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Note that (Yi - y)/(x i - x) is the slope of the line between the central point (x, y) and the data point (Xi' yJ Thus the slope ~ of the estimated regression line is a kind of average of these slopes. More precisely, it is a weighted average. Note that the weights Wi are nonnegative and their sum is 1. (An ordinary average is the special case of a weighted average in which all the weights are equal to lin.) Each data point is weighted proportionally to the square of its x-distance from the center. This implies that data points far from the center of the data have a large influence on the estimate of the slope of the regression line.

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In the reversecopy function, we attempt to copy each char in from into the corresponding position in string to (Ignore the fact that this is not the best way to do it) Clearly, if operator [ 1 returns a value, then to [ i 1 cannot appear on the left-hand side of the assignment statement Thus operator [ ] should return a reference But then even though from is a constant string an expression such as from [ i ] =to [ i ] would still compile because from [ i ] would be a simple reference and thus modifiable Oops!

7 Grand Unification The electroweak SU(2) X U(l) gauge theory is in impressive agreement with experiment However, does it really unify the electromagnetic and weak interac-.

A string ~lass1 bool operator==( const string 2 { 3 return strcrnp( 1hsc-str( 4 1 5 6 bool operator!=( const string

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& ) ,

lhs, const string rhsc-str(

tions The SU(2) X U(1) gauge group is a product of two disconnected sets of gauge transformations: the SU(2) group with coupling strength g and the U(1) group with strength g'. Therefore, these two couplings are not related by the theory; and, as we know from 13, their ratio g' = tan Ow

Formal Justification of the Formulas. Suppose a and b are candidates for the regression estimates and ~. Using the line Y= a + bX, the sum of squares of the residuals is L(Yi - a - bxY. Considering this as a function of a and b, its minimum can be found by using calculus. Take the partial derivatives with respect to a and b, and solve for the values of a and b that

== 0 ;

lhs, const string rhsc-str(

(15.44)

8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29

return strcmp( 1hsc-str(

{3 = 0

!= 0;

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has to be measured experimentally. Only if the SU(2) and U(I) gauge transformations are embedded into a larger set of transformations G can g and g' be related by the gauge theory. Symbolically, we write

, rhsc-str (

return strcrnp( 1hsc-str(

G::) SU(2) X U(I),

i:: (1) E 80 (1)

< 0;

bool operator<=( const string i return strcmp( 1hsc-str(

lhs, const string rhsc-str(

(15.45)

<= 0 ;

... ::s '" '"

return strcmp( 1hsc-str(

and some of the new transformations in the group G will link the previously disconnected SU(2) and U(1) subsets of gauge transformations. So, g and g' are related by a number (actually a Clebsch-Gordan coefficient of G) whose value depends on the choice of "unifying" group G. In the quest for the" ultimate" theory, it seems natural to attempt to unify strong interactions with the electroweak SU(2) X U(I) interaction. That is, we seek a group G that also contains the color gauge group S U(3) which successfully describes the strong interactions. Let us speculate that such a "grand unified group" G exists. Then (15.45) would be generalized to some grand unified group

rhsc-str(

> 0;

& ) ,

G::) SU(3) X SU(2) X U(I),

70 60 50

lhs, const string rhsc-str(

return strcrnp( 1hsc-str(

(15.46)

>= 0 ;

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