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Magnetic resonance imaging (MRI) is based on the science of nuclear magnetic resonance (NMR). Magnetic resonance states that certain atomic nuclei (such as the protons in water molecules) can absorb and emit radio-frequency energy when placed in an external magnetic field. The emitted energy is proportional to important physical properties of a material such as proton density. Therefore in physics and chemistry, magnetic resonance is an important method for studying structures of chemical substances, and its discoverers were awarded the Nobel Prize in Physics in 1952.
In man-made environments, most objects of interest are rich in regular, repetitive, symmetric structures. Figure 15.1 shows images of some representative structured objects. An image of such an object clearly inherits such regular structures and encodes rich information about the 3D shape, pose, or identity of the object.
This book is about modeling and exploiting simple structure in signals, images, and data. In this chapter, we take our first steps in this direction. We study a class of models known as sparse models, in which the signal of interest is a superposition of a few basic signals (called “atoms”) selected from a large “dictionary.” This basic model arises in a surprisingly large number of applications. It also illustrates fundamental tradeoffs in modeling and computation that will recur throughout the book.
In the previous chapters, we have studied how either a sparse vector or a low-rank matrix can be recovered from compressive or incomplete measurements. In this chapter, we will show that it is also possible to simultaneously recover a sparse signal and a low-rank signal from their superposition (mixture) or from highly compressive measurements of their superposition (mixture). This combination of rank and sparsity gives rise to a broader class of models that can be used to model richer structures underlying high-dimensional data, as we will see in examples in this chapter and later application chapters. Nevertheless, we are also faced with new technical challenges about whether and how such structures can be recovered correctly and effectively, from few observations.
In Chapter 8, we introduced optimization techniques that efficiently solve many convex optimization problems that arise in recovering structured signals from incomplete or corrupted measurements, using known low-dimensional models. In contrast, as we saw in Chapter 7, problems associated with learning low-dimensional models from sample data are often nonconvex: either they do not have tractable convex relaxations or the nonconvex formulation is preferred due to physical or computational constraints (such as limited memory). In this chapter, we introduce optimization algorithms for nonconvex programs.