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Experimental loophole-free violation of a Bell inequality using entangled electron spins separated by 1.3 km

B. Hensen, H. Bernien, A. E. Dréau

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A. Reiserer, N. Kalb, M. S. Blok, J. Ruitenberg, R. F. L. Vermeulen, R. N. Schouten, C. Abellán, W. Amaya, V. Pruneri, M. W. Mitchell, M. Markham, D. J. Twitchen, D. Elkouss, S. Wehner, T. H. Taminiau, R. Hanson

2015 · arXiv

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From the abstract

For more than 80 years, the counterintuitive predictions of quantum theory have stimulated debate about the nature of reality. In his seminal work, John Bell proved that no theory of nature that obeys locality and realism can reproduce all the predictions of quantum theory. Bell showed that in any local realist theory the correlations between distant measurements satisfy an inequality and, moreover, that this inequality can be violated according to quantum theory. This provided a recipe for experimental tests of the fundamental principles underlying the laws of nature. In the past decades, numerous ingenious Bell inequality tests have been reported. However, because of experimental limitations, all experiments to date required additional assumptions to obtain a contradiction with local realism, resulting in loopholes. Here we report on a Bell experiment that is free of any such additional assumption and thus directly tests the principles underlying Bell's inequality. We employ an event-ready scheme that enables the generation of high-fidelity entanglement between distant electron spins. Efficient spin readout avoids the fair sampling assumption (detection loophole), while the use of fast random basis selection and readout combined with a spatial separation of 1.3 km ensure the required locality conditions. We perform 245 trials testing the CHSH-Bell inequality $S \leq 2$ and find $S = 2.42 \pm 0.20$. A null hypothesis test yields a probability of $p = 0.039$ that a local-realist model for space-like separated sites produces data with a violation at least as large as observed, even when allowing for memory in the devices. This result rules out large classes of local realist theories, and paves the way for implementing device-independent quantum-secure communication and randomness certification.

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7 selected excerpts · 7 total mentions

eigenket
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Ok I think I understand your intention with the code now. Sorry I was wrong before. I think what you're talking about here is what gets called the "detection loophole" in most of the literatire. The idea that if we detect only a small enough fraction of the events then they can be a sufficiently unrepresentative sample that we think we violated a Bell inequality even though the full statistics don't. This has (in my opinion) been comprehensively addressed already. You can check out the references in the section of the wiki article here https://en.wikipedia.org/wiki/Bell_test#Detection_loophole but basically if you detect enough of the possible events in the experiment…
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there is no way for nature to "trick" you in this way, "enough" is 83% for the standard CHSH inequality or 66% if you use a slightly modified. Recent experiments (in the last decade or so) are substantially over the threshold for the detection loophole to be a problem. This is one of the earliest papers where this loophole was closed with space-like seperated detectors from 2015. In this paper they used entangled NV centers in diamond as their qubits of choice, and so essentialy had zero events lost. https://arxiv.org/abs/1508.05949 This is a second one from the same time. This one uses a more standard setup with photons and worked with about 75% detector efficiency for each party (well above the 66% required) https://arxiv.org/abs/1511.03189 And this is a third with an efficiency of 78% for Alice and 76% for Bob https://arxiv.org/abs/1511.03190 I therefore have a new challenge - break the CHSH inequality, while rejecting fewer than 17% of the events, or break the (easier) modified Bell inequality used in papers 2 & 3 while rejecting fewer than a third. Edit: This is another, more recent paper where they use superconducting qubits and again lose no events https://www.nature.com/articles/s41586-023-05885-0
Schroedingers2c
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You can think of scenarios in which any classical state (i.e. the shared state is completely specified by the local states of the two kids) does the task with some success probability that is upper bounded, say by 75%. And you can even include some unspecified hidden variable in your classical state and could even allow the two kids to share some classical randomness (think: each of them has a button that returns the same random number for both kids). This hidden variable could be anything (a single unknown property, a whole collection of unknown properties or whatever really) and represents possibly incomplete knowledge, for example due to imperfect microscopes or…
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equipment. Since you don't specify what this hidden variable is, it encapsulates anything that is allowed by classical physics (remember we started out with a classical state). Now lets allow entangled states between the kids (states that can only be specified if you have both subsystems, locally if you measured such a state your result will look at least a bit random or even completely random). Then you can prove that the two kids can do the task (that has classical success probability 75%) with success probability ~85% all of a sudden. You can write down general inequalities that describe such behaviour and that's what Bell inequalities are. The fact that entangled states in quantum mechanics violate the classical bound (which you cannot break if you demand your two kids can only share states allowed by classical physics, even if you allow unspecified hidden variables), proves that nature is not classical. It doesn't prove that nature is quantum, it just proves that nature is not classical. Bell inequalities have also been unambiguously experimentally verified [1]. In conclusion, nature allows for two-party (or multi-party) states that cannot be described by just describing the local parts of it. There is no information in the local parts, but if you look at both parts together then there is information. Think "the whole is more than the sum of its parts". Classically, the whole is the sum of its parts. Classically, you read a book page by page. If your pages are entangled with each other, you could only read your book by looking at all pages together, because if you looked a single pages separately anything written there would look like random garbage to you. The question that remains is: Where is the information then, physically? In some sense you could say it does not exist before measurement, because only when you look at the correlations between the local measurement results of the two kids will you find out that the underlying state must have been entangled (which you get to know if the state violates a Bell inequality). But that is just one possible interpretation, there still is a lot of scientific debate about what quantum mechanics really means. These are exactly the scenarios that make quantum so weird but fascinating at the same time. [1] https://www.nature.com/articles/nature15759
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GistNoesis
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Replying here due to max comment depth tree, to explain in more detail. About the link between boole's and bell's inequalities : There are tons of paper : A quick search for example https://arxiv.org/pdf/quant-ph/0406004.pdf (I just skimmed it for a few seconds but it's probably talking about the right thing) In the paper you suggest https://arxiv.org/abs/1508.05949, there is nothing which looks like a probability definition. Assuming the world is using continuous fields, defining the probability for what register as a discrete event like a "blip" must be done carefully, it's not a trivial thing. Otherwise when you are taking joint probabilities and condition probability, it just tells you that those are questions you can't ask.
semi-extrinsic
Neutral mention · rule
It is a travesty to put forward such unfounded claims, and then point to as source a paper by the great Anthony Leggett on the use of condensed matter systems to probe the quantum measurement problem. What you are claiming is merely the proposition of "hidden variables" aka "local realism", a theory which has been thoroughly rejected by experimental measurements [1,2,3]. [1] https://www.nature.com/articles/nature15759 [2] https://doi.org/10.1103%2FPhysRevLett.115.250401 [3] https://doi.org/10.1103%2FPhysRevLett.115.250402
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jmcmichael
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Fine, here's another from Ronald Hensen at Delft: Experimental loophole-free violation of a Bell inequality using entangled electron spins separated by 1.3 km 2015 https://arxiv.org/abs/1508.05949v1 "...This result rules out large classes of local realist theories, and paves the way for implementing device-independent quantum-secure communication and randomness certification. "
eigenket
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If by Boole's inequality you mean the thing that I know as the union bound, then it is far from obvious to me that it is exactly the same as Bell's theorem. In fact they seem to me to be completely different. Boole's inequality also does not tell you "you're doing the math wrong when defining your measure", it tells you that the probability that either A or B happens is not greater than the sum of the probability of A happening and the probability of B happening. I'm not sure what you mean in the first part of your comment, could you indicate specifically what probability measure is defined incorrectly (or not defined) in (e.g.) this paper? https://arxiv.org/abs/1508.05949
jmcmichael
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In this instance, the popular understanding corresponds to the latest research better than realist theories like pilot-wave theory. Proponents of realist interpretations of QM have relied for decades on identifying possible classical channels of relativistic communication, or theorizing the existence of hidden variables. The double slit experiment has been used in various forms to, over time, eliminate these channels. I'm not a physicist, but the language that they are using quite a few papers leads me to believe that these channels have been closed, and the realists are out of remaining options for maintaining realism. For instance: An experimental test of non-local…
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realism, 2007 https://arxiv.org/abs/0704.2529 Wherein the authors show, using previously untested correlations between two entangled photons, that maintaining realist interpretations of quantum mechanics (such as pilot-wave theory) as a fundamental concept require the introduction of locality-defying 'action at a distance' actions. Quantum erasure with causally disconnected choice, 2012 https://arxiv.org/abs/1206.6578 Wherein the authors, using an interferometric quantum eraser experiment, eliminate past and future communication channels by enforcing Einstein locality via a mechanism that I don't understand yet. They conclude that, "No naive realistic picture is compatible with our results because whether a quantum could be seen as showing particle- or wave-like behavior would depend on a causally disconnected choice. It is therefore suggestive to abandon such pictures altogether." Experimental non-classicality of an indivisible quantum system, 2011 https://arxiv.org/abs/1106.4481 I understand even less of this one, looks like it has to do with performing the kinds of simultaneous measurements of various properties that one would expect to be able to, if realist interpretations were true. They conclude, "Not only is a single qutrit the simplest system in which such a contradiction is possible, but, even more importantly, the contradiction cannot result from entanglement, because such a system is indivisible, and it does not even allow the concept of entanglement between subsystems." UPDATE: Experimental loophole-free violation of a Bell inequality using entangled electron spins separated by 1.3 km 2015 https://arxiv.org/abs/1508.05949v1 "For more than 80 years, the counterintuitive predictions of quantum theory have stimulated debate about the nature of reality. ... In the past decades, numerous ingenious Bell inequality tests have been reported. However, because of experimental limitations, all experiments to date required additional assumptions to obtain a contradiction with local realism, resulting in loopholes. Here we report on a Bell experiment that is free of any such additional assumption and thus directly tests the principles underlying Bell's inequality. ... This result rules out large classes of local realist theories, and paves the way for implementing device-independent quantum-secure communication and randomness certification." I'm not aware of any significant challenges to these studies.

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