S.
Castellanos
,
F.
Kapteijn
and
J.
Gascon
*
Catalysis Engineering, Chemical Engineering Department, Delft University of Technology, Julianalaan 136, 2628 BL Delft, The Netherlands. E-mail: j.gascon@tudelft.nl
First published on 1st February 2016
The ability of modulating the properties of metal–organic frameworks (MOF) on demand by external light-stimuli is a most appealing pathway to enhance their performance in storage and separation and to render novel advanced applications. Photoswitchable linkers of different nature have been inserted in several MOF structures either as integral parts of their scaffolds or as guests in the pores. In this highlight we analyse the different strategies and expose some aspects that should be considered in the design of new generations of photoswitchable MOFs.
For instance, if the sorption capacity of the MOF can be increased and decreased at will through reversible changes in its structure by simple illumination (Fig. 1 top), the storage and release cycle would require less expensive procedures than traditional high temperature and low pressure conditions. Having two interconvertible pore configurations is also appealing for catalysis,6 for example, by gating the selective entrance of one or another reagent with light stimuli, block-copolymerization could be fully controlled (Fig. 1 center). Moreover, by promoting the desorption of the formed products due to changes inside the pore (polarity, geometry, etc.), one could mimic the natural activity of enzymes.
In addition to host/guest interactions, there are other features arising from MOFs periodicity7 whose modulation by light can find applications in different technological fields. The capability of switching a material from an ON state to an OFF state, e.g. from a fluorescent to a not fluorescent state or from a conductive to a not conductive state, can be exploited for binary coding.8–10 It is known that photochromic small molecules do not perform efficiently in the solid state due to their motion restriction in the dense crystalline packing stabilized by intramolecular interactions.11,12 If photochromic units are embodied in the frameworks, their separated arrangement or their confinement in the pores can enhance their light-triggered response.
This highlight describes the strategies that have successfully provided MOFs with photoswitchable properties, that is, with the possibility of modifying in a reversible way the framework's features by means of external light stimuli. Despite the topic has been briefly addressed as part of previous reviews,2–5 here we make a global evaluation of each design considering the nature of the photoactive component and how it is integrated in the MOF. Further, some considerations about key issues for the optimization of this kind of photoresponsive materials are exposed, aiming at their future implementation in practical uses.
Scheme 1 Prototypical structures of photoswitchable molecular compounds: top, azobenzene (AB); center, dithienylethene (DTE); bottom, spiropyrane/merocyanine (SP/MC). |
Coming back to the porous hybrid composition of MOFs mentioned above, one can think of incorporating photoswitchable units into MOFs as guests in the voids (extrinsically) or as linkers integrated as building blocks in the framework (intrinsically). Within this last approach, linkers that undergo changes along their backbone and thus alter the connection between the metal-based secondary building units (SBUs) will work fundamentally different from linkers that are provided with a photoresponsive side-group oriented towards the pore. The strategies that have proven successful in the literature are summarized in Table 1 and discussed in the following sections.
Intrinsic photoresponse approach | ||||
---|---|---|---|---|
Design | MOF | Unit | Modulated properties | Ref. |
Back-bone | Zn2(R-TC)(L-N,N′) | DTE | Fluorescence | 13 |
Zn2(R-DC)2(L-N,N′) | DTE | CO2 sorption | 14 | |
Zn2(R1-DC)2(R2-N,N′) | AB | CO2 sorption | 15 | |
Isoret. UiO-66 (Zr) | AB | Inactive | 16 | |
Side group | Isoret. ZIF-8 | AB | Light absorption | 17 |
MOF-74 (Mg) | AB | Cargo release | 18 | |
MIL-53 (Al), UiO-66 (Zr) | AB | CO2 sorption vis. absorption | 19 | |
Cu2(L-DC)2(R-N,N′) | AB | Butandiol sorption | 20 | |
Isoret. MIL-101 (Cr) | AB | Inactive | 21 | |
Isoret. MIL-101 (Cr) | AB | Vis. absorption CH4 sorption | 22 | |
Zn2(R-DC)2(L-N,N′) | AB | Vis. absorption | 23 | |
M2(R-DC)2(L-N,N′) (M = Co, Cu, Zn) | AB | Vis. absorption | 24 | |
Isoret. MOF-5 | AB | CO2 sorption | 25 | |
UBMOF-1 (Zn) | DTE | Vis. absorption | 26 | |
UBMOF-2 (Zn) | DTE | Vis. absorption | 27 | |
Cu2(R-DC)2(L-N,N′) and Cu2(L-DC)2(R-N,N′) | AB | Vis. absorption, butandiol sorption | 28 | |
Cu2(R-DC)2(L-N,N′) | AB | IR spectrum | 29 |
Shustova et al. used DTEs featuring two terminal pyridines to pillar 2D frameworks based on Zn-porphyrin linkers and dimeric Zn-SBUs. While DTEs linkers are in the open form, the Zn-porphyrin linkers display fluorescence. In contrast, when the ring closure of the DTEs is induced by UV irradiation, non-radiative energy transfer to the closed DTEs occurs and fluorescent emission is quenched (Fig. 2).13
Fig. 2 Energy transfer to the DTE-based linker in it closed form quenches fluorescence of the porphirine-based linker. In this way, the MOF can be switched from an fluorescent to a non-fluorescent version by means of light. Reprinted with permission from ref. 13. Copyright 2014 American Chemical Society. |
The same kind of pyridine terminated DTEs were employed by Guo and coworkers.14 In this case the interpenetrated Zn-MOF exhibited reversible photochromism and could be switched between yellow to dark blue by UV exposure, and back to yellow through visible light irradiation. Importantly, the structural changes promoted by the light-induced ring-closure of DTE linkers resulted in a 4-fold enhancement of CO2 sorption capacity. In addition, CO2 uptake experiments showed that optimal gas uptake and release could be attained by adsorbing under UV irradiation and desorbing under 600 nm light. Another dual linker Zn-MOF prepared from dicarboxylic azobenzenes was also reported by Lyndon et al. to modulate CO2 sorption under dynamic conditions, but in this case CO2 desorption was more efficient under UV light exposure, instead.15
Judging from the number of publications, functionalizing the linkers with the photoswitchable functionality as a side-group, seems a more reliable approach. Furthermore, such design is accessible also via post-functionalization of the MOFs.21,22 This synthetic pathway already provides the desired framework and, at the same time, guarantees that the network will take only as many side groups as it can accommodate in its voids. Regardless of the synthesis method, light-induced configurational changes by azobenzene side-groups is so far the most efficient strategy to modulate the storage properties of MOFs, from small gas molecules like CO2 or CH4,19,23,25 to bigger ones, like butandiol20,28 or propidium iodide fluorescent dye.18 The reason is that not only the geometrical alterations upon trans/cis isomerization are fairly large but also the alterations in polarity can have a strong influence in the sorption capacities. As a matter of fact, Heinke et al. observed that trans to cis isomerization decreased butandiol permeability in AB-based SURMOFs.20 Intriguingly, the trend in the sorption modulation is not constant, i.e. the cis configuration in some cases increases the sorbant uptake capacity20,22,28 and in some others produces the opposite effect.25 In addition, isomerization of the AB side-groups can also be used to generate a dynamic situation to expel the guest in the pore under continuous irradiation of the MOF.18
The combination of photoactive side-group and crystalline lattice is vital to attain light-induced response. This involves not only assuring that the most thermodynamically stable form of the photoactive unit that protrudes from the linker fits in the pores but also that its light-triggered isomerization mechanism can occur and that the resulting isomeric form can be accommodated within the resulting lattice. Such questions have been addressed by Wang et al., who observed that small differences in the framework dimensions have shown to suppress the photoresponse of Cu-containing surface-attached metal–organic frameworks (SURMOF) due to the lack of a free trajectory for the photoisomerization mechanism of the azobenzene pending groups (Fig. 3).28 Further, depending on the length of these linkers, interpenetration may occur during synthesis, which normally results in lower accessible volume and smaller pore sizes than expected for the primary network.23,24
Fig. 3 Changes in the pore dimensions of SURMOFs arising from the different linkers lengths enable or disable the photoisomerization of azobenzene side-groups. Ref. 28 – Published by the PCCP Owner Societies. |
Steric hindrance is thus usually undesired but can though be used as a way to provide MOFs with gas uptake modulation by means of light. Castellanos and coworkers reported a MIL-53-like structure synthesized with terephthalic acids provided with fluorinated azobenzene side-group (Fig. 4).19 In this structure, the crowded packing of the side-groups in the pores was claimed to prevent isomerization. As a consequence, upon light absorption the only relaxation pathway for the linkers was via non-radiative vibrational processes, which increased the surface energy of the crystalline lattice, thus resulting in the decrease of CO2 sorption capacity.
Fig. 4 Terephthalic linkers featuring fluorinated azobenzene side-groups yielded a photochromic MOF isoreticular to UiO-66 (Zr) that switches E to Z upon green light irradiation and Z to E upon blue light exposure (a, b) and a MOF with similar to MIL-53 (Al) with sterically crowded channels (c, d). The impossibility to isomerize in the last case gave place to a photothermal effect that decreased CO2 sorption under visible light. Reprinted from ref. 19 with permission from John Wiley and Sons. |
Alternative to ABs, DTEs as side groups of the linkers have also been implemented in MOFs to yield photochromic properties, that is, the framework rendered a drastic change of color upon UV irradiation. However, the system could not revert to its original configuration by visible light exposure, contrarily to the typical DTE behavior, thus indicating that the closed form of the DTE was too stabilized in the crystalline lattice.26 Such lack of reversibility was overcome replacing the terminal methyl groups in the thiophene heterocycles with phenyl groups. This “minor” modification in the linker structure enabled the isoreticular MOF with back thermal ring-opening, yet with low fatigue resistance.27
When the same hosting MOF built from terephthalate and triethyldiamine bifunctional linkers was used to embed DTEs, the guests aligned in the [001] direction. Upon UV irradiation and thus promotion of ring-closure of the DTEs, this directional preference led to a linear dichroism in the visible light absorption of the MOF, that is, absorption of polarized visible light was stronger in certain directions of the crystal.31
Hermann and coworkers studied the influence of the size and shape of the pore on the photoresponse degree by means of IR spectroscopy. Again, this study pointed out how the spatial restrictions of the MOF cavities are vital for the isomerization efficiency. Whereas AB hosted in MIL-69 (In or Ga) can isomerize in the pores, in MIL-53 (Al) the dense packing of ABs in the voids hindered its light-driven configurational changes.30
To the best of our knowledge, the only photoswitchable MOF system involving SP/MC couple in the literature have been prepared by encapsulating the SP molecule during the crystallization of an In-based MOF with cubic zeolitic MTN topology, named JUC-120 and analogous to MIL-100 (Al, Fe or Cr).33 Noteworthy, inside the pores the MC form is better stabilized and it only transforms into its SP counterpart upon UV irradiation. This behavior is opposite to the one usually observed for this kind of photochromic molecules and is known as reverse photochromism.
To begin with, other chromophores will take their share of light, which will decrease the photon flux arriving to the photoresponsive unit. Most importantly, the covalent attachment of the photoswitching molecule to the metals can give place to new excited states that may not relax toward the targeted configurational change. For instance, ligand-to-metal charge transfer can be promoted instead of a more linker-centered excited state. Even in the case of reaching the desired excited state, other relaxation pathways might compete with the isomerization mechanism, such as energy transfer or electron transfer. Computational studies can be a great tool to inspect the topology and energy of the crystalline molecular orbitals in order to comprehend the origin of their properties,39–41 as well as mechanistic aspects concerning the photoisomerization the building units28,42,43 and thus assist in the design of photoswitchable MOFs.
The competing light-triggered processes can be overcome by selectively irradiating the photoresponsive units, which requires that the light absorption spectrum of the photoresponsive building blocks does not overlap the bands associated with other optical transitions. As a matter of fact, photoswitchable MOFs that require UV light to be active usually exhibit low fatigue resistance.17,22,27 That is what makes MOFs displaying forth and back photoisomerization in the visible light regime remarkable.19 Of particular interest are materials that could undergo structural changes upon very low energetic light irradiation, such as near infrared, since this property would be most relevant for drug release biomedical applications.44
In addition to molecular design, crystal engineering can be an essential tool to improve the efficiency in the incident photons' usage. Light penetration could be in principle enhanced by increasing the surface to volume ratio of the MOF's particles, for instance by growing the crystalline frameworks as thin films, such us in SURMOFs. The epitaxial growth of the later further allows to implement the photoisomerizable struts only at the surface of the film. Such approach was nicely employed by Heinke and coworkers,20 who prepared SURMOFs with a basement layer of biphenyl dicarboxylic linkers and a roof layer of analogous AB-containing linkers. Indeed, this work proved that is not necessary to provide the whole bulk of the MOF with photoswitchable units to attain light-mediated sorption modulation. This result could thus be extrapolated to core–shell structures45 in the future.
The integration of SP in MOFs has also proven challenging. As reported for fully organic nanoporous materials,46 the switching between the SP neutral form and the charged MC form can allow for the modulation of several tasks. However, precisely this zwitterionic isomer might interact strongly with the metallic ions, and together with the relatively large molecular size of both SP and MC the number of suitable frameworks that could accept them is quite reduced. As a consequence, up to date only a zeolitic-like MOF hosting MC and exhibiting reverse photochromism has been reported,33 and SP/MC-based MOFs still remain unexplored.
Despite some impressive modulation, the efficiency of light utilization could be improved by inducing the response with selective irradiation of the photoswitchable units. The use of visible light or even less energetic radiation is a most appealing target. Furthermore, the effects of other photochromic compounds involving greater polarity changes, such as spiropyrans, must still be pursued, since it is predicted that many properties in the MOF could be drastically modified when going from the neutral species to the charge merocyanine species. Last but not least, MOFs' crystalline nature and synthetic versatility should be exploited via smart crystal engineering47 that can lead to an optimized utilization of light.
This journal is © The Royal Society of Chemistry 2016 |