[dropcap style=”font-size:100px; color:#992211;”]G[/dropcap]iven that we, being composed of matter, are not much more than a collection of whirling atoms squished into a pattern.
And that, seeing as the materials that form those atoms are basic star-stuff, it’s actually the information that organises them which is the important bit.
And that, seeing as that information is encoded at a quantum level, and quanta can exist in various states and dimensions.
Given all this, wouldn’t it be nice if we could somehow coax our quanta into picking, out of the infinite possibilities, a parallel universe/dimension where it’s A BIT BLOODY WARMER?
Until recently measuring a 27-dimensional quantum state would have been a time-consuming, multistage process using a technique called quantum tomography, which is similar to creating a 3D image from many 2D ones.
Professor Sam Beckett (right) displays the dangers of quantum leaping into another body mid-funeral.
Researchers at the University of Rochester have been able to apply a recently developed, alternative method called direct measurement to do this in a single experiment with no post-processing. The work is of interest because fast, accurate and efficient methods for characterizing high-dimensional states like this could be central in developing high security quantum communications systems, as well as to probe our fundamental understanding of quantum mechanics.
The work was published this week in Nature Communications by a team of researchers from the University of Rochester and the University of Glasgow. In the paper they demonstrate direct measurements of the quantum state associated with the orbital-angular momentum.
[quote]In quantum mechanics the
act of measuring a quantum state
disturbs it irreversibly, a
phenomenon referred to as
collapse of the wavefunction.
The trick lies with the first
measurement being so gentle
that it only slightly disturbs
“Our work shows that direct measurement offers an exciting alternative to quantum tomography,” said Robert Boyd, Professor of Optics and Physics at the University of Rochester and Canada Excellence Research Chair in Quantum Nonlinear Optics at the University of Ottawa.
“As the field of quantum information continues to advance, we expect direct measurement to play an increasingly important role in this.” Boyd added that although it is unclear exactly how much more efficient direct measurement is compared to quantum tomography, the lack of post-processing is a major factor in speeding-up direct measurements.
The uncertainty principle
Such direct measurements of the wavefunction might have appeared to be ruled out by the uncertainty principle – the idea that certain properties of a quantum system could be known with precision only if other properties were known poorly. However, direct measurement involves a “trick” that makes it possible.
Direct measurements consists of two types of measurements performed one after the other, first a “weak” measurement followed by a “strong” measurement. In quantum mechanics the act of measuring a quantum state disturbs it irreversibly, a phenomenon referred to as collapse of the wavefunction. The trick lies with the first measurement being so gentle that it only slightly disturbs the system and does not cause the wavefunction to collapse.
“It is sort of like peeking into the box to see if Schrodinger’s cat is alive, without fully opening the box,” said lead author Dr. Mehul Malik, currently a post-doctoral research fellow at the University of Vienna and who was a Ph.D. in Boyd’s group when the work was performed.
“The weak measurement is essentially a bad measurement, which leaves you mostly uncertain about whether the cat is alive or dead. It does, however, give partial information on the health of the cat, which when repeated many times can lead to near certain information as to whether the cat is alive or dead.”
Malik adds that the beauty of the weak measurement is that it does not destroy the system, unlike most standard measurements of a quantum system, allowing a subsequent measurement—the “strong” measurement of the other variable.
This sequence of weak and strong measurements is then repeated for multiple identically prepared quantum systems, until the wave function is known with the required precision.
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