Peaks, Passes and Pits From Topography to Topology (via Quantum Mechanics)

Slides:



Advertisements
Similar presentations
From Quantum Mechanics to Lagrangian Densities
Advertisements

Eric Prebys, FNAL.  We have focused largely on a kinematics based approach to beam dynamics.  Most people find it more intuitive, at least when first.
An old friend with a new twist!
Vector integrals Line integrals Surface integrals Volume integrals Integral theorems The divergence theorem Green’s theorem in the plane Stoke’s theorem.
The electromagnetic (EM) field serves as a model for particle fields
A journey inside planar pure QED CP3 lunch meeting By Bruno Bertrand November 19 th 2004.
Prolog Line, surface & volume integrals in n-D space → Exterior forms Time evolution of such integrals → Lie derivatives Dynamics with constraints → Frobenius.
1 Electromagnetism We want to apply the reaction theory developed in the first few lectures to electronuclear interactions. It is worthwhile reviewing.
Kalman Filtering, Theory and Practice Using Matlab Wang Hongmei
2.5 Conductors Basic Properties of Conductors Induced Charges The Surface Charge on a Conductor; the Force on a Surface Charge
COVARIANT FORMULATION OF DYNAMICAL EQUATIONS OF QUANTUM VORTICES IN TYPE II SUPERCONDUCTORS D.M.SEDRAKIAN (YSU, Yerevan, Armenia) R.KRIKORIAN (College.
Standard Model Requires Treatment of Particles as Fields Hamiltonian, H=E, is not Lorentz invariant. QM not a relativistic theory. Lagrangian, T-V, used.
The electromagnetic (EM) field serves as a model for particle fields  = charge density, J = current density.
EEE340Lecture : Magnetic Forces and Torques A moving charge q with velocity in a magnetic field of flux density experiences a force This equation.
PAEN - 2nd Section Stability of structures Methods Initial Imperfections.
02/19/2014PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
10 Lecture in calculus Projects Surfaces Flux Substitution Perpendicularity.
Chapter 3 Phase Transitions and Chemical Reactions.
Monday, Apr. 2, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #12, 13, 14 Monday, Apr. 2, 2007 Dr. Jae Yu 1.Local Gauge Invariance 2.U(1) Gauge.
Deformable Models Segmentation methods until now (no knowledge of shape: Thresholding Edge based Region based Deformable models Knowledge of the shape.
Quantum Two 1. 2 Time Independent Approximation Methods 3.
Chapter 8 Conservation Laws 8.1 Charge and Energy 8.2 Momentum.
Math 3120 Differential Equations with Boundary Value Problems
Maxwell’s Equations If we combine all the laws we know about electromagnetism, then we obtain Maxwell’s equations. These four equations plus a force law.
Maksimenko N.V., Vakulina E.V., Deryuzkova О.М. Kuchin S.М. GSU, GOMEL The Amplitude of the Сompton Scattering of the Low-Energy Photons at Quark-Antiquark.
Wednesday, Feb. 28, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #9 Wednesday, Feb. 28, 2007 Dr. Jae Yu 1.Quantum Electro-dynamics (QED) 2.Local.
Dr. Hugh Blanton ENTC Energy & Potential Dr. Blanton - ENTC Energy & Potential 3 The work done, or energy expended, in moving any object.
Geometrical Optics LL2 Section 53. Local propagation vector is perpendicular to wave surface Looks like a plane wave if amplitude and direction are ~constant.
Wednesday, Mar. 5, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #13 Wednesday, Mar. 5, 2003 Dr. Jae Yu Local Gauge Invariance and Introduction.
SPECIALIST MATHS Differential Equations Week 1. Differential Equations The solution to a differential equations is a function that obeys it. Types of.

“Significance of Electromagnetic Potentials in the Quantum Theory”
Landau Theory Before we consider Landau’s expansion of the Helmholtz free Energy, F, in terms of an order parameter, let’s consider F derived from the.
Seminar on Computational Engineering by Jukka-Pekka Onnela
Basis The concept of a basis is critical for quantum chemistry. We can represent any wavefunction using the basis of our choice. The basis we choose is.
The first pair of Maxwell’s equations Section 26.
Announcements Generalized Ampere’s Law Tested I I Consider a parallel plate capacitor that is being charged Try Ampere’s modified Law on two nearly identical.
Monday, Mar. 10, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #14 Monday, Mar. 10, 2003 Dr. Jae Yu Completion of U(1) Gauge Invariance SU(2)
A.Sako S.Kuroki T.Ishikawa Graduate school of Mathematics, Hiroshima University Graduate school of Science, Hiroshima University Higashi-Hiroshima ,Japan.
Monday, Apr. 4, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #16 Monday, Apr. 4, 2005 Dr. Jae Yu Symmetries Why do we care about the symmetry?
In this chapter we will introduce the following concepts:
3.1 Laplace’s Equation Common situation: Conductors in the system,
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Nanoelectronics Chapter 3 Quantum Mechanics of Electrons
LORENTZ AND GAUGE INVARIANT SELF-LOCALIZED SOLUTION OF THE QED EQUATIONS I.D.Feranchuk and S.I.Feranchuk Belarusian University, Minsk 10 th International.
Quantum Two 1. 2 Time-Dependent Perturbations 3.
Syed Ali Raza Supervisor: Dr. Pervez Hoodbhoy. A brief Overview of Quantum Hall Effect Spinning Disk Spinning Disk with magnetic Field Kubo’s Formula.
§1.6 Green’s functions; Helmholtz Theorem Christopher Crawford PHY
Chapter 3 Postulates of Quantum Mechanics. Questions QM answers 1) How is the state of a system described mathematically? (In CM – via generalized coordinates.
Wednesday, Apr. 6, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #17 Wednesday, Apr. 6, 2005 Dr. Jae Yu Symmetries Local gauge symmetry Gauge.
Differential Equations
Lecture from Quantum Mechanics. Marek Zrałek Field Theory and Particle Physics Department. Silesian University Lecture 6.
Wednesday, Nov. 15, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #19 Wednesday, Nov. 15, 2006 Dr. Jae Yu 1.Symmetries Local gauge symmetry Gauge.
Electromagnetic Theory
Canonical Quantization
SLOPE FIELDS & EULER’S METHOD
SLOPE FIELDS & EULER’S METHOD
§2.4 Electric work and energy
Gravity-Khovanov Homology-QFT
Construction of a relativistic field theory
Time-Independent Perturbation Theory 1
§2.4 Electric work and energy
Quantum One.
First Order Nonlinear ODEs
The propagation of waves in an inhomogeneous medium
Quantized K
Quantum mechanics II Winter 2011
Relativistic Classical Mechanics
PHYS 3446 – Lecture #19 Symmetries Wednesday, Nov. 15, 2006 Dr. Jae Yu
Classical Principles of Electromagnetism
Presentation transcript:

Peaks, Passes and Pits From Topography to Topology (via Quantum Mechanics)

James Clerk Maxwell,

1861 – “On Physical Lines of Force” 1864 – “On the Dynamical Theory of the Electromagnetic Field” 1870 – “On Hills and Dales” hilldale.pdf

Scottish examples

Peak Pass Pit

Critical points of a function on a surface Peaks (local maxima) Passes (saddle points) Pits (local minima) Can identify by looking at 2 nd derivative “Topology only changes when we pass through a critical point”.

Basic theorem (# Peaks) – (# Passes) + (# Pits) = Euler Characteristic (V-E+F) Euler Characteristic is a topological invariant; 2 for the sphere; 0 for the torus. Does not depend on which Morse function we choose!

The Hodge equations The Euler characteristic can also be obtained by counting solutions to certain partial differential equations – the “Hodge equations”. They are geometrical analogs of Maxwell’s equations! To see how PDE can relate to topology, think about vector fields and potentials…

The physics connection Ed Witten, Supersymmetry and Morse Theory, 1982

Witten’s method Consider the Hodge equation as a quantum mechanical Hamiltonian. Different types of ‘particle’ according to the Morse index (‘peakons, passons and pitons’). Euler characteristic given by counting the low energy states of these particles.

Perturbation theory Replace d by e sh d e -sh, where h is the Morse function and s is a real parameter. This perturbation does not change the number of low energy states. But it does change the Hodge equations!

In fact, it introduces a potential term, which forces our particles to congregate near the critical points of appropriate index. The potential is s 2 |  h| 2 + sX h where X h is a zero order vectorial term.

The term X h has a ‘zero point energy’ effect which forces each type of particle to congregate near the critical points of the appropriate index; ‘peakons’ near peaks, ‘passons’ near passes and so on.

Thus the number of low energy n-on modes approaches the number of critical points of index n, as the parameter s becomes large. Appropriately formulated, this proves the fundamental result of Morse theory; peaks – passes + pits = Euler characteristic.

James Clerk Maxwell,