Spin quantum number – ms

Slides:



Advertisements
Similar presentations
1. To describe Rutherford’s model of the atom 2. To explore the nature of electromagnetic radiation 3. To see how atoms emit light 11.1 Objectives.
Advertisements

Chapter 8 Periodic Properties of the Elements. Energy of atomic orbitals For an atom, electrons are in atomic orbitals.
CHAPTER 3 Introduction to the Quantum Theory of Solids
Laser Physics I Dr. Salah Hassab Elnaby Lecture(2)
Objectives To learn about the shapes of the s, p and d orbitals
Textbook: Electronic Devices and Circuit Theory Robert L.Boylested.
1 Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure of.
ENE 311 Lecture 4.
Electrons and Bonding. Valence Electrons The electrons that are located in the outer energy shell of each atom These electrons are available to be shared,
10.7 The Hydrogen Orbitals  In the Wave Mechanical model of the atom an orbital represents the space around the nucleus occupied by an electron.  An.
1 SEMICONDUCTORS Semiconductor atomic structure. 2 SEMICONDUCTORS We are going to look at the basic structure of an atom and compare and contrast the.
Chapter 5 : Electrons in Atoms. Problems with Rutherford’s Model Chlorine # 17 Reactive Potassium # 19 Very reactive Argon # 18 Not reactive.
EEE 3394 Electronic Materials
Quantum Mechanics and Atomic Theory Wave models for electron orbitals.
Section 11.1 Atoms and Energy 1.To describe Rutherford’s model of the atom 2.To explore the nature of electromagnetic radiation 3.To see how atoms emit.
ELECTRON AND PHONON TRANSPORT The Hall Effect General Classification of Solids Crystal Structures Electron band Structures Phonon Dispersion and Scattering.
Quantum-Mechanical View of Atoms
Quantum Theory and the Electronic Structure of Atoms Chapter 7.
Chapter 5 Electrons in Atoms.
Chemical Bonding Chapter 8. Atomic Orbitals The wave equation tells us the probability of finding an electron in space. Some areas have higher probability.
Electrons in Atoms Chapter Wave Nature of Light  Electromagnetic Radiation is a form of energy that exhibits wavelike behavior as it travels through.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Chemistry FIFTH EDITION Chapter 7 Atomic Structure and Periodicity.
The Development of A New Atomic Model
Origin of energy band formation:
1 Ionic and Metallic Bonding Ch Review What is a valence electron? –Electrons in the highest (outermost) occupied energy level Related to the group.
The Quantum Mechanical Atom Chapter 8. Electron Distribution When 2 or more atoms join to form a compound, the nuclei of the atoms stay relatively far.
Chapter 7 Atomic Structure.
TITLE” ENERGY BANDS OM INSTITUTE OF TECHNOLOGY
Chapter Energy Bands and Charge Carriers in Semiconductors
CONCURRENT ENROLLMENT CHEMISTRY
10.7 The Hydrogen Orbitals In the Wave Mechanical model of the atom an orbital represents the space around the nucleus occupied by an electron. An orbital.
Electrical Engineering Materials
7. Quantum-Mechanical View of Atoms
Orbitals and Electron Configurations
Electronic Structure of Atoms
SOLIDS AND SEMICONDUCTOR DEVICES - I
Schrödinger's Cat A cat is placed in an airtight box with an oxygen supply and with a glass vial containing cyanide gas to be released if a radiation detector.
Electron Configuration
ELECTRON CONFIGURATION
What value of wavelength is associated with the Lyman series for {image} {image} 1. {image}
ECEE 302: Electronic Devices
Polytetrafluoroethylene
ELECTRONS IN ATOMS.
Physics 342 Lecture 28 Band Theory of Electronic Structure in Solids
Unit 1:Atomic Structure Part 2
Homework # 10 Worksheet: Quantum Numbers
Electrons in Atoms Chapter 5.
SOLIDS AND SEMICONDUCTOR DEVICES - I
Energy Band Diagram (revision)
Atomic Structure and Periodicity
Electronic Fundamental Muhammad Zahid
Electrons in Atoms Chapter 5.
Chapter 6 Electronic Structure of Atoms
Electronic structure in atoms
QUANTUM MECHANICAL MODEL OF THE ATOM
Chapter 6 Quantum Mechanical Model & Electron Configurations
Light Energy and Electron Configurations
Chapter 4.1 The Development of a New Atomic Model
7. Quantum-Mechanical View of Atoms
PDT 264 ELECTRONIC MATERIALS
Atomic Structure and Periodicicity
SOLIDS AND SEMICONDUCTOR DEVICES - I
Energy Band View of Semiconductors
Development of a New Atomic Model
5.2 – Quantum Theory and the Atom
Electronic Physics Dr. Ghusoon Mohsin Ali E    8.857eV  1400
In term of energy bands model, semiconductors can defined as that
Atomic Structure and Periodicity
Quantum Theory and the Electronic Structure of Atoms
Presentation transcript:

Spin quantum number – ms Electronic Physics Dr. Ghusoon Mohsin Ali The magnetic quantum number (m) can be any integer between -l and +l. If l = 2, m can be either -2, -1, 0, +1, or +2. s: l = 0 has 1 orbital p: l = 1 has 3 orbitals d: l = 2 has 5 orbitals f: l = 3 has 7 orbitals Spin quantum number – ms This fourth quantum number describes the spin of the electron. Electrons in the same orbital must have opposite spins. Possible spins are clockwise or counterclockwise, spin quantum number ms is arbitrarily assigned the numbers +1/2 and -1/2. Pauli Exclusion Principle: No two electrons in an atom have the same set of four quantum numbers Electron configuration:The electron configuration for chlorine is (Z=17) 1s2 2s2 2p6 3s2 3p5 The large numbers represent the energy level. The letters represent the sublevel. The superscripts indicate the number of electrons in the sublevel Example

Electronic Physics Dr. Ghusoon Mohsin Ali 1s2 2s2 2p5 means "2 electrons in the 1s subshell, 2 electrons in the 2s subshell, and 5 electrons in the 2p subshell" Fig. 1.4. The sequence of orbital filling is, from the bottom of this diagram, upwards. The electrons in the outermost orbital are known as valence electrons and determine the physical and chemical properties of the elements. An arrangement of element in term of their valence electrons forms the basis

Table 1.2. Relationship among values of n, l and ml Electronic Physics Dr. Ghusoon Mohsin Ali of the periodic table. Elements in the groups І to VІІ have from one to seven valence electrons respectively. Interatomic forces are caused by electrons in outer shell (valence shell). Atoms with 8 electrons in their outer shell ( completely filled s and p sub shell they are very stable. Most other elements attempt to reach this stable structure by one of three mechanics: Losing electrons:-potassium (Z=19) 1s2 2s2 2p6 3s2 3p6 4s1 losing 4s electron leaving the potassium ion with stable structure. Gaining electrons:-chlorin (Z=17) 1s2 2s2 2p6 3s2 3p5 can have a stable filled shell if they receive one electron. Sharing electrons:-silicon 1s2 2s2 2p6 3s2 3p2 share 4 electrons with 4 other silicon atoms each of which also shares silicon atom. There are three very important ways in which binding energy provided to form a stable structure. These are ionic bond, covalent bond, metallic bond. Table 1.2. Relationship among values of n, l and ml

Electronic Physics Dr. Ghusoon Mohsin Ali The Energy-band Theory of Crystals Most metals and semiconductors are crystalline in structure. A crystal consists of a space array of atoms or molecules (ions) built up by regular repetition in three dimensions of some fundamental structural unit. The electronic energy levels discussed for a single atom do not apply to the same atom in a crystal. When atoms form crystals it is found that the energy levels of the inner-shell electrons are not affected appreciably by the presence of the neighboring atoms. However, the level of the outer- shell electrons is changed considerably, since these electrons are shared by more than one atom in a crystal. For example consider a crystal of Si consist of N atoms. If the atoms are so far apart that the interaction between them negligible. The outer two subshell of Si contain two s electrons and two p electrons. There are 2N electrons completely filling the 2N possible s level. Since the p atomic sub shell has six possible states with 2N electrons. Because the coupling between atoms, the crystal becomes an electronic system which must obey the Pauli exclusion principle. The separation between level are small, but since N is very large (5×1022 cm-3), this large number of discrete but closely spaced energy levels called energy band. The 2N states of s band are completely filled with 2N electrons, the p band of 6N states which only 2N of its levels has occupied by electrons. Note that there is an energy gap between two bands and this gap decrease as the atomic spacing decreases. These bands will overlap for small enough distance. The 6N upper states merge with the 2N lower states, giving total of 8N levels, half of which are occupied by the available electrons. At this spacing each atom has given up four electrons to the band, these electrons can no longer be said to orbit in s or p subshell of an isolated atom, but rather they belong to the crystal as a whole. At the crystal lattice spacing, we find the valance band filled with 4N electrons separated by a forbidden

Electronic Physics Dr. Ghusoon Mohsin Ali band (Eg) from an empty band consisting of 4N additional states. This upper vacant band is called the conduction band. (a) Vacuum level E0 χ Electron affinity Conduction band Ec Energy gap Eg Valence band Ev Electron (b) Fig.1.5. Formation of energy bands for electrons in a silicon crystal with a diamond-type lattice structure

Electronic Physics Dr. Ghusoon Mohsin Ali The most electrical properties of importance to engineers are related to the upper two bands of energy levels called the conduction band and valence band. The valence band contains energies of the same level as those of valence electrons. The conduction band energies are the empty levels above the valence band. Electrons in the valence band can leave their band to join conduction band if given sufficient energy to jump the forbidden energy band gap (Eg). The size of Eg is a prime factor to determining a solid is conductor, an insulator or semiconductor. Fig. 1.6. The size of Eg to determine a solid is conductor, an insulator or semiconductor Conductors contain a large number of electrons in the conduction band at room temperature. No energy gap exist and the valence and conduction band overlap. An insulator is a material in which the energy gap is so large that practically no electron can be given enough energy to jump this gap. A semiconductor is a solid with an energy gap small enough for electrons to cross from valence band to conduction band at room temperature Silicon (Eg=1.1eV), Germanium (Eg=0.7eV)

Electronic Physics Dr. Ghusoon Mohsin Ali Problems Q1: Calculate the radius r of orbit and velocity of an electron with total energy of -3.4 eV in hydrogen atom. (Ans:- 2.1164Å, 1.0936 ×106 m/s) Q2: Write all quantum number for the final electron for potassium Z=19 and chlorine Z=17. Q3: An electron drop from n=2 to ground state calculate The energy of emitted radiation The radius when n=2 Compare between the wavelength of an electron exist in a stable orbit n=1 and the wavelength of dust particle of mass 1×10-6kg and velocity 1ms-1 (Ans:- 10.19eV, 0.212nm, 1.05×10-10m, 6.626×10-29m) Q4: Calculate the energy momentum and de Broglie wave length of electron accelerated from rest by 200V. (Ans:3.2×10-17J, 7.639×10- 24kg.m.s-1,0.867×10-10m) Q5: An electron drops from specific energy level to ground state (n=1) in hydrogen atom. The energy difference between these two levels is 12.75 eV. Calculate the initial state of the electron and λ of the emitted radiation. (Ans: ni = 4, 972.54 Å)