Page 14 - Unlikely Stories 1
P. 14

Perils of Scanference



        It  shows  possible  and  impossible  zones  for  all  world  lines  passing
        through one point in space-time. That point is B , in the center lying
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        in a hypersphere of the present—three-dimensional space  flattened
        to  a  plane  on  the  diagram;  time,  the  fourth  dimension,  runs
        perpendicular to it. The cones formed by the possible space-time to
        which  B   could  be  connected  flow  into  it  from  the  past  and away
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        from  it  into  the  future.  That  absolute  perimeter  is  formed  by  the
        speed of light, the limiting velocity in space-time. Any point outside
        those cones is inaccessible to B : the latter can have no knowledge of
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        the former. Possible world lines are called time-like; impossible ones
        are space-like, requiring faster than light movement through space-
        time. Do you follow that?

        Gen. Esel: For the moment.
        Dr. Silberfisch: One particular world line we shall call A B C . You
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        can see that B  could have been arrived at from other A points in its
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        past, and proceeded to other C points in its future. Of course, the
        farther away that line gets from the vertical in this diagram, the faster
        the  movement  between  two  points.  Electromagnetic  signals  are
        traveling  on  the  surface  of  the  cones:  light  from  the  most  distant
        interstellar  objects,  reaching  us  after  billions  of  years,  help  us
        establish the parameters of the past. But that is not relevant here.
        Gen. Esel: Thank you. I don’t need a lecture in cosmology.

        Dr. Silberfisch: Certainly. Now presuming we are at B , as I said, we
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        can imagine coming to it from any of several A possibilities close to
        A0. Similarly, all the subsequent possibilities for B , its C future, if
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        you  will,  would  be  clumped  around  the  only  one  we  actually  do
        experience, called C . All other possibilities for B  in the hypersphere
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        of C ’s present are simultaneously and automatically excluded, just as
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        going from one C point to another and from one A point to another
        are impossible. Each  present  knows only one  past, and  can  be  the
        only  past  known  by  its  future—that  is,  until  Gibbons  came  along.
        Now, look at this second diagram.


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