Question About The Role of Observation in Quantum Mechanics

In summary: Ok, but isn't it the case that when the electrons are being detected they act like particles, and instead of making a pattern like the one you posted, they make a pattern of two strips?What aspect of the detection device in this experiment caused the electrons to act differently?
  • #1
ray3400
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TL;DR Summary
Does observing a particle cause it to exhibit a certain quality? What is the cause and effect relationship involved with observation?
In the double-slit experiment when a detector was placed before the two slits, a 2 strip pattern was produced after the two slits. When there was no detector placed before the two slits, a different pattern was produced after the two slits. Why does the presence of a detector before the two slits cause a different pattern to be produced after the two slits?
 
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  • #2
ray3400 said:
Summary: Does observing a particle cause it to exhibit a certain quality? What is the cause and effect relationship involved with observation?

What constitutes an "observation" in quantum mechanics?

No one has resolved that issue. It could mean modifying quantum mechanics to allow for gravity to cause collapse of the wave function, for example.

A good book you can try reading is 'Sneaking a Look at God's Cards' https://www.amazon.com/dp/069113037X/?tag=pfamazon01-20
 
  • #3
ray3400 said:
I don't understand how observation can "cause" anything.

"Observation" is an interaction. Interactions cause things. Certainly your observations of, for example, your door cause things to happen in your brain.

The reason observing your door can't make it open is that your door is a massive object and you observe it with piddly little photons that can't appreciably affect its state. But that's a particular fact about that particular observation; it's not a general property of all observations. In QM, many observations do not have that property.
 
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  • #4
PeterDonis said:
"Observation" is an interaction. Interactions cause things. Certainly your observations of, for example, your door cause things to happen in your brain.

The reason observing your door can't make it open is that your door is a massive object and you observe it with piddly little photons that can't appreciably affect its state. But that's a particular fact about that particular observation; it's not a general property of all observations. In QM, many observations do not have that property.

Is there any effort to mitigate the effects sensors have on the quantum particles being observed?

In the case of the double slit experiment with electrons, when the electrons are sent down the slits without detection they create an interference pattern and act like a wave. When the electrons are being detected they change to create a pattern of two strips and act like particles. What about the detector in this situation caused the elections to act like particles instead of waves?
 
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  • #5
StevieTNZ said:
No one has resolved that issue. It could mean modifying quantum mechanics to allow for gravity to cause collapse of the wave function, for example.

A good book you can try reading is 'Sneaking a Look at God's Cards' https://www.amazon.com/dp/069113037X/?tag=pfamazon01-20

Thanks, I will look into it. This is certainly a huge jump from classical physics.
 
  • #6
hi,

Concerning young's slits, in any case, the electron leaves an impact as a corpuscle.

As the electron/photon/.../"corpuscle" arrives on the Ꜫ plate, the following phenomenon occurs: their impacts are randomly distributed, and it is only when a large number of them have arrived on Ꜫ that the distribution of impacts seems to have a continuous aspect. The impact density at each point of Ꜫ corresponds to the interference fringes.

244801


/Patrick
 
  • #7
microsansfil said:
hi,

Concerning young's slits, in any case, the electron leaves an impact as a corpuscle.

As the electron/photon/.../"corpuscle" arrives on the Ꜫ plate, the following phenomenon occurs: their impacts are randomly distributed, and it is only when a large number of them have arrived on Ꜫ that the distribution of impacts seems to have a continuous aspect. The impact density at each point of Ꜫ corresponds to the interference fringes.

View attachment 244801

/Patrick
Ok, but isn't it the case that when the electrons are being detected they act like particles, and instead of making a pattern like the one you posted, they make a pattern of two strips?

What aspect of the detection device in this experiment caused the electrons to act differently?
 
  • #8
ray3400 said:
Is there any effort to mitigate the effects sensors have on the quantum particles being observed?

In the case of the double slit experiment with electrons, when the electrons are sent down the slits without detection they create an interference pattern and act like a wave. When the electrons are being detected they change to create a pattern of two strips and act like particles. What about the detector in this situation caused the elections to act like particles instead of waves?

If you have an hour to spare, it might be worth watching the Feynman lecture on the QM view of nature.

Also, there is a lot of stuff out there about QM that is designed to confuse rather than explain. For example: "that electrons sometimes behave like particles and sometimes like waves". This stuff makes it more difficult to get a grasp of what QM is really about. It might be an idea to watch the Feynman lecture with an open mind: forget what you think you already know about QM.

 
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  • #9
ray3400 said:
Is there any effort to mitigate the effects sensors have on the quantum particles being observed?

Past a certain point, you can't. In QM you cannot make interactions as small as you like; there is a minimum interaction.
 
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  • #10
ray3400 said:
When the electrons are being detected

You mean, when they are being detected at the slits, i.e., when the result when you send each electron through the apparatus is not just "electron made a dot at this point on the screen", but either "electron went through slit A and made a dot at this point on the detector screen" or "electron went through slit B and made a dot at this point on the detector screen". In the latter case there is no interference. But it is not true that electrons "act like particles" only in the latter case. Each electron makes a dot on the screen whether there is a way to detect which slit it went through or not. Making a dot on the screen is acting like a particle.
 
  • #11
PeterDonis said:
You mean, when they are being detected at the slits, i.e., when the result when you send each electron through the apparatus is not just "electron made a dot at this point on the screen", but either "electron went through slit A and made a dot at this point on the detector screen" or "electron went through slit B and made a dot at this point on the detector screen". In the latter case there is no interference. But it is not true that electrons "act like particles" only in the latter case. Each electron makes a dot on the screen whether there is a way to detect which slit it went through or not. Making a dot on the screen is acting like a particle.
In the experiment when the electrons are being observed using a detector they produce a different output pattern than when they are not being observed with a detector. What about the detector observing them causes the output pattern to change?
 
  • #12
ray3400 said:
In the experiment when the electrons are being observed using a detector they produce a different output pattern than when they are not being observed with a detector. What about the detector observing them causes the output pattern to change?

You should watch the Feynman lecture! There are four cases:

1a) Only first slit open

1b) Only second slit open.

2) Two slits with a detector.

3) Two slits without a detector.

The first three cases result in the same pattern, in the sense that 2) is the sum of 1a) and 1b). This leads to the conclusion that all the detector is doing is determining a slit through which the particle passes. It's not doing anything else.

The key point is that 3) is NOT the sum of 1a) and 1b).

Watch the Feynman lecture!
 
  • #13
PeroK said:
You should watch the Feynman lecture! There are four cases:

1a) Only first slit open

1b) Only second slit open.

2) Two slits with a detector.

3) Two slits without a detector.

The first three cases result in the same pattern, in the sense that 2) is the sum of 1a) and 1b). This leads to the conclusion that all the detector is doing is determining a slit through which the particle passes. It's not doing anything else.

The key point is that 3) is NOT the sum of 1a) and 1b).

Watch the Feynman lecture!

Why does the observer collapse the wave function simply by observing? By what mechanism does this happen? How can looking at something cause it to physically change?
 
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  • #14
ray3400 said:
Ok, so its not the case that by simply observing the particles in motion (and not changing any other factor of the experiment) we are changing the output? Lots of people make it seem like observation in and of itself changes the output. If that's the case, I was wondering by what mechanism does observation cause a different output?

Every "observation" is an "output". With a detector you have two outputs: a definite slit and a final point on the screen. Without a detector there is only one output: the point on the screen.

It's at this point, to explain why 3) is not the simple sum of 1a) an 1b), that you need QM. That's is really the issue. Statements like "observations cause changes in output" are just words. They don't really mean anything.

Watch the Feynman lecture!
 
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  • #15
PeroK said:
Every "observation" is an "output". With a detector you have two outputs: a definite slit and a final point on the screen. Without a detector there is only one output: the point on the screen.

It's at this point, to explain why 3) is not the simple sum of 1a) an 1b), that you need QM. That's is really the issue. Statements like "observations cause changes in output" are just words. They don't really mean anything.

Watch the Feynman lecture!

Why does the observer collapse the wave function simply by observing? By what mechanism does this happen?

The bottom line is - the sensors caused a 2 strip pattern output as opposed to an interference pattern output. How can looking at something cause it to change? Is there some sort of energy or matter being emitted from the sensor that interacts with the electrons to cause them to change behavior?

If there is no transfer of matter or energy from the sensor to the electrons to form a cause and effect relationship, this is the equivalent of saying "because I looked at my door, the door changed positions".
 
  • #16
ray3400 said:
Why does the observer collapse the wave function simply by observing? By what mechanism does this happen?

How can looking at something cause it to physically change? Did the sensors they used to observe the electrons before they went into the slits interact with the electrons in a way to force them to act like particles and form a 2 strip pattern as opposed to an interference pattern which occurred when there is no sensor observing?

An observation gives you information about something. To say it changed implies it was definitely doing something and then it changed to definitely doing something else. The first thing you should learn about QM is that a particle does not have a definite position unless you measure where it is.

Furthermore, particles at the QM scale do not have classical trajectories.

Fundamentally, you have not learned the basics of QM. You're now just asking the same questions, based on the same preconceptions and misconceptions. At some point, be it IT, chemisty or QM, you do actually have to learn the basics.

If you use a phrase like "electrons being forced to act like particles", then you need a fresh start.
 
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  • #17
PeroK said:
An observation gives you information about something. To say it changed implies it was definitely doing something and then it changed to definitely doing something else. The first thing you should learn about QM is that a particle does not have a definite position unless you measure where it is.

Furthermore, particles at the QM scale do not have classical trajectories.

Fundamentally, you have not learned the basics of QM. You're now just asking the same questions, based on the same preconceptions and misconceptions. At some point, be it IT, chemisty or QM, you do actually have to learn the basics.

If you use a phrase like "electrons being forced to act like particles", then you need a fresh start.

Referring to the double slit experiment:
I do the same experiment twice, and keep everything exactly the same except in one case the electrons are being observed, and in the second case the electrons are not being observed. In the first case I get a two strip pattern output on the screen, and the second case I get an interference pattern output on the screen.

Why does the experiment produce different results when the electrons are observed as opposed to when they are not observed?

Is it correct to conclude that observing the electrons caused the output to be different on the screen?
If so, by what mechanism does observing the electrons cause the output to be different on the screen?
 
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  • #18
ray3400 said:
Ok, but isn't it the case that when the electrons are being detected they act like particles, and instead of making a pattern like the one you posted, they make a pattern of two strips?

What aspect of the detection device in this experiment caused the electrons to act differently?
The confusion comes only from the fact that some people, obviously and unfortunately many of which write popular-science articles/books, that the world is not behaving as they think from everyday experience with macroscopic systems, which appear to behave as described by classical physics. This is, because for macroscopic objects we need to describe only quite rough macroscopic observables and neglect (average over) the many microscopic degrees of freedom they consist of.

The intuitive worldview from this experience breaks usually down when dealing with small systems like electrons. You cannot describe them as classical particles nor as classical fields. Rather, from the most fundamental point of view we have today about them, they are certain states of a quantized Dirac field.

Under "non-relativistic" circumstances, i.e., when the electron runs with speeds much less than the speed of light, you can describe it by a wave function ##\psi(t,\vec{x})## (where I neglect the spin degree of freedom, which is not important for the explanation of the double-slit experiment). This wave function obeys the Schrödinger equation, which describes the time evolution of the wave function.

Though there are many people, who cannot accept this view, and I'm sure there'll be tons of following answers to your question denying it, yet the only consistent interpretation of this wave function (it's called the minimal statistical interpretation, since there's a plethora of other interpretations all trying to somehow deny the very fact of generic indeterminism in our description of nature, which is due to some philosophical prejudices but not founded on any observations): The function ##P(t,\vec{x})=|\psi(t,\vec{x})|^2## describes the probability distribution to find the electron at a place ##\vec{x}## when looked there at time ##t##.

The specific form of the wave function is determined by the "preparation of the electron" at some initial time ##t=0##. Then its time evolution is given by the Schrödinger equation. So given the preparation you can determine the probability distribution of its location at any time. You can also calculate the probability distributions for any other observable, like momenta, by certain mathematical manipulations (in this case going from the position representation to the momentum representation it tells you to take the Fourier transform of the wave function).

This interpretation implies now that observables of a particle are usually not determined but have only certain probabilities do be found when you measure them, given by the wave function.

Now take the double-slit experiment. Now say you want to figure out through which slit each electron comes you shoot at the double-slit, but it should not be determined beforehand, that each electron goes through one of the specific slits (this possibility is not very surprising, yielding a priori the same thing as you expect from classical physics).

As an experimental physicist you now have to ask, how to realize this case, i.e., you have to think how you have to prepare each electron to describe this situation. Now the above described formalism tells you that if you prepare an electron to have a very well defined position initially, this implies that the wave function is narrowly peaked around this position. Now the momentum wave function is given by the Fourier transform of this wave function that's narrowly peaked in position space, which implies that it is a pretty broad distribution in momentum space. This is quantified by the famous position-momentum uncertainty relation: If the standard deviation (which quantifies the uncertainty, i.e., the width of the wave function around the expectation/average value) of the position-vector-##x## component is ##\Delta x##, then there's a an uncertainty momentum-vector-##x## component ##\Delta p_x## which is so large that ##\Delta x \Delta p_x \geq \hbar/2##. So if you initially localize the electron very well, you get a quite uncertain momentum, and the Schrödinger equation for a free electron accordingly tells you that the electrons position-wave function gets broader and broader with time.

In order to avoid the case that your electron's position wave function is still so narrow and the experimentalist aimed at on slit well enough (i.e., he's chosen the momentum, though broad, to be pointing into the corresponding direction) that with certainty it goes through one slit, you simply have to put your slit far away enough from the electron source, so that the wave function gets so broad that its peak covers well both slits. You can arrange this such that it goes with equal probabilities through one or the other of the two slits, if it goes through at all, i.e., many electrons will simply be absorbed by the material making up the double slit, but some will go through, and you cannot with certainty say through which of the two slit any individual electron will have come.

However, at the position of the slits, each electron only goes as a whole through one of the slits. This implies that those electrons that went through the slits at all, at the slit it's with certainty localized with an accuracy given by the width of this slit, and that implies that directly at the slits each single electron is uniquely at the one or the other slit.

Closely behind the slits the wave function thus now shows two narrow peaks corresponding to the pobabilities to go through one or the other slit. The two peaks are well separated, i.e., their width (given by the width of each slit) is much smaller than their distance (given by the distance of the centers of the slit).

Behind the slits the electron's wave function again goes on according to the Schrödinger equation, i.e., it broadens again, but not too far from the slit, i.e., after not too long times, the wave function will still show two well-distinct bumps. Although these bumps got a bit broader, they are still not too much overlapping, so that for each electron the probability distribution is such that with quite high certainty you can say through which slit they came.

This means that, if you want to know (with high certainty) through which of the two slits each electron came you simply have to put your electron dectector (e.g., a CCD cam like the one in your cell phone) close enough to the double slit. Sending through a lot of such prepared electrons in this setup you'll just see two well-disitinct bumps according to the probabilities given by the wave function at the position of the CCD cam. Each electron being in one of the bumps very likely came through the corresponding slit. Thus, here you obviously have which-way information with high certainty.

On the other hand, if the wave function develops further from the slits the two bumps get broader and broader and then overlap more or less. The longer you wait and the farther the electron goes away from the slits the less certain you can determine through which slit this electron came. I.e., if you put the CCD cam far enough away from the slits, there's no possibility anymore to know from the position the electron hits the cam, through which slit it has come.

Now the Schrödinger equation is mathematically a wave equation, and this implies that the partial waves of electrons coming through the one or the other slit simply add like ##\psi=\psi_1+\psi_2##. Now the probability is given by ##|\psi|^2=|\psi_1|^2+ |\psi_2|^2 + \psi_1^* \psi_2 +\psi_1 \psi_2^*##. The last to terms are called the "interference terms". In the situation where the CCD cam is placed far away from the two slits ##\psi_1## and ##\psi_2## have a large overlap and thus the interference term is significant, and depending on the specific position at the CCD cam the contributions of the partial wave may add (constructive interference) or cancel each other out (destructive interference) or something in between, and that's precisely the interference pattern you expect from wave phenomena, i.e., in this situation where you don't know which way the electron took the probability distribution shows a significant interference pattern.

Of course you can argue with the interference piece also in the case discussed above, when the CCD cam is close enough to the slits to still resolve which-way information with high certainty: Then the partial waves do not significantly overlap, corresponding to the still well separated two bumps, and thus ##\psi_1 \psi_2^*+\psi_1^* \psi_2 \simeq 0## everywhere at the CDD screen. Thus you get just well distinct bumps on the CCD screen but no (significant) interference.

Note that still, each electron makes one single dot on the CCD screen, i.e., a single electron cannot appear as some smeared distribution at the screen. In this sense it has always particle features when detected, and the above given probabilistic "interpretation of the wave function" is at least non-contradictory with these observational facts and also not contradicting any other fundamental laws of physics (like causality and all that). I know of no other interpretation that is consistent in this sense (except Bohmian mechanics, which however is consistent only in the here discussed non-relativistic limit, and also doesn't lead to other phenomenological implications of the quantum-theoretical formalism than the minimal interpretation).
 
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  • #19
vanhees71 said:
The confusion comes only from the fact that some people, obviously and unfortunately many of which write popular-science articles/books, that the world is not behaving as they think from everyday experience with macroscopic systems, which appear to behave as described by classical physics. This is, because for macroscopic objects we need to describe only quite rough macroscopic observables and neglect (average over) the many microscopic degrees of freedom they consist of...

Thanks for the explanation. I think I have a much better idea of how the double-slit experiment works after reading. There is still one aspect of it I don't understand - Why does the experiment produce different results when the electrons are observed as opposed to when they are not observed? Or is this not a feature of the double slit experiment? If it is the case, I don't understand how the act of observation can cause different results.
 
  • #20
What do you mean the experiment produces different results when the electrons are observed as opposed when they are not observed? If you don't observe the electrons, there's no experiment, because nothing is observed. Physics is about observations, and measurements are just observations giving precise numbers. If you don't measure the electron's position, all you know are the probabilities to find it at any given position, provided you know its wave function well enough due to some knowledge about it at an earlier time (and this also only if you have accurate knowledge about how the electron interacts with anything around it, i.e., if you can solve the Schrödinger equation given the Hamiltonian of the electron).
 
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  • #21
vanhees71 said:
What do you mean the experiment produces different results when the electrons are observed as opposed when they are not observed? If you don't observe the electrons, there's no experiment, because nothing is observed. Physics is about observations, and measurements are just observations giving precise numbers. If you don't measure the electron's position, all you know are the probabilities to find it at any given position, provided you know its wave function well enough due to some knowledge about it at an earlier time (and this also only if you have accurate knowledge about how the electron interacts with anything around it, i.e., if you can solve the Schrödinger equation given the Hamiltonian of the electron).

In the double-slit experiment when a detector was placed before the two slits, a 2 strip pattern was produced after the two slits. When there was no detector placed before the two slits, a different pattern was produced after the two slits. Why does the presence of a detector before the two slits cause a different pattern to be produced after the two slits?
 
  • #22
Here is another study that explores the same question:
https://www.sciencedaily.com/releases/1998/02/980227055013.htm

"REHOVOT, Israel, February 26, 1998--One of the most bizarre premises of quantum theory, which has long fascinated philosophers and physicists alike, states that by the very act of watching, the observer affects the observed reality. "

"the very act of watching, the observer affects the observed reality"

How does the "observer effect" cause the two different output patterns in the double slit experiment for electrons? There is a different output pattern when the electrons are being observed before the going through the slits and when they are not being observed before going through the slits.
 
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  • #24
ray3400 said:
In the double-slit experiment when a detector was placed before the two slits, a 2 strip pattern was produced after the two slits. When there was no detector placed before the two slits, a different pattern was produced after the two slits. Why does the presence of a detector before the two slits cause a different pattern to be produced after the two slits?
If you put a detector in front of one slit to somehow register, that an electron goes through, there's some interaction of this electron with this device, and this has to be taken into account when solving the Schrödinger equation. Usually such an interaction destroys the intereference pattern, because it destroys the coherence of the partial waves concerning the case that the electron goes through the slit, where you detect it, or through the other slit. To analyze this in detail you have to give a specific example for the detector and analyse its effect on the electron. That's why I provided the most simple thinkable example of the dependence of what's observed from the choice of which experiment you do, i.e., an experiment which shows interference patterns vs. one that provides which-way information.
 
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  • #25
ray3400 said:
Is there any effort to mitigate the effects sensors have on the quantum particles being observed?
Yes, see nondemolition measurements. But this doesn't apply for the double slit.
ray3400 said:
by the very act of watching, the observer affects the observed reality. "
The pattern changes since a detector at the slit has a serious impact on the microscopic stuff going through the slit:
ray3400 said:
How can looking at something cause it to physically change?
The change in an observed object due to an observation is large if the means of observing it is comparable (or larger) in size and impact to the observed object. If you magnify the situation sufficiently strongly, it is qualitatively like (though not really like) observing a sand castle by a big wave from the shore.
 
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  • #26
ray3400 said:
Here is another study that explores the same question:
https://www.sciencedaily.com/releases/1998/02/980227055013.htm

"REHOVOT, Israel, February 26, 1998--One of the most bizarre premises of quantum theory, which has long fascinated philosophers and physicists alike, states that by the very act of watching, the observer affects the observed reality. "

"the very act of watching, the observer affects the observed reality"

How does the "observer effect" cause the two different output patterns in the double slit experiment for electrons? There is a different output pattern when the electrons are being observed before the going through the slits and when they are not being observed before going through the slits.

This is the sort of thing that you need to start ignoring if you are going to learn any QM.

There is a common experiment where you measure the speed of a bullet by firing it into block of wood and measure the momentum of the block after the collision. In this case, the measurement of the bullet's speed/momentum fairly brutally changes the speed of the bullet. This is clearly of no significance to the question here.

The fundamental point about the double-slit experiment is that if you do not measure which slit the electron passes through, then the question of which slit it passes through no longer has meaning.

In the Feynman lecture (which you really should watch), he sums it up as follows (in the case where thjere is no detector):

Proposition: the electron must either pass through slit A or pass through slit B.

He then shows that, using the experimental results of the double slit, that proposition fails. That proposition seems so close to basic logic that it is hard to understand how it could fail. But, the proposition fails, nevertheless. You cannot say that the electron passed through either slit A or slit B; and, you cannot say that the electron passed through both slits; and, you cannot say that the electron passed through neither slit. You cannot say the electron behaved like a particle; you cannot say the electron behaved like a wave; and you certainly cannot say that an electron behaved like a wave until it was observed and thereafter it behaved like a particle.

This is where it becomes fundamentally important to understand the electron not as a classical particle that has a well-defined trajectory, but as a quantum object whose position (if and when you measure its position) is governed by a probabilistic wave-function.

The electron never is anywhere or doing anything that is changed by an observation. That's the difference with the bullet and the block. The bullet, statistically at least, really has a well-defined position, momentum and trajectory which is changed by its collision with the block. It makes no sense to ask where the electron was if you didn't measure where it was.

One final point is that it is also worth studying the single-slit behaviour of quantum objects. Another lecture I would recommend in this respect is the following. The single-0slit experiment is analysed and carried out from about 32 mins in (although the whole lecture is worth watching if you want to understand QM).

 
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  • #27
ray3400 said:
In the experiment when the electrons are being observed using a detector they produce a different output pattern than when they are not being observed with a detector. What about the detector observing them causes the output pattern to change?

The fact that the detectors at the slits are physical systems that interact with the electrons and change their behavior. "Observation" is an interaction, and interaction changes things.

Exactly how they interact with the electrons and change their behavior is what you need the detailed math of QM for.
 
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  • #28
ray3400 said:
In the double-slit experiment when a detector was placed before the two slits, a 2 strip pattern was produced after the two slits. When there was no detector placed before the two slits, a different pattern was produced after the two slits. Why does the presence of a detector before the two slits cause a different pattern to be produced after the two slits?

Generally, no one can explain the "why" of physics when you are discussing fundamentals. And the fundamental rule for the double slit setup is: If it is *possible* to know which slit a particle goes through, then there will be NO interference. QM properly explains this without explaining "why" physics is like this in the first place. Of course the explanation involves a good deal of QM, here is an example using optics (photons instead of electrons or ions):

https://arxiv.org/abs/quant-ph/0703126
In several posts, you speculated that the detector itself causes the pattern to change. But that is not really the case, as you can see according per the rule above. And there are in fact experiments that demonstrate this. That is because you do NOT need a detector at all to control the presence or absence of interference. In an optical version of the experiment, you can place *parallel* polarizers at 45 degrees in front of the slits (like: / /) . There WILL be interference. So there must not be a detector present.

BUT... if you re-orient the polarizers so they are *crossed* (perpendicular, orthogonal, still at 45 degrees, like: \ /): there will NOT be interference. Same apparatus otherwise, and note that we have no idea which slit the photons go through. So what gives?

Going back to the rule above: When the polarizers are crossed, it is POSSIBLE to determine which slit the photon passes through even though we didn't attempt to learn that information. Therefore, no interference, and there is no detector present at all. So it can't be the detector.

http://sciencedemonstrations.fas.ha...-demonstrations/files/single_photon_paper.pdf
 
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  • #29
ray3400 said:
Summary: Does observing a particle cause it to exhibit a certain quality? What is the cause and effect relationship involved with observation?

Observation does have a special role in quantum mechanics (using the orthodox or Copenhagen interpretation of quantum mechanics). For example, a "particle" is not assigned a position until its position is measured. In this interpretation, the question of cause and effect is avoided, because quantum mechanics is simply a tool to predict the probability of what is observed.

ray3400 said:
In the double-slit experiment when a detector was placed before the two slits, a 2 strip pattern was produced after the two slits. When there was no detector placed before the two slits, a different pattern was produced after the two slits. Why does the presence of a detector before the two slits cause a different pattern to be produced after the two slits?

ray3400 said:
Is there any effort to mitigate the effects sensors have on the quantum particles being observed?

In quantum mechanics, we cannot get information about a system without disturbing it.
https://arxiv.org/abs/0706.3526
 
  • #30
PeroK said:
In the Feynman lecture (which you really should watch), he sums it up as follows (in the case where thjere is no detector):

Proposition: the electron must either pass through slit A or pass through slit B.

He then shows that, using the experimental results of the double slit, that proposition fails. That proposition seems so close to basic logic that it is hard to understand how it could fail. But, the proposition fails, nevertheless. You cannot say that the electron passed through either slit A or slit B; and, you cannot say that the electron passed through both slits; and, you cannot say that the electron passed through neither slit. You cannot say the electron behaved like a particle; you cannot say the electron behaved like a wave; and you certainly cannot say that an electron behaved like a wave until it was observed and thereafter it behaved like a particle.

Feynman was wrong on this point. It is conceptually possible that the electron went through either A or B. https://en.wikipedia.org/wiki/De_Broglie–Bohm_theory
 
  • #31
atyy said:
Feynman was wrong on this point. It is conceptually possible that the electron went through either A or B. https://en.wikipedia.org/wiki/De_Broglie–Bohm_theory

Okay, but Bohmian mechanics generally undermines most of what can be said about orthodox QM.

And, invoking Bohmian mechanics hardly helps someone understand the basics of QM.
 
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  • #32
atyy said:
In quantum mechanics, we cannot get information about a system without disturbing it.
https://arxiv.org/abs/0706.3526

The below reference could be considered a counter-example to your reference. Interference is made to disappear without detection (and without any discernible disturbance, other than change of context). And even if (which slit) information were to be obtained, the act of detection is not responsible for the change in outcomes. I would challenge the idea that the system was "disturbed" as part of obtaining information. Only the relative orientation of the polarizers changes - nothing else.

http://sciencedemonstrations.fas.ha...-demonstrations/files/single_photon_paper.pdf
 
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  • #33
I now understand how and why observation in quantum mechanics is handled differently than in everyday life, or classical Newtonian physics. Thanks everyone for your responses.
 
  • #34
DrChinese said:
The below reference could be considered a counter-example to your reference. Interference is made to disappear without detection (and without any discernible disturbance, other than change of context). And even if (which slit) information were to be obtained, the act of detection is not responsible for the change in outcomes. I would challenge the idea that the system was "disturbed" as part of obtaining information. Only the relative orientation of the polarizers changes - nothing else.

http://sciencedemonstrations.fas.ha...-demonstrations/files/single_photon_paper.pdf

No it does not challenge it. The author means it in a precise sense, and gives it as Theorem 2.
 
  • #35
PeroK said:
Okay, but Bohmian mechanics generally undermines most of what can be said about orthodox QM.

And, invoking Bohmian mechanics hardly helps someone understand the basics of QM.

I don't think Bohmian mechanics undermines most of what can be said about orthodox QM. I agree it is not helpful to invoke BM, but unfortunately, Feynman brought up the topic and made an error. I think it undermines orthodox QM, if errors about orthodox QM are left uncorrected.
 
<h2>1. What is the role of observation in quantum mechanics?</h2><p>The role of observation in quantum mechanics is to collapse the wave function and determine the state of a particle. In quantum mechanics, particles exist in a superposition of states until they are observed, at which point they "choose" a specific state. This is known as the observer effect.</p><h2>2. How does observation affect the outcome of a quantum experiment?</h2><p>Observation can affect the outcome of a quantum experiment because it causes the wave function to collapse and the particle to "choose" a specific state. This means that the act of observing can change the behavior of the particle and the outcome of the experiment.</p><h2>3. Can the observer influence the outcome of a quantum experiment?</h2><p>There is currently no scientific evidence to suggest that the observer can consciously influence the outcome of a quantum experiment. However, the observer's presence and actions can indirectly affect the outcome through the observer effect.</p><h2>4. Is observation necessary for quantum mechanics to work?</h2><p>Yes, observation is necessary for quantum mechanics to work. Without observation, particles would remain in a superposition of states and the behavior of quantum systems would not be fully understood. Observation is a crucial aspect of quantum mechanics and is necessary for making predictions and understanding the behavior of particles.</p><h2>5. How does the role of observation differ in classical mechanics and quantum mechanics?</h2><p>In classical mechanics, observation does not play a significant role as particles have well-defined states and their behavior can be accurately predicted. However, in quantum mechanics, observation is crucial as particles exist in a superposition of states and their behavior is probabilistic. Observation causes the wave function to collapse and determines the state of the particle, leading to different outcomes in quantum experiments compared to classical ones.</p>

1. What is the role of observation in quantum mechanics?

The role of observation in quantum mechanics is to collapse the wave function and determine the state of a particle. In quantum mechanics, particles exist in a superposition of states until they are observed, at which point they "choose" a specific state. This is known as the observer effect.

2. How does observation affect the outcome of a quantum experiment?

Observation can affect the outcome of a quantum experiment because it causes the wave function to collapse and the particle to "choose" a specific state. This means that the act of observing can change the behavior of the particle and the outcome of the experiment.

3. Can the observer influence the outcome of a quantum experiment?

There is currently no scientific evidence to suggest that the observer can consciously influence the outcome of a quantum experiment. However, the observer's presence and actions can indirectly affect the outcome through the observer effect.

4. Is observation necessary for quantum mechanics to work?

Yes, observation is necessary for quantum mechanics to work. Without observation, particles would remain in a superposition of states and the behavior of quantum systems would not be fully understood. Observation is a crucial aspect of quantum mechanics and is necessary for making predictions and understanding the behavior of particles.

5. How does the role of observation differ in classical mechanics and quantum mechanics?

In classical mechanics, observation does not play a significant role as particles have well-defined states and their behavior can be accurately predicted. However, in quantum mechanics, observation is crucial as particles exist in a superposition of states and their behavior is probabilistic. Observation causes the wave function to collapse and determines the state of the particle, leading to different outcomes in quantum experiments compared to classical ones.

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