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    photocatalysis, and leads to inactivate bacteria, viruses,
    spores, yeasts (5).
    This photocatalysis/biology interface has been pioneered
    by the photoelectrochemical sterilization of microbial cells
    by platinized semiconductors,which opened the door to the
    application of photocatalysis to the life science and enlarged
    its potential applications (6). In contrast to photocatalysis
    applied to chemicals, photocatalysis applied to biological
    targets remainedmainly focused on the treatment of liquids
    and on self-decontaminating surfaces, mainly targeting
    bacteria (especially Escherichia coli bacteria), viruses, fungi,
    algae, and protozoa (7, 8). By contrast, despite the interest
    in terms of public health and a large spectrumof applications,
    the photocatalytic disinfection of contaminated air remained
    scarcely studied, due to the complexity of working with
    bioaerosols, which combines difficulties inherent to micro-
    biology and to aerosol sciences. Works on bioaerosols
    concerned E. coli, Microbacterium sp., Bacillus subtilis,
    Bacillus cereus, Staphylococcus aureus, Aspergillus niger,a
    Candida famata yeast or theMS2 and λ phage viruses (9 13).
    Our previous works were devoted to the UV-A photo-
    catalytic treatment of flowing air contaminated by E. coli
    and L. pneumophila (14, 15). This paper reports on the need
    of photoreactors specifically designed for biological applica-
    tions, since up to now, the chemical approach was themain
    concern.Whentargeting biological agents, themainresearchs
    concerned the increase in the biocidal propertiesmainly by
    metallic promotion of the photocatalyst (5). In contrary to
    works reporting on innovative designs proposed for removing
    chemical pollutants and on the corresponding tools devel-
    oped for their scaling-up, works for reducing the biological
    contamination level by optimizing the reactor geometry
    remained scarce, with few articles focused on the photo-
    catalytic treatment of bioaerosols with reactor design
    (9 11, 14, 15).
    Novel designs of photoreactors should be engineered for
    overcoming restrictive efficiency limitations and formeeting
    the requirements for achieving a commercial implementation
    (16). Paradoxically,many commercial photocatalytic devices
    claimtheir efficiency for inactivating AMOs at high flowrates,
    although a large part of them have only been designed and
    tested for chemical applications, only assuming the risky
    hypothesis that a similar efficiency toward pathogens was
    reached.Results usually obtained raisemany questions about
    the efficiencies of photoreactors for removing AMOs at high
    flowrates, since theywere only assessed at lowlabscale rates.
    However, more than in the case of VOCs for which any
    concentration reduction is valuable, air treatment for reduc-
    ing infections due to AMOs onlymakes sense if the removal
    rate is high (see the dose response function to pathogenic
    exposure fitted using a beta-Poisson law in Supporting
    Information (SI) Figure S1).Commercial devices should thus
    absolutely incorporate only highly efficient reactors. The
    impact of AMOs on the photoactive surface appeared to be
    critical, and the development of efficient photocatalytic
    systems has to focus on that point. Hence, the design of
    photoreactors for decontaminating bioaerosols substantially
    differs from that targeting the treatment of chemical pol-
    lutants and it appeared necessary to specifically develop
    photoreactors devoted to the reduction of the biological
    pollution under realistic conditions, like was done in Grin-
    shpun et al. (12).
    Recently, first-principles computational fluid dynamics
    (CFD) has become a promising tool for the design of
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