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Dummy Coding and the Interaction Instead of using the contrast code CONTRREC, we could have employed a dummy code DUMMREC to represent the respeci ed two-group recommendation variable, where DUMMREC = 1 for the REC group and 0 for the NOREC group. (Recall that the group coded 0 in a dummy-coded scheme is the reference group.) The crossproduct term is BENEFITC*DUMMREC. The regression equation to be estimated in this instance is Y = b0 + b1 BENEFITC + b2 DUMMREC + b3 BENEFITC*DUMMREC (19.36)

1 X1

live more than three months. The statistics at that time of her diagnosis on the outcome of a metastasized hypernephroma, the form of kidney cancer that she had, indicated that no more than 4 in 1000 cases experienced remission from the disease, let alone cure. Now, many years after that diagnosis, Alice has no detectable signs of cancer and has been considered cured for more than 15 years. Whether her belief that the psychotherapy actually saved her life is correct is not at issue here. What is of primary interest is the rapid resolution of deep-seated problems through the use of fantasy that usually require a prolonged period of intensive psychotherapy. However, given increasing evidence of the relation of emotions to the immune system, it would be unwise to summarily reject her belief that her psychological recovery contributed to her physical recovery. It is possible that the experiential system has a relation to physical well-being much stronger than orthodox medicine recognizes. The following is one of the early fantasies described by Alice in her book: In the session preceding the fantasy, she had expressed hostility toward her mother for her mother s behavior to her during a period of extended turmoil in the household. During that period, the mother surprisingly gave birth to Alice s younger sister after denying being pregnant and attributing the change in her appearance to a gain in weight from eating too much. During the same period, the mother s mother, who shared the household with the family, and to whom the mother was deeply attached, was dying of cancer. After the session in which Alice Epstein (1989) expressed her hostility to her mother, she experienced a prolonged feeling of isolation and loneliness that lasted until she reported and discussed the following fantasy with her therapist.

To transform freely:

(18.20)

0.4 l

Alexander, F. (1950). Psychosomatic medicine. New York: Norton. American Board of Health Psychology. (1984). By-Laws, Section II. American Psychological Association Council of Representatives. (1997, August). Archival description of Clinical Health Psychology as a specialty in professional psychology. Minutes of the Council of Representatives meeting. Chicago, IL. American Psychological Association Task Force on Health Research. (1976). Contributions of psychology to health research: Patterns, problems and potentials (pp. 264 272). Washington, DC: Author. Anagnostopoulu, T. (1998). The state of health psychology in Greece. In T. McIntyre (Chair), The state of health psychology in Europe: Education and practice. Symposium conducted at the 12th Conference of the European Health Psychology Society, Vienna, Austria. Anderson, N. B. (Ed.). (1995). Health Psychology, 14(7), 588 656. Baban, A. (1998). Health psychology in Romania: Present aspects and future trends. In T. McIntyre (Chair), The state of health psychology in Europe: Education and practice. Symposium

i=1

Pr[Z < log N ] = Pr[Z < (1 )E[Z]] < e ( It is easy to verify that (21) holds whenever (1 )E[Z] = log N

where Z1 N(0, N1 ) and Z2 N(0, N2 N1 ). Extending the results of this section to the Gaussian case, we can show that the capacity region of this channel is given by R1 < C R2 < C P N1 (1 )P P + N2 , (15.240) (15.241)

Figure 1-3

This result is exact in the limit of large R, where the diffusive resistance dominates, and at small R where there is really a Maxwell Boltzmann distribution for the impinging molecules. This is true in our three-dimensional (3D) case of a small particle surrounded by a gas even when the sticking probability is less than 1 because re ected molecules are converted back into the distribution before they can strike the particle again. However, we note that the situation is very different for absorption on a plane surface where a 1D current is incident, and the question of the distribution adjacent to the surface is much more complicated [15]. It is convenient to express the mass current in this simple interpolation model as a ratio to its value in the diffusive limit: J = 4 mDRF(Int)[c ( ) c e (R)] where F (Int) = 1/[1 + (D/R Sp )(2 m/kB T )1/2 ] (3.25) (3.24)