[tt] Curiosity doesn't have to kill the quantum cat - fundamentals - 09 May 2007 - New Scientist
Brian Atkins
<brian at posthuman.com> on
Thu May 10 04:07:48 UTC 2007
http://www.newscientist.com/article.ns?id=mg19426031.400&feedId=fundamentals_rss20
It may not have the swirling cameras and intense music of a TV emergency room,
but John Martinis's laboratory is about to provide just as much drama. Martinis,
a physicist at the University of California, Santa Barbara, is preparing a
landmark experiment. The objective? To bring an animal back from the brink of death.
It is not just any animal. This is Schrödinger's cat, the most famous feline in
physics. In a macabre thought experiment first mooted by Erwin Schrödinger in
1935, the cat's life is endangered by a quirk of quantum theory. Contained
within a closed box, the cat either lives or dies depending on the quantum state
of an atom, which is rigged up to a vial of poison gas. In one quantum state the
vial breaks, killing the cat. In the other it remains sealed. The twist is that
the atom's quantum state only takes a definite value when someone looks at it.
Before the box is opened, the cat is in a "superposition" of being both alive
and dead, and opening the box and looking in either kills the cat or saves it.
At least, that's the standard view. It now seems that the equations of quantum
theory offer a startling alternative, according to Andrew Jordan of the
University of Rochester in New York. Even when perilously close to death, the
cat can be saved.
There is more than an imaginary cat's life at stake here. Martinis's experiment
offers an insight into the fundamental nature of quantum measurement, and could
bring enormous pay-offs: the cat-in-a-box experiment might help the development
of computers that use quantum rules to dramatically speed up their calculations,
for example. The predicament of Schrödinger's cat may even have implications for
national security. What's more, discovering exactly how this quantum drama
unfolds may prove vital to our understanding of how the universe really works.
Even if our curiosity does ultimately kill the quantum cat, at least we'll know
it didn't die in vain.
At the centre of the Schrödinger's cat dilemma is the phenomenon of
superposition. In everyday life, we imagine a particle or object can exist only
in one particular state or position: either in position A or position B, say. In
the quantum realm, however, things can exist at both A and B simultaneously.
The only trouble is, we can never see this phenomenon. Experiments have
indirectly proved that superpositions really do occur, yet we never seem to
happen upon a cat that is both dead and alive. The act of observation or
measurement somehow forces the superposition to revert to the "classical" state,
in which the quantum particle takes one position or the other, but not both. Two
of the biggest questions in quantum physics are exactly how measurement achieves
this and whether there is a way to undo its effects. The answers, it seems, are
related, and are both to do with the fact that, in quantum mechanics, nothing
happens in a magic flash.
Physicists have long assumed that, like the death of a cat, measurements on
quantum systems are irreversible. But it turns out that is only because they
have made a simplifying assumption - one that they are now rejecting. "Quantum
measurement is usually taught in textbooks as an instantaneous process," Jordan
says. "What we've learned in the last few years is that real measurements don't
work that way. In nature, all processes take a finite time."
The breakthrough proof came last year, when Nadav Katz of the University of
California, Santa Barbara, working with some UCSB colleagues and Alexander
Korotkov of the University of California, Riverside, used an array of impressive
technologies to take a quick peek inside the box and glimpse the cat's state
(Science, vol 312, p 1498). They discovered that, rather than collapsing in an
instant, the superposition marches toward collapse one step at a time.
It is this gradual collapse that might save Schrödinger's cat. Korotkov, this
time working with Jordan, has figured out how one could monitor the cat's state
and then undo any damage that monitoring has done (Physical Review Letters, vol
97, p 166805). Martinis will soon be putting the idea to the test. "We think we
can do the experiment readily in the next few months," he says.
Performing the experiment will involve manipulating the quantum state of a loop
of superconducting wire known as a phase qubit. First, the researchers fire a
finely tuned microwave pulse at the loop. This puts the qubit into a "cat
state", akin to the dead-and-alive state of Schrödinger's cat, in which it sits
in an equal superposition of both of the qubit's possible energy states.
Until, that is, the measurement begins. As soon as the researchers begin to
perform a measurement, the superposition slides towards one state or the other.
The question is, which one? Is the cat going to live or die?
To answer that question without killing the cat, the researchers will look to
see whether or not the qubit performs a quantum trick called tunnelling. Faced
with an insurmountable barrier, there is nothing that a classical particle can
do. A quantum particle, on the other hand, can take advantage of the uncertainty
principle, which says you can never precisely define all the particle's
properties. That means that in certain circumstances there is a small
probability you will find it on the far side of this apparently insurmountable
barrier. The more energy a particle has, the more likely it is to tunnel when
given the opportunity; if the researchers see the qubit has tunnelled they will
know it has collapsed to the higher energy state.
In itself, that is disastrous, of course: if the researchers see the burst of
magnetic energy that indicates the particle has tunnelled to a higher energy
state, it means the measurement was completed and the cat is dead or alive. The
trick is to catch the qubit before it actually gets there.
To sneak a peek at the qubit's state midway through its collapse, the
researchers induce a steadily increasing voltage across the wire ring. This is
like teasing the qubit into "thinking" about tunnelling by making it easier to
cross the barrier. Then, at a certain threshold, they drop the voltage back down
again. It is equivalent to opening the box and then quickly closing the lid again.
Because quantum processes take a finite time, lowering the energy barrier then
raising it again acts as a "weak" form of measurement (New Scientist, 10 May
2003, p 28). If we don't see the qubit tunnel, we learn that there is some
finite probability that it is in the lower energy state. In other words, we have
gained information about a quantum system without destroying its delicate
superposition. The more time we risk leaving the barrier down without the qubit
tunnelling, the more certain we are of its low energy state.
Now it is time to undo any harm we have inflicted in the process. To do this,
the physicists fire another kind of microwave pulse, known as a pi-pulse, at the
qubit. This inverts the quantum states of the qubit: the higher energy level is
now the lower level and vice versa. The voltage is then ramped up and dropped
again. If the qubit doesn't tunnel this time, it becomes more likely that it is
in what is now the lower energy level. Where the first weak measurement pushed
the superposition one way, the second pushes it by the same amount the other
way, which means we end up right where we started. It is as if the qubit, or the
cat, had never been disturbed at all.
Jordan and Korotkov say that their prescription will work to undo any weak
quantum measurement, regardless of the experimental apparatus. Step one: take a
weak measurement that shifts a superposition state toward one definite state or
the other. Step two: swap the states around and take an identical second weak
measurement. Because the states have been swapped around in the interim, the
second measurement only serves to cancel out the effects of the first. You got
to see the cat, and without doing it any harm.
Not that it is a guaranteed success: if the qubit does tunnel during either the
first or the second weak measurement, the researchers have to begin again. The
other drawback is that you have to repeat the process many times to get the
information you want: each repeat only gets you a little more certainty about
the state of the cat. "From a single weak measurement we cannot say with
certainty that the cat is dead or alive," says Markus Buttiker, a theoretical
physicist at the University of Geneva in Switzerland. The more you repeat this
process, however, the more information you gain about the most likely
configuration of the superposition. In other words, you can satisfy your
curiosity without (for the most part) killing the cat.
If confirmed by experiment, the researchers believe they will have ruled out one
of the most popular explanations for how quantum things turn classical.
"Decoherence theory" suggests that the superposition never really collapses - it
only appears to collapse. What actually happens, according to this idea, is that
all the information about the system disperses into the environment: when a
quantum system interacts with a classical measuring device, it becomes
irreversibly entangled with all the particles that make up the measuring device
and its surroundings. All the information about the original state of the system
in superposition is then spread so thinly throughout the massively bigger
environment that it is, essentially, lost. The odds of identifying the original
state become far worse than the odds of randomly shuffling a deck of cards back
into perfect order.
According to Jordan, the weak measurement experiment should demonstrate that
decoherence theory cannot be correct. Weak measurements make superpositions
evolve towards one of the well-defined original states of the isolated system,
not into an ever-bigger mess of entanglements with everything around it. "In our
analysis of continuous weak measurements, we see that the system gets drawn to
one state or another," Jordan says. "That rules out decoherence theory." The
reversibility of weak measurements also stands against decoherence: if
information does spread into the environment, it shouldn't be possible to get it
back.
It would be useful to know whether decoherence is real or not, as it is seen as
one of the major obstacles to building a useful quantum computer (New Scientist,
26 June 2005, p 18). Also the reversibility of weak measurements may have
implications for cryptography based on quantum rules (see "Cracking the code").
But, more fundamentally, what will this all mean for Schrödinger's hapless cat?
Well, like doctors and surgeons, we still can't work miracles. If the quantum
state has tunnelled - if we find the cat completely dead, in other words - then
we will know the superposition has collapsed and we can't bring the cat back to
life.
However, weak measurements seem to indicate that if we peek into the box just
long enough to partially determine the cat's fate - say, if we find it very
close to dying - we can undo our weak measurement and restore the cat to the
relative safety of the original unknown state. "We wanted to find out, is
quantum measurement written in pen or pencil?" Jordan says. "Now we know it is
written in pencil."
This could be a very profound discovery. Since the birth of quantum theory we
have become used to thinking of quantum measurements as creating reality: until
things are measured, they don't have an absolute, independent existence. But if
some forms of measurement, such as weak measurement, are reversible, then the
fundamentals of quantum mechanics go even deeper than we realised. If you create
reality with weak quantum measurements, does undoing them erase the reality you
created?
It seems that Martinis's experiment might have a shocking twist just before the
end. To save the quantum cat, we might have to be willing to throw away the idea
that we live in a real, permanent cosmos that can't unravel before our eyes.
It's a true cliffhanger: will Martinis save Schrödinger's cat or the durable
fabric of your universe? Stay tuned for the next episode...
From issue 2603 of New Scientist magazine, 09 May 2007, page 32-36
Cracking the uncrackable code
If we really can perform "weak" quantum measurements whose disturbing effects
can be undone, it might have serious implications for the security of nations.
Quantum cryptography has been hailed as the future of cryptography because its
codes are impossible to crack; the US government and some major financial
institutions are already looking at ways to implement the technology. Commercial
quantum cryptography systems are available off the shelf for those with concerns
about corporate security. The unhackable nature of the technology, though,
relies upon the fact that a measurement of a quantum system changes the system
indelibly. If measurements can be undone, quantum cryptography could be in big
trouble.
In quantum cryptography, two people (usually referred to as Alice and Bob) must
agree upon a secret key that will be used to decipher a message. They do this by
exchanging entangled photon pairs - particles of light in a quantum state that
is extremely sensitive to disturbance by a standard quantum measurement. An
eavesdropper, Eve, might attempt to intercept the message, but this will disturb
the entanglement and Alice and Bob will become aware of her presence.
That all changes if Eve is able to make a weak measurement and then undo it
without leaving a trace. "An Eve who makes only a weak measurement will probably
be hard to detect by Bob and Alice," says Markus Buttiker, a theoretical
physicist at the University of Geneva in Switzerland.
There is a catch for Eve, though: with a weak measurement she will only gain a
small amount of information and so can't be certain what a message says.
However, she might get enough clues to decide whether to keep that information -
and risk getting caught - or use another weak measurement procedure to undo her
original measurement and remain undetected.
Quantum cryptography researchers are now trying to work out how to defeat this
threat. According to Andrew Jordan of the University of Rochester in New York,
it is not yet clear just how big a problem weak measurement might pose. "We're
working on that at the moment," he says.
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