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Subatomic Physics

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172 Structure of <strong>Subatomic</strong> Particles<br />

x f(x)<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1<br />

x<br />

Figure 6.22: Plot of parton distribution functions, f(x), times x, as a function of x for the proton.<br />

From PDG.<br />

we will discuss in more detail in Chapter 10. The decrease in the ratio of F2 for<br />

0.2 � x � 0.7 is now known to be, at least in part, due to the binding of the nucleon<br />

in the nucleus and the increase beyond x ≈ 0.7 is caused by the motion of these<br />

bound nucleons (see Chapter 16). (58) Is this the complete explanation, or are there<br />

subtle differences between a bound and free nucleon? Is a nucleon somewhat larger<br />

(say ∼ 5%) in a nucleus than when free? Such questions have been raised and the<br />

so-called EMC effect remains of keen interest, because it has not yet been fully<br />

explained.<br />

6.11 More Details on Scattering and Structure<br />

The material in Sections 6.3–6.10 demonstrates that much information concerning<br />

subatomic structure can be obtained from scattering experiments. Even a glance at<br />

a differential cross section, without detailed computation, can reveal gross features.<br />

As an example, the information contained in Figs. 6.3, 6.5, 6.11, and 6.13 is reproduced<br />

schematically in Fig. 6.24. It highlights one difference between heavy nuclei<br />

and nucleons: Typical heavy nuclei have well-defined surfaces; as in optics, interference<br />

effects then produce diffraction minima and maxima in the differential cross<br />

section. Nucleons, in contrast, do not have such surfaces; their density decreases<br />

smoothly, and they do not show prominent diffraction effects.<br />

The Scattering Amplitude In the present section, we shall treat scattering in<br />

somewhat more detail than we have done before. A glance at any current book on<br />

scattering (59) will show that the material presented here constitutes only a minute<br />

58 D.F. Geesaman, K. Saito, and A.W. Thomas, Annu. Rev. Nucl. Part. Sci. 45, 337 (1995).<br />

59 M. L. Goldberger and K. M. Watson, Collision Theory, Wiley, New York, 1964; R. G. Newton,<br />

Scattering Theory of Waves and Particles, McGraw-Hill, New York, 1966; L. S. Rodberg and R. M.

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