Scientists use quantum mechanics to show that glass should melt near absolute zero
- Date:
- February 4, 2011
- Source:
- American Friends of Tel Aviv University
- Summary:
- By cooling glass to a temperature near absolute zero (-459.67 degrees Fahrenheit), a professor is demonstrating that, at the quantum level, glass exhibits a very different behavior than might be expected from traditional physics -- in fact, it melts.
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Quantum mechanics, developed in the 1920s, has had an enormous impact in explaining how matter works. The elementary particles that make up different forms of matter -- such as electrons, protons, neutrons and photons -- are well understood within the model quantum physics provides. Even now, some 90 years later, new scientific principles in quantum physics are being described. The most recent gives the world a glimpse into the seemingly impossible.
Prof. Eran Rabani of Tel Aviv University's School of Chemistry and his colleagues at Columbia University have discovered a new quantum mechanical effect with glass-forming liquids. They've determined that it's possible to melt glass -- not by heating it, but by cooling it to a temperature near absolute zero.
This new basic science research, to be published in Nature Physics, has limited practical application so far, says Prof. Rabani. But knowing why materials behave as they do paves the way for breakthroughs of the future. "The interesting story here," says Prof. Rabani, "is that by quantum effect, we can melt glass by cooling it. Normally, we melt glasses with heat."
Turning the thermometer upside-down
Classical physics allowed researchers to be certain about the qualities of physical objects. But at the atomic/molecular level, as a result of the duality principle which describes small objects as waves, it's impossible to determine exact molecular position and speed at any given moment -- a fact known as the "Heisenberg Principle." Based on this principle, Prof. Rabani and his colleagues were able to demonstrate their surprising natural phenomenon with glass.
Many different materials on earth, like the silica used in windows, can become a glass -- at least in theory -- if they are cooled fast enough. But the new research by Prof. Rabani and his colleagues demonstrates that under very special conditions, a few degrees above absolute zero (−459.67° Fahrenheit), a glass might melt.
It all has to do with how molecules in materials are ordered, Prof. Rabani explains. At some point in the cooling phase, a material can become glass and then liquid if the right conditions exist.
"We hope that future laboratory experiments will prove our predictions," he says, looking forward to this new basic science paving the way for continued research.
Classical glass
The research was inspired by Nobel Prize winner Philip W. Anderson, who wrote that the understanding of classical glasses was one of the biggest unsolved problems in condensed matter physics. After the challenge was presented, research teams around the world rose to it.
Until now, structural quantum glasses had never been explored -- that is, what happens when you mix the unique properties in glass and add quantum effects. Prof. Rabani was challenged to ask: if we looked at the quantum level, would we still see the hallmarks of a classical glass?
What the researchers unearthed is a new and unique hallmark, showing that quantum glasses have a unique signature. Many materials he says can form a glass if they're cooled fast enough. Even though their theory is not practical for daily use: few individuals own freezers that dip down nearly 500 degrees below zero.
Prof. Rabani is currently on sabbatical at the University of California, Berkeley, as a Miller Visiting Professor.
Story Source:
Materials provided by American Friends of Tel Aviv University. Note: Content may be edited for style and length.
Journal Reference:
- Thomas E. Markland, Joseph A. Morrone, Bruce J. Berne, Kunimasa Miyazaki, Eran Rabani, David R. Reichman. Quantum fluctuations can promote or inhibit glass formation. Nature Physics, 2011; 7 (2): 134 DOI: 10.1038/nphys1865
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