Robert M. Dimeo Summer School on Methods and Applications of Neutron Spectroscopy HFBS Measurement...
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![Page 1: Robert M. Dimeo Summer School on Methods and Applications of Neutron Spectroscopy HFBS Measurement Team Zema Chowdhuri, Craig Brown, Terry Udovic June.](https://reader036.fdocuments.us/reader036/viewer/2022062804/56649ee05503460f94bf055b/html5/thumbnails/1.jpg)
Robert M. Dimeo
Summer School on Methods and Applications of Neutron Spectroscopy
HFBS Measurement TeamZema Chowdhuri, Craig Brown, Terry Udovic
June 9-13, 2003
NIST Center for Neutron ResearchGaithersburg, MD 20899
Quantum Rotations in Methyl Iodide
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What are quantum rotations?
• Molecules in molecular solids can undergo reorientational motion
• H2 is a dumbell rotor and its quantum rotations are nearly “free” (i.e. no barrier hinders its motion)
• Hindered rotors can perform torsional oscillations and even rotational tunneling through the barrier!
I2B
,2,1,0,1BE2
l)l(ll
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Why study quantum rotations?
• Rotational dynamics as studied with neutrons reflect the molecular environment, i.e. the energy landscape
• Neutron tunneling spectroscopy provides extremely detailed information on the shape and magnitude of the potential energy of the molecular groups.
• Rotational tunneling measurements can be used to quantify interatomic interactions.
• Good test of first-principles/DFT calculations
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Bulk CH3IA Canonical Rotational System
PropertiesMP: -66.5oCMW: 141.94 g/molDipole moment: = 1.62 debye
Projection onto the a-c plane (Prager et.al.,J.Chem.Phys. 86, 2563 (1987))
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The Methyl Group: CH3
I[CH3] = 5.310-47 kg•m2
meV65.0I2
B2
• We want to study the dynamics about the main molecular axis
Free rotor energy levels: ,2,1,0j,BjE 2j
Useful conversions1 meV 4 ps1 eV 4 ns
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Bulk CH3I Dynamics
• Interaction potential of methyl group (1) van der Waals term, (2) short-range steric repulsion, and (3) additional multipole terms
• Simplified model based on symmetry alone:
tunneling
libration
stochasticreorientation
kBT
θ3cos12
VθV 3
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Bulk CH3I Dynamics
Tunneling energy very sensitive to the barrier height!
θ3cos12
V
dθ
dBH 3
2
2
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Rotational Tunneling
0
10
20
30
40
50
-50 0 50 100 150 200 250 300
(o)
nLIB
= 0
V(
) (m
eV)
nLIB
= 1
nLIB
= 2
• Tunneling rate (…and energy) proportional to the overlap of the wavefunctions through the barrier
• Overlap increases with librational level (nLIB) hence tunneling rate increases with librational level
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Librational Motion
• Librations are torsional oscillations• Harmonic approximation:
30 BV30LIBn 2
1nE
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Measurement TechniqueInelastic Neutron Scattering
• Neutrons are highly penetrating
• Wavelengths on order of intermolecular spacing (~Å)
• Energies on order of molecular excitations (~eV-meV)
• No symmetry-based selection rules as in optical techniques
• Simple interpretation of spectra
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Using Inelastic Neutron Scattering to See Quantum
Rotations
• Neutrons can induce a spin flip in hydrogenous species
• Incoherent scattering
• Simple case: H2
= rot ns elvib (elvib are in the totally symmetric ground state)
must be AS upon nuclear exchange (composed of 2 fermions)
ns must be AS(S) if rot is S(AS)
21AS
ns
21
Sns
J = 1, ortho
J = 0, para
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Using Inelastic Neutron Scattering to See Quantum
Rotations
• For a methyl group rotation three spins involved so must construct the S and AS spin functions
• Observed transitions: AE and EE• Situation is more complex but still need to flip a spin to induce a
transition between rotational states
= ei2
*
*
*
*
313
13
13
1
ASns
313
1SnsA
E
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Using Inelastic Neutron Scattering to See Quantum Rotational
Tunneling
9
3QRj45QA
2
1QA1QA,QS
00
tt00
Neutron scattering law for methyl tunneling
R: radius of methyl groupt: tunneling energyA0: elastic incoherent structure factor
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High Flux Backscattering Spectrometer
NIST Center for Neutron Research
• High energy resolution is often necessary to observe rotational tunneling directly.
• Typical neutron techniques to study tunneling include TOF, backscattering, and neutron spin-echo
• No other neutron spectrometer in North America is capable of measuring the tunnel splitting of CH3I!
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Are the HFBS measurements enough?
• Measuring the tunneling energy allows you to estimate the barrier height V3
• With knowledge of the barrier height you can estimate the librational transition energy E0
• Confirmation that this model is correct requires that we perform an independent measurement like measuring the librational transition and comparing the measurement with our estimate
Can we stop here and declare victory?….NO!
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Filter Analyzer Neutron SpectrometerNIST Center for Neutron Research
• S(Q,E) reflects density of vibrational (librational) modes, G(E)
• Vary initial energy, fix final energy
• Measures energy transfers of order 10’s-100’s meV