Tunable solid-state fluorescent materials are ideal for applications in security printing technologies. A document possesses a high level of security if its encrypted information can be authenticated without being decoded, while also being resistant to counterfeiting. Herein, we describe a heterorotaxane with tunable solid-state fluorescent emissions enabled through reversible manipulation of its aggregation by supramolecular encapsulation. The dynamic nature of this fluorescent material is based on a complex set of equilibria, whose fluorescence output depends non-linearly on the chemical inputs and the composition of the paper. By applying this system in fluorescent security inks, the information encoded in polychromic images can be protected in such a way that it is close to impossible to reverse engineer, as well as being easy to verify. This system constitutes a unique application of responsive complex equilibria in the form of a cryptographic algorithm that protects valuable information printed using tunable solid-state fluorescent materials.
Photoluminescent solid-state materials have been widely applied in dye lasers1, organic light emitting diodes (OLEDs)2,3,4, data recording and storage5,6, and security printing7,8. These materials can be easily applied inexpensively to different surfaces and have been implemented widely as security inks to protect high-value merchandise, government documents and banknotes9. Materials with static luminescent outputs, however, are familiar to counterfeiters. In contrast, stimuli-responsive photoluminescent materials, which change their optical outputs in response to external stimuli, possess extra security features that are difficult to mimic, making them suitable for the next generation of security printing. In recent years, a series of stimuli-responsive photoluminescent materials, including those that are thermochromic10,11,12,13, photochromic14,15,16, mechanochromic17,18,19, solvochromic20,21,22,23 and electrochromic24,25, have been developed. These smart materials respond to external stimuli with reversible changes to their chemical constitutions or superstructures in the solid state, causing them to emit different luminescent colours. Coding these fluorescent colours in one or two dimensions –a practice which is similar to digital coding (for example, barcodes and QR codes) in computer science– has been suggested26 as a potential strategy to prevent tampering or counterfeiting. Current stimuli-responsive photoluminescent materials, however, can only provide a small matrix of colours as optical codes. Developing wide-spectrum tunable photoluminescent solid-state materials with multiple fluorescent emissions (a large matrix) remains a major challenge.
Herein, we report the unexpected discovery, during synthesis by a cooperative capture strategy27,28,29, of a heterorotaxane R4·4Cl, which contains pyrene stoppers and a diazaperopyrenium unit, derived from 1·Cl and 2·2Cl, respectively. Its fluorescent emission in the solid state can be fine-tuned rapidly and reversibly over a wide (∼100 nm) range of wavelengths as a result of stimuli-responsive aggregation and de-aggregation processes that are governed by a network of supramolecular equilibria. The unique features of this heterorotaxane include (i) the widely tunable colour of its fluorescent emission, providing a large analogue matrix of optical outputs, (ii) variations in fluorescent emission colour that occur when the heterorotaxane is deposited on different types of paper and (iii) the non-linear variation in its colour profile in response to simple chemical stimuli. These properties have allowed us to demonstrate a system of chemical encryption, in which the heterorotaxane is employed as a fluorescent security ink and its complex supramolecular equilibria serve as an encryption algorithm. By encrypting graphical information using these inks, printed images are nigh impossible to mimic, counterfeit and reverse engineer, yet can be easily verified on application of an appropriate authentication reagent, without revealing the original information.
Synthesis of hetero[n]rotaxanes
The key compound in our investigations is the heterorotaxane R4·4Cl, which was isolated (Supplementary Figs 1−10) as an unexpected side product during the synthesis (Fig. 1a) of the heterorotaxane R3·4Cl (Supplementary Figs 11−14) from cucurbituril (CB6), γ-cyclodextrin (γ-CD) and two fluorescent precursors, one (1·Cl) derived from pyrene and the other (2·2Cl) from a diazaperopyrenium (DAPP) dication. In common with many fluorophores, DAPP exhibits a high fluorescence quantum yield30,31 in solution (Φ=53%) but not in the solid state (Φ=0%) as a result of aggregation-induced quenching. To ‘turn on’ the fluorescence of DAPP in the solid state, we attempted to de-aggregate32 DAPP by encapsulating 2·2Cl with γ-CD. No complexation, however, between 2·2Cl and γ-CD was observed (Fig. 1b) in aqueous solution (Supplementary Figs 15−17). We anticipated that a more effective strategy would be to fix two bulky CB6 rings at the periphery of the DAPP dye as part of a mechanically interlocked molecule, formed by means of the highly efficient and rapid cooperative capture synthesis27,28,29 in aqueous solution. To our surprise, the reaction not only afforded the anticipated heterorotaxane R3·4Cl (yield=80%), but also another heterorotaxane R4·4Cl (yield=9%). The formation of R4·4Cl, in which γ-CD encircles the DAPP unit, seems to be at odds with the observation that γ-CD does not bind 2·2Cl. The unfavourable energetics of threading γ-CD onto the dumbbell of the heterorotaxane are outweighed by the positive contribution from the hydrogen bonding network formed between γ-CD and the neighbouring CB6, an observation which is supported by molecular mechanics simulations (Supplementary Fig. 43), as well as the release of high-energy water molecules33 from the macrocycles. Increasing the amount of γ-CD to 10 equiv. in the reaction mixture favours the formation of R4·4Cl, which was isolated as the major product in 83% yield in 3 h (Supplementary Table 1). Although both heterorotaxanes dissolve to some extent in water, R3·4Cl, which lacks a solubilizing γ-CD ring, is poorly soluble and undergoes aggregation. In contrast, R4·4Cl exhibits significant water solubility of up to 3 mM at room temperature. 1H NMR spectroscopy reveals that, while R4·4Cl undergoes aggregation (Fig. 1c and Supplementary Figs 18−19) at room temperature, it experiences de-aggregation to its monomeric form (Fig. 1d) on heating to 80 °C. 2D-NOESY and variable temperature NMR experiments indicate (Supplementary Figs 20−21) that the γ-CD ring in R4·4Cl has a fixed orientation and position, and does not shuttle along the dumbbell rapidly on the 1H NMR timescale.
The UV/Vis absorption spectrum (Fig. 2a) of R4·4Cl has two characteristic absorption bands at 341 and 443 nm, which can be attributed to electronic transitions in the pyrenyl and DAPP units, respectively. Despite the presence of the CB6 and γ-CD rings, R4·4Cl forms aggregates (R44+agg) in water, as confirmed (Supplementary Fig. 22) by dynamic light scattering experiments. A blue shift (7 nm) of the absorption band near 450 nm is recorded (Fig. 2b) in the concentration-dependent UV/Vis absorption spectrum of R4·4Cl on dilution from 500 to 25 μM, while the shoulder evident at around 350 nm, arising from the pyrene stopper, diminishes. The isosbestic points observed (Fig. 2b) at 431 and 492 nm suggest34,35 that the aggregation is homogenous and non-cooperative36,37,38. By fitting the data to a dimerisation model39,40, the aggregation constant Kagg was determined (Supplementary Figs 23−25) to be 1.4 × 104 M−1, indicating strong interactions between R4·4Cl monomers.
Irradiating a dilute solution (5 μM) of R4·4Cl at excitation wavelengths of either 340 or 443 nm results in identical fluorescence emission spectra (Supplementary Fig. 26), with an emission maximum (Φ=52.4%, Supplementary Table 2 and Supplementary Figs 27−44) at 510 nm. No emission is observed at 390 nm, indicating (Fig. 2a and Supplementary Fig. S41) the transfer of the excited state energy from pyrene to DAPP by a Förster resonance energy transfer (FRET) mechanism with near-quantitative (>99%) efficiency. This remarkable FRET efficiency can be rationalised by considering the geometric constraints enforced by the rings that impart (i) a close-to-ideal spatial separation (∼1.2 Å, calculated by molecular mechanics, Supplementary Figs 45−47) between the FRET donors (pyrene) and acceptor (DAPP) in R4·4Cl, while (ii) limiting conformational flexibility and (iii) preventing aggregation-induced quenching. These observations suggest that cooperative capture strategies have the potential to control the distances between fluorophores for applications such as bio-sensing41,42.
As R4·4Cl undergoes increased aggregation at higher and higher concentrations, its narrow emission band (Fig. 2c) at 510 nm is gradually replaced by a broad, featureless band around 610 nm, implying that either excimers (DAPP homodimers) or exciplexes (pyrenyl–DAPP heterodimers) are being formed in the excited state. Circular dichroism spectra reveal (Fig. 2d) that the aggregation of R4·4Cl (200 μM) is temperature dependent. As the temperature is lowered from 80 °C (monomeric state) to 2 °C (aggregated state), the positive induced circular dichroism (ICD) signals diminish, as a negative ICD peak43,44,45 attributable to the pyrene stoppers appears at around 350 nm, indicating that these stoppers congregate near the rims of the γ-CD ring. As γ-CD encircles DAPP, it follows that pyrene–DAPP heterodimers (Figs 1c and 2d), and their corresponding exciplexes, are responsible for the observed aggregation and emission behaviour of R4·4Cl.
Dynamic supramolecular equilibria of the heterorotaxane
In aqueous solution, the disassembly (Fig. 3a) of aggregated heterorotaxanes (R44+agg) is promoted by introducing γ-CD, which encircles the pyrene moieties of R4·4Cl and prevents aggregation. The stepwise encapsulation process, which occurs via the formation of a R44+⊂CD intermediate, favours a monomeric R44+⊂CD2 complex in the presence of excess of γ-CD, with an averaged equilibrium constant KCD=(K1·K2)1/2. As a result of the complex equilibria in solution, it is not easy to measure KCD directly. To obtain a good estimate of the binding affinities between the pyrene moieties of R4·4Cl and γ-CD, a reference heterorotaxane SR4·4Cl was synthesised and the averaged binding affinity (0.9 × 104 M−1) between its pyrene moiety and γ-CD was measured (Supplementary Figs 48−55) in D2O. This encapsulation process can be reversed (Fig. 3a) by introducing a competitive binding agent (CBA), which competes for γ-CD in solution with an association constant, KCBA. As the aggregation constant Kagg and the encapsulation constant KCD are of the same order of magnitude, addition of even a weak CBA, for example, 2-adamantylamine hydrochloride (Ad·Cl, KCBA=90 M−1, Supplementary Figs 56−59), will efficiently perturb the equilibria between R44+agg, R44+⊂CD2 and R44+.
The dynamic nature of R44+ in aqueous solution affords us the opportunity to customize an emission profile that remains preserved in the solid state after removal of the solvent. The fluorescent emission spectrum (Fig. 3b and Supplementary Figs 60−64) of the amorphous R44+agg (λmax=610 nm, Φ=7.7%) is very similar to its emission (Fig. 2c) in a concentrated aqueous solution (Supplementary Figs 65−66). On the addition of γ-CD, the solid-state fluorescent emission spectra become gradually blue-shifted to 510 nm (Φ=42.5%), with the emission colour (Fig. 3c) changing from red to green. Solid-state emission is also conserved from solution in the presence of a CBA. For example, the addition of 200 equiv. of Ad·Cl to a mixture comprising R4·4Cl:γ-CD (molar ratio: 1:200) results in a red-shift (Fig. 3b,c) of the emission back to λmax=580 nm. Thus, by changing the ratio of R4·4Cl, γ-CD and Ad·Cl, the solid-state fluorescence of the material can be tuned reversibly over a wide range of colours from green through to red. This stimulus-responsive tuning of fluorescence spectra in the solid state, over such a wide range of colours and under ambient conditions, is unique and holds promise for applications in security printing technology.
Applications as fluorescent inks
By loading R44+-based aqueous solutions (inks) into fountain pens, information can be written (Fig. 4), which is then revealed under UV light. By applying colourless γ-CD and Ad·Cl inks on top of the fluorescent R4·4Cl ink (Fig. 4a), additional information can be added (R44+agg→R44+⊂CD2) or erased (R44+⊂CD2→R44+agg) on pre-existing images that is only noticeable (Supplementary Fig. 67 and Supplementary Movie 1) under UV light. During handwriting experiments, we found that the R44+⊂CD2 ink exhibits an unusual phenomenon, that is, the colour of its emission depends (Fig. 4b) on the type of paper (Supplementary Movie 2). For example, on rag paper, newsprint and banknotes, R4·4Cl appears reddish-orange and R44+⊂CD2 appears green (Fig. 4b) under UV light, which is consistent (Fig. 3c) with the corresponding powders. On different kinds of ordinary white paper (Fig. 4b, Supplementary Figs 68−70 and Supplementary Table 3), however, both of these inks appear reddish-orange. The change of colour is most likely a result of noncovalent bonding interactions with papers of different compositions.
R44+-based inks are also compatible with inkjet printing technology. A monochromic barcode and a QR code printed (Fig. 4c) on paper from an inkjet cartridge contains information that, although invisible under natural light, can be read (Supplementary Figs 71−72 and Supplementary Movie 3) on a smartphone under UV light. The supramolecular encapsulation/competition between R44+, γ-CD and Ad·Cl is established rapidly (milliseconds) before the inks dry during the printing process, making it possible to print polychromic fluorescent images. By loading aqueous solutions of R44+⊂CD2 (R44+:γ-CD=1:50), γ-CD and Ad·Cl into a tri-colour inkjet cartridge (Fig. 4d and Supplementary Fig. 73), we have printed a fluorescent reproduction (Fig. 4e) of van Gogh’s ‘Sunflowers’ with good colour resolution. The colour range of the fluorescent inks can be expanded to accommodate RGB printing (Fig. 4f and Supplementary Figs 74-76) by choosing a fluorescent CBA with blue emission, such as the terminal fragment of R4·4Cl, 1-pyrenemethylamine hydrochloride (PyMe·Cl). It is worth noting that, by reducing the amount of R4·4Cl applied to the paper, the images produced are invisible to the naked eye (Fig. 4f, right) under natural light.
Supramolecular encryption and authentication theory
At a fundamental level, the R44+-based fluorescent inks provide an extensive fluorescent colour matrix for encryption coding. More importantly, the nonlinear dependence of this system’s output on the concentrations of components and their equilibrium constants (Fig. 3a) points towards a general concept whereby complex supramolecular equilibria in aqueous solutions can be used as a chemical encryption method (Fig. 5). In principle, the colour of a dot printed by the customized tri-colour ink cartridge reflects a complex supramolecular equilibrium in the solution state, which can be simplified as
Since Kagg and KCD are fixed, three key parameters control the supramolecular equilibria and the subsequent fluorescent colour (Fig. 5 and Supplementary Fig. 77) under UV light for a given dot after printing: (1) [R44+]0, reflecting the absolute amount of R44+ ink applied on paper, (2) [CD]0 and [CBA]0, reflecting the ratio of R44+agg and R44+⊂CD2 on paper and (3) the chemical composition of CBA, reflecting a different KCBA in the supramolecular equilibrium. These variables constitute the encryption settings, which can be defined by the user in charge of security printing. By simply varying (i) the sequence (Fig. 5) of inks in Channels , , , (ii) the chemical composition of the CBA and (iii) the concentration of the inks, it is possible to generate a large number of fluorescent colour combinations. It is also worth noting that, a combination of different CBAs could be loaded in channels and simultaneously, thus introducing even more variables to the supramolecular equilibria. In this manner, it would be challenging for counterfeiters to reproduce a printed colour palette even if they had access to the R4·4Cl ink, as they would also require a complete knowledge of (i) the CBA, of which there could be a large number of possibilities, as well as (ii) the paper media, (iii) channel assignments and (iv) initial ink concentrations. Even relatively small errors in initial concentrations can lead to obvious differences in the colour palette, by a margin which cannot be easily reverse engineered on account of the non-linearity of the equilibrium equations,
where the fluorescence intensity Iλ at a given wavelength λ is the sum of the emission intensities of each component in an aqueous solution containing R4·4Cl, γ-CD and CBA. F° is the molar fluorescence coefficient at wavelength λ, and m is the molar concentration of CBA being encapsulated by γ-CD. See Supplementary Discussion for detailed derivations.
The dynamic nature of the inks also makes them amenable to a variety of fraud detection mechanisms. In principle, applying a layer of authentication agent(s) can re-establish the supramolecular equilibria in solution and shift the colour outputs (Fig. 5) on paper non-linearly, as described by equations (1) and (2). As the colour-changing process is dynamic and depends on the amount of the authentication agent(s) that has been applied, it is close to impossible that the dynamic colour-changing process could be precisely mimicked. Apart from applying authentication agent(s), which could induce a supramolecular equilibrium shift, mechanisms such as counterion exchange and fluorescence quenching can also be utilized (Fig. 5 inset) to change emission colours in real time.
Demonstration of the supramolecular encryption theory
In an attempt to demonstrate the non-linear nature of this system, we have printed fluorescent colour palettes (Fig. 6a−f) using various ink concentrations and different CBAs. A broad range of colours from green to red can be printed (Fig. 6b) when Ad·Cl is used as the competitor. The colour palette is sensitive to the association strength of the competitor as predicted and evidenced by the differences between images printed from equally concentrated solutions of Ad·Cl (Fig. 6b) and a stronger-binding competitor (Fig. 6c), namely, 1-adamantanemethylamine hydrochloride (AdMe·Cl, KAdMe=127 M−1, Supplementary Figs 58−59). Reducing the concentrations of either CBA (Fig. 6c,d) or γ-CD (Fig. 6c,e) redistributes the colour spectrum in the yellowish-red region or greenish yellow region, respectively. The colour spectrum is expanded (Fig. 6f) by choosing a blue fluorescent CBA, for example, PyMe·Cl. The ability to exchange fluorescent and non-fluorescent CBAs in a modular and user-controlled manner elevates the anti-counterfeiting features possessed intrinsically by this new security ink.
Demonstration of authentication methods
Authentication mechanisms have also been demonstrated. For example, exposure of an encrypted image (Fig. 6g, centre) to aqueous solutions of non-fluorescent AdMe·Cl or γ-CD changes the existing colour gradient of the image, while printing fluorescent PyMe·Cl aqueous solution creates new colours, such as blue and purple by shifting the complex equilibria. Printing 1,3,6,8-pyrenetetrasulfonic acid tetrasodium (PTSA·4Na) solution gives rise to new colours (Fig. 6g) as a result of counterion exchange. A characteristic colour change can also be brought about through the application of a quencher, such as tryptophan, or even by simply soaking the printed image in water for as little as 1−2 min, during which time γ-CD and the CBA are washed away to some extent, thus shifting the equilibria. These authentication agents can discriminate, not only between images produced by the R44+-based ink and other fluorescent dyes, but also between images produced using different R44+/CBA/γ-CD ink formulations. In a blind test, blocks of a given fluorescence colour (Fig. 6h, top), which appear almost identical to one another under UV light, but are formulated differently, were found to result in noticeably different colours (Fig. 6h bottom) after the application of the same amount of authentication agents. For further details, see Supplementary Fig. 78. As hundreds of chemicals meet the criteria to be CBAs, an extremely large library of different ink systems and authentication tests using this supramolecular encryption method can, in principle, be generated.
In summary, we have developed a stimulus-responsive solid-state fluorescent heterorotaxane, which is easily prepared from simple starting materials in high yield by a cooperative capture method. We have applied it as a component of fluorescent security inks with built-in supramolecular encryption. The inks are well-placed for assimilation into a commercial setting on account of the simple and high-yielding synthesis of the heterorotaxane from commodity chemicals. The solid-state emission of these security inks can be fine-tuned over a wide emission range (∼100 nm) with rapid response (milliseconds) to chemical stimuli. Printed information is encrypted in a chemical language based on a nonlinear equation that describes the dynamic equilibrium network. A potentially enormous library of different fluorescent colour combinations can be generated. In contrast with conventional dyes, the encrypted information printed using the heterorotaxane inks can be verified by chemical authentication methods without revealing the original colour image information. The interplay of fluorescence output with dynamic supramolecular equilibria that we observed quite fortuitously could be a general phenomenon that is not exclusive to the heterorotaxane, or even to mechanically interlocked molecules. It opens up a new way to encrypt and protect information in a manner that is far from easy to mimic.
Synthesis and characterization of the heterorotaxane R4·4Cl
Stopper precursor 1·Cl (67 mg, 0.22 mmol), dumbbell precursor 2·2Cl (54 mg, 0.10 mmol) and γ-CD (1287, mg, 1.00 mmol) were mixed in H2O (35 ml) and stirred at 60 °C for 10 min before CB6 (250 mg, 0.25 mmol) was added. The reaction mixture was stirred at 60 °C for 3 h. Insoluble residues were filtered off from the reaction mixture. The filtrate was loaded directly onto a reverse phase C18 column (150 gram, RediSep Rf Gold C18Aq) on an automatic column chromatographic system (Combiflash Rf200, Teledyne Isco) and chromatographed in H2O/MeCN/0.1% TFA with a gradient from 0 to 60% MeCN over 40 min at a flow rate of 85 ml min−1. Fractions containing R44+ were collected and the counterions of R44+ were exchanged to PF6− on addition of an excess of aqueous NH4PF6. The product R4·4PF6, which precipitates on removal of MeCN from these fractions under reduced pressure, was collected by vacuum filtration and washed extensively with H2O. The heterorotaxane R4·4Cl was obtained after a second counterion exchange by precipitation from an MeCN solution of R4·4PF6 with an excess of tetrabutylammonium chloride. The yellow precipitate was collected by vacuum filtration, washed with excess MeCN and dried under vacuum to afford R4·4Cl (371 mg, 83%) as an orange powder. 1H NMR (600 MHz, D2O, 353 K): δ=10.92 (s, 2H), 10.63 (s, 2H), 9.73 (d, J=9.5 Hz, 2H), 9.68 (d, J=9.4 Hz, 2H), 9.11 (d, J=9.3 Hz, 2H), 9.05 (d, J=9.3 Hz, 2H), 8.81 (dd, J=12.4, 9.3 Hz, 2H), 8.50 (dd, J=11.5, 7.9 Hz, 2H), 8.40–8.22 (m, 8H), 8.18 (d, J=8.9 Hz, 4H), 8.08–7.98 (m, 2H), 6.67 (s, 1H), 6.63 (s, 1H), 5.96 (t, J=8.8 Hz, 2H), 5.86 (d, J=15.3 Hz, 6H), 5.80 (m, 2H), 5.76 (d, J=15.5 Hz, 6H), 5.62 (d, J=15.5, 6H), 5.60 (d, J=15.5, 6H), 5.40 (s, 12H), 5.39 (s, 12H), 5.26 (s, 4H), 4.86 (d, J=3.8 Hz, 8H), 4.66 (s, 4H), 4.53 (t, J=9.0 Hz, 2H), 4.29 (t, J=8.9 Hz, 2H), 4.10 (m, 24H), 3.65 (t, J=9.5 Hz, 8H), 3.50 (dd, J=10.0, 3.8 Hz, 8H), 3.41–3.20 (m, 32H). HR-ESI-MS: calcd for [M − 4Cl]4+ m/z=1,074.8630, found m/z=1,074.8623; [M − H − 4Cl]3+ m/z=1,432.8149, found m/z=1,432.8123; [M − 3Cl]3+ m/z=1,445.1406, found m/z=1,445.1369.
Detailed synthesis and characterisation of stopper and rod precursors, rotaxanes R3·4Cl and SR4·4Cl are available in Supplementary Methods.
Photophysical studies of the heterorotaxane R4·4Cl
The UV/Vis spectra of the sample solutions were measured on a Shimadzu UV/Vis/NIR spectrometer (UV 3600 model) with a cell temperature controller. Quartz cuvettes with 1 or 10 mm pathway were used to record the UV/Vis spectra. The fluorescence excitation and emission spectra of the sample solutions were recorded on a HORIBA fluorometer (fluoroMax-4 model). Circular dichroism spectra were recorded on a JASCO circular dichroism spectrophotometer (J-815 model) with a temperature controller. Solid-state UV/Vis spectra were recorded on a Perkin Elmer UV/Vis/NIR spectrometer (LAMBDA 1050 model) equipped with an integrating sphere. Solid-state fluorescence spectra were recorded on an ISS fluorometer (PC1 model) equipped with a variable-angle, front surface sample compartment.
Ink writing tests
Four types of inks for pen writing were prepared using R4·4Cl (0.5 mM), Ad·Cl (100 mM), γ-CD (100 mM) and R4⊂CD2 (R4·4Cl=0.5 mM, γ-CD=100 mM) solutions, respectively. Typically, 0.5 ml of the ink was loaded in a fountain pen for writing tests. A wide selection of paper-based printing media has been tested, including copy papers (various brands and models), matte presentation paper (HP), glossy presentation paper (HP), resume paper (25 and 100% cotton), newsprint paper, rag paper (100% cotton, without optical brightener) and cigarette rolling paper. Banknote identification tests were performed on genuine banknotes of US dollars, British pounds sterling, Euros, Chinese Yuan and Japanese Yen. In these tests, the corresponding currency symbols ($, £, € and ¥) were drawn on the testing banknotes using the fountain pen filled with R4⊂CD2 ink.
Ink printing tests
Printing tests were performed on an HP inkjet printer (Photosmart CP4780 model) and an HP colour laser printer (CP1025nw model) with customized ink cartridges and original toners, respectively. Rag paper (100% cotton, without optical brightener, no surface coating side) was chosen for most printing tests based on the ink writing test results.
Ink cartridges for printing tests were customized from HP black and tri-colour cartridges (HP60 model). The filled inks were removed from the cartridge, which was washed extensively with H2O and EtOH. Aqueous solutions of R4·4Cl (4 mL, 0.5 mM) and R4⊂CD2 (4 ml, R4·4Cl=0.5 mM, γ-CD=100 mM) were loaded in two empty, clean black ink cartridges, respectively, to perform the monochromic printing tests. In the polychromic printing tests, aqueous solutions of Ad·Cl (2 ml, 100 mM), R4/γ-CD (2 ml, R4·4Cl=0.5 mM, γ-CD=25 mM) and γ-CD (2 ml, 100 mM) were loaded in the magenta, yellow and cyan channels of the cleaned tri-colour ink cartridge, respectively. Fluorescent colour under UV light was tuned by controlling the proportion of the three inks in the customized tri-colour ink cartridge.
How to cite this article: Hou, X. et al. Tunable solid-state fluorescent materials for supramolecular encryption. Nat. Commun. 6:6884 doi: 10.1038/ncomms7884 (2015).
The authors dedicate this manuscript to Professor Yoshihisa Inoue on the occasion of his retirement. We thank Professor Yoshihisa Inoue from Osaka University and Professor Frank Würthner from Universität Würzburg for their useful suggestions. We acknowledge financial support from Northwestern University (NU). X.H. gratefully acknowledges support from the Ryan Fellowship and the Northwestern University International Institute of Nanotechnology.
Fluorescence colour changing and recovery of "NU" written with R44+⊂CD2 ink demonstrated by applying an aqueous solution of Ad·Cl and γ-CD consecutively. An inexpensive UV-LED light is used as the light source in the movie.
Fluorescence colour changing of the R44+⊂CD2 ink applied on different types of paper. An inexpensive UV-LED light is used as the light source in the movie.
Fluorescent UV barcode and QR code produced using the R44+⊂CD2 ink, which could be recognised by a smart phone camera only under UV light.