Introduction to Spin, Magnetic Resonance and Polarization

T. Niinikoski
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Abstract

In this chapter, we shall review the mathematical formalism required for the understanding of the spin physics of polarized targets. Particular focus is given to the problems treating the situations that are favorable for obtaining high polarizations: high magnetic field and low lattice temperature. In the following sections we shall first discuss the concept of the spin and magnetic moment and work out in detail some standard quantum mechanical problems involving these variables. The quantum statistics of a system of spins is then overviewed, before briefly introducing the thermodynamics of spin systems. Most of these can be found in well-known textbooks of quantum mechanics, such as those of Dicke and Wittke [1] and of Landau and Lifshitz [2], and of magnetic resonance, such as Abragam [3], Goldman [4], Abragam and Goldman [5] and Slichter [6]. The main justification for presenting textbook material is that we need to make frequent reference to this basic formalism. Three further reasons are:
自旋、磁共振和极化导论
在本章中,我们将回顾理解极化目标的自旋物理所需要的数学形式。重点讨论了在高磁场和低晶格温度条件下有利于获得高极化的处理问题。在下面的章节中,我们将首先讨论自旋和磁矩的概念,并详细地计算出涉及这些变量的一些标准量子力学问题。然后概述自旋系统的量子统计,然后简要介绍自旋系统的热力学。这些都可以在著名的量子力学教科书中找到,如Dicke和Wittke [1], Landau和Lifshitz[2],以及磁共振教科书,如Abragam [3], Goldman [4], Abragam和Goldman[5]和Slichter[6]。呈现教科书材料的主要理由是我们需要经常引用这个基本的形式主义。进一步的三个原因是:
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