Physics 2 - Lecture 7: Quantum Mechanics - Huynh Quang Linh

CONTENTS
• Wave – Particle Duality of Matter
• De Broglie’s Hypothesis – Matter wave
• Diffraction of electron wave by single slit
• Heisenberg’s Uncertainty Principle
“„Quantum mechanics‟ is the description of the
behavior of matter and light in all its details and, in
particular, of the happenings on an atomic scale.
Things on a very small scale behave like nothing that
you have any direct experience about. They do not
behave like waves, they do not behave like particles,
they do not behave like clouds, or billiard balls, or weig 
pdf 22 trang thamphan 02/01/2023 880
Bạn đang xem 20 trang mẫu của tài liệu "Physics 2 - Lecture 7: Quantum Mechanics - Huynh Quang Linh", để tải tài liệu gốc về máy hãy click vào nút Download ở trên.

File đính kèm:

  • pdfphysics_2_lecture_7_quantum_mechanics_huynh_quang_linh.pdf

Nội dung text: Physics 2 - Lecture 7: Quantum Mechanics - Huynh Quang Linh

  1. QUANTUM MECHANICS Tran Thi Ngoc Dung – Huynh Quang Linh – Physics A2 HCMUT 2016
  2. CONTENTS • Wave – Particle Duality of Matter • De Broglie’s Hypothesis – Matter wave • Diffraction of electron wave by single slit • Heisenberg’s Uncertainty Principle
  3. “Double-slit” Experiment for Electrons  Electrons are accelerated to 50 keV l = 0.0055 nm  Central wire is positively charged bends electron paths so they overlap  A position-sensitive detector records where they appear.  << 1 electron in system at any time [A. TONOMURA (Hitachi) pioneered electron holography] Exposure time: 1 s 10 s 5 min 20 min
  4.  M (x,y,z) r Electromagnetic Wave: z k z Consider a light plane wave, O v propagating in the z direction: Wave function at point O: o = A cos (t) Wave function at point M: (M, t)=A cos ((t-z/v)) =Acos(t-kz) (M,t) Acos(t k.r) in complex description : Ψ(M,t) Ae-i(t-k.r)  wavenumber : : complex wavefunction i(t-k.r)   2 2 Ψ(M,t) Ae  k with theconvention : Ψ(M,t) Re Ψ(M,t) v vT l    2 real realpart of complex wave wavevector :k n wave function function l n : unit vector
  5. Wave function of a monochromatic wave Wave function of a electromagnetic monochromatic wave i(t k.r) (M,t) oe Wave function of a free particle of momentum p and kinetic energy E: i (Et p.r) i(t k.r)  (M,t) oe oe
  6. DIFFRACTION OF ELECTRONS BY 2 SLITS
  7. The statistic meaning of the Wave Function of a particle: Intensity of Light is proportional to the square of the amplitude of the wave at that point: I=kA2 (W/m2) Intensity of Light is proportional to the photon density at that point. I=e.c =N. hf.c 2 1 2 1 B e: energy density of electromagnetic wave. (J/m3) e oE 2 2  N : photon density (photon/m3) o IA2 N The amplitude squared of the wave is proportional to the photon density => proportional to probability of finding the photon per unit volume. For the matter wave , the amplitude squared of the wave is the probability of finding the particle per unit volume= probabilty density 2 * 2 | (r,t) | (. ) o
  8. Constraints on Wavefunction In order to represent a physically observable system, the wavefunction must satisfy certain constraints: (x,t) - Must be a single-valued function - Must be normalizable. This implies that the wavefunction approaches zero as x approaches infinity. - Must be a continuous function of x. - the first derivative of (x,t) must be continuous
  9. HEISENBERG’S UNCERTAINTY PRINCIPLE OF POSITION AND MOMENTUM The uncertainty in the x position x. p h x a a x x a Consider the diffraction of electrons by 2 2 a single slit. The uncertainty in the x-component of the momentum : x 0 px psin q px psin q l è sin q a q x a h l h p p psin q . x x l a a h x. p a. x a x. px h
  10. x 5 10 11m   x. p p x 2 x 2 x  p 1.055 10 24(kg.m / s) x min 2 x  p 1.055 10 24(kg.m / s) x min 2 x p 1.055 10 24(kg.m / s) p2 (1.055 10 24)2 KE 6.1 10 19 J 3.82eV 31 2me 2 9.1 10