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Security patterns are an evolving sub-discipline within the pattern community. This book is the first compilation of security patterns contributed by the pattern community. The scope of potential security patterns and the changing nature of security issues are such that we cannot address all security problems in a single book. The mining of new security patterns therefore will remain an important activity for the future. The main goal is to define the overall landscape of security patterns and to provide a significant start toward making solutions available. We ask you to use the security patterns that are documented here. Use them to improve the security of your organization and to improve the design of your applications and systems. In doing so, we ask that you evaluate them and determine whether they could be improved. Although many people, both authors and reviewers, have contributed and tried hard to deliver high-quality patterns, there is always room for improvement. Give us feedback if you find blind spots, or if you feel that a particular detail is missing or could be made more specific. When you use security patterns and get used to the benefits of applying patterns, you might identify your own patterns. Share them with others and integrate them. We recommend highly that you visit a pattern conference, in part to experience the spirit of patterns personally. During shepherding and writer s workshops, groups of



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c 8(k. t) = ik 1\ A(k, t),

see (9.25). The four-momenta are given in (12.71). The constituent cross sections, (12.69) and (12.70), are therefore

534 16

(5.94)





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and the longitudinal component of the electric field depends only on the scalar potential: (5.95) 1I(k, t) = -ikU(k, t). So the vector potential is rid of all redundant degrees of freedom, with the scalar potential being determined completely by the dynamic variables of the charged particles. This is the great advantage of the Coulomb gauge. There are. however. some disadvantages. The Coulomb gauge is not so well suited to the relativistic theory because it is not manifestly covariant8 [108. 314J. Moreover. the instantaneous Coulomb scalar potential raises a causality question [108.314]. We do not address this problem here. I refer the reader to Brill and Goodman [75J or Cohen-Tannoudji et al. [108J for a detailed discussion. Now we show that the canonical variables of our system are ra. Pa. A(k, t), and II(k, t). where Pa and II(k, t), the conjugate momenta of ra and A(k, t), respectively. are given by

experienced software engineers take a critical look at candidate patterns. This helps to ensure that both the structure and the content of patterns are useful for potential readers.

----;;r'

(5.96) (5.97)

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If you would like to give us feedback or submit a new pattern candidate, send us an e-mail to book@securitypatterns.org. Over time, accompanying material for the book, as well as errata, will be made available at our security patterns site, which can be accessed at the following URL:

II(k, t)

(12.73)

[Abrams95]

. A(k, t).

1 { qa 2m a Pa - -;;

/L+d) = G 2 XS(1 _ y)2. ."

M. Abrams, S. Jajodia, H. Podell, eds., 1995: Information Security An Integrated Collection of Essays, IEEE Computer Society Press, January 1995

", e d kA(k, t) (211")3/2

[ACL]

+ C.c.]

(12.74)

d 3 k {II*(k, t) . II(k, t)

[ACM] [Ack03] [AD01]

+ c2 k 2 A*(k, t) . A(k, t)},

The appropriate vq -+ /Lq' center-of-mass energy is XS, where now S refers to vN -+ /LX (see Exercise 9.3). Using these results, together with the nucleon structure functions J;(x) introduced in 9, we can calculate the deep inelastic vI' N -+ /L X cross section. To confront these parton model predictions with experiment, it is simplest to take an isoscalar target, in which the nuclei contain equal numbers of protons and neutrons. The neutrinos interact only with d or u quarks. They therefore measure

ACM: http://www.acm.org R. Ackermann: Gateways and Components for Supplementary IP Telephony Services in Heterogeneous Environments, PhD Thesis, July 2003 C. J. Alberts, A. J. Dorofee: SEI, OCTAVE Criteria, Version 2.0, CMU/SEI2001-TR-016, December 2001

(5.98)

where the first term on the right-hand side of (5.98) is the minimal coupling term describing the interaction with matter. Hamilton equations of motion for the discrete variables {ra, Pa} are obtained from the Hamiltonian H by [108]

[ADE+99] [ADV] [AfB1999]

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