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Afterburner. The business of virtual particles is attributable to Einstein. It comes out of Heisenberg's Uncertainty Principle. The Uncertainty Principle was formulated after Heisenberg considered the effects of a photon striking an electron.
Picture an electron stealthily moving along at some velocity v, but unseen by you in a darkened room. You are given a laser pointer that emits single photons of visible light, at one second intervals (it's arbitrary). When your photon hits the electron, it's absorbed and re-emitted in your direction, you"see" it (technically not true for the retina, but we labor for simplicity here). However, the photon carries momentum E/c...so the electron may have it's original velocity vector affected by the impact...it may gain energy and momentum from the photon. This bothered Heisenberg. If you don't fire a photon, you can't "see" the electron, but when you do...you change the momentum of the object you are looking for. There is no way out here. In order to measure the position of the electron you need to input your measuring method, and the consequence of that is you affect the system you are measuring. Heisenberg expressed this numerically as ....(delta x)(delta p) = or > h/2pi delta x is the uncertainty in the position of the object delta p is the uncertainty in the momentum of the object (p=mv) h is Planck's constant h/2pi is sometimes written as h with a bar over it It has units of action (energy times time) in erg-sec or Mev-sec... Einstein hated this. He thought he could devise a thought experiment wherein one could determine both the position and momentum with arbitrary uncertainty simultaneously. While you can improve either quantity....whatever you do to better one...worsens the other. For example you could use a violet photon with a smaller wavelength, to fix the position more precisely....but it's increased momentum means you now know the momentum of the struck electron more vaguely. Bohr argued with Einstein over this for a long time...pointing out every time how Heisenberg was right. Finally Einstein accepted it, but he didn't like it. Soon Einstein realized something else was up....if you replace delta x, the position with c delta t...for a particle moving at ~ c AND... if you replace delta (mv) with delta (mc) in delta p ...for that same particle, then you get (mc)(c delta t) = or > h/2 pi Rearranging the algebra delta mc2 (delta t) = or > h/2 pi. Now you have E=mc2....so you can replace the delta mc2 with delta E This yields (delta E)(delta t) = or > h/2 pi This equation says the energy (E) of an object is uncertain in the same way that the momentum and position are ...and the uncertainty is time dependent. What it means physically is that the energy of a photon may increase briefly over small time intervals. The larger the interval, the smaller the increase....but for sufficiently small intervals the fluctuation may be quite large, and the object may "use" this energy to create short-lived particle/antiparticle pairs. Like Cinderella, they must return to a state of annihilation by "Midnight"...delta t' massive pairs are very short-lived. Massless ones much longer (Z/anti-Z) Enter Hideki Yukawa. He reasoned that the time for a force carrier to traverse the width of a proton...~ one Fermi was so short that the particle should have a mass of ~ 250 Mev. Eventually, after a misidentification of the muon as the strong force carrier, the pion fit the bill. Nobel Prize for Yukawa. Other particles can emit virtual pairs transiently, but are similarly restricted by the time interval. Like Cinderella, they must disappear by Midnight...delta t to conserve mass and energy. It's not true that the neutrino can only interact via massive force carriers in the weak interaction, the W+, W-, or Z0. The Z can be a photon/ anti-photon ...it is it's own anti-particle...or a neutrino/antineutrino pair. They are both massless and have infinite range. No charged particle will ever travel at c...SR forbids it. However if an electron is exchanging virtual photons with a proton in hydrogen, binding them in the elctromagnetic interaction....and you "kick" the atom with heat, or photons...you can promote some of the virtual photons into reality...the hydrogen spectrum. With regards to the wave function collapsing...yes that's how your radio works too. Hope this helps. Pete.
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A third rate theory forbids A second rate theory explains after the fact A first rate theory predicts...A. Lomonosov Last edited by trinitree88 : 27-August-2006 at 11:01 PM. Reason: spelling |
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Thank you for the explanation trinitree88.
However, I just dont see why the energy of a photon (or any particle) would increase even slightly over small intervals of time. It just doesnt make sence in my head.I can see why Einstein had problems with the Uncertainty Principle. Although we cant measure the electrons position and momentum at the same time, it does not necessarily mean that the particle experiences an uncertainty. If we were to ask the particle, it would tell us all what we want to know (the electron does something when its in the electron cloud, its not uncertain about what its doing, it just doesnt want to "tell", and we have no way of getting the information out of it so to speak). Similarly, if we were to ask the Universe, it would also tell us what we want to know, assuming it can account for every particle that exists in it (and the language problem ) ![]() |
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Or have I got the wrong end of the stick about what you're saying? |
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RobA...snippet:
I've always wondered about this. While it's undoubtedly true that hitting something with a more powerful bullet means that you affect the thing you're measuring more, there's got to be more to it than that. The uncertainty principle limits natures own knowledge of the particle, not just our ability to measure - otherwise we're left with the particle really going through one slit. Or have I got the wrong end of the stick about what you're saying?[/quote] Take the case of a pot of warm water. You pick up a thermometer, put it in the water up to it's calibrated immersion level. You wait for thermal equilibrium. You read the thermometer. 40 degrees + or -...right? Well, Yes and NO. It's pretty close, with an error bar....but was the thermometer warmer than the water, or colder? If it was warmer...then there's added heat from the thermometer, if it was colder there's subtracted heat (MCdelta T). So you have the equilibrium temperature of the two objects, not the water alone. You can reduce the size of the thermometer, but you can't make it disappear....so you never get the temperature of the water only....you only get the equilibrium temperature of the water-thermometer system. They're not the same. There's no way out of this. Your measuring device affects what you are measuring...hence Heisenberg. Only the supernatural can "know" perfectly. I'm not arguing against what nature knows. ....or seems to know. Pete
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A third rate theory forbids A second rate theory explains after the fact A first rate theory predicts...A. Lomonosov |
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Pete,
What if I don't care about the temperature of the water -- I want to know the temperature of the thermometer! -- Jeff, in Minneapolis
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http://www.FreeMars.org/jeff/ "The other planets? Well, they just happen to be there, but the point of rockets is to explore them!" -- Kai Yeves |
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Pete.
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A third rate theory forbids A second rate theory explains after the fact A first rate theory predicts...A. Lomonosov |
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The quantum world really is different than the classical one with which we are familiar. It's not just a miniaturized version with similar concepts and behaviors.
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"I have a cunning plan that cannot fail." S. Baldrick |
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Afterburner, ...very Einsteinian of you...lol. Interrogating the particle would require a communication.Even a single photon of communication will carry away some energy and momentum....hence, object changed, just as in a collision. Some things we have to accept...like it or not. Ciao. Pete
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A third rate theory forbids A second rate theory explains after the fact A first rate theory predicts...A. Lomonosov |
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Of course this is true, but most of the treatments I've read on this topic include the school of thought that Heisenberg Uncertainty is not simply a limitation in our ability to measure, as RobA and swansont have indicated. It's a more fundamental limitation....
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Everyone is entitled to his own opinion, but not his own facts. |
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In QM, the wave function of conjugate variables, like momentum and position, are Fourier transforms of each other. The uncertainty is inherent in that.
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"I have a cunning plan that cannot fail." S. Baldrick |
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Assume that I know nothing about "the wave function of conjugate variables" or "Fourier transforms". Can you explain why anyone should think that a particle really is in two mutually-exclusive states simultaneously, rather than simply being in an unknown state? -- Jeff, in Minneapolis
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http://www.FreeMars.org/jeff/ "The other planets? Well, they just happen to be there, but the point of rockets is to explore them!" -- Kai Yeves |
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conjugate variables" or "Fourier transforms" stuff mean, in simple language)? Or how an experiment (or series of experiments) could rule out 'hidden variables'? Or, perhaps, what the experiments were that actually produced the results we interpret as 'no hidden variables' (and cause Einstein to spin in his grave, no doubt)? |
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Some time ago, I asked whether or not there is a limit to how much or how litle energy a photon can have. The answer was no.
Would this not mean that we could technically use photons that have extremely small energy levels (I'm talking really small here) to interrogate the particle, so that the energy lost/gained is so insignificantly small, that we would be satisfied? (Scenario for above: We have large bubble Universe, (100 billion light year redius) at the center of this large, empty space, we have some particle. From the outside of this bubble, we send a photon with a wavelength of 30 billion light years straight at the particle. IT HITS!!! My question is...whats going to happen? Would this kind of communication be effective for interrogating the particle and having it tell us what we want to know?) Just as a side note...All things cast a shadow in the neutrino sea..right? Do subatomic particles also have their own shadow in this sea, or is it only larger objects? And another thing...Are there even any advantages to knowing the precise position and momentum of a particle?...As in, if we knew the position and the momentum at the same time...what could we potentially do differently? New technologies perhaps? Or is there no point to it at all? Thanks. |
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So you've got a choice : - high energy photon, which tells you precisely where something was before you sent it barrelling away, or - low energy photon, which tells you roughly where something is Quote:
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Unfortunately, that's all predicated on "If it were possible". QM says that even nature itself doesn't "know" the precise position and momentum, so we never will. |
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there are limits to how little energy a photon can have and yet be able to interact with a particle or a detector. Quote:
would not hit the particle. The wavelength needs to be about the same size as a particle, or smaller, in order to interact with the particle. For the same reason, there would be no way to detect such a photon. The longest-wavelength photon which can be detected as an individual is probably in the infrared part of the spectrum, with a wavelength less than a millimeter. Longer wavelengths, such as microwaves and radio waves, can only be detected by the combined effects on a detector of very large numbers of photons acting together. Quote:
then the neutrino ceases to exist (something else is formed), and you will have a "shadow". I don't see that this fact is of any practical value. Quote:
other things to be more precise, and less noisy. So that it might be possible to measure some things that currently can't be measured at all because the signal can't be distinguished from noise. But I can't come up with a specific example. -- Jeff, in Minneapolis
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http://www.FreeMars.org/jeff/ "The other planets? Well, they just happen to be there, but the point of rockets is to explore them!" -- Kai Yeves |
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a complete explanation of quantum mechanics and quantum electrodynamics, written for a twelfth-grade reading comprehension. Seriously, maybe the thing to do would be to start with a specific and work toward the more general, basic ideas. Here, I'll start by just asking what measurements swansont referred to: Quote:
get into what those measurements imply. -- Jeff, in Minneapolis
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http://www.FreeMars.org/jeff/ "The other planets? Well, they just happen to be there, but the point of rockets is to explore them!" -- Kai Yeves |