Pineapple Peel-Derived Carbon Dots: Applications as Sensor, Molecular Keypad Lock, and Memory Device.

Herein, the fluorescent carbon dots (CDs) with blue emission were prepared by hydrothermal treatment using pineapple peel as a source of carbon. The as-prepared CDs exhibited turn-Off fluorescence behavior toward Hg2+ and subsequent turn-On behavior for l-cysteine along with enhanced biocompatibility and negligible cytotoxicity for cell imaging. The practical applicability of carbon dots was used for the quantification of Hg2+ in water. On the basis of the spectral characteristic changes, we have designed individual elementary logic operations such as NOT and IMP gates, by utilizing CD as probe and Hg2+ and l-Cys as chemical inputs. We have also demonstrated the utility of this system in electronic security devices and as memory element, with the idea of the switching.

Introduction

Carbon dots (CDs), a new member of fluorescent nanosized carbon materials, with sizes of less than 10 nm, have received increased attention of many researchers because of their superior resistance to photobleaching, increased chemical- and photostability, least toxicity, low cost, and abundant availability as raw materials in nature.[1] The recent developments of CDs were due to their promising applications in biological imaging,[2] sensor materials,[3] drug carriers,[4] photocatalysts,[5] and photothermal therapy.[6] Much efforts have been focused on the facile synthesis of CDs by electrochemical method, thermal method, hydrothermal method, acidic oxidation, microwave, ultrasonic treatment, and laser ablation.[7] More recently, hydrothermal treatment was used because of low cost and nontoxic routes for producing novel carbon materials; it involves dehydration followed by in situ surface passivation.

CDs obtained from different natural resources have been reported from small molecules to wastes, vegetables, and fruits.[8−11] Mostly, carbon dots have least solubility in water and this has limited their analytical applications.[12] Pineapple peel is widely produced during the processing of pineapple to get juices and salads.[13] The main contents of the pineapple peel are cellulose, hemicellulose, lignin, and pectin, in which cellulose occupies 20–25% of the dry weight.[14] Hg2+ is the most dangerous inorganic pollutant and causes environmental and health concerns.[15] Mercury exposure may lead to digestive, renal, and neurological diseases.[16] Due to these adverse effects of Hg2+ ions, there is an urgent need to develop a convenient and rapid method to detect Hg2+.[17] Herein, in this study, pineapple peel was chosen as a precursor to prepare CDs. The CDs were successfully applied as a fluorescence probe for cell imaging and sensitive detection of Hg2+ in living cells, and also applications as a molecular keypad lock and memory device have been reported.

Results and Discussions

The CDs were prepared by simple hydrothermal treatment of pineapple peel as precursor. The main constituents of pineapple peel were cellulose (40–46%), hemicellulose (16–20%), lignin (12–16%), and pectin (8–12%).[18] The resultant CDs exhibited excellent water solubility and a blue color under a UV lamp (365 nm), illustrating that the carbon dots are showing strong blue fluorescence. The quantum yield of the CDs (quinine sulfate in 0.1 mol L–1 H2SO4, excited at 340 nm) was about 42% (Figure S1, Supporting Information), which is much higher than that in previous reports.[9d,10a−10c]

The dimension and morphology of the CDs observed under high-resolution transmission electron microscopy (HRTEM), as shown in Figure A, clearly demonstrate unvarying and monodisperse nature of the CDs. HRTEM image (Figure B inset) shows lattice fringes with an interplanar spacing of 0.20 nm, which is close to the (102) facet of graphite.[10a] The particle size distribution (Figure C) of CDs displays the size distribution as mainly between 2 and 3 nm. Raman spectra of CDs (Figure D) showed the bands at 1374 and 1589 cm–1 for the structure of polyaromatic sp2-hybrid carbon network in two-dimensional hexagonal lattice of a graphite cluster.[19]

Figure 1

(A, B) HRTEM images (inset lattice fringe); (C) particle size distribution from HRTEM; (D) Raman spectra of CDs.

The X-ray diffraction (XRD) pattern of as-prepared CDs in Figure A revealed a broad diffraction peak centered at 2θ = 24.7°, which is attributed to crystalline graphite (sp2 hybridization). Generally, Fourier transform infrared (FT-IR) spectrum is used to identify the surface functional groups of CDs. The CDs exhibited a broad peak at ∼3315 cm–1, which is characteristic of the stretching vibrations of −OH. The peaks centered at 1634 and 1040 cm–1 were ascribed to the stretching vibration of C=C and C–O–C respectively, indicating the presence of sp2 (Figure B).

Figure 2

(A) XRD pattern; (B) FT-IR spectra of CDs.

To get an insight into the elemental composition and chemical bonds of the prepared carbon dots, X-ray photoelectron spectroscopy (XPS) measurements are carried out. The high-resolution XPS spectra for C 1s are divided into three unit moieties, with the binding energy being 284.1, 285.7, and 288.3 eV (Figure A). They are assigned as C=C/C–C, C–OH/C–O–C, and O–C=O, respectively.[9] Similarly deconvoluted O 1s (Figure B) peaks centered at 530.6 and 532.1 correspond to the C=O and C–OH groups, respectively.[21] The presence of these C=O and C–OH groups suggests that these hydrophilic moieties facilitate CDs to disperse in aqueous solution. The photophysical properties of the CDs were investigated by UV–vis and fluorescence spectroscopy. The characteristic absorption peak at 280 nm is assigned to the π–π* transition of C=C, as observed from the CDs prepared by the carbonization of carbon-based materials.[8d,10a] As illustrated in the insets of Figure A, the solution color of CDs is yellow under visible light (left), whereas a blue emission is observed upon exciting with UV light of 365 nm (right).

Figure 3

High-resolution XPS spectra of (A) C 1s and (B) O 1s.

Figure 4

(A) UV–vis absorption, photoluminescence (PL) excitation, and emission spectra and (inset) images of the CDs under room light (left) and UV light (right) in an aqueous solution. (B) Excitation-dependent PL spectra of the CDs in an aqueous solution.

Figure B demonstrates the optical properties of CDs, i.e., excitation-dependent PL behavior. Upon changing the excitation wavelength, the peak is red-shifted and the peak intensity decreases due to different surface sites and particle size. The fluorescence intensities remain constant at high salt concentrations (up to 1000 mM), showing high stability of the CDs even under high ionic strength conditions and also showing maximum intensity at physiological pH (Figures S2 and S3, Supporting Information). This might be due to the protonation and deprotonation of the surface oxygeneous groups in acidic and basic environment, which agrees with earlier reports.[19,20] To determine whether these might affect measurement of CDs, interference experiments were conducted on common metal ions in the presence of the CDs (0.1 mg mL–1, Figure S4, Supporting Information). The fluorescence response of CDs was examined under identical conditions by treatment of 0.1 mg mL–1 CD solution with 50 μM Ag+, Al3+, Co2+, Cd2+, Cr3+, Cu2+, Ca2+, Fe2+, Fe3+ Pb2+, Mn2+, Mg2+, Ni2+, Zn2+, and Hg2+ ions. Figure A shows a gradual decrease in fluorescence intensity with increasing concentration of Hg2+.

Figure 5

(A) Titrimetric quenching pattern of the fluorescence intensity of CD (1 mg mL–1) in phosphate-buffered saline solution (pH 7.4) after addition of Hg2+ ion; (B) Stern–Volmer fitting.

We checked the interference of other metal ions by competitive binding, such as Ag+, Al3+, Co2+, Cd2+, Cr3+, Cu2+, Ca2+, Fe2+, Fe3+, Pb2+, Mn2+, Mg2+, Ni2+, and Zn2+, toward Hg2+ sensing by CDs; it is found that there is no interference for Hg2+ sensing. The fluorescence quenching of CDs upon addition of Hg2+ ions may be attributed to the excited-state electron-transfer reaction of the CDs to the Hg2+ ion.[21] As shown in Figure B, the Stern–Volmer plot shows linearity in the concentration range of 0.1–100 μM, yielding a KSV of 2.2 × 104 M–1. The detection limit is estimated to be 4.5 nM. The reversibility of the CD–Hg2+ complex been investigated by adding amino acids.

The emission spectra of CD–Hg2+ complex with various amino acids, such as alanine (Ala), lysine (Lys), aspartic acid (Asp), arginine (Arg), methionine (Met), proline (Pro), threonine (Thr), tryptophan (Trp), histidine (His), valine (Val), phenylalanine (Phe), serine (Ser), and l-cysteine (Cys), were recorded (Figure S5, Supporting Information).[10e] The results clearly indicate that other amino acids except cysteine do not show any fluorescence changes, i.e., the intensity of fluorescence remained constant. However, addition of l-Cys resulted in the enhancement of emission intensity. The limit of detection of CDs/Hg2+ ensembles with l-Cys was calculated to be 8.7 × 10–7 M on 3σ/s. However, a decrease in the excited-state lifetime after the Hg2+ complex formation confirms that the quenching process is dynamic in nature. Figure shows the excited-state lifetime in the absence and presence of Hg2+ ions.

Figure 6

Lifetime data of only CDs and with Hg2+ (λex = 320 nm; λem = 435 nm).

The lifetime quenches from 2.95 ns (τ1 = 2.38, τ2 = 0.57) to 2.51 ns (τ1 = 2.22, τ2 = 0.29) upon addition of Hg2+. The significant reduction in the lifetime value indicates that the quenching process is dynamic in nature and takes place via an excited-state electron-transfer reaction.[19a]

The Stern–Volmer constant (KSV of 2.2 × 104 M–1) suggests the dynamic quenching of fluorescence on the addition of Hg2+ to CDs; this dynamic quenching by ultrafast electron transfer from Hg2+ to CDs is further confirmed by fluorescence lifetime measurements. Hence, the Hg2+-induced quenching of CDs is due to electron transfer from Hg2+ to CDs. The sensing properties of CDs toward Hg2+ are reproducible; we carried out the addition of ethylenediaminetetraacetic acid to CD–Hg2+ system to check their reproducibility; it is noticed that even after five cycles, the CDs are able to sense Hg2+, indicating that the CD sensing performance is reproducible. We studied the temperature dependency to the fluorescence of CDs with varying temperature; it is observed that increase in temperature leads to decrease in fluorescence intensity.

The exciting photophysical properties, such as high sensitivity, selectivity, and fast response, of CDs with Hg2+ prompted us to investigate their potential use in real-time monitoring of Hg2+ ions in living cells via fluorescence imaging. It is well known that apart from being toxic, Hg2+ ion has a tendency to bind with estrogen receptors in breast cancer cells, causing amplified cell growth and estrogenic effects, such as irregular menstruation, reproductive tract, the urinary tract disorders, and formation of abnormal secondary sexual characteristics like armpit hair and neural disorders. Hence, the recognition of the mercury ions in these cells is a challenge.

To demonstrate the possible cellular toxicity of CDs toward HeLa and MCF-7 cells, the 3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium bromide assay was carried out. The cell viabilities were calculated upon exposure of different concentrations to the carbon dots (Figure S6 Supporting Information), which revealed that the CDs exhibited extremely low cytotoxicity, i.e., viability of about 92% at a concentration of 0.5 mg mL–1 after 24 h incubation, and viability over 84% even high concentration (1 mg mL–1).

HeLa cells incubated with carbon dots and imaged through the fluorescence microscope show distinct fluorescence inside the cells, confirming the cellular uptake of CDs (Figure ). The cells treated with CDs were incubated with Hg2+ ions for 10 min. The results showed that Hg2+ reduces the intensity of the fluorescence of CDs in biological systems, also thereby making CDs as efficient probe for intracellular Hg2+ detection. The bright-field image of cells treated with carbon dots and Hg2+ inveterate that the cells were viable throughout the experimental conditions. This observation established that the CDs could act as a potential candidate for the intracellular detection of Hg2+.

Figure 7

Fluorescence microscopic imaging of HeLa cells: (A–D) 0.50 mg mL–1 CDs at 37 °C for a 3 h excitation by 408 nm (B), 488 nm, (C) and 561 nm (D) and bright-field images (A). The scale bar indicates 20 μm.

Turn-On fluorescence and selective sensing of l-Cys among all other amino acids by CDs–Hg2+ ensemble encouraged us to explore its use for the cellular imaging of l-cysteine in living fibroblasts (Figure S9) and HeLa cells (Figure S7, Supporting Information). The cells were incubated with CD–Hg2+ ensemble (10 μM) for 10 min and the CD–Hg2+ added cells were washed with buffer before imaging through confocal fluorescence microscopy. Very bright blue fluorescence from the inside of the cells was observed, showing the presence of intracellular biothiols, as shown in Figure S9B. Another set of cells was pretreated with a known biothiol quencher N-ethylmaleimide (NEM) in culture media. The NEM pretreated cells are incubated with CD–Hg2+ ensemble. The cells did not exhibit any observable fluorescence changes, as shown in Figure S9C. This proved the CD–Hg2+ is permeable to cell wall and the resulted changes account for the changes in the intracellular thiol level. The bright-field images confirmed that the cells were viable throughout the experiments. These results provided a way to monitor the changes of l-cysteine levels in the living cells. To ensure the intrusion of glutathione (GSH) during cysteine detection in living cells, we intend to verify whether the fluorescence increase is due to cys or GSH. We used an inhibitor for GSH synthesis l-buthionine sulfoximine (BSO) assay. BSO-treated cells were imaged, showing the increase in fluorescence when compared with the control that is untreated with BSO. On the other hand, when the cells were treated with BSO + H2O2, they showed decrease in fluorescence intensity (Figure S8, Supporting Information). Further, confocal images of the BSO + H2O2-treated cells on treatment with N-acetyl cysteine (a precursor for Cys), showed a dramatic increase in fluorescence intensity, obviously indicating that the fluorescence enhancement is exclusively due to changes in intracellular cysteine rather than intracellular GSH.[10]

Design of the Logic Gate

Designing logic gates utilizing electronic circuits in nanoregime is essential in molecular computation. Molecular logic gates mimic electronic circuits by performing Boolean arithmetic operations in the form of physicochemical and biological changes as their inputs. This type of logic gate was fabricated using the fluorescence response of the probe used with the different analytes on the basis of the consequent changes in the fluorescence intensity of the probe.

On the basis of the spectral characteristic changes, we have designed individual elementary logic operations, such as NOT and IMP gates, by utilizing CDs as probe and Hg2+ and l-Cys as chemical inputs.[22a] The fluorescence intensity change at 435 nm was fixed as the output signal. The output signal is considered as “On” state with a Boolean arithmetic value of “1” with the original or initial value of the emission intensity and considered as “Off” state with Boolean arithmetic value of “0” when the emission is quenched by 50%.

Interpretation of Logic Gate with Two Inputs

In a two-input logic operation, CD operates as gate and analytes (Hg2+, l-Cys) as the two chemical inputs (Figure ). Boolean arithmetic expressions 0 and 1 were considered as inputs for the gate with and without of the analytes, correspondingly.[22] Difference in the emission intensity at 435 nm of CD was considered as the output signal for analyzing On and Off states in the system. Different chemical inputs with four possible input string combinations (0,0; 1,0; 0,1; 1,1) were carried out. Presence of the metal ion Hg2+ as input in the absence of its counter anion l-Cys, the system expressed NOT gate (Figure ), the simplest of all logic gates. The quenching of the CD fluorescence is due to the formation of CD–Hg2+ complex aided by the presence of oxygenous hydrophilic groups. These results corroborate with the NOT gate, i.e., Off state. Further, upon addition of the counter anion l-Cys (input 2), the fluorescence behavior was reversed, with almost 85% increase in the emission intensity (Figure ). The high affinity of Hg2+ for the −SH group favors the formation of Hg2+–l-Cys complex, which separates the metal ion from the hydrophilic groups on the surface of CD, thereby recovering the fluorescence of CDs. Thus, an IMP gate has been constructed by using Hg2+ and l-Cys as inputs 1 and 2, respectively. The presence of both inputs 1 and 2 in the system expressed an On state. This clearly confirms that the decreased emission intensity in CD–Hg2+ is recovered by the stable Hg2+–l-Cys complex formation. The truth table also confirms the IMP gate (Figure ) behavior. The overall gate functions are represented in the Scheme . Thus, this CD nano-chemosensor can be used as a chemical logic gate for identification of mercury in real samples via fluorescent switching behavior pattern.

Figure 8

(A) Truth table for one and two strings and its corresponding digital input and output signals represent NOT and IMP gates, respectively, (B) bar diagram representing the two-input system, (C) schematic representation of logic functions of CD with two chemical inputs Hg2+ and l-Cys.

Scheme 1

Schematic Representation of Binary Logic Gates for CD System with Hg2+ and CD–Hg2+ + l-Cys Representing NOT and IMP Gates

Security Lock Device

The keypad lock development is interesting because a new approach for protecting information at a molecular level and has been utilized for various sensitive restricted data applications.[23] We have tried the utility of this system in electronic security devices, with the idea of a switching behavior in the present CD system (Figure ). We checked the difference in the emission behavior in a keypad security lock system (Figure ). The utility of CD is as a probe in a security keypad sensing device for Hg2+; fluorescent probe CD was subjected to the chemical inputs (Hg2+, l-Cys) either separately or in combination with CD (CD–Hg2+, CD–l-Cys). The molecular thiol in l-Cys will form a strong Hg2+–SH bond, resulting in desorption of Hg2+ from CD surface, leading to a “Off–On” behavior. Thus, while operating, if we first add l-Cys to the system containing CD–Hg2+ (quenched state), the relative emission intensity will be close to that of CD, i.e., fluorescence was almost recovered to 85%, which implies On state, with respect to the probe CD, whereas if we added Hg2+ to the system containing CD–l-Cys (already fluorescence), the fluorescence was almost the same (no change in fluorescence) with respect to CD, which denotes the Off state. Thus, with the change in the regulation of the inputs, the output signals (fluorescence) will be changed, enabling us to use the probe CD in a molecular keypad lock. The lock can be removed (“turn-On” state) using the order of inputs as 1 → Hg2+ → l-Cys, whereas we can lock (“turn-Off” state) the device using the order of inputs as 1 → l-Cys → Hg2+.

Figure 9

(A) Schematic representation of a keypad security lock model using CD as the molecular fluorescence system; (B) bar diagram representing the change in the emission intensity of CD. Chemical inputs were represented as H and C for Hg2+ and l-Cys and O and F for On and Off states, respectively.

To demonstrate the security lock device in terms of crossword puzzles, the analytes used as chemical inputs were named as H and C for Hg2+ and l-cysteine, respectively, and the fluorescence emission was considered as the output signal. The symbols O and F were noted for On and Off states. While executing the password, pressing C followed by H, the emission output will turn the switch on (O), i.e. turn-On state. However, pressing H and then C will cause no change in the output emission; the device remains locked, i.e., turn-Off state (F). Thus, the password “HCF” will lock the device whereas the password “CHO” opens the lock without fail.

Memory Device

This system can be used as a memory element, in molecular-level information processing for its unique switching nature: reversible response with alternate addition of Hg2+ and l-Cys (Figure ). Generally, sequential circuits in memory devices store the information and operate through a response loop, where one output in the logic system serves as a memory element.[24] For mimicking the memory element, we have used the chemical input Hg2+ (input 1) and Cys (input 2) as Reset (R) and Set (S), respectively. The emission intensity is taken as the output signal (Figure ). When the reset input (input 1) shows a quenching effect, i.e., low emission, the system is considered in “Off-state”, where the system “Read” the information, “Erase” it, and saves the “output” as 0. The above stored information, in other words, memorized information, was considered as “Write” by set input (input 2) and saves the output as 1. This “Write-Erase” cycle on CD probe can be performed for multiple cycles by adding Hg2+ and Cys in alternate sequence. This Off–On reversible behavior using chemical analytes represents the “Write-Read-Erase-Read” nature (Figure ). Thus, this system can be used as molecular microprocessors, a substitute for the traditional memory element in integrated logic circuits. To test and ensure the practical applications of the carbon dots to sense Hg(II) in water samples (lake and tap water), standard recovery experiments were performed. The water samples were added with different known quantities of Hg2+ and l-cysteine to compare and to imitate the real-environment measurements. It is apparent that the carbon dot-based Hg(II) chemosensor system is reliable and valid for detecting Hg2+ in water samples (Table S2, Supporting Information).

Figure 10

(A) Reversibility of the CD probe with alternate addition of Hg2+ and l-Cys, (B) truth table of the memory unit, (C) the feedback loops with Write-Read-Erase-Read function, (D) the sequential logic circuit of the memory unit.

Conclusions

In summary, we have presented a simple, low-cost, direct, and green one-pot method to produce CDs from the pineapple waste (peel) without any oxidizing agents through hydrothermal treatment. The CDs in aqueous solution emit strong blue light under a UV lamp with a fluorescent quantum yield of 0.42. This CD-based sensing system shows an ultraselective and sensitive fluorescent probe for label-free Hg2+ ion detection and has been successfully used for visual identification and quantitation of Hg2+ in real water samples from lake and tap water with satisfactory results. Further studies showed that the CDs can be used as a fluorescent probe for cellular imaging of Hg2+. The CDs exhibited multiple logic gates and were capable of mimicking a security keypad lock device at the molecular level with chemical inputs of Hg2+ ion and l-Cys. The CDs have also been used as molecular microprocessors, an alternative for the traditional memory element in integrated logic circuits.

Experimental Section

Synthesis of Carbon Dots

CDs were prepared from pineapple peel by hydrothermal method similar to the procedure used by us.[21a] In a typical procedure, the peel of pineapple was rinsed many times with water to remove the filth particles and was made into juice. Ten milliliters of the extract and 10 mL of ethanol were taken, and the reaction was preceded in an autoclave at 150 °C for 2 h, followed by extraction with methylene chloride and dialysis through a cellulose dialysis membrane. The aqueous solution was centrifuged at 10 000 rpm for 15 min to separate the less-fluorescent deposit. Excess acetone was added in the upper brown solution and centrifuged at high speed (15 000 rpm) for 15 min to obtain highly fluorescent CDs of average size 3–4 nm. As-obtained CDs were lyophilized and redispersed in water (1 mg mL–1) for further use.