News Release

Mapping the optimal route between two quantum states

Experiment measures millions of quantum trajectories to predict 'most likely' route

Peer-Reviewed Publication

Chapman University

Cover of July 30 issue of Nature

image: This is the cover of the July 30 issue of Nature. view more 

Credit: Nature

As a quantum state collapses from a quantum superposition to a classical state or a different superposition, it will follow a path known as a quantum trajectory. For each start and end state there is an optimal or "most likely" path, but it is not as easy to predict the path or track it experimentally as a straight-line between two points would be in our everyday, classical world.

In a new paper featured on the July 30 cover of Nature, scientists from the Institute for Quantum Studies at Chapman University, the University of Rochester, University of California at Berkeley, and Washington University in St. Louis have shown that it is possible to track these quantum trajectories and compare them to a recently developed theory for predicting the most likely path a system will take between two states.

Andrew N. Jordan, professor of physics at the University of Rochester and member of Chapman's Institute for Quantum Studies, is one of the authors of the paper. His group had developed this new theory in an earlier paper. The results published this week show good agreement between theory and experiment.

For their experiment, the Berkeley and Washington University teams devised a superconducting qubit with exceptional coherence properties, permitting it to remain in a quantum superposition during the continuous monitoring. The experiment actually exploited the fact that any measurement will perturb a quantum system. This means that the optimal path will come about as a result of the continuous measurement and how the system is being driven from one quantum state to another.

Kater Murch, co-author and assistant professor at Washington University in St. Louis, explained that a key part of the experiment was being able to measure each of these trajectories while the system was changing, something that had not been possible until now. This was made possible by using a breakthrough called "weak measurements" introduced by Chapman University's Yakir Aharonov.

"Everybody knows that if your only tool is a hammer, then you tend to treat everything as if it were a nail" says Prof. Jeff Tollaksen, Director of Chapman's Institute for Quantum Studies. "But a whole new world opens up when we make weak measurements."

Jordan compares the experiment to watching butterflies make their way one by one from a cage to nearby trees.

"Each butterfly's path is like a single run of the experiment," said Jordan. "They are all starting from the same cage, the initial state, and ending in one of the trees, each being a different end state."

By watching the quantum equivalent of a million butterflies make the journey from cage to tree, the researchers were in effect able to predict the most likely path a butterfly took by observing which tree it landed on (known as post-selection in quantum physics measurements), despite the presence of a wind, or any disturbance that affects how it flies (which is similar to the effect measuring has on the system).

"The experiment demonstrates that for any choice of final quantum state, the most likely or 'optimal path' connecting them in a given time can be found and predicted," said Jordan. "This verifies the theory and opens the way for active quantum control techniques."

He explained that only if you know the most likely path is it possible to set up the system to be in the desired state at a specific time.

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Jordan and Tollaksen recently wrote about these results in a Springer book titled Quantum Theory: a Two-Time Success Story. Yakir Aharonov Festschrift (edited by Struppa and Tollaksen). Jordan also recently gave a talk at the Institute for Quantum Studies on the subject of the cover story for Nature. The talk can be viewed at http://ibc.chapman.edu/Mediasite/Play/2620fe48c1e243388d890ab0352f2fa41d.

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