Showing posts with label quantum teleportation. Show all posts
Showing posts with label quantum teleportation. Show all posts

Sunday, April 16, 2017

That Nature is a Heraclitean Fire

Nick meets a Luck Wave (design by August O'Connor)
THAT NATURE IS A HERACLITEAN FIRE

I have spent more than a third of my life speculating (with congenial physicist friends) about what quantum mechanics might actually mean -- and have even written a book about it. The gist of the quantum dilemma is that we have a Quantum Theory that successfully predicts the results of every physical measurement. But with this theory comes an utter inability to tell a plausible story about what's really going on in the world -- both before, during and after a measurement. Physicists today possess an essentially perfect Quantum Theory, know how to experimentally produce subtle and delicate Quantum Facts, but cannot convincingly tell their kids a Quantum Reality story that adequately explains both Quantum Theory and Quantum Facts.

Many words concerning quantum reality were exchanged by quantum theory's founders -- especially Albert Einstein and Niels Bohr -- but not much progress was made until the remarkable discovery of Irish physicist John Stewart Bell who formulated an experimental test that could confidently eliminate an entire class of quantum reality models. Not only is it rare for physicists (or anybody else) to TALK ABOUT REALITY, it is even rarer (such was the importance of Bell's discovery) to come up with EXPERIMENTS ON REALITY. Consequently, Bell's original 1964 paper has become one of the most-cited publications in physics.

Bell's original experiment involved TWO ENTANGLED PHOTONS -- one sent to Alice and one to Bob. About this setup, quantum theory says two seemingly contradictory things: 1. that the quantum state of Bob's photon depends instantly (faster-than-light) on Alice's choice of what to measure; 2. that this apparent instantaneous action can never be used for signaling.

The physics jargon for instantaneous voodoo-like connections is the word "non-local". Non-local effects (either in theory or in practice) are as welcome in physics as a corpse at a wedding feast.

So before Bell came along, the theory of entangled systems was manifestly non-local (BAD!), but the same theory also assured that no experiment would ever be able to directly reveal this non-locality (GOOD!).

So quantum theory of entangled systems is NON-LOCAL: But all quantum facts are LOCAL.

What about quantum reality -- the underlying causal dynamics behind both theory and fact? Do we live in a world that's deep-down linked by abominable (to the physicist) non-local connections? Or is quantum reality nicely local, just like the quantum facts?

Bell's surprising conclusion (a powerful mathematical proof, not a mere conjecture) is that no local reality can underlie this everywhere local world.

Quantum reality must be non-local, according to Bell's proof.

To a physicist, Bell's conclusion is preposterous and must certainly be wrong. My first entry into the Bell's Theorem game was an attempt to disprove John Bell. Which ended in my formulating the world's shortest proof for the non-local nature of quantum reality.

Bell's Theorem is so simple that it is difficult to find a flaw. But Bell's greatest weakness can be summed up in the dichotomy: if reality exists, then it must be non-local; but if you DENY REALITY, then you are let off the hook.

But what could "denying reality" possibly mean?

One innocent (but crucial) assumption in Bell's proof is called "contrafactual definiteness" (or CFD, for short).

When you do the Bell experiment on a single pair of entangled photons, both Alice and Bob can set their detectors at only ONE SETTING. But to prove BT, you need to consider the possible results of FOUR SETTINGS. Four settings for the same two-photon event.

CFD assumes that: if we had performed three other measurements -- other than the actual one -- we would have gotten three definite (but unknown) results.

But if the nature of the quantum world is such that CFD is not valid, then you can't prove Bell's theorem. In fact, in a non-CFD world, you cannot even formulate Bell's theorem.

A recent paper by Gerold Gründler from Nürnberg, Germany, (What Does Bell's Inequality Actually Prove?) analyzes a few ways of "denying reality" by postulating (and perhaps even proving -- I am not sure) that we live in a world which does not support CFD. Gründler revisits and revises an earlier work by Israeli physicist, the late Asher Peres, entitled Unperformed Experiments Have No Results (3 page pdf).

Peres's paper suggests that we might live in a world where Unperformed Experiments Have No Results. But what are the details of such a world? How does it actually work?

What would it be like to live in a world where CFD is inconceivable?

Here's one attempt to visualize such a world.

Our thinking about the classical world is dominated by movies. It is easy to imagine rewinding the film, changing only one thing, then doing an (imaginary) retake. Certainly this cinematic model of reality allows us to at least imagine what the results of Unperformed Experiments might look like.

We can even add quantum randomness to the picture by allowing some features of the scene to depend on pure chance. Imagine filming a gambling table -- each reshoot, even of the same game, will give definite but different outcomes -- outcomes that are governed by statistical laws -- analogous to the probabilistic outcomes predicted by quantum mechanics. Bell's Theorem can be proved in a world like this -- a world of definite but statistically determined results.

To move into a non-CFD world, consider the case of a single Uranium atom. Physics considers all Uranium atoms to be EXACTLY THE SAME. Yet this one decayed in one second, while its identical sister is still alive after a million years. The first atom's short life is not due to some defect in its constitution. That's just the way the quantum world works -- identical quantum objects behave differently -- FOR NO REASON AT ALL.

Now consider how the movie analogy might work in a fully quantum world. We rewind the film, KEEP EVERYTHING THE SAME. Then change just one setting and reshoot the experiment.

Keeping everything the same is easy in a quantum world: every photon, electron, quark has always been just the same as every other. But the big problem is that each particle in the universe now behaves differently than in the first take -- giving rise to an entirely different universe -- a universe in which not only does the camera not exist, but the cameraman, the human species, and all life on Earth have vanished. In this second take on our present quantum reality the familiar Earth has no doubt disappeared as well.

As Heraclitus warned, you cannot step twice into the same river, because the river is never the same.

Might an Asher-Peres world in which Unperformed Experiments Have No Results be "hyper-Heraclitean" in the sense that in this kind of quantum reality even the same river is not the same river? In fact this river revisited second time round might not even be a river at all but the insides of a black hole.

Trying to visualize quantum worlds in which CFD is inconceivable might push us to think more deeply not only about fully quantum concepts such as "superposition", "entanglement" and "wave/particle duality" but also to revise our old-fashioned assumptions about everyday classical concepts such as "same", "different", "spontaneity" and even how to correctly use the word "again" when it comes to properly refilming in our imagination the very same event that has already happened once.

JUJITSU UNIVERSE
We house-broke quantum reality
Trained Schrödinger's Cat to purr
Now daily life's more uncanny
Than atoms ever were.

Asher Peres, who titled his bio "The cat who walks by himself", played a vital part in publicizing the role both he and myself played in the discovery of the quantum "no cloning rule". (How the no-cloning theorem got its name.) which eventually inspired MIT professor David Kaiser to write his popular science history book: How the Hippies Saved Physics. In addition to his pioneering work in quantum information theory, Asher Peres will probably be remembered most as a member of the team of six people who devised the remarkably clever Quantum Teleportation process.

The title of this post was taken from Gerard Manley Hopkins's splendid poem: That Nature is a Heraclitean Fire and of the comfort of the Resurrection.

Asher Peres (bottom right) and his five buddies who invented Quantum Teleportation


Wednesday, October 10, 2012

Quantum Teleportation

Alice and Bob make measurement choices concerning entangled photons A and B
One reason why medieval philosophers such as Thomas Aquinas never developed a sophisticated description of the material world might have been that the priorities of thinkers in the Middle Ages were different than our own. The aim of Thomas Aquinas and his colleagues was to discover the nature of God. Hence they treated the world not as a physical object with its own intrinsic laws but as the personal creation of a divine being. The facts of this world, unimportant in themselves, could tell us about the nature of God in much the same way as a painting or sculpture might inform us about the nature of the artist that created it. A bit of this same theological spirit surfaces in Einstein's famous statement: "I want to know the mind of God; all else is details."

Anyone seeking to know the nature of God by studying the physical universe will certainly be fascinated by quantum theory, our deepest and most successful theory of matter. Quantum theory is deeply paradoxical and seems to obey a distinctly non-human logic. One of the most peculiar feature of this theory is the way it seems to effortlessly embody seemingly contradictory aspects in the same phenomena. One of the most elegant examples of quantum theory's union of opposites is the recently discovered fact of quantum teleportation which unites in one system both a faster-than-light transmission of information plus a clear prohibition against humans using this undeniable FTL connection for sending FTL messages.

Quantum theory also embodies the unusual feature that the world we see depends on the questions that we pose. Hence the more sophisticated we become in asking questions of Nature, the more sophisticated will be Her replies.

Quantum teleportation is a special feature of quantum entanglement in which two photons emitted from a special source give up their individual identities and enter a collective state. The collective two-photon state has definite properties but the individual photons do not, until they are actually observed. For example, in the entangled state W(A,B,+), photons A and B will always be observed to have the same polarization; in the state X(A,B, -), photons A and B are always observed to have opposite polarization. These two entangled states W and X are part of a complete set of entangled two-photon states W, X, Y and Z, called the "Bell states" (after Irish physicist John Stewart Bell). Any two-photon state, whether entangled or not, can be expressed as a sum of the 4 Bell states. This fact is essential to the process of teleportation.

Alice obtains unknown photon "?" she wants to send to Bob

Alice acquires a photon "?" with an unknown polarization which she wants to teleport to Bob. This photon IS NOT ENTANGLED with Alice's photon A but Alice employs a clever trick--only possible in quantum theory. Alice expresses the quantum state of photon "?" and photon A as the sum of the four entangled Bell states W, X, Y and Z. She does this sum in such a way that all the entanglements cancel and the total quantum state of "?" and "A" is unentangled.

Alice's move reminds me of a string trick I learned as a kid in which you wrap a loop of string around your fingers in a complicated way so that it looks as though the fingers are entangled in the string. But upon pulling the string the fingers are freed--every loop of string was cancelled by an anti-loop. It's the same with the two photons--every seeming entanglement is cancelled somewhere by an anti-entanglement.

However because Bob's B photon is entangled with Alice's A photon, a kind of quantum magic occur in which the polarization "?" of Alice's unknown photon is transferred to Bob's photon B, although in a somewhat hidden form. To every term W, X, Y, Z in Alice's expression for her two states, there corresponds on Bob's side of things a quantum state that is either identical to "?" or differs from "?" only by a rotation R and/or a phase shift S. (R and S are fixed by the nature of the original AB entanglement and do not depend on "?".)

Given this setup, here's how quantum teleportation works.

Alice asks the question: which Bell state is my system in? This question can have one of four answers W, X, Y or Z. If the answer is W, then Bob's photon has the polarization "?". Teleportation is accomplished.

If the answer is X, Y or Z, the polarization of Bob's photon differs from "?" only by a rotation R, a phase shift S or a combination of both. So for 100% efficient teleportation all Bob has to know is what Alice's result was--W, X, Y or Z--a piece of knowledge that consists of only 2 bits of information. Without these two bits all that Bob sees is a random hash. With these two bits an infinite amount of information can be teleported. (The polarization of a photon can point anywhere on a sphere. The teleported information corresponds then to sending an unknown latitude and longitude on the surface of the Earth to a distant location faster than light. However this information cannot be decoded without the 2-bit key which must be sent by Alice to Bob at light speed or slower.) Thus a large quantity of quantum information can be teleported faster-than-light but this information is unrecognizable in the absence of a 2-bit code which can only be transferred over conventional channels.

Alice sends a 4-bit signal allowing Bob to decode an infinite-bit message

Quantum teleportation was discovered by a six-man team in 1993 and experimentally demonstrated a few years later. Teleportation is a particularly elegant example of quantum theory's subtle union of opposites--in this case the coexistence of a large FTL data transmission with the impossibility of sending signals faster-than-light.

Let's face it. We are only at the beginning of experiencing and appreciating the inhumanly beautiful mysteries of the quantum world.

QUANTUM REALITY

Shall I look at Her
Or shall I not?

Hard, small, separated
If I look;
Soft, spread-out, connected
If I don't.

Hard particle and soft wave: both?
Utterly random and perfectly predictable: both?
Small right-here and spread-out everywhere: both?
Deep connected yet lonely separate?

Honey
Some day You gotta show me
How You do that.