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Interestingly, even though Yahoo! owns all of these search engines, they each operate independently. So if you search HotBot (which is powered by Inktomi), you get different results than if you search AllTheWeb or AltaVista. Also interestingly, Yahoo! does not use any of the search engines it owns to power the search results on its own Web site. It uses Google for that. (Why Because they had a contract before Yahoo! went on its acquisition spree.) So who s left to compete with the Yahoo!/Inktomi/Overture/AllTheWeb/ AltaVista combination Well, there s Google, of course (and it competes quite well, thank you). There s also Ask Jeeves, which owns the Teoma search

li(r)

Fig. 9.3 The" statistical potential" between particles in an ideal gas arising from the symmetry properties of the N-particle wave function.

The simplest form of variable declaration is to list it within a class's attri bute compartment Underlining the attribute indicates the static nature of the variable The visibility of an attribute is indicated by preceding the attribute with + for public, # for protected, and - for private

right side of (9.53) by 1 [/;]. To the same order of approximation, however, we can also write 1 where

[Ii]

[1(1

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engine. Finally, in terms of directory results, you also have LookSmart and the Open Directory. What does this matter to you Not much, probably. But if Yahoo! does start con solidating its search holdings, it s possible that you ll end up with less search choices than you ve had in the past. Until that happens, enjoy the fact that if you can t find what you want on one site, there s still other sites to search even if most of them all happen to be owned by Yahoo!. But don t get confused by all this search engine ownership stuff (it s easy to do). HotBot, which is powered by Inktomi (which is owned by Yahoo!), is not owned by Yahoo!. HotBot is owned by Terra Lycos. Yahoo! doesn t own Terra Lycos. So Yahoo! doesn t own HotBot. It just owns the company that provides HotBot s primary search results. Got all that

Figure 4 - 3

Ii]) =

(-f3 [Vi})

(9.56)

This form of declaration may come about for basic data that is needed for the class Such variables do not generally have any specific significance from a broader modeling perspective Examples include variables you require for storing basic pieces of information that make an object what it is, variables required for internal logic, and so on Such variables are based on objects that usually cannot be decomposed further

== - kT log 1 Ii] = - kT log 1 exp -

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I". ( 2'7Tlr-rf)]

(9.57)

Variables may also manifest themselves due to an object's relationships with other objects (for example, a collection of some sort) We discuss such relationships and their usage in the " Representing Relationships " section later in this chapter

with the plus sign for bosons and the minus sign for fermions. Therefore an improvement over (9.55) is the formula

(9.58)

This shows that the first quantum correction to the partition function of an ideal gas has the same effect as that of endowing the particles with an interparticle potential* v(r) and treating the problems classically. The potential v(r) is attractive for bosons and repulsive for fermions, as illustrated in Fig. 9.3. In this sense we sometimes speak of the "statistical attraction" between bosons and the "statistical repulsion" between fermions. It must be emphasized, however, that v(r) originates solely from the symmetry properties of the wave function. Furthermore, it depends on the temperature and thus cannot be regarded as a true interparticle potential.

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