Making molecules sing: Quantum beats and interference as probes of molecular structure Katharine Reid Inaugural lecture, May 27 th 2010.

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Presentation transcript:

Making molecules sing: Quantum beats and interference as probes of molecular structure Katharine Reid Inaugural lecture, May 27 th 2010

Wolverley High School, Kidderminster

Science at Wolverley Melvyn Kershaw

University of Sussex

Chemical Physics at Sussex Harry KrotoTony StaceTony McCafferyJohn Murrell

Light Sources

FlashlampLaser Broad band Incoherent Pulsed Narrow band Coherent Continuous

Spectral profile and bandwidth FlashlampContinuous laser

Molecules in excited states

Laser induced fluorescence

State-selection and detection

excitationcollisionemission Probing the dynamics of chemical reactions

Dick Zare

Stanford University

Interference Thomas Young A double slit

Interference Constructive: bright spot

Interference Destructive: dark spot

d L y Interference The first bright spot occurs at y = L/d If = 530 nm (green), L = 14 m and d = 50 microns Maximum of first bright spot is at y = 14.8 cm

Electron waves Atomic orbitals – bound electrons

Ejecting electrons with light

Simplifying spectra Thermal congestion State selection

Photoelectron interference patterns Laser polarization direction Constructive interference Destructive interference These patterns provide unique information on molecular structure

University of Nottingham Lunch time near the School of Chemistry, University Park!!

The “younger chemists” c. 1996

Who is the odd one out?

Time-resolved measurements

Photoinitiation of H 2 + Cl 2

Flash photolysis The Nobel Prize in Chemistry 1967 EigenNorrishPorter "for their studies of extremely fast chemical reactions, effected by disturbing the equilibrium by means of very short pulses of energy"

Understanding photochemistry visionphotosynthesissolar cells

Laser Bandwidth narrow band continuous/long pulse broad band short pulse

State-selection... Narrow band Long pulse Broad band Short pulse

Vibrational states in polyatomic molecules

On excitation only certain vibrational states can be prepared

Vibrations can be coupled

Time-resolved measurements t = 0 t1t1 t2t2

Nano what? 1 ps = 1000 fs

Femtochemistry The Nobel Prize in Chemistry 1999 "for his studies of the transition states of chemical reactions using femtosecond spectroscopy” Ahmed Zewail

Intramolecular vibrational energy redistribution Timescale: tens of picoseconds

Questions 1.What is the timescale? 2.What is the mechanism (which dark states are involved)? 3.Can we influence the process? (Bond-selective chemistry, coherent control, mode-specificity) 4.What can we learn about chemical reactivity?

The experiments!

Toluene absorption spectrum

Photoelectron imaging

t = 0 t1t1 t2t2

0 ps

1 ps

2 ps

3 ps

4 ps

5 ps

6 ps

Time-resolved photoelectron spectra

Peak intensities versus time Time delay / picoseconds

Quantum beats

Beating patterns E Hz F Hz

Making molecules sing?

Coupled vibrational states Three states = two observable frequencies

Analysis of quantum beats in toluene From this we can learn: 1.The timescale of the dynamics 2.The “coupling matrix elements” 3.The exact vibrational energies More importantly, we have developed and tested a method that can be used to interrogate more complicated dynamical processes.

Toluene at higher excitation energy... Intensity decreases with time Intensity increases with time

Where to from here?

Support Neil Barnes Mike Towrie Pavel Matousek Kate Ronayne The workshop Students Dave Townsend Paul Whiteside Chris Hammond Paul Hockett Mick Staniforth Alistair Green Jonathan Midgley Postdocs Simon Duxon Tom Field Jon Underwood Julia Davies Susan Bellm Adrian King Help with this lecture Neil Barnes Paul Gaetto Collaborators Ivan Powis Tim Wright Thanks to: Mentors Melvyn Kershaw Tony McCaffery Dick Zare

And thanks to everyone for their support.