Abstract

Introduction to Average Hamiltonian Theory. I. Basics,

A. Brinkmann*,
Concepts Magn. Reson. A (2017), in press for the special issue in honor of Alex Bain.

Figure from paper

Understanding the dynamics of electron or nuclear spins during a magnetic resonance experiment requires to solve the Schrödinger equation for the spin system considering all contributions to the Hamiltonian from interactions of the spins with each other and their surroundings. In general, this is a difficult task as these interaction terms can be both time-dependent and might not commute with each other. A powerful tool to analytically approximate the time evolution is average Hamiltonian theory, in which a time-​independent effective Hamiltonian is taking the place of the time-dependent Hamiltonian. The effective Hamiltonian is subjected to the Magnus expansion, allowing to calculate the effective Hamiltonian to a certain order. The goal of this paper is to introduce average Hamiltonian theory in a rigorous but educational manner. The application to two composite pulses in NMR spectroscopy is used to demonstrate important aspects of average Hamiltonian theory.

Dr. Andreas Brinkmann
Measurement Science and Standards
National Research Council
1200 Montreal Road, M-40
Ottawa, Ontario K1A 0R6
Canada
Tel. +1-613-990-0319
Fax. +1-613-990-1555
Andreas.Brinkmann@nrc-cnrc.gc.ca
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