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PH427 are periodic oscillations ubiquitous or merely just a paradigm? Paradigm: Periodic Systems...
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Transcript of PH427 are periodic oscillations ubiquitous or merely just a paradigm? Paradigm: Periodic Systems...
PH427PH427are are periodicperiodic oscillations ubiquitous oscillations ubiquitous
or merely just a paradigm?or merely just a paradigm?
Paradigm: Periodic Systems
Instructor: Matt GrahamTA: Rabindra Bajracharya
Winter 2015
PH427 …smaller goal:
full mathematical description of physically & eletronically
coupled “stuff”
BIG GOAL: show how symmetry, oscillations and quantum mechanics really describe “everyday stuff”
35% problem sets (3)
15% pick a “solid state physics” journal article, give a 10 min. talk
50% final exam (M of exam week)
Roadmap
DAYS 1- 7: •Coupled pendulum, railroad cars, atoms, etc •Coupled LC resonators (HW #1)•Atoms is crystals extend coupling to infinity and define a dispersion relation for atomic system
DAYS 7- 15: •Quantum wavestates in periodic systems•10 minute journal presentations
Translational Symmetry and Noether’s Theorem
Graphene
Any system with translational symmetry has an associated momentum conservation law.
An electron moving through a perfectly periodic crystal maintains its momentum like the electron was travelling though a vaccuum
Graphene
Draw the “Unit Cell”
Graphene
Draw the “Unit Cell”
Draw the “Unit Cell”
Celtic knot Protein/DNA
Draw the “Unit Cell”
Celtic knot Protein/DNA
PERIODIC SYSTEM IN BIOLOGY:Light Harvesting Complex II
Bacterial Light Harvesting
Bahatyrova, et al.Nature (2004) 430 1058
Hu, et al. J. Phys. Chem. B (1997) 101 3854
“Beats” in Motion of Coupled Oscillator
2sin ab
2sin ab
1
2
Chain of Many (N) Spring-Coupled Masses
m m
m n n-1 n+1
Two Masses Connected to Hooke’s Law Springs
m1 m2
Positive direction
Force on m1: 121211 F
Force on m2: 211222 F
Low frequency mode: mlow
Symmetric mode: A1 = A2
High frequency mode:mhigh
122
Antisymmetric mode: A1 = A2
From Fig. 8.3, I. G. Main,Vibrations and Waves inPhysics
symmetric mode (low frequency)
anti-symmetric mode (high frequency)
5 Mass Chain – Mode n=1 = 12a k = 2 6a
5 Mass Chain – Mode n=2 = 6a k2 = 2 3a
2k
5 Mass Chain – Mode n=3 = 4a k3 = 2 2a
3k
5 Mass Chain – Mode n=4 = 3a k4 = 2
3a4k
5 Mass Chain – Mode 5 = 12a/5 k5 =
2a5k
5 Mass Chain – Mode 6 = 2a k6 = 2a
6k
5 Mass Chain – Mode 7 = 12a/7 k7 =
2a7k
5 Mass Chain Dispersion Relation
M m
m n n-1 n+1
M M
a
Diatomic chain, 16 masses, 8 unit cells
Dispersion Relation for m =1, M = 2
0.2
0.4
0.6
0.8
1
1.2
-2 0 2
22
411112
ak
MmmMmMopt sin
22
411112
ak
MmmMmMac sin
Dispersion Relation for m = 1, M = 1.1
0.2
0.4
0.6
0.8
1
1.2
-2 0 2k
opt
opt
Amplitude (m)/Amplitude (M) (m = 1, M = 2)
-4
-2
0
2
4
-2 0 2
opt
ac
Amplitude (m)/Amplitude (M) (m = 1, M = 1.1)
-4
-2
0
2
4
a
-2 0 2k
opt
ac
Damped Wave in Forbidden Frequency Range(Evanescent Wave)
maxmax
maxcosh
12n
n e