From: WWalker on
Eric,

I am sorry to insist, but it does not matter what the reason is. If I have
a communication link that allows me to transmit a pulse over a distance
faster than a light propagated pulse, then the pulse propagates faster than
light. If I use the pulse to denonate a bomb located a distance away, the
bomb will explode sooner than if the pulse propagated at the speed of
light. This is absolutly true and cannot be argued. The only question is if
the dipole simulation demonstrates that a pulse can be detected over a
distance faster than light. I think it has.

The Andor circuit is only phase shifting the signal so that it appears the
signal outputs before it is sent. The proof is that you can not use the
circuit to turn itself off before the message was sent, thereby preventing
the message from being sent in the first place. This is clearly shown in
Fig. 7. Also note that in my dipole system the pulse always arrives after
it is sent, not before as in Andor's circuit.

Figure 2 in the Sten paper is showing the propagation of a pulse in the
nearfield using the transverse electric field, where I and talking about
the magnetic field component and my signals always arrive at the detector
after they are sent, not before. Note the transverse electric field pulse
in Fig 2b arrives before the signal was sent. This is because the
transverse field is being created 1/4 wavelength outside the source and
propagates both back toward the dipole and away from the source. At
distances larger than the 1/4 wavelength the pulse is seen to propagate
away from the dipole. If you plot Stens group speed Eq. 18 you can clearly
see this. Refer my paper Eq. 72, and plot Fig.14. An animation showing this
is shown in Fig. 20, 21, 23


William


>On 3/28/2010 4:24 AM, WWalker wrote:
>> Eric,
>>
>> I think you are missing the point. Refering to the Low Pass Filtered
Pulse
>> simulation I posted, the simulation clearly shows that if I transmit a
>> pulse, the pulse edge arrives sooner than if it had propagated faster
than
>> light. If my detector at the receiving end is threshold detector which
is
>> set to look for anything above the noise level, it will fire earlier
than
>> if the pulse had propagated at light speed. In other words, it shows
that
>> if I push a button launching the narrowband pulse signal and propagate
it
>> via a dipole to a nearfield receiver with the threshold detector, the
>> pressed button will be detected sooner than a light propagated signal.
This
>> clearly shows that an action (informaton) in this nearfield dipole
system
>> can be detected faster than light. If this is true than I have proven
my
>> point that information propagtes faster than light in the nearfield of
a
>> dipole.
>>
>> William
>
>I get the impression that you either haven't read or haven't understood
>any of our previous dialogue.
>
>What you are seeing appears consistent with a phase advance of a
>bandlimited signal, not accelerated propagation. The same sort of
>bandlimited pulse is shown, and I'm sure everybody is getting weary of
>me citing these same references over and over again, with apparent
>acceleration in Andor's blog (Figures 4 and 5) and in Sten's paper (Fig.
>2.a).
>
>Both show apparent arrival of the output pulse before the input, but it
>is only a small phase advance of the signal due to the nature of the
>medium (i.e., an unusual group delay). Both authors acknowledge this.
> You do not. Andor demonstrated, pretty clearly, that the system is,
>in fact, causal, by turning off the input signal and observing the
>output signal end in Fig. 7. This is why people here have been trying
>to get you to do something similar, because otherwise the logical
>explanation is that there's just a slight phase advance in the signal.
>
>
>--
>Eric Jacobsen
>Minister of Algorithms
>Abineau Communications
>http://www.abineau.com
>
From: Eric Jacobsen on
On 3/28/2010 11:40 AM, WWalker wrote:
> Eric,
>
> I am sorry to insist, but it does not matter what the reason is. If I have
> a communication link that allows me to transmit a pulse over a distance
> faster than a light propagated pulse, then the pulse propagates faster than
> light.

I suppose you can argue semantics here about what defines the "pulse",
but understand that "information" is not propagating faster than light
in any of the examples, and neither is energy. This seems to be the key
point that must be understood. A simple small phase advance of a
signal is NOT indicative of information exceeding the speed of light.

If you just want to claim that the signal has phase advanced and appears
to arrive earlier than expected, that's fine, I don't think anyone will
argue with you there. That's what has led to discussion and study on
this topic in many places.

> If I use the pulse to denonate a bomb located a distance away, the
> bomb will explode sooner than if the pulse propagated at the speed of
> light. This is absolutly true and cannot be argued. The only question is if
> the dipole simulation demonstrates that a pulse can be detected over a
> distance faster than light. I think it has.

If you want to wave your hands about the definition of the pulse, sure.
If you want to claim that actual information has been accelerated,
then, no. You've demonstrated something that's been known for a long
time, that bandlimited signals have a predictable quality than can be
exploited. That's not new.

> The Andor circuit is only phase shifting the signal so that it appears the
> signal outputs before it is sent. The proof is that you can not use the
> circuit to turn itself off before the message was sent, thereby preventing
> the message from being sent in the first place. This is clearly shown in
> Fig. 7. Also note that in my dipole system the pulse always arrives after
> it is sent, not before as in Andor's circuit.

The relevant part of the argument is that the signal arrives before
expected. Whether the acceleration is due to negative group delay or
phase velocity or some other mathematical arrangement, the point is that
a bandlimited signal can appear to be predicted by fairly simple
processes. The circuit in Andor's example isn't very complicated. The
mechanisms by which the dispersion or phase response is affected in the
near field of an antenna doesn't appear to be out of that realm at all.
The key point is that there is a straightforward explanation that
doesn't involve non-causality or propagation faster than light.

So when somebody comes along and shows the exact same sort of small
phase advance associated with bandlimited prediction and says, "this
proves propagation faster than c!", it cannot be taken as true by anyone
who knows of the more likely explanation. There is a very large burden
of proof that goes with such a claim, and I haven't seen anything that
would indicate to me a single step past the ordinary explanation.


> Figure 2 in the Sten paper is showing the propagation of a pulse in the
> nearfield using the transverse electric field, where I and talking about
> the magnetic field component and my signals always arrive at the detector
> after they are sent, not before. Note the transverse electric field pulse
> in Fig 2b arrives before the signal was sent. This is because the
> transverse field is being created 1/4 wavelength outside the source and
> propagates both back toward the dipole and away from the source. At
> distances larger than the 1/4 wavelength the pulse is seen to propagate
> away from the dipole. If you plot Stens group speed Eq. 18 you can clearly
> see this. Refer my paper Eq. 72, and plot Fig.14. An animation showing this
> is shown in Fig. 20, 21, 23

Perhaps what you think you're demonstrating is the mechanism by which
the system achieves the same sort of bandlimited prediction experienced
in a negative group delay filter. Again, that's far, far more
believable than propagation faster than c, especially when it's a known
and understood phenomenon.

Yet again let me point out that a discontinuity like that shown in
Andor's analysis might be able to be measured through your system. It's
clear you're not trying to show causality, but propagation. So why not
demonstrate the discontinuity propagating faster than c? I'd think it'd
be a good experiment and might reveal something useful about the system.

I think until you can demonstrate something like that the more likely
explanation of bandlimited prediction would be expected to prevail.


--
Eric Jacobsen
Minister of Algorithms
Abineau Communications
http://www.abineau.com
From: glen herrmannsfeldt on
WWalker <william.walker(a)n_o_s_p_a_m.imtek.de> wrote:

> I am sorry to insist, but it does not matter what the reason is. If I have
> a communication link that allows me to transmit a pulse over a distance
> faster than a light propagated pulse, then the pulse propagates faster than
> light. If I use the pulse to denonate a bomb located a distance away, the
> bomb will explode sooner than if the pulse propagated at the speed of
> light. This is absolutly true and cannot be argued. The only question is if
> the dipole simulation demonstrates that a pulse can be detected over a
> distance faster than light. I think it has.

No it doesn't.

A narrow band pulse has to build up slowly. If it has a sudden
edge then it necessarily has a wide bandwidth. A common case
is a wave packet with a Gaussian envelope. With such a pulse,
there is some signal long before the main part of the pulse, and
that can be detected. There are materials that can amplify the
leading edge of a pulse, and attenuate the rest. The result is
a new pulse that seems to have gone faster than c. If you try
to use it for information transmission, though, you will find
that it does not violate special relativity.

-- glen
From: Jerry Avins on
Eric Jacobsen wrote:

...

> I think until you can demonstrate something like that the more likely
> explanation of bandlimited prediction would be expected to prevail.

Even allowing the unlikely possibility that the 6-degree phase advance
*in the near field* represents a real speed increase, and that the
"pulse" in the far field is expected to show no advance at all, What
practical use can this have?

Jerry
--
Discovery consists of seeing what everybody has seen, and thinking what
nobody has thought. .. Albert Szent-Gyorgi
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From: steveu on
>On 3/28/2010 11:40 AM, WWalker wrote:
>> Eric,
>>
>> I am sorry to insist, but it does not matter what the reason is. If I
have
>> a communication link that allows me to transmit a pulse over a distance
>> faster than a light propagated pulse, then the pulse propagates faster
than
>> light.
>
>I suppose you can argue semantics here about what defines the "pulse",
>but understand that "information" is not propagating faster than light
>in any of the examples, and neither is energy. This seems to be the key
>point that must be understood. A simple small phase advance of a
>signal is NOT indicative of information exceeding the speed of light.
>
>If you just want to claim that the signal has phase advanced and appears
>to arrive earlier than expected, that's fine, I don't think anyone will
>argue with you there. That's what has led to discussion and study on
>this topic in many places.

Now you're getting to the crux. Information is energy. Real physical
energy. Not virtual photons, and other smoke and mirrors. Its real physical
energy of the kind that gets water hot. Show energy flow faster than light
and you've shown information flow faster than light. Fail, and you
haven't.

>> If I use the pulse to denonate a bomb located a distance away, the
>> bomb will explode sooner than if the pulse propagated at the speed of
>> light. This is absolutly true and cannot be argued. The only question is
if
>> the dipole simulation demonstrates that a pulse can be detected over a
>> distance faster than light. I think it has.

Bombs dissipate real physical energy. This is why nobody disputes the
carriage of information - typically the news that someone is seriously
pissed off. Until the energy starts to dissipate, the information has not
arrived (although side channel information, like seeing the bomb fly over,
may well arrive earlier). Demonstrate an energy flow faster than light, and
we'll all be amazed, and you'll be rich.

Steve