FROM INDUCTION TO QUANTUM SPIN: TRAINING STUDENTS TO BECOME PHYSICISTS

Similar documents
Upper-Level Physics: Ken Krane Oregon State University. New Faculty Workshop June 18, 2013

SPIN and QUANTUM MEASUREMENT INSTRUCTOR GUIDE

Math 31 Lesson Plan. Day 5: Intro to Groups. Elizabeth Gillaspy. September 28, 2011

i = cos 2 0i + ei sin 2 1i

Let us go back to what you knew in high school, or even earlier...

Physics 430IA Quantum Mechanics Spring 2011

Physics 162a Quantum Mechanics

Physics 351 Wednesday, January 10, 2018

1 Measurement and expectation values

Reference Texts. Principles of Quantum Mechanics R Shanker Modern Quantum Mechanics J.J. Sakurai

Procedure for Setting Goals for an Introductory Physics Class

ENV level elective. ENV 200 Intro to Environmental Science 4 credits ENV 330 Ecosystems and Ecological Design 4 credits

Stellar Astronomy 1401 Spring 2009

Physics Fall Semester. Sections 1 5. Please find a seat. Keep all walkways free for safety reasons and to comply with the fire code.

Lesson Plan. 1) Students will be aware of some key experimental findings and theoretical

Co-requisite: University Physics Lab I (PHYS 3013) Requisite: Calculus (MATH 3051 or equivalent)

Vector Spaces for Quantum Mechanics J. P. Leahy January 30, 2012

2 Foundations of Quantum mechanics

Comprehensive Course Syllabus

Physics 343: Modern Physics Autumn 2015

Integrating Practices and Core Ideas into Introductory Physics Courses

Physics 3220 Homework 13 Due Dec. 7, 2012

Total Angular Momentum for Hydrogen

Interactive Engagement in Upper-Level Physics

1 Now, Why do we want to learn Quantum Mechanics

Quantum Physics II (8.05) Fall 2002 Outline

Motivating Questions: How many hurricanes happen in a year? Have the number of hurricanes per year changed over time?

Mission Statement. Program outcomes

Math 31 Lesson Plan. Day 2: Sets; Binary Operations. Elizabeth Gillaspy. September 23, 2011

Stern-Gerlach Experiment and Spin

3. Quantum Mechanics in 3D

Hestenes lectures, Part 5. Summer 1997 at ASU to 50 teachers in their 3 rd Modeling Workshop

PH 352-2G & PH 352L-T6: Modern Physics II Spring Semester 2014

Mechanics Physics 151

Mechanics Physics 151. Fall 2003 Masahiro Morii

Academic Affairs Assessment of Student Learning Report for Academic Year

4/21/2010. Schrödinger Equation For Hydrogen Atom. Spherical Coordinates CHAPTER 8

Quantum Mechanics- I Prof. Dr. S. Lakshmi Bala Department of Physics Indian Institute of Technology, Madras

Calculus II. Calculus II tends to be a very difficult course for many students. There are many reasons for this.

(n, l, m l ) 3/2/2016. Quantum Numbers (QN) Plots of Energy Level. Roadmap for Exploring Hydrogen Atom

Select/ Special Topics in Atomic Physics Prof. P. C. Deshmukh Department of Physics Indian Institute of Technology, Madras

Modern Physics (PHY 371)

Instructors Manual Algebra and Trigonometry, 2e Cynthia Y. Young

QM and Angular Momentum

Meeting of Modern Science and School Physics: College for School Teachers of Physics in ICTP. 27 April - 3 May, 2011

26 Group Theory Basics

PHYS304 Quantum Physics II (2005) Unit Outline

AP Physics B Course Syllabus and Framework 2011/12

Physics 342 Lecture 27. Spin. Lecture 27. Physics 342 Quantum Mechanics I

and Transitional Comprehensive Curriculum. Algebra I Part 2 Unit 7: Polynomials and Factoring


Active Learning in Upper-Division Physics

MATH 341, Section 001 FALL 2014 Introduction to the Language and Practice of Mathematics

C/CS/Phys 191 Uncertainty principle, Spin Algebra 10/11/05 Fall 2005 Lecture 13

Physics 622: Quantum Mechanics -- Part II --

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

CHEMISTRY 2H Honors General Chemistry I Fall 2013 Course Syllabus

L z L L. Think of it as also affecting the angle

1 Fundamental physical postulates. C/CS/Phys C191 Quantum Mechanics in a Nutshell I 10/04/07 Fall 2007 Lecture 12

Lecture 11 Spin, orbital, and total angular momentum Mechanics. 1 Very brief background. 2 General properties of angular momentum operators

AP Physics Curriculum Guide Scranton School District Scranton, PA

Classical behavior of magnetic dipole vector. P. J. Grandinetti

Welcome back to PHYS 3305

Testing Heisenberg s Uncertainty Principle with Polarized Single Photons

Physics 112 Spring 2014

Department of Physics & Astronomy Trent University

University of Houston-Downtown

Spacecraft Attitude Dynamics for Undergraduates

Harmonic Oscillator I

Weather Observations. Weather Observations. 1 of 10. Copyright 2007, Exemplars, Inc. All rights reserved.

Volume vs. Diameter. Teacher Lab Discussion. Overview. Picture, Data Table, and Graph

Physics Capstone. Karsten Gimre May 19, 2009

Lesson Plan Bond Prediction Tenth Grade Chemistry By Rich Wilczewski

MITOCW watch?v=pqkyqu11eta

Introduction to NMSI through Experimental Design Module 1

Review of the Formalism of Quantum Mechanics

The David P. Weikart Center for Youth Program Quality, Bringing together over fifty years of experience and the latest research,

Lecture3 (and part of lecture 4).

Student Difficulties in Understanding Probability in Quantum Mechanics

Evidence and Theory in Physics. Tim Maudlin, NYU Evidence in the Natural Sciences, May 30, 2014

EASTERN OREGON UNIVERSITY Chemistry-Biochemistry

C/CS/Phys C191 Quantum Mechanics in a Nutshell 10/06/07 Fall 2009 Lecture 12

Math 200 A and B: Linear Algebra Spring Term 2007 Course Description

SYLLABUS FORM WESTCHESTER COMMUNITY COLLEGE Valhalla, NY lo595. l. Course #: PHYSC NAME OF ORIGINATOR /REVISOR: ALENA O CONNOR

1 Algebra of State Vectors

ADVENTURES IN THE FLIPPED CLASSROOM FOR INTRODUCTORY

Unit 1 Lesson 6: Seeing Structure in Expressions

16.2 Coupling of angular momentum operators: The Clebsch Gordon coefficients and the Wigner 3j symbols. J(i) (16.62) J = i

The Postulates of Quantum Mechanics Common operators in QM: Potential Energy. Often depends on position operator: Kinetic Energy 1-D case: 3-D case

PH 425 Quantum Measurement and Spin Winter SPINS Lab 2

Making sense of how students make sense of science. Richard Steinberg City College of New York

Linear Algebra in Hilbert Space

Physics 321 Theoretical Mechanics I. University of Arizona Fall 2004 Prof. Erich W. Varnes

Calculus, Series and Differential Equations

10520EE Modern Physics Instructor: 陳明彰 LAs:??

Physics 610: Electricity & Magnetism I

ESSEX COUNTY COLLEGE Mathematics and Physics Division PHY 203 General Physics III Course Outline

Sommerfeld (1920) noted energy levels of Li deduced from spectroscopy looked like H, with slight adjustment of principal quantum number:

Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur

Physics 610: Electricity & Magnetism I

Transcription:

FROM INDUCTION TO QUANTUM SPIN: TRAINING STUDENTS TO BECOME PHYSICISTS MARCH 2010 Dedra Demaree, Oregon State U

Acknowledgements: Corinne Manogue and David McIntyre (primarily responsible for development of the QM course) The entire OSU physics dept (all curricular reform is committee-based and department-wide) Eugenia Etkina (developing ISLE and mentoring me in its use) www.physics.oregonstate.edu/portfolioswiki www.islephysics.net

The physics major at OSU 1 st year: background courses (math, chemistry) and start of intro physics 2 nd year: rest of intro physics and intro to modern physics, plus programming 3 rd year: paradigms (described next) 4 th year: capstones and independent research Other computational, lab-based courses, and so on are mixed into the 3 rd and 4 th year depending on the students area of concentration within physics

Paradigms in Physics <P P> ~12 years of curricular development, 3 rd year physics Roughly 1 st half of Griffiths level QM and E&M, classical mechanics, plus Thermo, Oscillations &Waves, Reference Frames Taught in 3 week intensive short-courses grouped by concept/math, i.e. central forces : planetary orbits and the hydrogen atom in one course Aim to develop deep knowledge of canonical problems (4 th year capstones do 2 nd half of those texts, along with math methods, optics, and statistical mechanics)

Paradigms in Physics <P P> Fast-paced, intensive structure: Students meet daily: 1 hour MWF, 2 hours T and R 2-hr blocks facilitate integrated lab experience Homeworks/labs due once or twice per week Exam is the Monday that the next paradigm starts Pedagogical tools used: Classroom designed to facilitate quick transitions between lecture, small group activities, and lab Compare and contrast activities, small white board questions, kinesthetic activities, computer simulations, small group activities, integrated labs, homework, and lecture

Paradigms in Physics <P P> Goals based reform: Teach physics as physicists think about it: concepts that broadly underlie multiple subfields Encourage mastery of concepts Teaching math just in time as applied to physics Student quote: The paradigms curriculum constructed my knowledge from a fundamental level, with each paradigm building on the last. The emphasis on big-picture learning and universal problem-solving carries over in my graduate studies today and the apace and difficulty prepared me for graduate school (a student currently in physics grad studies at the U of Illinois)

Spins Course: Quantum measurement FIRST introduction to QM, middle of 3 rd year Based on a historically important, physical experiment with tangible objects (Stern-Gerlach) Silver atoms, oven, inhomogeneous magnetic field, screen Justify mathematical calculations by applying to physical observations The math (the model) explains the observations Based in matrix mechanics, mostly spin ½ and spin 1 systems (easier math than differential equations)

Spins course content goals: Understand and analyze sequential Stern-Gerlach (SG) measurements on spin systems Analyze generic quantum problems using matrix mechanics Use time evolution to understand spin precession Analyze generic time dependent quantum problems using matrix mechanics 4 key example problems given based on above, plus finding eigenvectors/values, commutation and uncertainty, probabilities, expectation value and standard deviation

Building a solid understanding of main QM postulates 1. States are defined by kets that contain all we can know 2. Physical observables are described mathematically by operators 3. The only possible result of a measurement is an eigenvalue of the corresponding Hermitean operator 4. How to calculate the probability of obtaining a specific eigenvalue 5. The system is in a new state that is the normalized projection of the original system ket onto the ket (or kets) corresponding to the result of the measurement 6. Time evolution is determined by the Schrodinger equation

First objective: ground the students The classical result for a current loop in an inhomogeneous magnetic field is derived with student input: μ = (q/2m)l Historic motivation for SG prove Bohr model wrong Bohr model says non-zero L, so atoms should be deflected When found deflection S&G bowed to Bohr, he s right! But then why discrete if atoms are random out of oven? 5 years later, determined that these atoms have L=0, separately, spin had been postulated Experiment re-evaluated and determined to be evidence for spin Discuss Falsification: scientific process!

KEEP students grounded in the concrete! Needed to repeat daily that these are atoms QM, spin, matrix math is all VERY abstract to them Short activity: Identify what each of the following objects in the diagram represents

Second objective: get familiar with system, observations, calculations Lab 1 (day 2 of course) Investigate the effect of N (statistics review) Observing and calculating simple probabilities: do observations match theory? Observe and calculate all combinations of 2 SG devices, look for patterns

Third objective: test by expanding observations to new situations Next day students model is challenged must make sense of findings with the math then find conceptual understanding Probability calculations are easier than sense-making Conceptual understanding can come from crossed polarizers as an analogy: grounded physical observation! (a) Z X x Z

Daily refreshers: List the postulates (and how we know/evidence) Restate the physical situation Repeat SPIN is NOT physically spinning but is intrinsic angular momentum Start most days with students doing a short calculation to refresh what they just learned Have students write definitions for terminology and give examples (tying words to math)

Example of student activity Given the above: Row 1: write +> and -> in terms of +> y and -> y Row 2: show that the +> y and -> y states are orthonormal Row 3: write +> x in terms of +> y and -> y

Show one then have them do the rest: In the z-basis, use what we know about how to write the kets +> x (given below) to find the matrices S y and S x

Have them look for patterns and build understanding: As a class you ll calculate all combinations of Sx, Sy, and Sz operators acting on all the eigenstates: +>, ->, +> x, -> x, +> y, -> y, and we ll try to determine what this operation does There are 18 combinations each of you will do 2 They already learned a matrix acting on a vector linearly transforms it in the preface (pure mathematical perspective) We already used that language when introducing operators within the spins course Students need to make meaning for it themselves!

Address their curiosity: How do we know how many eigenvalues a matrix has? What is COLLAPSING? (Copenhagen vs. multiverse) What ARE operators, and what do they do? (better question: what do Hermitean operators represent?) Don t all measurements perturb a system? Is quantization odd? What is a basis, and when do we have to be in a particular one? Should some calculations be basis independent? They ask GREAT questions if given the opportunity!

Test understanding: lab 2 (day 4) Take relevant data to use probabilities to find what the initial state is working backwards! Tests math understanding complex manipulations, Euler s formula, ability to realize two angles can be possible, the need to take more data

Lab calculations are NOT easy!! (below: the easiest spin-1 unknown)

Other content (2 nd half of 3 the weeks): Time evolution: Solving Schrodinger equation for time-independent Hamiltonian Operator (matrix form) Spin precession Rabi Oscillations Neutrino Oscillations NMR Atomic Clocks 2 more labs to extend calculations to spin 1 systems

Intro to stationary States activity: Our system starts in one particular energy eigenstate at t=0, say E 2 >, how do we write the state at some later time t? How will the probability of finding the state with energy E 2 (or any energy) after time t differ from at time t=0? How will the probabilities associated with any observations of this state after time t differ from at t=0? What name might you give such a state to explain how it behaves with time?

Harder group activity: Find <Sx(t)> <Sy(t)> And <Sz(t)> For the general state ψ(t)> e i 0 2 t cos 2 e i 0 t sin 2 Then COLLECT all their work to form <S(t)> and ask: What is <S(t)>: if we start in a +>x state?, If we start in a +>y state?, If we start in a +> state? What does this describe?

Challenges: Math Many students have their first introduction to linear algebra in 1 week just before this course Statistics aren t viewed as relevant Language/Representations Many new terms, and it is difficult to speak quantum mechanics accurately Representations for QM don t always map to real space Concepts State collapse, probabilistic nature, quantization These ideas can be grounded in observations!!

Course reform: Investigative Science Learning Environment (ISLE): Teaching scientific abilities and practicing skills needed to succeed in physics in an authentic way (experimental approach) Constructivist: students know how they know what they know Goal-based reform: Representing information, conducting experiments, thinking divergently, collecting and analyzing data, constructing, modifying and applying relationships and explanations, being able to coordinate these abilities

The Spins course fits the ISLE cycle Observe: Outcome of simple SG measurements Model: Using matrix math, how to calculate probabilities and collapsed states Test: Counterintuitive Z-X-Z SG experiment Apply: Working backwards to find an initial state Observe: What Si operators do to a state j> Model: What do operators do? Test: With more sophisticated calculations Apply: to understanding the Hamiltonian How do we know? How do we construct the knowledge for ourselves? How do we apply it?

Oregon State University Intro physics Large enrollment (~200 students per lecture section) with 1 instructor and multiple 30-student labs 3 1-hour lectures per week (MWF) and 1 3-hr lab Goal-based reform: setting a foundation for scientific reasoning, problem solving skills and other practices of authentic scientists Bringing paradigms reform to the lower division ISLE is primary source for new curriculum

Example ISLE cycle in Intro physics: Induction Observe: Watch instructor move a magnet within a coil and see the induced current ASK students what else they d like to see me do (move it faster, move the coil instead ) Explain/Model: Do NOT explain the phenomenon but have students brainstorm a quasimathematical statement for inducing current Test: Try with different coils, alignments Refine models then apply: problem solving, generators Falsification: induction is NOT from having B IN loop!

ISLE is effective: HAKE plot for FCI gains We are here

Integration of ISLE and Peer Instruction Engage students in physics practices Development of a classroom community Students participate and make meaning in class to build a shared repertoire of knowledge Do student buy in to social learning and develop identities that promote productive participation?

Chance to study impact of lecture hall remodel: back to back in 2 rooms Traditional Lecture Hall Remodeled lecture hall BOTH rooms Close packed fixed seats 2 rows per tier with swivel chairs instructor circulation Multiple screens and projectors Designed to promote interactive learning FCI gain = 0.40, Surveys, Audio/video data

Changes starting Spring 2010 (April) 2 1-hr lectures, 2 hours of studio learning, 2 of lab Lecture introduces topics, can facilitate observation portion of ISLE cycle, demonstrate representations, define terminology, show quality problem solving Studio for group work and skill development Lab for testing and applying knowledge and coordinating the use of multiple skills $260k and 1.5 years of work to build studio room Open house hosted the week before I arrived here

Open house in studio classroom

Where to go next: Amelia always sat in the first two rows of class. During small group discussions in class, she frequently grouped and talked with the same students yet she did not often feel confident asserting her answer. On the occasions she spoke up in class, she more often asked questions rather than make statements she justified. Amelia got an A in PH211. GET Amelia to take ownership!

So Deep interactive-learning can take place at the upper division with very successful results A model (ISLE, and constructivism) often viewed as low-level is very deep and applicable to understanding the success of the paradigms approach Interactive-learning requires a lot of social-practices and improving effectiveness requires moving beyond traditional physics views

Practices within our classroom Problem solving and physics conventions such as language and representations Practices to support goals of ISLE Shared authority for meaning making Communicate ideas and explain understanding of physics concepts Convincing others of their reasoning Practices developed in social learning environment that switches between whole class and small group modes Transition between social learning and lecture Help other students make sense of problem/concept Maintaining positive social relationships with other students while engaging in argumentative discourse

Assessing goal implementation Researcher observes back to back lecture classes Records audio/video data of instructor and a subset of student groups Takes notes on observation rubric Researcher and Instructor both journaling after class Post-class discussions

Results: participation Ten paired small group activities in Fall 2008 coded Full Partial Non Average group size Remodeled 23% 48% 29% 2.60 Traditional 24% 50% 26% 2.80 Chi test show group work participation and group size are not statistically different in the two rooms

Results: participation comparison 100 80 60 40 20 Active Participation Mixed Participation Passive 0 1 2 3 4 5 Rem Trad Rem Trad Averaged Data Single Day

Example of participation mediator: how the instructor facilitates the activity Voting question had two possible correct answers In both classes most students quickly saw one of the correct answers In first class asked vote again, and see if you have any different ideas students did not change votes and were not engaged in follow-up discussion on other correct answer In second class asked vote again, and see if you can change your neighbor s mind students still did not change their votes, but a student chimed up to explain what happened in the group discussion and the whole class was engaged (nods, audible agreements )

Abstract At Oregon State University, we have a unique approach to upper division undergraduate physics (roughly equivalent to 2 nd and 3 rd year UCT physics courses). These courses re-arrange the traditional content to center around conceptual and mathematical ideas in physics, with the aim of having students engage in authentic practices of physics in an interactive environment. I teach the quantum measurement course, our physics majors first introduction to QM. I was hired to reform the introductory courses, and am using a curricular model that mirrors these upper division courses. I will explain this QM course, and link it to the model I am using for the introductory course reform. This will build a unified view of our 4- year program aimed at teaching skills needed for success in physics, and scaffolding our physics majors from being apprentices to practicing scientists.