I did not want to go classical to quantum without due cause, as it is an 
intellectual arms race, but once you start referring to particles as 
having individual wavelengths, you are talking quantum, and I must 
respond like Pakistan.  My apologies.
    The easiest way to point out the problems with finding an exact 
position is wavelength is the notorious Heisenberg uncertainty 
principle. I almost hesitate to bring it up as it is the only element of 
quantum physics that has made it into pop physics, (along with e=mc^2 
and that bit about Galileo dropping things off the Tower of Pisa)and 
thus is the most misunderstood theorum of quantum physics, as all the 
others are merely unknown.  This is not because it is complex, it is 
because people tell lies about it (or perhaps .2 Truths).  
Unfortunately I have no mathematical symbols at my disposal, so words 
must do.
The uncertainty principle states that it is impossible to precisely 
measure a particle's momentum and position simultaneously.  If one is 
measured precisely, the other becomes unbounded.  This has practical 
significance towards the question of whether a photon is or is not blue 
according to whether it lies within the range of 540-560 nm. As the 
wavelength of the photon may lie arbitrarily close to the cutoff point 
of 540 nm, the wavelength must be specified to infinite precision. The 
wavelength of a photon is determined by the relationship x=h/E, where x 
is the wavelength, h is Planck's constant, and E is energy.  I will 
further translate E into mc^2(which describes all aspects of momentum 
but the direction).  x=h/mc^2.     Planck's constant is constant, as is 
the speed of light.  The wavelength is therefore determined by the mass 
variable.  The observational task at hand is to pin down the mass to 
infinite precision so that it can be determined whether or not the 
stated photon is or is not blue.  However, once you have accomplished 
this the position of the photon becomes unbounded!  Since the photon is 
just as likely to be in the Andromeda galaxy as on the surface of the 
Earth, I do not think it possible to draw any conclusions about the 
color of the sky from your precise measurement of wavelength.
In practice both precision and momentum can be constrained to a very 
small range, although there is always a remote possibility (assuming 
non-infinite precision of momentum) that a photon emitted from your 
flashlight will end up in the Andromeda Galaxy. In our blueness 
defintion this suggests that there is actually some ambiguity at every 
wavelength, although in most cases infitesimally small.  We can perceive 
blue because the cones in our eyes are tolerant to small fluctuation of 
wavelength,and the sheer number of photons that enter our eyes make 
precise positions unimportant due to statistical mass.
>> The change 
>> over time destroys any attempt at certainty.
>Hardly.  We can see this from a macroscopic example: if I lead you in a
>simple waltz on the Mexican border facing north, my left foot will be 
in
>America during the first measure and in Mexico on 2 and 3 of the second
>measure.  (Ignore the fence.)  It will truly be wherever it is at any
>given time, however. 
The question is not the truth value at points well within boundries. It 
is what truth value to prescribe exactly at the border.  I will not try 
to extend the analogy to your macroscopic example,as feet are not point 
particles and will overlap the border.  Photons, when well behaving, are 
point particles and do not cause this sort of confusion.
>
>
>>       In fact, it seems that allowing for a discrete range of 
blueness 
>> has made the ambiguity twice as bad.  If blue was defined as light 
with 
>> a wavelength of 550nm, at almost every point the Tarskian truth value 
of 
>> the statement 'le laser est bleu' would be false, except at 550nm 
which 
>> would be ambigous.  By creating a range, there is an area of clear 
>> truth, clear falsehood, and TWO ambigous points.  It does not seem to 
me 
>> that Tarskian logic is the path to finding absolute truth if there 
are 
>> necesarily ambiguities wherever one tries to draw boundries. Indeed, 
the 
>> only way to create a genuinely universal Tarskian logic statement 
would 
>> be by defining blue as being the set of all wavelengths, i.e., an 
>> infinite statement.
>As noted, in light of the above definition, this discussion of 
ambiguity
>is fishy.  Since particles have a discrete location at a given time, 
and
>since their instantaneous velocities ARE given by calculus, there's no
>ambiguity at all on the Newtonian scale.
 
  Unfortunately Newtonian physics had to be abandoned because it does 
not adequately explain the behavior of light (and other things, but 
light was the initial problem).  Your explanation works slightly better 
because it is not Newtonian.  Photons cannot have frequencies 
independent of other photons within Newtonian physics.
       The gist of my argument is that when attempting to map all 
statements (in a metalanguage) onto the world, wherever boundries are 
drawn there will be fundamentally unavoidable ambiguities.  At some 
point (in this case at the points of 540 and 560 nm), it will be 
impossible to give a truth value of either true or false.  I suppose if 
you insist on maintaining the Tarskian diagram, you could say "le laser 
est bleu' is Truly True or False, but I don't think this is what Tarsky 
had in mind! If you find multivalence truly abhorrent, I find no 
objection to making a Tarskian diagram with three Truth values, True, 
False, and Ambiguous (or Not Applicable).  However, as I pointed out 
above, the uncertainty principle would make Ambiguous the correct Truth 
value at every point (each photon may or may not be blue). While 
accurate, it doesn't do much good to anybody.
You could get around the problem of Ambiguity by redefining blue in 
terms of complex numbers, but your new defintion would not bear any 
relation to what anybody else thought of as blue.
 
   -Christian Whitaker
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