The paragraph explains the difference between n-type and p-type semiconductors. N-type materials have pentavalent impurities added, which contribute an extra electron, making them donor impurities and increasing the number of free electrons, thus enhancing conductivity. Examples of n-type impurities are phosphorus and arsenic. On the other hand, p-type materials have trivalent impurities added, which create vacancies or holes, making them acceptor impurities. Aluminum and boron are cited as examples of p-type impurities. The paragraph also discusses how the majority charge carriers in n-type materials are electrons, while in p-type materials, they are holes. The effect of temperature on the generation of electron-hole pairs is also mentioned, as well as the fact that the majority carriers in extrinsic semiconductors are determined by the type of impurity added.

10:02

πŸ”© Understanding P-Type Semiconductor Materials

The final paragraph focuses on p-type semiconductor materials, which are formed by adding trivalent impurities with three electrons in their outer orbit. This addition results in the creation of holes or vacancies in the electron structure, which are referred to as acceptor impurities because they can accept electrons. The paragraph explains that these holes are the majority charge carriers in p-type materials, while electrons are the minority carriers. The process of how covalent bonds can be broken, leading to the generation of electron-hole pairs, is discussed in three scenarios: increasing temperature, applying a higher potential difference, or applying a higher electric field. The paragraph concludes by summarizing the basics of semiconductor materials and inviting viewers to ask questions or share comments for further clarification.

Mindmap

Keywords

πŸ’‘Semiconductor

A semiconductor is a material that lies between a conductor and an insulator in terms of its electrical conductivity. It can control the flow of electrical current. In the video, semiconductors are the central theme, with the speaker explaining how they are classified into intrinsic and extrinsic types, and how they function at different temperatures.

πŸ’‘Intrinsic Semiconductor

An intrinsic semiconductor is a pure form of semiconductor material, such as silicon or germanium, that does not have any impurities added. It is characterized by having a lower conductivity compared to extrinsic semiconductors. In the video, the speaker explains that in intrinsic semiconductors, all electrons are involved in covalent bonds, resulting in no free charge carriers at 0 Kelvin, which is why their conductivity is initially low.

πŸ’‘Extrinsic Semiconductor

Extrinsic semiconductors are materials where impurities are intentionally added to a pure semiconductor to modify its electrical properties. This addition of impurities increases the material's conductivity. The video discusses how extrinsic semiconductors are created by adding either n-type or p-type impurities to the base semiconductor material.

πŸ’‘Covalent Bonds

Covalent bonds are a type of chemical bond formed by the sharing of electron pairs between atoms. In the context of the video, covalent bonds are crucial in intrinsic semiconductors, where all electrons are involved in such bonds, leaving no free charge carriers. The speaker illustrates how breaking these bonds, such as by increasing temperature, can generate free electrons and holes, thus increasing conductivity.

πŸ’‘Electron-Hole Pair

An electron-hole pair refers to a free electron and the positively charged vacancy it leaves behind in a semiconductor material. When a covalent bond breaks, an electron can become free, creating a hole. The video explains that at 0 Kelvin, there are no free charge carriers, but as temperature increases, electron-hole pairs are generated, which is crucial for the conductivity of intrinsic semiconductors.

πŸ’‘Negative Temperature Coefficient

The negative temperature coefficient refers to the property of a material where its resistivity decreases as the temperature increases. This is discussed in the video in relation to intrinsic semiconductors, where the generation of electron-hole pairs with rising temperature leads to an increase in free charge carriers, thus reducing resistivity.

πŸ’‘N-Type Semiconductor

An n-type semiconductor is created by adding pentavalent impurities, such as phosphorus, to a semiconductor material. This results in an excess of free electrons, making electrons the majority charge carriers. The video explains that these impurities donate extra electrons, hence the term 'donor impurity,' and increase the material's conductivity.

πŸ’‘P-Type Semiconductor

A p-type semiconductor is formed by adding trivalent impurities, such as aluminum or boron, to a semiconductor material. This creates an excess of holes, making holes the majority charge carriers. The video describes these impurities as 'acceptor impurities' because they accept electrons, leading to an increase in the material's conductivity.

πŸ’‘Impurities

Impurities in the context of semiconductors refer to the deliberate addition of atoms that have a different number of valence electrons than the base semiconductor material. The video explains that impurities define the number of free electrons and holes in extrinsic semiconductors, which in turn determines the material's conductivity. The speaker distinguishes between pentavalent (n-type) and trivalent (p-type) impurities and their effects on semiconductor properties.

πŸ’‘Conductivity

Conductivity in semiconductors is the measure of a material's ability to conduct electric current. The video discusses how conductivity in intrinsic semiconductors is initially low due to the absence of free charge carriers but increases with temperature as electron-hole pairs are generated. In extrinsic semiconductors, conductivity is higher due to the presence of impurities that introduce free charge carriers.

Highlights

Introduction to semiconductor materials and their classification into intrinsic and extrinsic types.

Explanation of intrinsic semiconductors as pure materials with no impurities added.

Description of silicon as a prime example of an intrinsic semiconductor material.

Discussion on the lower conductivity of intrinsic semiconductors compared to extrinsic ones.

Explanation of how electron-hole pairs are generated in intrinsic semiconductors at increased temperatures.

The concept of negative temperature coefficient in intrinsic semiconductors.

Examples of intrinsic semiconductor materials, such as silicon and germanium.

Introduction to extrinsic semiconductors and their higher conductivity due to impurities.

Definition and role of impurities in defining the number of free electrons and holes in extrinsic semiconductors.

Explanation of n-type semiconductors with the addition of pentavalent impurities.

Details on how phosphorus impurities contribute to the creation of free electrons in n-type materials.

Introduction to p-type semiconductors with the addition of trivalent impurities.

Role of aluminum impurities in creating free holes in p-type semiconductor materials.

Discussion on donor and acceptor impurities in n-type and p-type semiconductors, respectively.

Explanation of majority and minority charge carriers in n-type and p-type semiconductors.

Mechanisms for breaking covalent bonds in semiconductors through temperature, potential difference, and electric field.

Summary of the basics of semiconductor materials and their practical applications.

Transcripts

play00:02

Hello friends welcome to engineering

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Panda family in this video I am going to

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explain you types of semiconductor

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material

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in my last video I have explained you

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how we have classification of solid

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material we have been having three

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categories conductor semiconductor and

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insulator

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and I have already explained how energy

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bands are there with material in my last

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video

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in this video I'll explain you how

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semiconductor materials are there so

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when you want to classify semiconductor

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material then there are in general two

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categories

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intrinsic semiconductor material and

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extrinsic semiconductor material

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intrinsic semiconductor material is a

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pure semiconductor material PR means

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there is no impurities added with

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semiconductor

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while with expensive semiconductor

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material we add some impurities

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let us try to understand Basics first

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after that I'll explain you how

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impurities are added and what will

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happen based on impurities so see with

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intrinsic semiconductor material we are

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having pure semiconductor material and

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you need to understand one thing see

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with pure semiconductor material we will

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be having lower conductivity compared to

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extrinsic semiconductor material how we

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can have lower conductivity that even

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I'll explain you but first of all you

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need to understand what is pure

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semiconductor material If You observe

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one example of silicon then silicon is

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pure semiconductor material in Silicon

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in its outer orbit there are four

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electrons and those four electrons are

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connected with their neighbor atom if

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you consider this silicon that is having

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let us say these four electrons are

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there right

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you can observe here four electrons are

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there

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so these four electrons are connected

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with covalent bonds you can observe see

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these four electrons

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of this atom that is connected with

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covalent bonds with their neighbor atom

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so you can say all the electrons are

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connected in covalent bond structure and

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as all the electrons are connected in

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covalent bond structure you can say here

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there is no free charge carrier in pure

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silicon and pure silicon that is

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referred as intrinsic semiconductor

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material and it is having lower

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conductivity I'll show you why it is

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having lower conductivity

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see at 0 Kelvin temperature there are no

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free charge carriers and as there are no

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free charge carriers conductivity will

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be less but as you increase the

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temperature there is a possibility that

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electron holes pair that will get

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generated let me show you how it will

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happen

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If You observe here see here we are

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having electrons right these are

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connected in covalent bonds so as if I

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say this electron that is getting out of

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this covalent bond and let us say this

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electron become free

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let us say this electron become free

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so what will happen here here there will

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be generation of holes

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here there will be generation of holes

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right so as you increase the temperature

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it is possible this covalent bond this

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covalent bond that will get

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break and as if covalent bond is getting

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break then three electron will get

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generated and at this place there will

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be whole right so here there is electron

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hole pair generation as if you increase

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temperature at 0 Kelvin there is no free

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charge carrier but as you increase

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temperature recharge carriers that will

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get generated over here right

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it has equal number of free electrons

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and holes why the reason is all the

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electrons are connected in covalent bond

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if one electron is getting free then

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there will be one hole right see

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electron is having negative charge whole

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is having positive charge that is how we

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consider things right so here equal

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number of holes and equal number of

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electrons will be there

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it has negative temperature coefficient

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now what is the meaning of negative

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temperature coefficient see here if you

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increase the temperature if you increase

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the temperature then resistivity will go

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down why resistivity will go down if you

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increase the temperature free electron

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hole pair that will get generated inside

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material and as if you have free charge

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carriers in the material then that its

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resistivity that will go down

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right so here

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with intrinsic semiconductor material we

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have negative temperature coefficient

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what it means if you increase the

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temperature

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recharge carrier will get generated and

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because of free charge carriers

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resistivity will go down here some basic

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examples that I have written

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with intrinsic semiconductor material we

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can have silicon and germanium widely

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this two semic these two semiconductor

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materials are widely used

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practically silicon that you will be

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observing most of the chips are using

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silicon right

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here let us discuss about x26

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semiconductor material first

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see in pure semiconductor material if we

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add impurities then it will become in

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extrinsic semiconductor material right

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see due to impurities it is having

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higher conductivity I'll show you

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practically how it will be having higher

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conductivity right now just consider due

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to impurities

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extrinsic semiconductor material will be

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having higher conductivity here

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impurities will Define number of free

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electrons and holes I'll show you that

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even how it will define it

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here we are adding impurities in the

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unit of PPM

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part per million so in terms of PPM we

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add impurities see for example part per

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million means as if I say one PPM

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impurity is added then one atom of

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impurity that we added per 1 million of

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pure atoms that is how unit is there

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right and basic example of actronic

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semiconductor material are n type and P

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type

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now I am going to explain you how

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impurities are added and how n-type and

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p-type material is there so if You

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observe basic silicon structure that we

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have now in this basic silicon structure

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with n-type material

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we are adding pentavalent impurities so

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Here If You observe here I have added

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phosphorus impurity and phosphorus is

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having five phosphorus is having five

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electrons in its outer orbit usually

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with silicon how many electrons are

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there with outer orbit 4. so here

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additional electron that we are adding

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right so four electrons that will get

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combined with this ovalent Bond but one

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electron that will stay free over here

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so in n-type material in N type material

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we add pentavalent impurities

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pentavalent impurities means Phi

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electrons in its outer orbit with

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silicon we have four electrons in its

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outer orbit so as you add five electrons

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impurity pentaval and impurity so you

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will be adding three electrons so as you

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add

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impurities over here you are adding free

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charge carriers right and as you add

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free charge carriers what will happen

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obviously conductivity will increase

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right I have told you you see intrinsic

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semicondable material is having lower

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conductivity why the reason is by

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default free charge carriers are not

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available but in extrinsic semiconductor

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material we add impurities that leads to

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higher conductivity why the reason is in

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pure silicon in pure silicon if you add

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pentavalent impurities it will add free

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electrons right in p-type semiconductor

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material we add trivalent impurities

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tribal and impurities means three

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electrons will be there in its outer

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orbit so what will happen if You observe

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here I have added aluminum so aluminum

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is having three electrons in its outer

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orbit silicon structure is having four

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electrons in its outer orbit so what

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will happen one electron space will be

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vacant over here and that is referred as

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three hole over here so as you add

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tribal and impurities

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in p-type material you are adding free

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holes and in n-type material you are

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adding free electrons so practically we

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are adding free charge carriers that

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leads to higher conductivity in

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extrinsic semiconder material like

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n-type and P type right now let us

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discuss about some basics of n-type and

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P type ce9 type we add pentavalent

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impurities means in its outer orbit Phi

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electrons will be there

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so with every impurity one free electron

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is added and that's why it is also

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referred as donor impurity donor

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impurity means here we are donating one

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extra

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recharge carrier as electron right

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here impurities can be formed from group

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of five like phosphorus and anti-money

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so in n-type semiconductor material

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practically we add phosphorus and

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anti-money

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here majority charge carrier with n type

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that will be electrons why the reason is

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number of impurities will leads to

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number of free electrons so here with

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this material majority charge carriers

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will be electrons and as you increase

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the temperature

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some electrons will go out of this

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covalent bond and it will generate

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electron hole pair that may leads to

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holes but minority carriers will be

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holes over here with pure semiconductor

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material with pure semiconductor

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material electron and holes are equal

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but with n-type semiconductor material

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we are adding additional impurity with

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additional electron so here majority

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carriers will be electrons and minority

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carriers will be holes now when you want

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to understand how P type semitender

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material is there then in p-type

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seminary material we add tribal and

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impurities which is having three

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electrons in its outer orbit and because

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of that what we do we are adding

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additional free hole means electron

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space is vacant that is referred as

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pre-hole right as if electron space is

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vacant that is referred as pre-hole so

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you can say here we are adding three

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holes over here with impurities

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and this is also referred as acceptor

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impurity why it is referred as acceptor

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impurity the reason is this whole this

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hole is having tendency to accept the

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electron this hole is having tendency to

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accept the electron that's why it is

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also referred as acceptor impurities

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some examples that I have listed here

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impurities from third group that could

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be aluminum or Boron right so here we

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can have herd group impurities like

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aluminum and Boron here majority charge

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carriers will be holes as we add

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trivaland impurities over here and

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minority charge carriers those are

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electrons over here and those minority

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carriers can be generated because of

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covalent bond is getting break due to

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some reason now if you want to

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understand how covalent bond is getting

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break in any semiconductor material then

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all you need to do is you need to

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increase the temperature for example if

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you apply heat if you apply heat to this

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material then these electrons will break

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covalent bond and it will get free so as

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if electron is getting free over here it

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will generate electron hole pair right

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there is one another way by which you

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can have breaking of covalent bond

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you can apply higher potential

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difference in between two terminal of

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material by which we can generate

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electron hole pair and Third Way is by

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applying higher electric field through

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the material if you apply higher

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electric field through the material then

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also you can generate electron hole pair

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over here so this is how

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Basics are there with semiconductor

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material I hope you have understood this

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still if anything that would like to

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share please note it down in comment

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section I'll be happy to help you thank

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you so much for watching this video

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Related Tags
SemiconductorsMaterials ScienceIntrinsic vs ExtrinsicConductivitySiliconGermaniumPhosphorusAluminumElectronsHoles