the four functions:I'm not sure why you're talking about complex-valued functions on R here. There are different R's you might mean - the x axis, the t axis - but what's really staring us in the face are some complex-valued functions on R^2 - the plane where the variables (t,x) live.exp(i(-x -t)) exp(i(x - t)) exp(i(-x +t)) exp(i(x + t))[...] span a 4-complex-dimensional subspace of the space of *all* complex-valued functions on R.
Here I'm using the *wrong* complex structure - the one where to compute i times f(x), you just multiply using ordinary complex arithmetic. With that definition, I'm sure our four functions are linearly independent.Your four functions are all of the form
With John's *clever* complex structure, I get a little confused. Do we really have four independent vectors, or am I seeing double?
exp(-i(wt - kx))
where w is the energy and k is the momentum, as usual. Let me Fourier transform and think of them as delta functions in (w,k) space, living at the following four points:
(w,k) = (1,1) (w,k) = (1,-1) (w,k) = (-1,1) (w,k) = (-1,-1)These span a little 4-complex-dimensional subspace of the space of complex-valued functions on the lightcone in Fourier transform land. 
Now, there are two interesting complex structures on this vector space.
The *stupid* complex structure is just the obvious one: multiplication by i.
The *clever* complex structure is multiplication by i in the cases where (w,k) lives in the forwards lightcone, and multiplication by -i on the backwards lightcone:
\ / \ / <------ forwards lightcone (w >= 0) \/ /\ / \ <------ backwards lightcone (w <= 0) / \In both cases we have a 4-dimensional complex vector space: only the complex structure is different.
Now, however, let us turn to the physics. We are studying the wave equation, but we have to decide what we are studying: *real* solutions of the wave equation, or *complex* solutions. The advantage of talking about *real* solutions is that it's it's obvious that we have to do something clever to get the right complex structure: ordinary multiplication by i isn't even available. So let's see what the above has to do with *real* solutions of the wave equation.
First of all, not every function in our little four-dimensional complex vector space corresponds to a real solution of the wave equation! There's a subspace of functions that do, which has *real* dimension four. It has a basis given by these functions:
leftward rightward --------- -------- sin(-t - x) sin(-t + x) cos(-t - x) cos(-t + x)Now, if you hit one of these functions with the *stupid* complex structure - that is, if you just multiply it by i - it won't be real any more, obviously. But if you hit it with the *clever* complex structure it stays real, I claim.
Well, being quantum field theorists, we go to Fourier transform land to do our serious thinking... it's much less crowded there. If you take the Fourier transform of a real function f(t,x), its value at (w,k) is the complex conjugate of its value at (-w,-k). If we take a function on the lightcone with this property and hit it with the stupid complex structure, it loses this property! But if we hit it with the clever complex structure, it still has this property. QED.
That was supposed to make it all obvious, but if it didn't, let's do an example. Take one of our real solutions of the wave equation, say
f = sin(-t + x)
and write it out using our basis of complex exponentials:
sin(-t + x) = exp(i(-t + x))/2i - exp(-i(-t + x))/2i
Now let's hit it with the clever complex structure, which we call J. The first term is the Fourier transform of a guy living on the forwards lightcone, while the second is the Fourier transform of a guy living on the backwards lightcone, so we multiply the first by i and the second by -i, and we get:
Jf = exp(i(-t + x))/2 + exp(-i(-t + x))/2 = cos(-t + x)Yes! A real-valued solution! And it's a wave moving in the same direction, rightward.
That's how it always goes, even in higher dimensions. When we we take a real solution of the wave equation and hit it with the clever complex structure, it stays real. If we start with a sine or cosine wave moving in a given direction, hitting it with the clever complex structure gives a similar wave moving in the same direction, with the same energy and momentum.
We already knew that, actually: on eigenstates of the Hamiltonian, the complex structure is just evolution backwards in time a quarter period. For example, if we evolve
sin(-t + x)
backwards in time by a quarter period, we get
cos(-t + x)
 If you complain that a delta function is not a function, let me remind you that this is physics. Either learn to live with inaccuracy, or take "function" to mean "distribution".