Physics 2D Lecture Slides Lecture 16: Feb 7th 2005 Vivek Sharma UCSD Physics Bohr’s Atom: Emission & Absorption Spectra photon photon 1
Another Look at the Energy levels ⎛ ⎞ 2 2 ke Z = −⎜ ⎟ E n 2 2 ⎝ ⎠ a n 0 Rydberg Constant Atomic Excitation by Electrons: Franck-Hertz Expt Other ways of Energy exchange are also quantized ! Example: • Transfer energy to atom by colliding electrons on it • Accelerate electrons, collide with Hg atoms, measure energy transfer in inelastic collision (retarding voltage) 2
Atomic Excitation by Electrons: Franck-Hertz Expt Plot # of electrons/time (current) overcoming the retarding potential (V) Equally spaced Maxima and minima in I-V curve Δ E Δ E Atoms accept only discrete amount of Energy, no matter the fashion in which energy is transffered Bohr’s Explanation of Hydrogen like atoms • Bohr’s Semiclassical theory explained some spectroscopic data � Nobel Prize : 1922 • The “hotch-potch” of clasical & quantum attributes left many (Einstein) unconvinced – “appeared to me to be a miracle – and appears to me to be a miracle today ...... One ought to be ashamed of the successes of the theory” • Problems with Bohr’s theory: – Failed to predict INTENSITY of spectral lines – Limited success in predicting spectra of Multi-electron atoms (He) – Failed to provide “time evolution ” of system from some initial state – Overemphasized Particle nature of matter-could not explain the wave- particle duality of light – No general scheme applicable to non-periodic motion in subatomic systems • “Condemned” as a one trick pony ! Without fundamental insight …raised the question : Why was Bohr successful? 3
Prince Louise de Broglie & Matter Waves • Key to Bohr atom was Angular momentum quantization • Why this Quantization: mvr = |L| = nh/2 π ? • Invoking symmetry in nature, Louise de Broglie (Da Prince of France !) conjectured: Because photons have wave and particle like nature � particles may have wave like properties !! Electrons have accompanying “pilot” wave (not EM) which guide particles thru spacetime A PhD Thesis Fit For a Prince • Matter Wave ! – “Pilot wave” of λ = h/p = h / ( γ mv) – frequency f = E/h • Consequence: – If matter has wave like properties then there would be interference (destructive & constructive) • Use analogy of standing waves on a plucked string to explain the quantization condition of Bohr orbits 4
Matter Waves : How big, how small 1.Wavelength of baseball, m=140g, v=27m/s × − 34 h 6.63 10 . h J s λ = = = × − 34 = p 1.75 10 m mv (.14 kg )(27 m s / ) ⇒ λ <<< size of nucleus baseball ⇒ Baseball "looks" like a particle 2. Wavelength of electr on K=120eV (assume NR) 2 p ⇒ = K= 2 p mK 2m − × × -31 19 = 2(9.11 10 )(120 eV )(1.6 10 ) × -24 =5.91 10 . / Kg m s − × 3 4 6.63 10 . h J s λ = = = × − 1 0 1.12 1 0 m − × e 2 4 5.91 10 . / p kg m s ⇒ λ � Size of at o m !! e Models of Vibrations on a Loop: Model of e in atom Fractional # of waves in a Modes of vibration loop can not persist due to when a integral destructive interference # of λ fit into loop ( Standing waves) vibrations continue Indefinitely 5
De Broglie’s Explanation of Bohr’s Quantization Standing waves in H atom: Constructive interference when λ π n = 2 r h h λ = s ince = p ...... ( ) NR m v n = 3 nh ⇒ = π 2 r m v ⇒ = � n mvr Angular momentum Quantization condit io ! n This is too intense ! Must verify such “loony tunes” with experiment Reminder: Light as a Wave : Bragg Scattering Expt Range of X-ray wavelengths scatter Off a crystal sample X-rays constructively interfere from Certain planes producing bright spots Interference � Path diff=2dsin ϑ = n λ 6
Verification of Matter Waves: Davisson & Germer Expt If electrons have associated wave like properties � expect interference pattern when incident on a layer of atoms (reflection diffraction grating) with inter-atomic separation d such that path diff AB= dsin ϑ = n λ Atomic lattice as diffraction grating Layer of Nickel atoms Electrons Diffract in Crystal, just like X-Rays !! Diffraction pattern produced by 600eV electrons incident on a Al foil target Notice the waxing and waning of scattered electron Intensity. What to expect if electron had no wave like attribute 7
Davisson-Germer Experiment: 54 eV electron Beam max Max scatter angle Scattered Intensity Cartesian plot Polar Plot Polar graphs of DG expt with different electron accelerating potential when incident on same crystal (d = const) Peak at Φ =50 o when V acc = 54 V Analyzing Davisson-Germer Expt with de Broglie idea λ de Broglie for electron accelerated thru V =54V acc 2 1 2 2 p eV eV • = = = ⇒ = = = 2 ; mv K eV v p mv m 2 2 m m m If you believe de Broglie h h h h λ = = = = λ predict = p mv 2 eV 2 meV m m ⇒ λ = × − 10 F or V = 54 Volts 1.6 7 10 (de Br og lie) m acc Exptal d ata from Davisson-Germer Observation: � × -10 d =2.15 A =2.15 10 m (from Bragg Scattering) nickel θ = m ax o 50 (observation from scattering intensity p lo t ) diff φ λ Diffraction Rule : d sin = n � λ = pred ict 1.67 A Excellent � ⇒ λ meas o F o r P rincipal Maxima (n=1); = (2.15 A)(sin 50 ) agreement � λ observ =1 .65 A 8
Davisson Germer Experiment: Matter Waves ! h = λ predict 2 meV Excellent Agreeme nt Practical Application � Electron Microscope ! 9
Electron Microscope : Excellent Resolving Power Electron Micrograph Showing Bacteriophage Viruses in E. Coli bacterium The bacterium is ≅ 1 μ size West Nile Virus extracted from a crow brain 10
So Just What is Waving in Matter Waves ? • For waves in an ocean, it’s the Imagine Wave pulse moving along water that “waves” a string: its localized in time and • For sound waves, it’s the space (unlike a pure harmonic wave) molecules in medium • For light it’s the E & B vectors • What’s waving for matter waves ? – It’s the PROBABLILITY OF FINDING THE PARTICLE that waves ! – Particle can be represented by a wave packet in • Space • Time • Made by superposition of many sinusoidal waves of different λ • It’s a “pulse” of probability What Wave Does Not Describe a Particle π 2 = − ω + Φ = = π y A cos ( kx t ) , 2 k w f y λ x ,t • What wave form can be associated with particle’s pilot wave? = − ω + Φ y A cos ( kx t ) • A traveling sinusoidal wave? • Since de Broglie “pilot wave” represents particle, it must travel with same speed as particle ……(like me and my shadow) = λ Phase velocity (v ) of sinusoid a l wave: v f Single sinusoidal wave of infinite p p In Matter: extent does not represent particle Conflicts with h h λ = ( ) = a Relativity � γ localized in space p mv γ 2 E m c Unphysical = (b) f = Need “wave packets” localized h h γ 2 2 E mc c ⇒ = λ = = = > Spatially (x) and Temporally (t) v ! f c p γ p m v v 11
Wave Group or Wave Pulse • Wave Group/packet: Imagine Wave pulse moving along – Superposition of many sinusoidal a string: its localized in time and waves with different wavelengths and frequencies space (unlike a pure harmonic wave) – Localized in space, time – Size designated by • Δ x or Δ t – Wave groups travel with the speed v g = v 0 of particle • Constructing Wave Packets – Add waves of diff λ , Wave packet represents particle prob – For each wave, pick • Amplitude • Phase – Constructive interference over the space-time of particle – Destructive interference elsewhere ! localized + Resulting wave's "displacement " y = y y : 1 2 [ ] = − + − cos( ) cos( ) y A k x w t k x w t 1 1 2 2 A+B A-B Trignometry : cosA+cos B =2cos( )cos( ) 2 2 ⎡ − − + + ⎤ ⎛ ⎞ ⎛ ⎞ k k w w k k w w ∴ = − − 2 1 2 1 2 1 2 1 y 2 A ⎜ cos( x t ) ⎟ ⎜ cos( x t ) ⎟ ⎢ ⎥ ⎝ ⎠ ⎝ ⎠ ⎣ 2 2 2 2 ⎦ ≅ ≅ ≅ ≅ Δ Δ � � since k , , , k k w w w k k w w 2 1 ave 2 1 ave ⎡ Δ Δ ⎤ ⎛ ⎞ k w ∴ = − − ≡ − ' 2 ⎜ cos( ) ⎟ cos( ) y = A cos( ) , A' oscillates in x,t y A ⎢ x t kx w t ⎥ ks wt ⎣ ⎝ ⎠ ⎦ 2 2 Δ Δ ⎛ ⎞ k w t = − ' 2 ⎜ cos( ) = modulated amplit ⎟ ud e A A x ⎝ ⎠ 2 2 w = Phase Vel V ave p k ave wave Δ w = Δ Group Vel V Group g k Or packet dw : Vel of envelope= V g dk 12
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