Light Cone Coordinates Explained

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Light cone coordinates are defined by the equations x^{+}= \frac{1}{\sqrt{2}} (x^{0}+x^{1}) and x^{-}= \frac{1}{\sqrt{2}} (x^{0}-x^{1}). These coordinates illustrate how light travels from the origin along the defined axes, emphasizing the relationship between time and space in relativistic physics. A light curve being zero in this system indicates that light emitted from the origin moves along the axes defined by x^{+}=0 and x^{-}=0. This framework parallels Cartesian coordinates, where specific axes are represented by zero values. Understanding these coordinates is crucial for grasping the behavior of light in spacetime.
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Hi guys, I'm trying to understand light cone coordinates for which I uploaded this picture. The light cone coordinates are given by
x^{+}= \frac{1}{\sqrt{2}} (x^{0}+x^{1})
x^{-}= \frac{1}{\sqrt{2}} (x^{0}-x^{1})

Now how should I think of this? I guess the space curves do only life in the space that is spanned by the x^{0} and x^{1}[/latex] axes. But what does it mean that a light curve is zero in this coordinate system?
 

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It means that a flash of light emitted at the origin travels along the two axes (because we chose them that way - that's what makes these coordinates "light-cone" coordinates). One axis is described by the equation ##x^{+}=0## and the other by ##x^{-}=0##, just as in Cartesian coordinates the y-axis is described by ##x=0## and the x-axis by ##y=0##.
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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