Delayed-choice quantum eraser: Difference between revisions

Browse history interactively ← Previous edit Next edit →Content deleted Content addedVisual WikitextInline

Revision as of 02:31, 6 February 2014 editPatrick0Moran (talk \| contribs)Extended confirmed users12,602 edits →Introduction: tweak← Previous edit		Revision as of 02:47, 6 February 2014 edit undoPatrick0Moran (talk \| contribs)Extended confirmed users12,602 edits →The experiment: Clarify a seemingly groundless affirmation.Next edit →
Line 90:		Line 90:
	The results from Kim, et al.<ref name="DCQE" /> have shown that whether the idler photon is detected at a detector that preserves its which-path information (D<sub>3</sub> or D<sub>4</sub>) or a detector that erases its which-path information (D<sub>1</sub> or D<sub>2</sub>) determines whether interference is seen at D<sub>0</sub>, even though the idler photon ''is not observed until after'' the signal photon arrives at D<sub>0</sub> due to the shorter optical path for the latter.		The results from Kim, et al.<ref name="DCQE" /> have shown that whether the idler photon is detected at a detector that preserves its which-path information (D<sub>3</sub> or D<sub>4</sub>) or a detector that erases its which-path information (D<sub>1</sub> or D<sub>2</sub>) determines whether interference is seen at D<sub>0</sub>, even though the idler photon ''is not observed until after'' the signal photon arrives at D<sub>0</sub> due to the shorter optical path for the latter.

	Some have interpreted this result to mean that the delayed choice to observe or not observe the path of the idler photon will change the outcome of an event in the past. However, an interference pattern may only be observed ''after'' the idlers have been detected (i.e., at D<sub>1</sub> or D<sub>2</sub>).		Some have interpreted this result to mean that the delayed choice to observe or not observe the path of the idler photon will change the outcome of an event in the past. However, an interference pattern may only be observed ''after'' the idlers have been detected (i.e., at D<sub>1</sub> or D<sub>2</sub>). That conclusion follows, as will be explained below, because a single photon showing up on D<sub>0</sub> could be making a contribution to one of four different assemblages of photons, two different diffraction patterns and two different interference patterns.

	Note that the total pattern of all signal photons at D<sub>0</sub>, whose entangled idlers went to multiple different detectors, will never show interference regardless of what happens to the idler photons.<ref name="Greene">{{cite book \| last = Greene \| first = Brian \| authorlink = Brian Greene \| title = The Fabric of the Cosmos \| publisher = Alfred A. Knopf \| year = 2004 \| isbn = 0-375-41288-3 \| page = 198}}</ref> One can get an idea of how this works by looking carefully at both the graph of the subset of signal photons whose idlers went to detector D<sub>1</sub> (fig. 3 in the paper<ref name="DCQE" />), and the graph of the subset of signal photons whose idlers went to detector D<sub>2</sub> (fig. 4), and observing that the peaks of the first interference pattern line up with the troughs of the second and vice versa (noted in the paper as "a π phase shift between the two interference fringes"), so that the sum of the two will not show interference.		Note that the total pattern of all signal photons at D<sub>0</sub>, whose entangled idlers went to multiple different detectors, will never show interference regardless of what happens to the idler photons.<ref name="Greene">{{cite book \| last = Greene \| first = Brian \| authorlink = Brian Greene \| title = The Fabric of the Cosmos \| publisher = Alfred A. Knopf \| year = 2004 \| isbn = 0-375-41288-3 \| page = 198}}</ref> One can get an idea of how this works by looking carefully at both the graph of the subset of signal photons whose idlers went to detector D<sub>1</sub> (fig. 3 in the paper<ref name="DCQE" />), and the graph of the subset of signal photons whose idlers went to detector D<sub>2</sub> (fig. 4), and observing that the peaks of the first interference pattern line up with the troughs of the second and vice versa (noted in the paper as "a π phase shift between the two interference fringes"), so that the sum of the two will not show interference.

Revision as of 02:47, 6 February 2014

Quantum mechanics
Part of a series of articles about
$i\hbar {\frac {d}{dt}}\|\Psi \rangle ={\hat {H}}\|\Psi \rangle$ Schrödinger equation
Introduction Glossary History
Background Classical mechanics Old quantum theory Bra–ket notation Hamiltonian Interference
Fundamentals Complementarity Decoherence Entanglement Energy level Measurement Nonlocality Quantum number State Superposition Symmetry Tunnelling Uncertainty Wave function Collapse
Experiments Bell's inequality CHSH inequality Davisson–Germer Double-slit Elitzur–Vaidman Franck–Hertz Leggett inequality Leggett–Garg inequality Mach–Zehnder Popper Quantum eraser Delayed-choice Schrödinger's cat Stern–Gerlach Wheeler's delayed-choice
Formulations Overview Heisenberg Interaction Matrix Phase-space Schrödinger Sum-over-histories (path integral)
Equations Dirac Klein–Gordon Pauli Rydberg Schrödinger
Interpretations Bayesian Consistent histories Copenhagen de Broglie–Bohm Ensemble Hidden-variable Local Superdeterminism Many-worlds Objective-collapse Quantum logic Relational Transactional Von Neumann–Wigner
Advanced topics Relativistic quantum mechanics Quantum field theory Quantum information science Quantum computing Quantum chaos EPR paradox Density matrix Scattering theory Quantum statistical mechanics Quantum machine learning
Scientists Aharonov Bell Bethe Blackett Bloch Bohm Bohr Born Bose de Broglie Compton Dirac Davisson Debye Ehrenfest Einstein Everett Fock Fermi Feynman Glauber Gutzwiller Heisenberg Hilbert Jordan Kramers Lamb Landau Laue Moseley Millikan Onnes Pauli Planck Rabi Raman Rydberg Schrödinger Simmons Sommerfeld von Neumann Weyl Wien Wigner Zeeman Zeilinger
v t e

A delayed choice quantum eraser, first performed by Yoon-Ho Kim, R. Yu, S.P. Kulik, Y.H. Shih and Marlan O. Scully, and reported in early 1999, is an elaboration on a quantum eraser experiment involving the concepts considered in Wheeler's delayed choice experiment. It was designed to investigate peculiar consequences of the well-known double slit experiment in quantum mechanics, as well as the consequences of quantum entanglement.

Introduction

In the basic double slit experiment, a very narrow beam of coherent light from a source that is far enough away to have almost perfectly parallel wave fronts, is directed perpendicularly towards a wall pierced by two parallel slit apertures. The widths of the slits and their separation are approximately the same size as the wavelength of the incident light.

If a detection screen (anything from a sheet of white paper to a digital camera) is put on the other side of the double slit wall, a pattern of light and dark fringes will be observed, a pattern that is called an interference pattern.

Early in the history of this experiment, scientists discovered that, by decreasing the brightness of the light source sufficiently, individual particles of light that form the interference pattern are detectable. They next tried to discover by which slit a given unit of light (photon) had traveled.

Unexpectedly, the results discovered were that if anything is done to permit determination of which path the photon takes, the interference pattern disappears: there is no interference pattern. Each photon simply hits the detector by going through one of the two slits. Each slit yields a simple single pile of hits; there is no interference pattern.

It is counterintuitive that a different outcome results based on whether or not the photon is constrained to follow one or another path well after it goes through the slit but before it hits the detector.

Two inconsistent accounts of the nature of light have long contended. The discovery of light's interfering with itself seemed to prove that light could not be a particle. It seemed that it had to be a wave to explain the interference seen in the double-slit experiment (first devised by Thomas Young in his classic interference experiment of the eighteenth century).

In the early twentieth century, experiments with the photoelectric effect (the phenomenon that makes the light meters in cameras possible) gave equally strong evidence to support the idea that light is a particle phenomenon. Nothing about a photon is observable between the time it is emitted (experimenters can determine the time energy was supplied to the electron emitter) and the time it appears as the delivery of energy to some detector screen (such as a CCD or the emulsion of a film camera).

Nevertheless, experimenters have tried to gain indirect information about which path a photon "really" takes when passing through the double-slit apparatus.

In the process they learned that constraining the path taken by one of a pair of entangled photons inevitably controls the path taken by the partner photon. Further, if the partner photon is sent through a double-slit device and thus interferes with itself, then very surprisingly the first photon will also behave in a way consistent with its having interfered with itself, even though there is no double-slit device in its way.

In a quantum eraser experiment, one arranges to detect which one of the slits the photon passes through, and also to construct the experiment so that this information can be "erased" after the fact.

In practice, this "erasure" of path information frequently means removing the constraints that kept photons following two different paths separated from each other.

In one experiment, rather than splitting one photon or its probability wave between two slits, the photon is subjected to a beam splitter. If one thinks in terms of a stream of photons being randomly directed by such a beam splitter to go down two paths that are kept from interaction, it is clear that no photon can then interfere with any other or with itself.

If the rate of photon production is reduced so that only one photon is entering the apparatus at any one time, however, it becomes impossible to understand the photon as only moving through one path because when their outputs are redirected so that they coincide on a common detector then interference phenomena appear.

In the two diagrams to the right, photons are emitted one at a time from the yellow star. They each pass through a 50% beam splitter (green block) that reflects 1/2 of the photons, which travel along two possible paths, depicted by the red or blue lines.

In the top diagram, one can see that the trajectories of photons are clearly known — in the sense that if a photon emerges at the top of the apparatus it appears that it had to have come by the path that leads to that point (blue line) and if it emerges at the side of the apparatus it appears that it had to have come by way of the other path (red line).

Next, as shown in the bottom diagram, a second beam splitter is introduced at the top right. It can direct either beam towards either path; thus note that whatever emerges from each exit port may have come by way of either path.

It is in this sense that the path information has been "erased".

Note that total phase differences are introduced along the two paths because of the different effects of passing through a glass plate, being reflected off its first surface, or passing through the back surface of a semi-silvered beam splitter and being reflected by the back (inner side) of the reflective surface.

The result is that waves pass out of both the top upwards exit, and also the top-right exit. Specifically, waves passing out the top exit interfere destructively, whereas waves passing out the upper right side exit interfere constructively.

A more detailed explanation of the phase changes involved here can be found in the Mach-Zehnder interferometer article. Also, the experiment depicted above is reported in full in a reference.

If the second beam splitter in the lower diagram could be inserted or removed one might assert that a photon must have traveled by way of one path or the other if a photon were detected at the end of one path or the other. The appearance would be that the photon "chose" one path or the other at the only (bottom left) beam splitter, and therefore could only arrive at the respective path end.

The subjective assurance that the photon followed a single path is brought into question, however, if (after the photon has presumably "decided" which path to take) a second beam splitter then makes it impossible to say by which path the photon has traveled.

What once appeared to be a black and white issue now appears to be a "gray" issue. It is the mixture of two originally separated paths that constitutes what is colloquially referred to as "erasure." It is actually more like "a return to indeterminability."

The experiment

The experimental setup, described in detail in the original paper, is as follows. First, a photon is generated and passes through a double slit apparatus (vertical black line in the upper left hand corner of the diagram).

The photon goes through one (or both) of the two slits, whose paths are shown as red or light blue lines, indicating which slit the photon came through (red indicates slit A, light blue indicates slit B).

So far, the experiment is like a conventional two-slit experiment. However, after the slits a beta barium borate crystal (labeled as BBO) causes spontaneous parametric down conversion (SPDC), converting the photon (from either slit) into two identical entangled photons with 1/2 the frequency of the original photon. These photons are caused to diverge and follow two paths by the Glan-Thompson Prism.

One of these photons, referred to as the "signal" photon (look at the red and light-blue lines going upwards from the Glan-Thompson prism), continues to the target detector called D₀. The positions where these "signal" photons detected by D₀ occur can later be examined to discover if collectively those positions form an interference pattern.

The other entangled photon, referred to as the "idler" photon (look at the red and light-blue lines going downwards from the Glan-Thompson prism), is deflected by a prism that sends it along divergent paths depending on whether it came from slit A or slit B.

Somewhat beyond the path split beam splitters (green blocks) are encountered that each have a 50% chance of allowing the idler to pass through and a 50% chance of causing it to be reflected. The gray-green blocks in the diagram are mirrors.

Because of the way the beam splitters are arranged the idler can be detected by detectors labeled D₁, D₂, D₃ and D₄. Note that:

If it is recorded at detector D₃, then it can only have come from slit B.

If it is recorded at detector D₄ it can only have come from slit A.

If the idler is detected at detector D₁ or D₂, it might have come from either slit (A or B).

Thus, which detector receives the idler photon either gives information as to whether the signal photon with which it is entangled went through slit A or B ("which-path information"), or implies that such information is not available (from this source). Insofar as which-path information was potentially available from the idler photon earlier, it is said that the information has been "erased".

By using a coincidence counter the experimenters were able to isolate the entangled signal from the overwhelming photo-noise of the laboratory, recording only events where both signal and idler photons were detected.

When the experimenters looked only at the signal photons whose entangled idlers were detected at D₁ or D₂, they found an interference pattern.

However, when they looked at the signal photons whose entangled idlers were detected at D₃ or similarly at D₄, they found no interference.

This result is similar to that of the double-slit experiment since interference is observed when it is not known which slit the photon went through, while no interference is observed when the path is known.

However, what makes this experiment possibly astonishing is that, unlike in the classic double-slit experiment, the choice of whether to preserve or erase the which-path information of the idler need not be made until after the position of the signal photon has already been measured by D₀.

There is never any which-path information determined directly for the photons that are detected at D₀, yet detection of which-path information by D₃ or D₄ means that no interference pattern is observed in the corresponding subset of signal photons at D₀.

The results from Kim, et al. have shown that whether the idler photon is detected at a detector that preserves its which-path information (D₃ or D₄) or a detector that erases its which-path information (D₁ or D₂) determines whether interference is seen at D₀, even though the idler photon is not observed until after the signal photon arrives at D₀ due to the shorter optical path for the latter.

Some have interpreted this result to mean that the delayed choice to observe or not observe the path of the idler photon will change the outcome of an event in the past. However, an interference pattern may only be observed after the idlers have been detected (i.e., at D₁ or D₂). That conclusion follows, as will be explained below, because a single photon showing up on D₀ could be making a contribution to one of four different assemblages of photons, two different diffraction patterns and two different interference patterns.

Note that the total pattern of all signal photons at D₀, whose entangled idlers went to multiple different detectors, will never show interference regardless of what happens to the idler photons. One can get an idea of how this works by looking carefully at both the graph of the subset of signal photons whose idlers went to detector D₁ (fig. 3 in the paper), and the graph of the subset of signal photons whose idlers went to detector D₂ (fig. 4), and observing that the peaks of the first interference pattern line up with the troughs of the second and vice versa (noted in the paper as "a π phase shift between the two interference fringes"), so that the sum of the two will not show interference.

Explanation by physical optics

By examining the positions of signal photons at detector D₀, which correspond to idler photons at D₁ or D₂, an interference pattern is found in the recorded data. There seems to be a misconception, where this pattern originates from. One might think, the signal photons shape the pattern on the way to detector D₀ by interfering with each other. But at detector D₀ only a blurred image of the double slit is projected by the converging lens, effectively smearing any direct interference patterns from the slits.

To understand the source of the derived interference pattern, one has to focus on the third beam splitter BS_C, where the photon paths from both slits merge. At this point a phase difference exists between the merging paths, which is dependent on the different path lengths from slit A or B respectively to the splitter. Furthermore path length and phase difference depend in part on the deviation angle of the idler photon leaving the Glan-Thompson prism. While a fixed position on detector D₀ is correlated to events at detector D₁ or D₂, only events at D₁ or D₂ are inspected, which share the same phase differences. After leaving the beam splitter BS_C, each phase difference may lead to constructive or destructive interference on the paths from the splitter to the detectors D₁ and D₂, while also allowing any arbitrary intermediate values. But one has to note, that the combined probabilities for both paths behind BS_C always add up to 1, as the difference of the phase shifts between that paths amounts to π or 180°.

By changing the detector D₀ position, different phase shifts at detector D₁ and D₂ lead to a different statistic in observed correlated events: A derived interference pattern builds up in the data. Consequently the derived patterns from detectors D₁ and D₂ add up to the Gaussian distribution, which is observed with the detectors D₃ and D₄.

Data from events correlated with photons at detectors D₃ and D₄ show no derived interference patterns, because there is no interference of different photon paths from both slits in the first place.

Time relations among data

Raw results for D₀ are all delivered to the same detector regardless of what happens at the other detectors.

By noting which photons reaching Detector 0 correspond with photons reaching Detectors 1, 2, 3, and 4, it is possible to sort photon records collected by Detector 0 into four groups. Only then will it become possible to see interference patterns in two groups and only diffraction patterns in the other two groups. If there were no coincidence counter, then there would be no way to distinguish any photon that arrives at Detector 0 from any other photon that reaches it.

Photons will not reach detectors one through four in regular rotation, so the only way to sort out the photons that are entangled twins with the ones that reached each of those detectors is to group them according to which of those four detectors was activated when a photon reached Detector 0. Note that in the schematic diagrams the fringes or interference patterns imaged by Detector 1 and Detector 2 will add together to form a solid band. The addition of the diffraction patterns paired with the diffraction patterns seen by Detector 3 and Detector 4 will make the center area somewhat brighter than it would otherwise be, but would have no other influence on the confused picture produced by the raw data gathered at Detector 0.

It is impossible to know which group a photon appearing at Detector 0 at time T₁ may belong to until after its entangled partner is found at one of the other detectors and their coincidence is measured at some slightly later time T₂.

Discussion

Problems with using retrocausality

This section does not cite any sources. Please help improve this section by adding citations to reliable sources. Unsourced material may be challenged and removed. (August 2012) (Learn how and when to remove this message)

This delayed choice quantum eraser experiment raises questions about time, time sequences, and thereby brings our usual ideas of time and causal sequence into question. If a determining factor in the complicated (lower) part of the apparatus determines an outcome in the simple part of the apparatus that consists of only a lens and a detection screen, then effect seems to precede cause. So if the light paths involved in the complicated part of the apparatus were greatly extended in order that, e.g., a year might go by before a photon showed up at D₁, D₂, D₃, or D₄, then when a photon showed up in one of these detectors it would cause the photon in the upper, simple part of the apparatus to have shown up in a certain mode a year earlier. Perhaps by re-routing light paths to the four detectors during that one year so that the number of possible outcomes is reduced to two or even perhaps to one, then the experimenter could send a signal back through time. Changing between the first possible arrangement and second possible arrangement of parts in the complicated part of the experiment would then function like the opening and closing of a telegraph key.

Details pertaining to retrocausality in the Kim experiment

In their paper, Kim, et al. explain that the concept of complementarity is one of the most basic principles of quantum mechanics. According to the Heisenberg Uncertainty Principle, it is not possible to precisely measure both the position and the momentum of a quantum particle at the same time. In other words, position and momentum are complementary. In 1927, Niels Bohr maintained that quantum particles have both "wave-like" behavior and "particle-like" behavior, but can exhibit only one kind of behavior under conditions that prevent exhibiting the complementary characteristics. This complementarity has come to be known as the wave-particle duality of quantum mechanics. Richard Feynman believed that the presence of these two aspects under conditions that prevent their simultaneous manifestation is the basic mystery of quantum mechanics.

According to Kim, et al., "The actual mechanisms that enforce complementarity vary from one experimental situation to another." In the double-slit experiment, the common wisdom is that complementarity makes it seemingly impossible to determine which slit the photon passes through without at the same time disturbing it enough to destroy the interference pattern. A 1982 paper by Scully and Drühl circumvented the issue of disturbance due to direct measurement of the photon, according to Kim, et al. Scully and Drühl "found a way around the position-momentum uncertainty obstacle and proposed a quantum eraser to obtain which-path or particle-like information without introducing large uncontrolled phase factors to disturb the interference."

Scully and Drühl found that there is no interference pattern when which-path information is obtained, even if this information was obtained without directly observing the original photon, but that if you somehow "erase" the which-path information, an interference pattern is again observed.

In the delayed choice quantum eraser discussed here, the pattern exists even if the which-path information is erased shortly later in time than the signal photons hit the primary detector. However, the interference pattern can only be seen retroactively once the idler photons have already been detected and the experimenter has obtained information about them, with the interference pattern being seen when the experimenter looks at particular subsets of signal photons that were matched with idlers that went to particular detectors.

The main stumbling block for using retrocausality to communicate information

The total pattern of signal photons at the primary detector never shows interference, so it is not possible to deduce what will happen to the idler photons by observing the signal photons alone, which would open up the possibility of gaining information faster-than-light (since one might deduce this information before there had been time for a message moving at the speed of light to travel from the idler detector to the signal photon detector) or even gaining information about the future (since as noted above, the signal photons may be detected at an earlier time than the idlers), both of which would qualify as violations of causality in physics. The apparatus under discussion here could not communicate information in a retro-causal manner because it takes another signal, one which must arrive via a process that can go no faster than the speed of light, to sort the superimposed data in the signal photons into four streams that reflect the states of the idler photons at their four distinct detection screens.

In fact, a theorem proved by Phillippe Eberhard shows that if the accepted equations of relativistic quantum field theory are correct, it should never be possible to experimentally violate causality using quantum effects (see reference for a treatment emphasizing the role of conditional probabilities).

Yet there are those who persevere in attempting to communicate retroactively

Some physicists have speculated about the possibility that these experiments might be changed in a way that would be consistent with previous experiments, yet which could allow for experimental causality violations.

References

^ Kim, Yoon-Ho (2000). "A Delayed Choice Quantum Eraser". Physical Review Letters. 84: 1–5. arXiv:quant-ph/9903047. Bibcode:2000PhRvL..84....1K. doi:10.1103/PhysRevLett.84.1. {{cite journal}}: Unknown parameter |coauthors= ignored (|author= suggested) (help)
Jacques, Vincent; Wu, E; Grosshans, Frédéric; Treussart, François; Grangier, Philippe; Aspect, Alain; Rochl, Jean-François (2007). "Experimental Realization of Wheeler's Delayed-Choice Gedanken Experiment". Science. 315 (5814): pp. 966–968. arXiv:quant-ph/0610241. Bibcode:2007Sci...315..966J. doi:10.1126/science.1136303. PMID 17303748. {{cite journal}}: |pages= has extra text (help)
Greene, Brian (2004). The Fabric of the Cosmos. Alfred A. Knopf. p. 198. ISBN 0-375-41288-3.
Scully, Marlan O. (1982). "Quantum eraser: A proposed photon correlation experiment concerning observation and "delayed choice" in quantum mechanics". Physical Review A. 25 (4): 2208–2213. Bibcode:1982PhRvA..25.2208S. doi:10.1103/PhysRevA.25.2208. {{cite journal}}: Unknown parameter |coauthors= ignored (|author= suggested) (help)
Eberhard, Phillippe H. (1989). "Quantum field theory cannot provide faster-than-light communication". Foundations of Physics Letters. 2 (2): p. 127–149. Bibcode:1989FoPhL...2..127E. doi:10.1007/BF00696109. {{cite journal}}: |pages= has extra text (help); Unknown parameter |coauthors= ignored (|author= suggested) (help)
Bram Gaasbeek. Demystifying the Delayed Choice Experiments. arXiv preprint, 22 July 2010.
John G. Cramer. NASA Goes FTL - Part 2: Cracks in Nature's FTL Armor. "Alternate View" column, Analog Science Fiction and Fact, February 1995.
Paul J. Werbos, Ludmila Dolmatova. The Backwards-Time Interpretation of Quantum Mechanics - Revisited With Experiment. arXiv preprint, 7 August 2000.

External links

Categories:

Misplaced Pages