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Semiconductors

Przegląd

Source: Derek Wilson, Asantha Cooray, PhD, Department of Physics & Astronomy, School of Physical Sciences, University of California, Irvine, CA

Semiconductors are materials whose ability to conduct an electrical current depends strongly on their temperature and level of impurity. The most common type of semiconductor material is crystalline silicon. Most pure semiconductors are not outstanding conductors; to improve conductivity, a pure semiconductor is often combined or "doped" with an impurity. These impurities are either donors, like phosphorus and arsenic, that donate electrons to the silicon, or acceptors, like boron and aluminum, that steal electrons from the silicon. When acceptors take electrons from the silicon, they leave regions of positive charge called "holes" that effectively behave as positively charged electrons.

A p-type semiconductor is formed when doping makes holes that are the dominant charge carrier in the material. An n-type semiconductor is formed when a semiconductor is doped such that the dominant charge carrier is the electron. As one might expect, a p-n junction is formed at the boundary between the p-type semiconductor and n-type semiconductor. The interaction of electrons and holes at the junction gives rise to the remarkable behavior seen in circuit components such as diodes and transistors. This lab will explore the properties of a single p-n junction in the form of a semiconductor diode.

Procedura

1. Observe the behavior of a p-n junction in the form of a semiconductor diode and measure its current-voltage characteristic curve.

  1. Obtain a semiconductor diode, an LED (light-emitting diode), a power source, two digital multimeters, a 1 kΩ resistor, some banana cables and connectors, and a thermometer.
  2. Look at the semiconductor diode. There should be a band on one of its ends. The side with the band is the "cathode". The side without the band is the "anode".
  3. Make su

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Wyniki

Typical results for the circuit measurements are shown in Table 1. The Shockley diode equation describes the current through a diode as a function of the temperature of the diode and the voltage drop across it. For a temperature of 293.0 K, a voltage of 555 mV across the diode, and an arbitrary (but representative) ideality factor of n = 1.5,

Equation 2
Equation 3

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Wniosek i Podsumowanie

This lab explored the properties of semiconductors and a p-n junction in the form of a semiconductor diode. A diode is a circuit component composed of one p-n junction. The characteristic curve of the diode was measured, and the diode was observed to conduct an electrical current in only one direction. An LED contains a special type of p-n junction that emits light in addition to conducting unidirectionally.

Semiconductors are used extensively in the electronics industry. Semiconductor diodes

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Tagi
SemiconductorsElectronicsSemiconductor IndustryConductivityInsulatorMetalsCrystalline SiliconWafersP typeN typeSemiconductor DevicesP n JunctionsTransistorsElectrical PropertiesDiodeProtocolCharacterizationReal world ApplicationsIntrinsic SemiconductorsCovalent BondsLattice StructureFree ElectronsImpuritiesDoping

Przejdź do...

0:05

Overview

1:24

Principles of Semiconductors

6:01

Characterizing a P-N Junction

9:10

Data Analysis and Results

10:39

Applications

12:20

Summary

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