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Scattering Summary ∂α/∂q
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Polarisability
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Scattering Theory Quantum Picture
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Raman
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●---● Rotational Raman Spectroscopy
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http://www.grc.nasa.gov/WWW/RT/2006/RT/RTB-nguyen3.html
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-iħ ∂/∂q Schrödinger Recipe
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H = ½ω(p 2 + q 2 ) The Harmonic Oscillator QM
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αα βαββ αβ Spin
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Double monochromater
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Example [p,q] = iħ So p the momentum and q the coordinate of a quantum system may not be measured precisely simultanoesly From this we deduce Heisenberg’s Uncertainty Principle ∆p∆q ~ ħ and ∆E∆t ~ ħ Which indicates that we can measure the energy of a molecule but when it had that energy
![Example [p,q] = iħ So p the momentum and q the coordinate of a quantum system may not be measured precisely simultanoesly From this we deduce Heisenberg’s Uncertainty Principle ∆p∆q ~ ħ and ∆E∆t ~ ħ Which indicates that we can measure the energy of a molecule but when it had that energy](http://images.slideplayer.com./27/8997696/slides/slide_21.jpg "Example [p,q] = iħ So p the momentum and q the coordinate of a quantum system may not be measured precisely simultanoesly From this we deduce Heisenberg’s Uncertainty Principle ∆p∆q ~ ħ and ∆E∆t ~ ħ Which indicates that we can measure the energy of a molecule but when it had that energy")
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