Chapter 9 – Emerging Biophysics Techniques 423
would imply a kinetic energy for the electron during the transition equivalent to ca. −0.6 eV,
which is negative and thus forbidden.
However, experimentally it is known that electrons undergo these transitions (you are
alive while reading this book, for example… one hopes…), and one explanation for these
observations is that the electrons undergo quantum tunneling between the donor and
acceptor sites, over a rapid time scale predicted to be ~10 fs (i.e., ~10−14 s). Quantum tun
neling is also predicted to occur over longer length scales between secondary donor/acceptor
sites; however, even though the time scale of tunneling transitions is within reach of the tem
poral resolution of electron spectroscopy measurements, no definitive experiments, at the
time of writing of this book, have yet directly reported individual quantum tunneling events
between electron transport carrier proteins in OXPHOS.
In a vacuum, quantum tunneling over such long distances would be highly improbable.
However, in proteins, such as the electron transport carriers used in OXPHOS, the inter
vening soft-matter medium facilitates quantum tunneling by providing lower-energy virtual
quantum states, which in effect reduce the overall height of the tunneling energy barrier,
significantly increasing the physiological tunneling rates. The question is then not whether
quantum tunneling is a component of the electron transport mechanism—it clearly is. Rather,
it is whether these proteins evolved to utilize quantum tunneling as a selective advantage to
the survival of their cell/organism host from the outset (see Chapter 2), or if the drivers of
evolution were initially more aligned with classical physics with later tunneling capability
providing a significant advantage. In several ways, one could argue that it is remarkable that
the entire biological energy transduction machinery appears to be based on this quantum
mechanical phenomenon of tunneling, given that much of biology does not require quantum
mechanics at all.
A second interesting biological phenomenon, which is difficult to explain using classical
physics, is the fundamental process by which plants covert the energy from sunlight into
trapped chemical potential energy embedded in sugar molecules, the process of photosyn
thesis (see Chapter 2). Photosynthesis utilizes the absorption of photons of visible light by
light-harvesting complexes, which are an array of protein and chlorophyll molecules typ
ically embedded into organelles inside plant cells called “chloroplasts,” expressed in high
numbers to maximize the effective total photon absorption cross-sectional area. Since the
early twenty-first century, there has been experimental evidence for coherent oscillatory
electronic dynamics in these light-harvesting complexes, that is, light-harvesting complexes
in an extended array, which are all in phase with regard to molecular electronic resonance.
When initially observed, it was tempting to assign this phenomenon to quantum coher
ence, a definitive and nontrivial quantum mechanical phenomenon by which the relative
phases of the wave functions of particles, electrons in this case, are kept constant. However,
these oscillation patterns alone are not sufficient evidence to indicate quantum mechanical
effects. For example, the effect can be modeled by classical physics as one of excitonic coup
ling to generate the appearance of coherence beating of the electronic excitation states across
an array of light-harvesting complexes.
KEY POINT 9.5
An exciton is a classical state describing a bound electron and electron hole that are
coupled through the attractive electrostatic Coulomb force that has overall net zero
electrical charge but can be considered as a quasiparticle, usually in insulators and
semiconductors, which has a typical lifetime of around a microsecond.
It is only relatively recently that more promising evidence has emerged for room tempera
ture quantum coherence effects in photosynthesis (O’Reilly and Olaya-Castro, 2014). When
the vibrations of neighboring chlorophyll molecules match the energy difference between
their electronic transitions, then a resonance effect can occur, with a by-product of a very
efficient energy exchange between these electronic and vibrational modes. If the vibrational