๊ณผ๋ชฉ ๋…ธํŠธ

๋Œ€ํ•™์› 1ํ•™๋…„ 1ํ•™๊ธฐ์— ์ˆ˜๊ฐ•ํ•˜๋Š” ์–‘์ž์—ญํ•™1 ๊ฐ•์˜ ํ•„๊ธฐ๋“ค

๊ฐ•์˜ ์ •๋ณด

๊ต์žฌ๋กœ Sakurai ์ฑ…์„ ์ด์šฉํ•œ๋‹ค.

์ค‘๊ฐ„๊ณ ์‚ฌ 4์›” 16์ผ
๊ธฐ๋ง๊ณ ์‚ฌ 6์›” 9์ผ(์˜ˆ์ •)

๊ฒฐ์„์„ ํ•˜๊ฒŒ ๋œ๋‹ค๋ฉด ๋‹ค์Œ ๊ฐ•์˜ ์‹œ์ž‘ ์ „๊นŒ์ง€ ๋ชป ๋“ค์€ ๊ฐ•์˜์˜ ํ•„๊ธฐ๋ฅผ ๋ณด๋‚ด๋ฉด ๊ฒฐ์„ ์ ์ˆ˜๊ฐ€ ์•„๋‹ˆ๋ผ ์ง€๊ฐ ์ ์ˆ˜๋ฅผ ๋ฐ›๊ฒŒ ๋œ๋‹ค.
LMS์— ๊ฐ•์˜๋ก์„ ๋‹ค ์˜ฌ๋ ค์ฃผ์‹ ๋‹ค๊ณ  ํ•œ๋‹ค.

Week 1-4: Chap. 1 Fundamental Concepts
Week 5-7: Chap. 2 Quantum Dynamics
Week 8: Midterm Exam
Week 9-13: Chap. 3 Theory of Angular Momentum
Week 14-15: Chap. 4 Symmetry in Quantum Mechanics
Week 16: Final Exam

๊ฐ•์˜ ํ•„๊ธฐ

ํ•„๊ธฐ ๋…ธํŠธ ํ…œํ”Œ๋ฆฟ

QM lecture note - Template

์ค‘๊ฐ„๊ณ ์‚ฌ ๋ฒ”์œ„

๊ฐ•์˜ ํ•„๊ธฐ

QM lecture note - Kets, Bras, and Operators
QM lecture note - Base Kets and Matrix Representation
QM lecture note - Measurements, Observables, and the Uncertainty Relations
QM lecture note - Basis Transformation Operator
QM lecture note - Position, Momentum, and Translation
QM lecture note - Position, Momentum, and Generators
QM lecture note - Gaussian Wave Packet
QM lecture note - Time Evolution Operator
QM lecture note - Heisenberg Picture and Equations of Motion
QM lecture note - Simple Harmonic Oscillator
QM lecture note - Wave Equation and Probability Conservation
โ†’ ํ•ด์„์—ญํ•™ ๋ฒ”์œ„์ธ Hamiton-Jacobi equation ์„ค๋ช…๋„ ์ž์„ธํ•˜๊ฒŒ ๋˜์–ด ์žˆ์Œ
QM lecture note - Propagators and Path Integral
QM lecture note - Path Integral Formulation
QM lecture note - Gauge Transformations
QM lecture note - Aharonov-Bohm Effect and Magnetic Monopole

์ˆ™์ œ์™€ ์ถ”๊ฐ€ ํ•„๊ธฐ

Sakurai 1์žฅ ๋ฌธ์ œ ํ’€๊ธฐ + Homework
Sakurai 2์žฅ ๋ฌธ์ œ ํ’€๊ธฐ + Homework
QM mini note - Canonical Commutation Relation from Translation
QM mini note - Generator as Differential Operator
QM mini note - Translation Operator in Generator Eigenket Basis

์‹œํ—˜ ์กฑ๋ณด

ํ›„๋ฐฐ๋ฅผ ์œ„ํ•ด ๋‚จ๊ธฐ๋Š” ์ด๋ฒˆ ์ค‘๊ฐ„๊ณ ์‚ฌ ์กฑ๋ณด
QM midterm 2026-1

๊ธฐ๋ง๊ณ ์‚ฌ ๋ฒ”์œ„

QM lecture note - Symmetry, Conservation Laws, and Degeneracy
QM lecture note - Discrete Symmetries
QM lecture note - Time Reversal Operator

์œผ์•… ์ค‘๊ฐ„๊ณ ์‚ฌ๊ฐ€ 24์‹œ๊ฐ„๋„ ์•ˆ ๋‚จ์•˜๋‹ค!

์ด๋ชจ์ €๋ชจ ๊นจ๋‹ฌ์€ ๊ฒƒ๋“ค์„ ์จ๋ณด์ž.

Heisenberg ์šด๋™๋ฐฉ์ •์‹์—์„œ commutator๋ฅผ ์Šˆ๋ขฐ๋”ฉ๊ฑฐ ์—ฐ์‚ฐ์ž๋กœ ๊ณ„์‚ฐํ•ด๋„ ๋˜๋Š” ์ด์œ 

๊ฐ€ ์‹œ๊ฐ„ ๋ฌด๊ด€ํ•  ๋•Œ, Heisenberg ์—ฐ์‚ฐ์ž์˜ ์ •์˜๋Š”

์ด๋ฏ€๋กœ commutator๋ฅผ ์ „๊ฐœํ•˜๋ฉด:

๋Š” ์ž๊ธฐ ์ž์‹ ์˜ ํ•จ์ˆ˜์ธ ์™€ commuteํ•˜๋ฏ€๋กœ, ์ง€์ˆ˜ ์ธ์ž๋“ค์„ ๋ฐ–์œผ๋กœ ๊บผ๋‚ผ ์ˆ˜ ์žˆ๋‹ค:

๋”ฐ๋ผ์„œ ์šด๋™๋ฐฉ์ •์‹์€:

๋งŒ ๊ณ„์‚ฐํ•˜๋ฉด ๋œ๋‹ค. ์œ ๋‹ˆํ„ฐ๋ฆฌ ์ƒŒ๋“œ์œ„์น˜๋Š” ๊ฒฐ๊ณผ๋ฅผ ํ•˜์ด์  ๋ฒ ๋ฅดํฌ ์—ฐ์‚ฐ์ž๋กœ ๋ฐ”๊ฟ”์ค„ ๋ฟ์ด๊ณ , ์šด๋™๋ฐฉ์ •์‹์˜ ๊ตฌ์กฐ(์–ด๋–ค ์—ฐ์‚ฐ์ž์— ๋น„๋ก€ํ•˜๋Š”์ง€)๋Š” ๋ฐ”๋€Œ์ง€ ์•Š๋Š”๋‹ค.

์กฐ๊ฑด

๊ฐ€ ์‹œ๊ฐ„ ๋ฌด๊ด€ํ•  ๋•Œ๋งŒ ์„ฑ๋ฆฝ. ์‹œ๊ฐ„ ์˜์กด ์—์„œ๋Š” ๊ฐ€ ์ž˜ ์ •์˜๋˜์ง€ ์•Š์œผ๋ฏ€๋กœ ์ด ๋…ผ๋ฆฌ๊ฐ€ ๊ทธ๋Œ€๋กœ ์ ์šฉ๋˜์ง€ ์•Š๋Š”๋‹ค.

Free Particle: Position Operator์˜ ์‹œ๊ฐ„ ์ง„ํ™”

Heisenberg ์šด๋™๋ฐฉ์ •์‹์œผ๋กœ ๊ตฌํ•˜๊ธฐ

์ž์œ ์ž…์ž ์— Heisenberg ์šด๋™๋ฐฉ์ •์‹ ์ ์šฉ:

๋ฅผ ์ด์šฉํ•˜๋ฉด:

๋”ฐ๋ผ์„œ:

์ž์œ ์ž…์ž์—์„œ ๋Š” ๋ณด์กด๋˜๋ฏ€๋กœ ( โ†’ ), ์ ๋ถ„ํ•˜๋ฉด:

๊ทธ๋ƒฅ ์ด๊ฒŒ ๋‹ค์ž„!!!! ์ง„์งœ์ž„!!!!

๊ณ ์ „์—ญํ•™์˜ ์™€ ์™„์ „ํžˆ ๊ฐ™์€ ํ˜•ํƒœ โ€” Ehrenfest ์ •๋ฆฌ์˜ ์—ฐ์‚ฐ์ž ๋ฒ„์ „.


Eigenket์œผ๋กœ ๊ฒ€์ฆ

์˜ eigenket ์กฐ๊ฑด:

Heisenberg eigenket์€ ์ด๋ฏ€๋กœ,
-representation์—์„œ:

๋Š” ์ „ํŒŒ์ž์˜ ์ผค๋ ˆ:

๋Œ€์ž…ํ•˜๋ฉด:

์ขŒ๋ณ€ ์ •๋ฆฌ:


๊ฒฐ๊ณผ ํ•ด์„

์˜ eigenket์€ ์ž์œ ์ž…์ž ์ „ํŒŒ์ž์— ์˜ํ•ด ํผ์ ธ๋‚˜๊ฐ„ ์œ„์น˜ ๊ณ ์œ ์ƒํƒœ๋‹ค.

  • ์—์„œ ์— ์™„์ „ํžˆ ๊ตญ์†Œํ™”๋œ ์ƒํƒœ๊ฐ€ ์‹œ๊ฐ„์ด ์ง€๋‚˜๋ฉด Gaussian ํ˜•ํƒœ๋กœ ํผ์ ธ๋‚˜๊ฐ
  • ๊ทธ๋Ÿฌ๋ฉด์„œ๋„ ์—ฐ์‚ฐ์ž ์˜ eigenvalue๋Š” ๊ณ ์ „์  ๊ถค์  ๋ฅผ ๊ทธ๋Œ€๋กœ ์ถ”์ ํ•จ

Heisenberg ๊ทธ๋ฆผ๊ณผ Schrรถdinger ๊ทธ๋ฆผ์ด ์™„๋ฒฝํ•˜๊ฒŒ ์ผ๊ด€๋จ์„ ํ™•์ธ. โœ…

์ž„์˜ ์Šคํ•€ ์œ„์น˜์˜ eigen vector

Bloch sphere