Quantum Mechanics: A Paradigms Approach David H. McIntyre. 27 July Corrections to the 1 st printing

Similar documents
Corrections and Minor Revisions of Mathematical Methods in the Physical Sciences, third edition, by Mary L. Boas (deceased)

PH 451/551 Quantum Mechanics Capstone Winter 201x

Errata Instructor s Solutions Manual Introduction to Electrodynamics, 3rd ed Author: David Griffiths Date: September 1, 2004

PHYS 3313 Section 001 Lecture # 22

Angular momentum. Quantum mechanics. Orbital angular momentum

ONE AND MANY ELECTRON ATOMS Chapter 15

Errata 1. p. 5 The third line from the end should read one of the four rows... not one of the three rows.

Chemistry 532 Practice Final Exam Fall 2012 Solutions

Chapter 4. Q. A hydrogen atom starts out in the following linear combination of the stationary. (ψ ψ 21 1 ). (1)

Angular Momentum. Classically the orbital angular momentum with respect to a fixed origin is. L = r p. = yp z. L x. zp y L y. = zp x. xpz L z.

Review of paradigms QM. Read McIntyre Ch. 1, 2, 3.1, , , 7, 8

Preliminary Examination - Day 1 Thursday, August 9, 2018

Sample Quantum Chemistry Exam 2 Solutions

Notes: Most of the material presented in this chapter is taken from Jackson, Chap. 2, 3, and 4, and Di Bartolo, Chap. 2. 2π nx i a. ( ) = G n.

Physics 217 Problem Set 1 Due: Friday, Aug 29th, 2008

Final Examination. Tuesday December 15, :30 am 12:30 pm. particles that are in the same spin state 1 2, + 1 2

Physics 214 Final Exam Solutions Winter 2017

Chapter-2 2.1)Page-28, Eq (2-9): should read (add parentheses around the terms involving the x-end-points):

Bohr & Wheeler Fission Theory Calculation 4 March 2009

Physics 2203, Fall 2012 Modern Physics

The Hydrogen atom. Chapter The Schrödinger Equation. 2.2 Angular momentum

Errata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity 1st printing

Chemistry 432 Problem Set 4 Spring 2018 Solutions

1 r 2 sin 2 θ. This must be the case as we can see by the following argument + L2

Fun With Carbon Monoxide. p. 1/2

Physics 4617/5617: Quantum Physics Course Lecture Notes

Physics 2203, 2011: Equation sheet for second midterm. General properties of Schrödinger s Equation: Quantum Mechanics. Ψ + UΨ = i t.

16.1. PROBLEM SET I 197

Collection of formulae Quantum mechanics. Basic Formulas Division of Material Science Hans Weber. Operators

Quantum Mechanics in Three Dimensions

Physics 505 Homework No. 12 Solutions S12-1

The Hydrogen Atom. Chapter 18. P. J. Grandinetti. Nov 6, Chem P. J. Grandinetti (Chem. 4300) The Hydrogen Atom Nov 6, / 41

Errata for Quantum Mechanics by Ernest Abers August 1, 2004

Physics 228 Today: Ch 41: 1-3: 3D quantum mechanics, hydrogen atom

PHYSICS 250 May 4, Final Exam - Solutions

Lectures 21 and 22: Hydrogen Atom. 1 The Hydrogen Atom 1. 2 Hydrogen atom spectrum 4

Errata. The following errors are known to be present in The Mechanics of Inhaled Pharmaceutical Aerosols: An Introduction:

Physics 443, Solutions to PS 8

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS

Further Quantum Mechanics Problem Set

PH425 Spins Homework 5 Due 4 pm. particles is prepared in the state: + + i 3 13

8 Quantized Interaction of Light and Matter

Modern Physics. Unit 6: Hydrogen Atom - Radiation Lecture 6.3: Vector Model of Angular Momentum

PHYSICS DEPARTMENT, PRINCETON UNIVERSITY PHYSICS 505 FINAL EXAMINATION. January 18, 2013, 1:30 4:30pm, A06 Jadwin Hall SOLUTIONS

Quantum Mechanics Final Exam Solutions Fall 2015

NANOSCALE SCIENCE & TECHNOLOGY

Errata for Quantum Mechanics by Ernest Abers Intermediate Level Errata as of July 1, 2007 (3rd printing)

ERRATA AND ADDITIONS FOR "ENGINEERING NOISE CONTROL" 4th Edn. First printing April 23, 2018

Quantum Mechanics Solutions. λ i λ j v j v j v i v i.

= ( Prove the nonexistence of electron in the nucleus on the basis of uncertainty principle.

Schrödinger equation for the nuclear potential

PHYS 404 Lecture 1: Legendre Functions

Physics 115C Homework 2

would represent a 1s orbital centered on the H atom and φ 2px )+ 1 r 2 sinθ

Rotation Matrices. Chapter 21

Approximation Methods in QM

xy 2 e 2z dx dy dz = 8 3 (1 e 4 ) = 2.62 mc. 12 x2 y 3 e 2z 2 m 2 m 2 m Figure P4.1: Cube of Problem 4.1.

PHYS Quantum Mechanics I - Fall 2011 Problem Set 7 Solutions

Summary: angular momentum derivation

More On Carbon Monoxide

Physics 443, Solutions to PS 2

Each problem is worth 34 points. 1. Harmonic Oscillator Consider the Hamiltonian for a simple harmonic oscillator. 2ml 2 0. d 2

p.46, Sidenote 11: Insert an equation reference "(12.17)" in the 3rd sentence so the Sidenote will read

Applied Statistical Mechanics Lecture Note - 3 Quantum Mechanics Applications and Atomic Structures

Prob (solution by Michael Fisher) 1

Columbia University Department of Physics QUALIFYING EXAMINATION

The Central Force Problem: Hydrogen Atom

Probability and Normalization

We now turn to our first quantum mechanical problems that represent real, as

1 Schroenger s Equation for the Hydrogen Atom

Physics 220. Exam #2. May 20, 2016

Physics 139B Solutions to Homework Set 4 Fall 2009

ECE 659, PRACTICE EXAM II Actual Exam Friday, Feb.21, 2014, FNY B124, PM CLOSED BOOK. = H nm. Actual Exam will have five questions.

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C4: PARTICLE PHYSICS

Quantum Mechanics I - Session 9

Wave Properties of Particles Louis debroglie:

1 Polarization of Light

3 Schroedinger Equation

Appendix: SU(2) spin angular momentum and single spin dynamics

( ) ( ) QM A1. The operator ˆR is defined by R ˆ ψ( x) = Re[ ψ( x)] ). Is ˆR a linear operator? Explain. (it returns the real part of ψ ( x) SOLUTION

A Quantum Mechanical Model for the Vibration and Rotation of Molecules. Rigid Rotor

Errata for Quantum Mechanics by Ernest Abers Intermediate Level Errata as of July 1, 2007 (1st and 2nd printings)

Ch120 - Study Guide 10

Quantum Mechanics: The Hydrogen Atom

d 1 µ 2 Θ = 0. (4.1) consider first the case of m = 0 where there is no azimuthal dependence on the angle φ.

Numerical Methods for Engineers, Second edition: Chapter 1 Errata

The original Renner-Teller effect Paul E.S. Wormer Theoretical Chemistry, University of Nijmegen December 31, 2003

ERRATA. Interest and Prices, Princeton University Press, updated February 2, 2008

Astronomy 9620a / Physics 9302a - 1st Problem List and Assignment

PHYS 771, Quantum Mechanics, Final Exam, Fall 2011 Instructor: Dr. A. G. Petukhov. Solutions

Relativity Problem Set 9 - Solutions

Physics 221A Fall 1996 Notes 13 Spins in Magnetic Fields

Lecture 6 Scattering theory Partial Wave Analysis. SS2011: Introduction to Nuclear and Particle Physics, Part 2 2

Quantum Mechanics II Lecture 11 ( David Ritchie

CHEM-UA 127: Advanced General Chemistry I

kg meter ii) Note the dimensions of ρ τ are kg 2 velocity 2 meter = 1 sec 2 We will interpret this velocity in upcoming slides.

Physics 70007, Fall 2009 Answers to Final Exam

Quantum Mechanics & Atomic Structure (Chapter 11)

8.04 Spring 2013 March 12, 2013 Problem 1. (10 points) The Probability Current

The 3 dimensional Schrödinger Equation

Transcription:

Quantum Mechanics: A Paradigms Approach David H. McIntyre 7 July 6 Corrections to the st printing page xxi, last paragraph before "The End", nd line: Change "become" to "became". page, first line after Eq. (.4): Change "gyroscopic" to "gyromagnetic". page, Problem.9, first line: Change "A pair of dice" to "Two dice". page 5, paragraph after Eq. (.), penultimate line: Change " " to " ". page 44, Eq. (.5): Change the "+" superscript in the nd and rd lines to the proper adjoint symbol " ": φ β β φ * { } * ψ A β β A ψ (.5) ψ A β β A ψ * page 7, Eq. (.8): Change the " + " ket in the nd line to " ": H + ω S z + ω + E + + H ω S z ω E (.8) page 8, Eq. (.65): In the st line, change the vertical bar on the st bra to a left angle bracket to make a proper bra symbol: ψ + y y + + y y + y y + + y y y + + y + y y (.65) i + y + i y page 84, last sentence of paragraph after Eq. (.68): Change sentence to read: "Neutrinos are so elusive because they interact via the weak force or weak interaction, which is much weaker than the strong nuclear force and electromagnetism, but not as weak as gravity." page 88, line before Eq. (.84): Delete duplicate "the".

page 96, Problem.6: (i) st line: After the term "Rabi oscillations", insert the parenthetic comment "(i.e., Rabi flopping)"; (ii) Part (b), Delete "complete" and after "flip" insert the parenthetic comment "(i.e., P + ( t) P and P ( t) P + )". page 4, lines before Eq. (4.5): Change "π-pulse" to "π/-pulse". page 6, rd reference (Mermin's moon article): Change issue number from "(5)" to "(4)". page 8, Eq. (5.): Change to π : f ij ω ij π E E i j h λ ij c hc f ij E i E j (5.) page 7, Eq. (5.7): Change the "ϕ " symbol to the "φ " symbol all places: P ψ >φ φ ψ φ * ( x)ψ ( x)dx (5.7) page 4, nd line: Change x < L to x > L. page 6, Eq. (5.97): (i) Change ϕ symbols in bra-ket to E, (ii) change last subscript from "m" to "n": page 4, Example 5.4: renumber to 5.5. E m qx E n ϕ m ( x) qx ϕ n ( x)d r (5.97) page 4, Eq. (5.): Insert in denominator of exponent term e ie nt in line : c n ϕ n x ψ x,t e ie nt c n L n 6 L n nπ n n sin nπx nπx sin L e in π t ml L e in π t ml page 44, nd line after Eq. (5.): Change "Example 5." to "Example 5.4". page 47, st line after Fig. 5.4: Change ".67 ev" to ".4 ev.4 ev". page 56, Problem 5.: Change ϕ symbols inside kets to E: and E n ψ ( t ) A E E + i E page 57, Problem 5.7: Change ϕ symbols inside kets to E: 5 and E n ψ ( t ) E i E page 58, Problem 5., end of second line: Change " x > L " to " x > a ". (5.) 7/7/6

page 7, Eq. (6.7): Add curly brackets to match the text in the subsequent paragraph: ψ (x,t) ( x pt m) { } + cos δ p π eip x p m t (6.7) page 74, Eq. (6.5): Add curly and square brackets to match the text in the subsequent paragraph: ψ (x,t) πα 4 γ e ip ( x p t m) { } e x p t m 4α γ (6.5) page 8, Eq. (6.75): Move zero subscript on momentum space representation of position eigenstate from p to x: Position space Position eigenstate x δ ( x x ) x Momentum eigenstate p π ei p x Momentum space π ei px p δ ( p p ) (6.75) page 99, Problem 6., centered equation: move "x" before division symbol: ψ (x) Ae i p x e x 4α page 7, Eqs. (7.77) and (7.78): Change the sign of the second term on the left-hand side of both equations: R( r) d dr r dr r + µ (E V (r))r dr Y ( θ,φ) L Y ( θ,φ) d dr r dr ( r ) dr R r function of r only + µ (E V (r))r Y θ,φ function of θ,φ only (7.77) L Y ( θ,φ) A (7.78) page 5, paragraph after Eq. (7.5), penultimate line: After the word "determine", insert the parenthetic comment "(with some ambiguity)". page, Eq. (7.48): Remove "*" indicating complex conjugate: P k (z)p (z)dz + δ (7.48) k page 5, Eq. (7.56): Place the normalization factor inside a square root: Θ m m ( +) ( m)! ( θ ) ( ) ( + m)! P m (cosθ), m (7.56) 7/7/6

page 9, Eq. (7.7): Change lower limit of sum to absolute value of m: P Lz m m ψ (7.7) m page 4, Spherical harmonic terms throughout this example are mislabeled, so (i) change to in Eqs. (7.7), (7.74), (7.75), and (7.76); and (ii) change energy and angular momentum values in sentence after Eq. (7.76): ψ ( θ,φ) Y ( θ,φ) + Y ( θ,φ) (7.7) ψ +, (7.74) c m m ψ δ δ m + δ δ m, (7.75) P E m ψ m δ δ + δ (7.76) New Sentence after Eq. (7.76): The probability of measuring the energy to be E I is %, as is the probability for measuring L 6. page 4, Eq. (7.77), st line: Change lower limit of sum to : P Lz ψ (7.77) page 47, Problem 7.7, centered equation: Change " " to "": P( φ,t) sin φ + π I t page 48, Problem 7.6, centered equation: Change sign to sign: L ± e ±iφ ± θ + i cotθ φ 7/7/6 4

page 5, Eq. (8.9): Change prefactors of H ( ρ) and H ρ d R dρ ρ e γρ ( ) ρ γ + γ ρ H ρ terms: + ( γρ ) H ( ρ) + ρ H ( ρ) (8.9) page 7, Eq. (8.97), nd line: Change in st denominator to 4 ; rd line: Change in st denominator to 4, change exponent in e r a to e r a, change 4 in last denominator to. ψ (r,θ,φ,t) ψ (r,θ,φ)e ie t/ + ψ (r,θ,φ)e ie t/ r 4 πa a e r /a e ie t/ + πa e ie t/ r 4 πa a e r /a + z e r /a a r cosθ e r /a ie e t/ 8a (8.97) page 7, Problem 8., both equations: Delete nm subscripts from wave functions: ψ (x, y,z) dx dy π ψ (ρ,φ,z) ρ dρ dφ P z P z page 74, Problem 8.5, centered equation: Add "x, y," to argument of function: V ( x, y,z), < x < L, < y < L, < z < L, otherwise page 75, two lines after Eq. (9.): Delete "to" before "zero". page 77, penultimate paragraph, rd line: Delete "what" near end of line. page 8, Eq. (9.8), st line: On right-hand side of equation, delete left parenthesis and change right parenthesis to right bracket: ae E ωa E ( E ω )( a E ) H a E page, last line: Insert spaces on either side of " p ". page, last paragraph, end of 4 th line: add space to separate "of ampli-". page, Problem 9., part (e): Change "that" to "than". page, Eq. (.47): Change subscript on "H" to "nn": (9.8) E () n H nn n () H n () (.47) 7/7/6 5

page, Eq. (.49): Insert and remove minus signs to correct sign error in energy: H µ i B ω S z ω ω ω ω (.49) page, nd line after Eq. (.49): (i) Insert and remove minus signs to correct sign error in energy, (ii) Change "decreasing" to "increasing". New line: ( E ) ( ω, E ) ( ω, E ) ( ω, and E ) 4 ω, labeled in order of increasing page, Eq. (.5): Insert and remove minus signs to correct sign error in energy: H µ i B ω S z ω ω ω ω (.5) page 4, Fig..4: Insert and remove minus signs on m labels: From top, m, m, m, m. page 4, Eq. (.5): Insert and remove minus signs to correct sign error in energy: ( E ) ω ( E ) ω ( E ) ω ( E ) 4 ω (.5) page, Eq. (.8): Insert and remove minus signs to correct sign error in energy: H µ i B ω S z ω ω ω ω (.8) page, nd line after Eq. (.8): Insert and remove minus signs to correct sign error in energy. New energies: ( E ) ( ω, E ) ( ω, E ) ( ω, and E ) 4 ω page, first line: Change subscript on B to : B B ˆx 7/7/6 6

page, Eq. (.8): Insert minus signs to correct sign error in energy: H µ i B ω S x ω ω 4 ω 4 ω ω ω (.8) page, Eq. (.85): (i) Sum over m, (ii) Insert minus signs ( E ) H m m E ( ) E ( ) ( ) m ω ( ω ω ) ω 4ω H E ( ) E ( ) ( ) (.85) page, Eq. (.86): (i) Sum over m, (ii) Insert and remove minus signs ( E ) H m m E ( ) E ( ) ( ) m H E ( ) E ( ) ( ) 4 ω ( ω ω ) + ω ω 4ω ω ω + H E ( ) E ( ) ( ) (.86) page 4, Eq. (.87): Remove minus signs: ( E ) ω 4ω ( E ) 4 ω 4ω (.87) 7/7/6 7

page 4, Eq. (.89): (i) Sum over m, (ii) Insert minus signs in nd line: m H m E ( ) E ( ) m ( ) m ω ω ω H E ( ) E ( ) ( ) (.89) ω ω page 4, Fig..8: Insert and remove minus signs on m labels: From top, m, m, m, m. page 48, Eq. (.4): (i) st line: Insert "" in denominator of wave function polynomial; (ii) rd line: Change " ± " symbol in wave function amplitude to " ". ψ ψ, ± ψ ± ( r,θ,φ) R ( r)y θ,φ ( r,θ,φ) R ( r)y θ,φ r ( r,θ,φ) R ( r)y ± θ,φ a a e r a 4π r e r a ( a ) a 4π cosθ r e r a ( a ) a 8π e±iφ sinθ (.4) page 49, Eq. (.47), nd line: (i) Insert a term before integral, (ii) Insert "" in denominator of wave function polynomial:: H ψ ( )* r,θ,φ ee r cosθ ψ ee ( a ) 4π π cos θ sinθ dθ π ( r,θ,φ)r sinθ dr dθ dφ r ( a ) 4π a a dφ e r a r 4 dr (.47) page 49, Eq. (.48): (i) st line: Insert "" superscripts in ket and bra; (ii) st line: Remove extraneous square right bracket before sign; (iii) st line: Insert " a " in 4π denominator before integral; (iv) nd line: Change denominator before square brackets to a 4 : H ee ( a ) 4πa π r 4 e r a dr a ee 4!a 5 4 6 5!a a a eea r 5 e r a dr (.48) 7/7/6 8

page 56, Eq. (.4): Insert factor of g e before st term in brackets: H hf µ g e µ B g p µ N 4π g e r I i L r S i I + r 5 page 64, Eq. (.45): Change 4 in top line to : ΔE hf µ g e µ B g p µ N α 4 m e c πa g g e p ( S i r) ( I i r) + 8π S i Iδ ( r) m e m p 5.88 6 ev h 4.45757667(9)MHz (.4) (.45) page 7, last paragraph: (i) rd line: Change "coupled" to "uncoupled", (ii) 7 th line: Change "the coupled and the coupled" to " the coupled and the uncoupled". pages 75 & 76, Tables..5: Header symbols j and m should be capitalized J and M to be consistent with text. page 98, Eq. (.6): Add minus signs to two elements of the matrix (second / and second / on diagonal): L z page 99, st line after Eq. (.67): Change "play" to "plays". page 4, Eq. (.86): Change exponent on st n to 4: α 4 mc 4n + 4 n + E fs m m s ( +),,,,,, (.6) (.86) page 48, Problem.4, part (b), st and nd lines: Change "the formula we derived in class" to "Eq. (.46)". page 46, Eq. (.6): Interchange last two wave functions on right hand side: SS ψ S ψ ( x, x ) ϕ ( x )ϕ ( x ) + ϕ ( x )ϕ ( x ) (.6) page 45, Eq. (.56): Interchange last two wave functions on right hand side: ψ AS M ϕ x ψ A x, x ϕ ( x ) ϕ ( x )ϕ ( x ) M (.56) 7/7/6 9

page 4, Eq. (.79): Add complex conjugation symbols to two wave functions on st line and remove them from two wave functions on nd line: E s, ψ * * * * ( r )ψ m ( r ) ± ψ m ( r )ψ r 4πε r r (.79) ψ r ψ m ( r ) ± ψ m ( r )ψ ( r ) d r d r page 44, Problem.7: Delete second half of last sentence after comma (no integrals required). page 444, Problem.7: (i) part (b): Change "wave function" to "quantum state vector", (ii) part (d): Change "wave functions" to "quantum state vectors". page 448, Eq. (4.6): Change the subscript on the second energy from "n" to "i": i dc k ( t) e i ( E k E i )t k H t dt e i (4.6) page 45, Figure 4., lower label: Insert "/" so that marked time interval is π ω fi ω. page 46, Eq. (4.69), second line: Change the first "E" symbol to a script font for electric field: R π V πe E g( E f ) ˆε i r A π E ω + A page 467, Problem 4.: Change starting time from "t " to "t ". page 468, Problem 4.: Change "l " to " ". (4.69) pages 48 and 48, Eqs. (5.8) and (5.9): An overall phase (which is physically meaningless) has been omitted from Eqs. (5.8) and (5.9). page 48, Fig. 5.: Each wave function is defined only over the range.5a x 8.5a (given that we are using periodic boundary conditions). page 485, Eq. (5.4): Insert absolute value symbols: g( E) g k ( k) dk de L dk π de page 485, Eq. (5.44): Insert minus sign: de dk (5.4) βasin ( ka ) (5.44) 7/7/6

page 485, Eq. (5.45): Insert absolute value symbol: g( E) L πβasin ka (5.45) page 486, last line: Change "-.6 mev" to "-.5 mev". page 488, middle of last paragraph before Section 5.8.: Change "- mev" to "- mev". page 49, Eq. (5.58): Change sign of κ term in exponents (4 times): e ika ψ I ( b) ψ II ( b + a) Ae iqb + Be iqb e ika Ce e ika ψ I '( b) ψ II '( b + a) q Ae iqb Be iqb + De iκ a b iκ a b κe ika iκ a b Ce De page 49, Eq. (5.59): Change sign of κ term in exponents (4 times): e iqb e iqb e ika iκ a b e e ika e q q κ κ iκ a b qe iqb qe iqb κe ika iκ a b e κe ika iκ a b e A B C D iκ a b (5.58) (5.59) page 49, Eq. (5.6): Add absolute value symbols to κ terms ( more times): cos( qb)cosh κ a b ( ) q κ q κ sinh κ a b sin qb page 5, Eq. (6.47): Insert prefactor before last term: ( ) cos( ka) (5.6) ψ U CNOT ψ (6.47) page 546, First line after Eq. (D.6): Insert "we" after "if". 7/7/6