Interference Pattern versus SR

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SUMMARY

The discussion centers on the implications of Special Relativity (SR) in the context of a double-slit experiment involving two frames of reference (FOR). The ground observer perceives two slits opening simultaneously, resulting in an interference pattern, while the moving observer sees the slits open sequentially, leading to confusion about the existence of the pattern. Both observers ultimately agree on the interference pattern due to the invariance of light reaching the same point on the screen, despite differing interpretations of the events. The conversation highlights the importance of relative simultaneity and the interpretation of quantum mechanics in understanding these phenomena.

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  • #61
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  • #62
Thanks a lot Mike, I may need some time to analyse your post, Thanks once again for everyone
 
  • #63
JDoolin said:
On Wikipedia http://en.wikipedia.org/wiki/Scalar_(physics)

It says: In physics, a scalar is a simple physical quantity that is not changed by coordinate system rotations or translations (in Newtonian mechanics), or by Lorentz transformations or space-time translations (in relativity).
This actually seems quite confusing because what is scalar in classical physics (3D-scalar) is vector in relativity (where scalars are defined in respect to 4D-spacetime) as we can describe 3D-space using (timelike) vector that is normal to that space and module of vector being scalar in that 3D-space.

And seems even more complicated about 4D-scalars in 3D-space plus time.
 
  • #64
zonde said:
This actually seems quite confusing because what is scalar in classical physics (3D-scalar) is vector in relativity (where scalars are defined in respect to 4D-spacetime) as we can describe 3D-space using (timelike) vector that is normal to that space and module of vector being scalar in that 3D-space.

And seems even more complicated about 4D-scalars in 3D-space plus time.

Part of the confusion comes from the fact that we should have three different definitions for length, namely,

(length1) the length of the meter-stick measured as the space-time interval between simultaneous events in the meter-stick's reference frame

(length2) the length of the meter-stick measured as the space-time interval between simultaneous events in the observer's reference frame

(length3) the coordinate distance Δx between two events

AND we seem to have two different definitions for scalar

(scalar1) Any single numeric quantity; i.e. can be represented in one-dimension.

(scalar2) Any quantity that is not changed by rotation or Lorentz Transformation

The first definition of length qualifies as a scalar either way, because it is a single number, AND it is Lorentz Invariant, but the second and third definitions of length are observer dependent, and will change under Lorentz Transformation.

Edit: I left off one definition of length:

(length4) The space-time interval Δs between two events
\Delta s=\sqrt{\Delta x^2+\Delta y^2+\Delta z^2-c^2 \Delta t^2}
This one is also a scalar according to both definitions of scalar.
 
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  • #65
Thanks, MikeLizzi.

You've given me a couple of ideas to play around with,

and Thanks Mentz

I will get back to you.

I hope I'll be able to put something together to clarify these ideas. I'm dreaming of a full-blown two-slit interference demo with arbitrary velocities of source, slits, and screen, complete with cross-sectional space-time diagram, showing just exactly why and how that interference pattern is invariant,
 
  • #66
https://www.physicsforums.com/attachment.php?attachmentid=43147&stc=1&d=1327565161

It is a bit different from the original experiment, but still need to work it out.
The source emits 2 beams of light at the same time. For the ground observer, her sees the slit A and B open simultaneously, so the pattern will form on his screen at the defined point to the left side. For the slit observer, the slit B opens before slit A initially to receive the beam from its right hand labeled in red. While, ultimately, the slit A should open first to release it to go to screen.
So which slit should open first?
And are you sure that the phase-difference is zero for the slit observer considering the whole paths?

It was a quick hit, I know, so i have to think about it again,,,
 

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  • #67
By the way, the slit is moving downward in the direction of the short black arrow
 
  • #68
Picking through the sarchastic replies, I can't seem to parse the answer to this question?

Does the ground observer see an interference pattern through the one open slit on the train?, if so, isn't that disturbingly close to a forbidden preferred frame of reference?
 
  • #69
Adel Makram said:
https://www.physicsforums.com/attachment.php?attachmentid=43147&stc=1&d=1327565161

It is a bit different from the original experiment, but still need to work it out.
The source emits 2 beams of light at the same time. For the ground observer, her sees the slit A and B open simultaneously, so the pattern will form on his screen at the defined point to the left side. For the slit observer, the slit B opens before slit A initially to receive the beam from its right hand labeled in red. While, ultimately, the slit A should open first to release it to go to screen.
So which slit should open first?
And are you sure that the phase-difference is zero for the slit observer considering the whole paths?

It was a quick hit, I know, so i have to think about it again,,,

If one observer sees the slits opening and the light goes through, then it will be so for all observers. It's the worldlines coinciding and that is absolute. If you add invariance of phase differences, it's obvious that all observers see the same pattern.
 
  • #70
spikenigma said:
Picking through the sarchastic replies, I can't seem to parse the answer to this question?

Does the ground observer see an interference pattern through the one open slit on the train?, if so, isn't that disturbingly close to a forbidden preferred frame of reference?

It's been stated several times that all observers will see the same thing. If the observer at rest in the frame of the apparatus sees a pattern, so will all observers. It's the worldlines ...
 
  • #71
Mentz114 said:
If one observer sees the slits opening and the light goes through, then it will be so for all observers. It's the worldlines coinciding and that is absolute. If you add invariance of phase differences, it's obvious that all observers see the same pattern.

Thanks for being back again!

So can i understand from that the simultaneous opening of A & B when the light goes through relative to the ground observer will be the same for the slit one? then where is the relativity?

And where is the answer to the question, which slit will open first for the slit-observer?
 
  • #72
Adel Makram said:
https://www.physicsforums.com/attachment.php?attachmentid=43147&stc=1&d=1327565161

It is a bit different from the original experiment, but still need to work it out.
The source emits 2 beams of light at the same time. For the ground observer, her sees the slit A and B open simultaneously, so the pattern will form on his screen at the defined point to the left side. For the slit observer, the slit B opens before slit A initially to receive the beam from its right hand labeled in red. While, ultimately, the slit A should open first to release it to go to screen.
So which slit should open first?

Your image is wrong. See attachment for corrected version. You are forgetting that source and screen are in motion.
 

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  • #73
Adel Makram said:
Thanks for being back again!

So can i understand from that the simultaneous opening of A & B when the light goes through relative to the ground observer will be the same for the slit one? then where is the relativity?

And where is the answer to the question, which slit will open first for the slit-observer?
Within certain constraints, it is possible to get interference if the slits are never simultaneously open in the ground frame nor the slit frame. It is also possible to see interference if either slit opens first.

So it doesn't matter which slit opens first, there would still be interference if the other slit opened before all the light from the early opener reached the screen.

If these constraints are satisfied all observers will see interference, maybe only for a short time.

If the openings are too far apart in time, every observer sees 2 spots of light.
 
  • #74
zonde said:
Your image is wrong. See attachment for corrected version. You are forgetting that source and screen are in motion.

you are right, i was about to change it any way,,, but there is still another challenge:
The accumulated phase between the source and the screen is the same for both ground and slit-observer, yet the phase at the slits is different. For the ground observer, the phase at A and B must be the same, while it is not the case as recorded by the slit-observer!

So if the phase is a scalar quantity, its value should be invariant at the time the light leaves the slit?
 
  • #75
https://www.physicsforums.com/attachment.php?attachmentid=43153&stc=1&d=1327589224

The phase will be the same at 2 slits ( A & B) only and only if:

λ/c = d/v

where λ is the wavelength of the light, d is the distance between 2 slits relative to the ground observer and v is the velocity of the slits

But this is a special case only which ensures the phase of 2 light beams will be equal at the time they hit the 2 slits, while for a ground observer, the phase will always be equal
 

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  • #76
Adel Makram said:
It is a bit different from the original experiment, but still need to work it out.
The source emits 2 beams of light at the same time. For the ground observer, her sees the slit A and B open simultaneously, so the pattern will form on his screen at the defined point to the left side. For the slit observer, the slit B opens before slit A initially to receive the beam from its right hand labeled in red. While, ultimately, the slit A should open first to release it to go to screen.
So which slit should open first?
And are you sure that the phase-difference is zero for the slit observer considering the whole paths?
The slits should open simultaneously in the reference frame of othe slits in order for the interference pattern to appear on the screen. The observers will then see what's displayed on the screen and all observers will see the interference pattern. It is irrevelant whether they see if the slits open at the same time or not. The observers do not observe the light directly but after the light is reflected from the screen in the bright spots.
 
  • #77
Adel Makram said:
The accumulated phase between the source and the screen is the same for both ground and slit-observer, yet the phase at the slits is different.
So what? The interference pattern depends on the phase at the screen, not at the slit.

Adel Makram said:
So if the phase is a scalar quantity, its value should be invariant at the time the light leaves the slit?
The phase is invariant, but the time is not.
 
  • #78
DaleSpam said:
So what? The interference pattern depends on the phase at the screen, not at the slit.

The phase is invariant, but the time is not.

If, the phase of the wave is represented by a single wave front, then the difference between the time of slit opening relative to the slit-observer depends on the the distance between the slits, the velocity of the source and the perpendicular distance between the slit and the source. While the difference in time according to Lorentz transformation depends on the distance between the slits and the velocity of the source only!

So how that could be conceived?

look at a similar nice demonstration from Mike

http://www.relativitysimulation.com/Documents/DoubleSlit.htm
 
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  • #79
Tantalos said:
The slits should open simultaneously in the reference frame of othe slits in order for the interference pattern to appear on the screen. The observers will then see what's displayed on the screen and all observers will see the interference pattern. It is irrevelant whether they see if the slits open at the same time or not. The observers do not observe the light directly but after the light is reflected from the screen in the bright spots.

As i understood from this discussion that the slits need not to be open simultaneously for the FOR of slits in order to see the pattern. The original experiment emphasize that the slits should open simultaneously relative to the ground observer only
 
  • #80
Adel Makram said:
If, the phase of the wave is represented by a single wave front, then the difference between the time of slit opening relative to the slit-observer depends on the the distance between the slits, the velocity of the source and the perpendicular distance between the slit and the source. While the difference in time according to Lorentz transformation depends on the distance between the slits and the velocity of the source only!

So how that could be conceived?

look at a similar nice demonstration from Mike

http://www.relativitysimulation.com/Documents/DoubleSlit.htm

That doesn’t read like what I was showing. I my reference, the slits would have to be opened at the same time (according to the FOR of the slit observer). That’s because I chose a wave front that was created when the source was directly opposite the slits and equidistant from both (according to the FOR of the slit observer). Of course the geometry is different in the FOR of the source.

Also the Lorentz transformation does not apply to light. In my reference the geometry/speed/time of source and slit are transformed using the Lorentz transformation, but not the geometry/speed of the light wave.

And, in general, I avoided writing about interference patterns because I don’t believe an observer would see anything on the other side of the slits. The material from which the slit is made is not reflective. The instrument would not work if it were. The material is supposed to be completely absorbent, no? So only photons with a clear line-of-sight path through the slit will make it out the other side. Trying to get an interference pattern from your setup where the source is moving with respect to the slits would seem to be impossible.
 
  • #81
MikeLizzi said:
Also the Lorentz transformation does not apply to light.
Yes, it does. The whole point of the Lorentz transform is that Maxwells equations re invariant under it.
 
  • #82
Adel Makram said:
If, the phase of the wave is represented by a single wave front, then the difference between the time of slit opening relative to the slit-observer depends on the the distance between the slits, the velocity of the source and the perpendicular distance between the slit and the source. While the difference in time according to Lorentz transformation depends on the distance between the slits and the velocity of the source only!
I haven't checked Mike's math, but again, so what? Differences in time are not frame invariant, so the fact that they are different in two frames is not surprising.
 
  • #83
MikeLizzi said:
That doesn’t read like what I was showing. I my reference, the slits would have to be opened at the same time (according to the FOR of the slit observer). That’s because I chose a wave front that was created when the source was directly opposite the slits and equidistant from both (according to the FOR of the slit observer). Of course the geometry is different in the FOR of the source.

Also the Lorentz transformation does not apply to light. In my reference the geometry/speed/time of source and slit are transformed using the Lorentz transformation, but not the geometry/speed of the light wave.

And, in general, I avoided writing about interference patterns because I don’t believe an observer would see anything on the other side of the slits. The material from which the slit is made is not reflective. The instrument would not work if it were. The material is supposed to be completely absorbent, no? So only photons with a clear line-of-sight path through the slit will make it out the other side. Trying to get an interference pattern from your setup where the source is moving with respect to the slits would seem to be impossible.

https://www.physicsforums.com/attachment.php?attachmentid=43180&stc=1&d=1327671188

Here is the setup of my experiment
 

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  • #84
DaleSpam said:
I haven't checked Mike's math, but again, so what? Differences in time are not frame invariant, so the fact that they are different in two frames is not surprising.

If the accumulative phase given the whole paths and the absolute value of the phase at A & B are invariant, then the different time of opening of slits would depend also on the geometry of the setup including the perpendicular distance to the source which is not a variable in a LT
 
  • #85
Perhaps you can show mathematically what your concern is, because I don't see any problem from your English descriptions.
 
  • #87
DaleSpam said:
Yes, it does. The whole point of the Lorentz transform is that Maxwells equations re invariant under it.

Ooops. So what is the formal way of saying "you can't transform the position or shape of a light sphere" using the Lorentz transformation because it is traveling at the speed of light and gamma is undefined".
 
  • #88
Adel Makram said:

Oh, your statement on that diagram is wrong. Your diagram shows the sequence of events if the slit is moving with respect to the observer. A does not open before B relative to the slit observer. A opens before B relative to the light source observer.

Disregard above. I misunderstood your diagram. Something is wrong with it. I'll get back to you.
 
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  • #89
MikeLizzi said:
Ooops. So what is the formal way of saying "you can't transform the position or shape of a light sphere" using the Lorentz transformation because it is traveling at the speed of light and gamma is undefined".

The Lorentz transform applies between frames moving at relative speed less than c. There is no frame for the light itself. The Lorentz transform is exactly how you you transform the the position or shape of a light sphere between observer A and observer B, who might be moving with relative speed .9c. The gamma relates to the .9c. The speed of light is invariant (between the two frames). Its direction and shape of a wave front will be different between A and B.
 
  • #90
PAllen said:
The Lorentz transform applies between frames moving at relative speed less than c. There is no frame for the light itself. The Lorentz transform is exactly how you you transform the the position or shape of a light sphere between observer A and observer B, who might be moving with relative speed .9c. The gamma relates to the .9c. The speed of light is invariant (between the two frames). Its direction and shape of a wave front will be different between A and B.

Are you sure about your wording? If I want to transform a scene having many spheres moving at different velocities to an observer traveling at .9c with respect to the current observer, I transform all the spheres using the Lorentz Transformation. The position, proper time and geometry (contraction) of all the spheres change. But, if there is a light sphere in the scene, I don't bother transforming it because it's stays a sphere. No? Or am I cheating?
 

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