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Explore the quantum decoherence of excited states in biomolecules, discussing complexity, quantum dynamics, and minimal models. Investigate the effects of water, role of environment, and essential physics parameters in quantum systems. Learn about decoherence mechanisms, decoherence timescales, and spectral density extraction methods.
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Quantum decoherence of excited states of optically active biomolecules Ross McKenzie
Outline • Optically active biomolecules as complex quantum systems • A minimal model quantum many-body Hamiltonian • Spectral density for system-environment interaction is well characterised. • Observing the ``collapse’’ of the quantum state! • Ref: J. Gilmore and RHM, quant-ph/0609075
Some key questions concerning biomolecular functionality Which details matter? • What role does water play? • Do biomolecules have the optimum structure to exploit dynamics for their functionality? • When is quantum dynamics (e.g., tunneling, coherence) necessary for functionality?
Why should quantum physicists be interested in biomolecules? Photo-active biomolecules are tuneable systems at the quantum-classical boundary • Retinal, responsible for vision • Single photon detector • Quantum dynamics when the • Born-Oppenheimer approx. breaks down • - Entanglement of electrons & nuclei • - Effect of decoherence on Berry’s phase Photosynthetic Light harvesting complexes Quantum coherence over large distances?
A complex quantum system: Photo-active yellow protein Quantum system = Ground + electronic excited state of chromophore Environment = Protein + Water bound to Protein + Bulk water
Seeking a minimal model for this quantum system and its environment • Must capture and give insights into essential physics. • Tells us which physical parameters lead to qualitative changes in quantum dynamics.
Independent boson model Hamiltonian • Chromophore is two level system (TLS). • The environment is modelled as an infinite bath of harmonic oscillators. • Effect of environment on quantum dynamics of TLS is completely determined by the spectral density:
Leggett’s important idea • We don’t need to know all the microscopic details of the environment, nor its interaction with the system. Only need J( ). • Spectral density can be determined from measurements of the classical dynamics. • Most spectral densities are ``ohmic’’, i.e., J( ) ≈ for < 1/t • t is relaxation time of the bath. • For a > 1 quantum dynamics is incoherent. Caldeira and Leggett, Ann. Phys. (1983); Leggett, J. Phys.: Cond. Matt. (2002).
Quantum dynamics of TLS TLS is initially in a coherent superposition state uncoupled from the bath. Reduced density matrix of TLS is Decay of coherence Spectral diffusion
``Collapse’’ of the wave function • Zurek (`82), Joos and Zeh (`85), Unruh (`89) • Environment causes decay of the off-diagonal density matrix elements (decoherence) • ``Collapse’’ occurs due to continuous ``measurement’’ of the state of the system by the environment. • What is the relevant time scale for these biomolecules? h/(kBT α) ~ 10 fsec
Spectral density can be extracted from ultra-fast laser spectroscopy • Measure the time dependence of the frequency of maximum fluorescence (dynamic Stokes shift) • Data can be fit to multiple exponentials. • Fourier transform gives spectral density!
An example • ANS is chromophore Pal, Peon, Zewail, PNAS (2002)
Femtosecond laser spectroscopy: Measurement of the time-dependent spectral shift of a chromophore in a solvated protein • Increasing pH unfolds (denatures) protein and exposes chromophore to more solvent. • Presence of protein reduces psec relaxation and adds ~50 psec relaxation. • Pal, Peon, Zewail, PNAS (2002)
Measured spectral densities • Three contributions of ohmic form • Bulk water (solvent) • as ~ 1-10 ts ~ 0.3-3 psec • Water bound to the protein, esp. at surface • ab ~ 10-100 tb ~ 10-100 psec • Protein • ap ~ 100-1000 tp ~ 1-100 nsec
Spectral density for diverse range of biomolecules & solvents
Classical molecular dynamics simulations C(t) for Trp (green) and Trp-3 in monellin (black) in aqueous solution at 300 K Nilsson and Halle, PNAS (2005).
Our continuum dielectric models for environment • We have calculated J(w) for 5 models for environment • Key feature is separation of time and distance scales: Protein much larger than chromophore • Relaxation time of Protein >> Bound water >> Bulk solvent • J(w) is sum of Ohmic contributions which we can identify with 3 different environments, protein, bound water, and bulk water
Key physics behind decoherence • Most chromophores have a large difference between electric dipole moment of ground and excited states. • Water is a very polar solvent (static dielectric constant s = 80) • Water molecules have a net electric dipole moment • Dipole direction fluctuates due to thermal fluctuations (typical relaxation time at 300K is ~1 psec) • Chromophore experiences fluctuating electric field • Surrounding protein does not completely shield chromophore from solvent.
What have we learned? • Complete characterisation of system-environment interaction for biomolecular chromophores. • These spectral densities can be used to make definitive statements about the importance of quantum effects in biomolecular processes. • Due to their tuneable coupling to their environment biomolecular systems may be model systems to use to test ideas in quantum measurement theory. • For chromophores the timescale of the ``collapse’’ is less than 100 fsec.
Incoherent Coherent t t t Localised Criteria for quantum coherent transfer of excitation energy between two chromophores J. Gilmore & RHM, Chem. Phys. Lett. (2006) Location of excitation with time
Realisation of spin-boson model for coupled chromophores • Excitation can be on either of two molecules • Each two energy levels What is the two level system? If only one excitation is present, effectively a two level system
Realisation of spin-boson model for coupled chromophores • Excitations transferred by dipole-dipole interactions (Forster) • Shine in blue, get out yellow! • Basis of Fluorescent Resonant Energy Transfer (FRET) spectroscopy • Used in photosynthesis to move excitations around What is the coupling?
Incoherent Coherent t t t Localised Criteria for quantum coherent transfer of excitation energy between two chromophores J. Gilmore & RHM, Chem. Phys. Lett. (2006) Location of excitation with time Coherent for α<1
Questions • How unusual is to have a physical system where the system-bath interaction is so well characterised? • What experiment would best elucidate the “collapse”?
A comparison: Retinal vs. Green Fluorescent Protein • Green Fluorescent Protein • Excited state 10000x longer • Fluoresces with high quantum efficiency • Bacteriorhodopsin • Non-radiative decay in 200fs • Specific conformational change Very different quantum dynamics of Chromophore determined by environment!
Flouresence from differentamino acid residues withinprotein Cohen et al, Science (2002)