 Open Access Article
 Open Access Article
Taha Alqahtania, 
Ali Alqahtania, 
Adil Alshehrib and 
Ahmed A. Almrasy *c
*c
aDepartment of Pharmacology, College of Pharmacy, King Khalid University, Abha, 62529, Saudi Arabia
bDepartment of Medicine, College of Medicine, King Khalid University, Abha, 62529, Saudi Arabia
cPharmaceutical Analytical Chemistry Department, Faculty of Pharmacy, Al-Azhar University, Cairo, 11751, Egypt. E-mail: ahmedalialmrasy8@gmail.com
First published on 21st October 2025
A novel, sensitive, and environmentally friendly fluorescence quenching method was developed for lisinopril determination using boron and nitrogen co-doped carbon quantum dots (B,N CQDs) as fluorescent probes. The B,N CQDs exhibited uniform nanoparticles with mean diameter of 3.97 nm and intense blue fluorescence with maximum excitation at 360 nm and emission at 429 nm. Upon increasing lisinopril concentration, a quenching of the B,N CQDs fluorescence was observed in a concentration-dependent manner. The fluorescence quenching mechanism was investigated through Stern–Volmer analysis, thermodynamic studies, and quantum mechanical calculations. Static quenching via ground-state complex formation was confirmed with Stern–Volmer constants (Ksv) decreasing from 7.94 × 105 to 5.48 × 105 M−1 as temperature increased from 298 to 313 K. Quantum mechanical studies using the PM6 method revealed binding energy of −33.58 kJ mol−1, in excellent agreement with experimental thermodynamic parameters (ΔG = −35.01 kJ mol−1). Two distinct interaction sites were identified: amino group of lisinopril with carboxylic group of B,N CQDs (4.4 Å) and carboxylic group of lisinopril with boron atom (3.6 Å). Experimental conditions were optimized using Box–Behnken response surface methodology. The developed method demonstrated a linear range of 0.02–2.0 μg mL−1, detection limit of 6.21 ng mL−1, and quantification limit of 18.63 ng mL−1. Method validation according to ICH Q2(R2) guidelines confirmed satisfactory accuracy (98.14 ± 0.857%) and precision (RSD < 1.25%). The method was successfully applied to commercial tablets and spiked plasma samples with excellent recovery (97.46–103.64%). Comprehensive greenness assessment using Analytical GREEnness Metric (AGREE), Modified Green Analytical Procedure Index (MoGAPI), Blue Applicability Grade Index (BAGI), and Click Analytical Chemistry Index (CACI) yielded scores of 0.77, 80%, 77.5, and 70, respectively. This work represents the first report of B,N CQDs for lisinopril determination, offering cost-effectiveness, room-temperature operation, and superior environmental profile.
Current analytical methods for lisinopril determination include various techniques, but each has their advantages and limitations that could restrict routine use. HPLC methods have been widely developed for pharmaceutical analysis of lisinopril.9–11 For example Beasley et al. established a stability-indicating HPLC method with high sensitivity (LOD 0.0075 μg mL−1), but the method requires lengthy gradient elution times and complex mobile phase optimization that reduces analytical throughput.9 LC-MS/MS approaches offer superior sensitivity for bioanalytical applications such as the work presented by Shah et al. which achieved high performance with LOQ of 0.50 ng mL−1 in human plasma using triple quadrupole MS, but the method requires expensive instrumentation, complex solid phase extraction using Waters Oasis HLB cartridges, and specialized technical expertise that limits laboratory accessibility.12 Another method by Qin et al. was developed using LC-MS/MS with LOQ of 1.03 ng mL−1, yet demands sophisticated mass spectrometric detection and high operational costs.13 Interestingly, electrochemical methods provide cost-effective alternatives but face selectivity challenges. For example, Coldibeli et al. developed voltammetric methods using boron-doped diamond electrodes with detection limits of 3.05 nmol L−1, but these methods suffer from electrode fouling and require specialized electrode materials.14 Spectrofluorimetric methods have gained attention for lisinopril determination due to their sensitivity, but face significant practical limitations. El-Emam et al. (2004) achieved high sensitivity using NBD-Cl derivatization with LOD of 0.008 μg mL−1 through HPLC-fluorescence detection, but requires expensive NBD-Cl reagent, elevated temperature (60 °C), and extended reaction time (70 minutes) that reduces analytical throughput.15 A recent method by Mohammed et al. introduced fluorescamine as a room-temperature probe achieving LOD of 0.182 μg mL−1, but still requires expensive fluorescamine reagent and alkaline pH conditions.16 However, these fluorimetric methods suffer from several drawbacks. The derivatization procedures are time-consuming and require expensive reagents. Moreover, the methods are susceptible to interference from endogenous amino acids in biological samples. These limitations restrict their routine application and highlight the need for simpler, more cost-effective fluorescence-based approaches.
Carbon quantum dots (CQDs) have emerged as promising fluorescent nanomaterials for analytical chemistry applications, representing a paradigm shift from traditional semiconductor quantum dots toward more sustainable and biocompatible alternatives.17 Since their discovery during carbon nanotube purification in 2004, CQDs have demonstrated remarkable analytical potential due to their unique size-dependent optical properties, excellent water solubility, low toxicity, and cost-effective synthesis from renewable precursors.18,19 The incorporation of heteroatoms, particularly boron and nitrogen co-doping, has significantly enhanced the optical and analytical performance of CQDs through synergistic electronic structure modifications that create new energy levels and narrow the HOMO–LUMO gap.20,21 B,N-doped CQDs exhibit superior quantum yields ranging from 15–59%, representing up to 12-fold improvements over undoped systems, while maintaining excellent photostability and pH tolerance across physiological ranges.22 These enhanced properties have enabled remarkable achievements in pharmaceutical analysis, with recent studies demonstrating nanomolar detection limits for various drug molecules including tetracycline (1 nM), dopamine (11 nM), and phenolic compounds (0.024–0.05 μM) through different fluorescence quenching mechanisms.23–25 These mechanisms primarily involve static quenching, photoinduced electron transfer, and inner filter effects, providing high selectivity and sensitivity for pharmaceutical compounds containing amino groups and aromatic systems.26 Despite these advances, the application of B,N-doped CQDs for ACE inhibitor determination remains largely unexplored, particularly for lisinopril, which presents unique analytical challenges due to its lack of strong chromophores and the complexity of biological matrices. Furthermore, as discussed earlier current fluorescence-based methods for lisinopril analysis suffer from expensive derivatization reagents and elevated temperature requirements highlighting the need for more practical and cost-effective analytical approaches.
Therefore, this study aims to develop and validate a novel, sensitive, and environmentally friendly “turn-off” fluorescence quenching method for lisinopril determination using boron and nitrogen co-doped carbon quantum dots (B,N CQDs) as fluorescent probes. The specific research objectives are: (1) to synthesize and comprehensively characterize B,N CQDs through physicochemical and optical techniques including size distribution, surface morphology, and structural analysis; (2) to investigate the fluorescence quenching mechanism between B,N CQDs and lisinopril using Stern–Volmer kinetics, thermodynamic studies, and quantum mechanical calculations to understand molecular-level interactions; (3) to systematically optimize experimental conditions (pH, B,N CQDs concentration, and reaction time) through Box–Behnken response surface methodology; (4) to validate the developed method according to ICH guidelines evaluating linearity, precision, accuracy, robustness, selectivity, and detection limits; (5) to demonstrate practical applicability through analysis of real pharmaceutical formulations and biological samples; and (6) to conduct comprehensive environmental assessment using different green analytical chemistry metrics to establish the method's sustainability profile. This work represents a novel report of B,N CQDs for lisinopril determination, offering advantages including cost-effectiveness, room-temperature operation, and superior environmental profile compared to conventional methods.
Britton–Robinson universal buffer systems were freshly prepared for each analytical session by combining equimolar amounts (0.04 M each) of orthophosphoric acid, boric acid, and glacial acetic acid. pH adjustment was achieved using standardized 0.2 M sodium hydroxide solution. All buffer pH values were confirmed using a calibrated pH meter to maintain accuracy within ±0.05 pH units.
Particle size analysis was conducted using dynamic light scattering (DLS) on a Malvern Zetasizer Nano ZS system. Morphological characterization was performed via transmission electron microscopy (TEM) using a JEOL JEM-2100 instrument operated at 200 kV. Structural analysis was accomplished through Fourier-transform infrared (FTIR) spectroscopy using a Nicolet iS5 FT-IR spectrometer across the wavenumber range of 4000–400 cm−1 with 4 cm−1 resolution. Samples were prepared as KBr pellets using the standard pelletization technique. Elemental composition of the purified B,N-CQDs was determined using CHN elemental analysis (PerkinElmer 2400 Series II CHNS/O analyzer).
Based on scouting results and risk analysis, three critical factors were selected for systematic optimization using Box–Behnken response surface methodology. The factor ranges were determined from preliminary studies and are presented in Table S1, ensuring adequate response coverage while maintaining analytical feasibility.
A total of 17 experimental runs were performed according to the Box–Behnken design matrix, including 5 center point replicates to estimate experimental error. Statistical analysis and model validation were conducted using Design Expert software (version 11, Stat-Ease Inc.). Analysis of variance (ANOVA) was employed to evaluate model significance and identify the most influential factors affecting analytical performance.
The volume was completed to the mark with the same solvent, and the solution was filtered through Whatman No. 42 filter paper to remove insoluble excipients. Appropriate aliquots of the filtrate were further diluted with deionized water to obtain concentrations within the validated linearity range and analyzed according to the general procedure.
For theoretical modeling purposes, a representative fragment of the B,N CQDs structure was constructed to maintain computational efficiency while preserving the essential electronic and structural features. The model fragment included the core aromatic system with boron and nitrogen heteroatoms, along with representative surface functional groups such as carboxyl (–COOH) and hydroxyl (–OH) groups that reflect the experimental synthesis conditions and characterization results. Interaction energies between B,N CQDs and lisinopril were calculated using the supermolecular approach:
| ΔE = E(complex) − E(B,N CQDs) − E(lisinopril) | (1) | 
![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) O stretching vibrations, which could arise from multiple carbonyl-containing functionalities including carboxylic acids, ketones, lactones, or amide groups formed during the hydrothermal synthesis process. The complex surface chemistry of thermally synthesized carbon quantum dots typically encompasses various oxygen-containing functionalities, making definitive assignment challenging based solely on vibrational spectroscopy. The characteristic peak observed at 1380 cm−1 has been consistently assigned to B–N stretching vibrations in boron–nitrogen co-doped carbon materials according to established literature. Chen et al. reported B–N in-plane tensile vibrations at 1371 cm−1 in B,N-doped graphene synthesized under hydrothermal conditions,28 while Ren et al. demonstrated that the peak at 1370 cm−1 is attributed to symmetric stretching of BN bonds in boron oxynitride systems.29 These surface functional groups are essential for enhancing water solubility and facilitating molecular interactions with target analytes. Additionally, CHN elemental analysis provided quantitative evidence for successful nitrogen incorporation into the carbon quantum dot framework. The elemental composition revealed: carbon (68.25%), hydrogen (4.12%), and nitrogen (11.84%), with oxygen and boron accounting for the remaining composition (15.79% by difference). The substantial nitrogen content of 11.84% falls within the typical range reported for N-doped carbon quantum dots and demonstrates efficient nitrogen incorporation during the hydrothermal synthesis process using urea as nitrogen source. While CHN analysis cannot directly quantify boron content, the combination of characteristic FTIR signatures at 1380 cm−1 (consistent with literature reports for B–N vibrations), enhanced optical properties, and synthesis methodology using boric acid provides supportive evidence for boron incorporation alongside the quantitatively confirmed nitrogen doping.
O stretching vibrations, which could arise from multiple carbonyl-containing functionalities including carboxylic acids, ketones, lactones, or amide groups formed during the hydrothermal synthesis process. The complex surface chemistry of thermally synthesized carbon quantum dots typically encompasses various oxygen-containing functionalities, making definitive assignment challenging based solely on vibrational spectroscopy. The characteristic peak observed at 1380 cm−1 has been consistently assigned to B–N stretching vibrations in boron–nitrogen co-doped carbon materials according to established literature. Chen et al. reported B–N in-plane tensile vibrations at 1371 cm−1 in B,N-doped graphene synthesized under hydrothermal conditions,28 while Ren et al. demonstrated that the peak at 1370 cm−1 is attributed to symmetric stretching of BN bonds in boron oxynitride systems.29 These surface functional groups are essential for enhancing water solubility and facilitating molecular interactions with target analytes. Additionally, CHN elemental analysis provided quantitative evidence for successful nitrogen incorporation into the carbon quantum dot framework. The elemental composition revealed: carbon (68.25%), hydrogen (4.12%), and nitrogen (11.84%), with oxygen and boron accounting for the remaining composition (15.79% by difference). The substantial nitrogen content of 11.84% falls within the typical range reported for N-doped carbon quantum dots and demonstrates efficient nitrogen incorporation during the hydrothermal synthesis process using urea as nitrogen source. While CHN analysis cannot directly quantify boron content, the combination of characteristic FTIR signatures at 1380 cm−1 (consistent with literature reports for B–N vibrations), enhanced optical properties, and synthesis methodology using boric acid provides supportive evidence for boron incorporation alongside the quantitatively confirmed nitrogen doping.
The optical characterization studies demonstrated that the B,N CQDs possessed superior photophysical properties arising from heteroatom doping effects. Initially, the UV-visible absorption spectrum (Fig. S1) revealed a strong absorption below 250 nm with high intensity (absorbance ∼3.0) attributed to π–π* transitions of the aromatic carbon framework, along with a secondary absorption band centered around 330 nm with moderate intensity (absorbance ∼0.8) corresponding to n–π* transitions involving nitrogen lone pairs and defect states introduced by heteroatom doping.24 Subsequently, the fluorescence properties were evaluated through excitation-emission spectroscopy (Fig. 1D), which demonstrated that upon excitation at 360 nm, the B,N CQDs exhibited intense blue fluorescence with maximum emission at 429 nm, resulting in a large Stokes shift of 69 nm that effectively minimizes interference from scattered excitation light. The 30 nm red shift from absorption maximum (330 nm) to optimal excitation wavelength (360 nm) is characteristic of heteroatom-doped carbon quantum dots, arising from n–π trap-state transitions involving lone-pair electrons on boron and nitrogen dopants and surface-defect emissive states that are optimally populated at longer excitation wavelengths. Notably, the quantum yield was calculated to be 64.2% using quinine sulfate as the reference, representing a significant enhancement compared to undoped CQDs due to the synergistic electronic effects of boron and nitrogen co-doping.30 These robust optical properties, combined with excellent photostability, make the synthesized B,N CQDs particularly suitable for analytical applications requiring consistent fluorescence response.
Initially, the possibility of inner filter effect was evaluated through UV-visible absorption analysis of lisinopril. The absorption spectrum of lisinopril (Fig. S2) revealed negligible absorption above 250 nm with virtually no measurable absorbance in the excitation and emission wavelength regions of the B,N CQDs. This absence of spectral overlap effectively excluded the inner filter effect as the primary quenching mechanism, thereby confirming that the observed fluorescence quenching resulted from genuine molecular interactions between the fluorophore and analyte.
Subsequently, Stern–Volmer analysis was conducted to quantify the quenching efficiency and determine the nature of the interaction mechanism (Fig. 2B). The linear Stern–Volmer plots at three different temperatures (298, 303, and 313 K) yielded Stern–Volmer constants (Ksv) of 7.94 × 105, 7.11 × 105, and 5.48 × 105 M−1, respectively (Table 1). Notably, the Ksv values demonstrated a systematic decrease with increasing temperature, which is characteristic of static quenching mechanisms rather than dynamic collisional quenching.31 To further validate this conclusion, the bimolecular quenching rate constants (Kq) were calculated using the relationship:
| Kq = Ksv/τ0 | (2) | 
| Temperature (K) | Ksv (105 M−1) | Ka (106 M−1) | ΔG (kJ mol−1) | ΔH (kJ mol−1) | ΔS (J mol−1 K−1) | 
|---|---|---|---|---|---|
| 298 | 7.94 | 1.36 | −35.01 | −26.00 | 30.21 | 
| 303 | 7.11 | 1.10 | −35.06 | ||
| 313 | 5.48 | 0.82 | −35.46 | 
Furthermore, the binding constants (Ka) were determined using the modified Stern–Volmer equation for static quenching:
| F0/F0 − F = 1/Ka[Q] + 1/Ka | (3) | 
The thermodynamic parameters provided additional insights into the nature of the binding interaction (Table 1) as analyzed using the van't Hoff plot (Fig. 2C). The negative Gibbs free energy values (ΔG = −35.01, −35.06, and −35.46 kJ mol−1 at 298, 303, and 313 K, respectively) confirmed the spontaneous nature of the binding process. The negative enthalpy change (ΔH = −26.00 kJ mol−1) suggested that the interaction was exothermic and primarily driven by van der Waals forces and hydrogen bonding. Additionally, the positive entropy change (ΔS = 30.21 J mol−1 K−1) indicated increased randomness upon complex formation, likely due to the release of bound water molecules from the interaction sites.33 These thermodynamic signatures are consistent with a static quenching mechanism involving hydrogen bonding and electrostatic interactions between the amino and carboxyl groups of lisinopril and the surface functional groups of B,N CQDs, as evidenced by the FTIR characterization results.
Geometry optimization using the PM6 semiempirical method yielded stable structures for both the individual components and their complex (Fig. 3). The optimized structure of lisinopril (Fig. 3A) demonstrated a total energy of −0.350620 hartree, while the B,N CQDs fragment (Fig. 3B) exhibited a slightly lower energy of −0.434781 hartree, indicating the inherent stability of both molecular systems. Subsequently, the optimized complex formation (Fig. 3C) resulted in a total energy of −0.798190 hartree, representing the energetically favorable binding configuration between the fluorophore and analyte.
The binding energy (ΔE) was calculated using the supermolecular approach according to eqn (1), yielding a value of −0.012789 hartree, which converts to −33.58 kJ mol−1 for the complex formation. This negative binding energy confirmed the thermodynamically favorable interaction between B,N CQDs and lisinopril, which correlates excellently with the experimentally determined Gibbs free energy values (ΔG = −35.01 to −35.46 kJ mol−1) obtained from the thermodynamic analysis, with less than 5% deviation. The outstanding agreement between theoretical and experimental values validates the computational model and demonstrates that the PM6 method adequately captures the essential binding interactions, despite the simplified model system and gas-phase calculations.
Detailed analysis of the optimized complex geometry revealed two distinct electrostatic interaction sites that govern the binding mechanism (Fig. 3C). The first interaction site involves the amino group of lisinopril and the carboxylic acid functional group of the B,N CQDs, with an intermolecular distance of 4.4 Å. This relatively short distance indicates strong interaction, which is consistent with the negative enthalpy change (ΔH = −26.00 kJ mol−1) observed experimentally and supports the proposed electrostatic bonding mechanism. The second interaction site occurs between the carboxylic acid group of lisinopril and a boron atom in the B,N CQDs framework, characterized by an intermolecular distance of 3.6 Å. This interaction represents a Lewis acid–base interaction where the electron-deficient boron atom acts as an electron acceptor for the oxygen lone pairs of the carboxylic group. This quantum mechanical calculations further revealed that the boron and nitrogen co-doping significantly enhances the selectivity of the B,N CQDs toward both the acidic and basic functional groups present in lisinopril. The incorporation of boron atoms creates electron-deficient sites within the carbon framework, thereby increasing the affinity for electron-rich functional groups such as carboxylic acids. This synergistic effect of heteroatom doping explains the superior analytical performance of B,N CQDs compared to undoped carbon quantum dots and provides a rational basis for the high selectivity observed in the experimental studies. Furthermore, the computational results validate the static quenching mechanism by demonstrating that stable ground-state complexes can form between B,N CQDs and lisinopril through multiple complementary interaction sites, as evidenced by the favorable binding energetics and optimal intermolecular geometries.
| Source | Sum of squares | df | Mean square | F-value | p-value | |
|---|---|---|---|---|---|---|
| Model | 5.62 | 5 | 1.12 | 49.69 | <0.0001 | Significant | 
| A-pH | 0.4288 | 1 | 0.4288 | 18.96 | 0.0011 | |
| B-B,N-doped CQDs conc. | 1.38 | 1 | 1.38 | 60.83 | <0.0001 | |
| AB | 0.1567 | 1 | 0.1567 | 6.93 | 0.0233 | |
| A2 | 1.99 | 1 | 1.99 | 87.86 | <0.0001 | |
| B2 | 1.47 | 1 | 1.47 | 64.97 | <0.0001 | |
| Residual | 0.2488 | 11 | 0.0226 | |||
| Lack of fit | 0.2034 | 7 | 0.0291 | 2.56 | 0.1901 | Not significant | 
| Pure error | 0.0454 | 4 | 0.0113 | |||
| Cor total | 5.87 | 16 | ||||
The mathematical relationship between the response variable and the independent factors was expressed through the following coded equation derived from multiple regression analysis:
| QE% = 2.96213 + 0.231511 × A + 0.414689 × B + 0.19792 × AB − 0.686 × A2 − 0.589935 × B2 | (4) | 
Model adequacy was rigorously evaluated through comprehensive statistical analysis (Table S2 and Fig. S3–S4). The coefficient of determination (R2 = 0.9576) indicated that 95.76% of the variability in quenching efficiency can be explained by the model, while the adjusted R2 (0.9383) accounts for the number of terms in the model and confirms excellent fit quality. The predicted R2 (0.8429) demonstrates satisfactory predictive capability, with the difference between adjusted and predicted R2 being less than 0.2, indicating good model stability. Furthermore, the adequate precision value of 19.2989 significantly exceeds the minimum threshold of 4.0, confirming that the model has sufficient signal-to-noise ratio for reliable optimization. The coefficient of variation (6.37%) falls within acceptable limits, indicating good reproducibility of the experimental measurements. Diagnostic plots (Fig. S3) including normal probability plots, predicted versus actual values, and residual analyses demonstrated random distribution of residuals without systematic patterns, confirming the validity of the regression assumptions. The run order analysis (Fig. S4A) demonstrated random distribution of residuals across the experimental sequence with no systematic trends, confirming the absence of time-dependent effects such as instrument drift or reagent degradation during the experimental campaign. Additionally, the leverage analysis (Fig. S4B) showed that all experimental points fell within acceptable limits, indicating that the experimental design was well-balanced and no individual runs exerted confirming no influence on the model parameters, further validating the model robustness and reliability.
The main effect plots (Fig. 4) provided comprehensive insights into the individual factor influences on quenching efficiency, directly correlating with the mathematical coefficients in eqn (4). The pH effect (Fig. 4A) demonstrated a clear optimum around pH 6.7, reflecting the complex relation between the protonation states of both the B,N CQDs surface functional groups and lisinopril. At lower pH values, excessive protonation leads to aggregation of B,N CQDs due to reduced electrostatic repulsion between particles. Conversely, at higher pH values, deprotonation of the amino group in lisinopril prevents its effective interaction with the negatively charged surface of deprotonated B,N CQDs, leading to electrostatic repulsion rather than attraction. This pH dependence aligns with the negative quadratic coefficient (A2 = −0.686) and explains the parabolic relationship observed experimentally. The B,N CQDs concentration effect (Fig. 4B) showed increasing quenching efficiency up to approximately 72 μg mL−1, beyond which a plateau was observed. This behavior reflects the saturation of available binding sites and is consistent with the positive linear coefficient (0.414689) and negative quadratic term (−0.589935). The reaction time effect (Fig. 4C) indicated rapid equilibration within 3 min, suggesting efficient complex formation kinetics that support the static quenching mechanism established in the mechanistic studies. Notably, reaction time was found to be statistically non-significant (p > 0.05) in the ANOVA analysis and was consequently excluded from the reduced quadratic model equation. This exclusion confirms that the binding equilibrium is rapidly achieved and that reaction time does not significantly influence the analytical response within the studied range, thereby simplifying the optimization process to focus on the two critical factors: pH and B,N CQDs concentration.
The interaction and three-dimensional response surface plots (Fig. S5) revealed the synergistic relation between pH and B,N CQDs concentration, as quantified by the positive interaction coefficient (AB = 0.19792). The two-dimensional interaction plot (Fig. S5A) demonstrated curved response lines at different B,N CQDs concentrations, indicating that optimal quenching efficiency requires simultaneous optimization of both factors rather than individual factor optimization. The three-dimensional response surface plot (Fig. S5B) clearly visualized the response maximum as a distinct peak in the surface, confirming the existence of well-defined optimal conditions at approximately pH 6.7 and B,N CQDs concentration of 72 μg mL−1. This synergistic behavior can be attributed to the pH-dependent surface charge of B,N CQDs, which affects the accessibility and reactivity of functional groups toward lisinopril binding. At the optimal pH, the B,N CQDs surface exhibits balanced protonation states that maximize both hydrogen bonding and electrostatic interactions, while sufficient concentration ensures adequate probe availability for complex formation.
Numerical optimization using the desirability function approach (Fig. S6) identified the optimal conditions as pH 6.68, B,N CQDs concentration 71.68 μg mL−1, and reaction time 3.12 minutes, yielding a predicted maximum quenching efficiency of 3.07. For practical analytical applications, these conditions were approximated to pH 6.7 ± 0.05, B,N CQDs concentration 70 μg mL−1, and reaction time 3 minutes, which provide convenient working parameters while maintaining optimal analytical performance. The excellent agreement between predicted and experimental values under these optimized conditions validates the model reliability and demonstrates the successful application of response surface methodology for method development. These optimized parameters were subsequently employed for all validation studies and real sample analyses, ensuring consistent and maximum analytical sensitivity throughout the investigation.
| Parameters | Lisiopril | |
|---|---|---|
| a Average of 9 determinations (3 concentrations repeated 3 times).b % RSD of 9 determinations (3 concentrations repeated 3 times) measured on the same day.c % RSD of 9 determinations (3 concentrations repeated 3 times) measured in the three consecutive days. | ||
| Excitation wavelength (nm) | 360 | |
| Emission wavelength (nm) | 429 | |
| Linearity range (μg mL−1) | 0.02–2.0 | |
| Slope | 1.9580 | |
| Intercept | 1.0998 | |
| Correlation coefficient (r2) | 0.9998 | |
| LOD (ng mL−1) | 6.21 | |
| LOQ (ng mL−1) | 18.63 | |
| Accuracy (% R)a | 98.14 ± 0.857 | |
| Repeatability precision (% RSD)b | 0.873 | |
| Intermediate precision (% RSD)c | 1.244 | |
| Robustness (% R) | Buffer (pH) | 101.80 ± 1.397 | 
| Reagent conc. (μg mL−1) | 98.90 ± 0.804 | |
| Reaction time (min) | 100.68 ± 0.889 | |
The accuracy evaluation revealed excellent recovery with an overall accuracy of 98.14 ± 0.857% based on nine determinations across three concentration levels, confirming minimal systematic bias in the analytical procedure (Table 3). Precision studies demonstrated satisfactory reproducibility with repeatability precision (intra-day) of 0.873% RSD and intermediate precision (inter-day) of 1.244% RSD, both well within the acceptable limits for pharmaceutical analysis (<2% RSD). Robustness evaluation assessed the method's resistance to small variations in critical parameters, yielding recoveries of 101.80 ± 1.397% for buffer pH variations, 98.90 ± 0.804% for reagent concentration changes, and 100.68 ± 0.889% for reaction time modifications. These results confirm that minor analytical variations do not significantly affect method performance, supporting the method's reliability for routine analytical applications.
Selectivity studies (Fig. S7) demonstrated the method's high performance for lisinopril determination in the presence of potential interferents commonly found in pharmaceutical formulations and biological matrices. While lisinopril exhibited remarkable quenching efficiency of approximately 67%, all tested interferents including inorganic salts (Na+, K+, Ca2+, Mg2+), transition metals (Ni2+, Cd2+), anions (SO42−, PO43−), excipients (starch, lactose, cellulose, magnesium stearate, sodium lauryl sulfate) and biological components (tryptophan, tyrosine, glutamic acid, glucose) showed negligible interference with quenching efficiencies below 5%. Importantly, structurally similar ACE inhibitors including captopril, enalapril, and ramipril demonstrated significantly lower quenching efficiencies (below 5%) compared to lisinopril despite their structural similarities, confirming excellent method selectivity even against closely related compounds. This high selectivity can be attributed to the specific interaction mechanism between B,N CQDs and the unique structural features of lisinopril, particularly its amino and carboxylic acid functional groups that enable optimal binding geometry as confirmed by quantum mechanical calculations.
The comprehensive validation study establishes that the developed B,N CQDs fluorescence quenching method meets all ICH requirements for pharmaceutical analysis with superior analytical performance characteristics. The combination of excellent linearity, high sensitivity, satisfactory precision and accuracy, robust performance, and high selectivity makes this method highly suitable for quantitative determination of lisinopril in pharmaceutical formulations and biological samples, offering significant advantages over existing analytical approaches in terms of simplicity and cost-effectiveness.
The method was successfully applied to the determination of lisinopril in commercial tablet formulations (Zestril®, 10 mg) with excellent analytical performance (Table 4). The developed fluorescence method yielded a mean recovery of 100.03 ± 0.724% (n = 5), demonstrating high accuracy and precision for pharmaceutical analysis. Statistical comparison with a reference HPLC method11 showed a mean recovery of 99.69 ± 0.99% for the same tablet samples. The two-tailed t-test (calculated t = 0.523) was significantly lower than the tabulated value (t = 2.306 at P = 0.05), indicating no statistically significant difference between the methods. Similarly, the F-test (calculated F = 1.873) was below the critical value (F = 6.338 at P = 0.05), confirming equivalent precision between the methods. The bias evaluation using the ±2% acceptance criterion showed θL = −0.920 and θU = 0.558, both within acceptable limits, establishing method equivalence and confirming the absence of systematic bias. These results validate the developed method's accuracy and reliability for pharmaceutical quality control applications.
| Method | Meana | SD | t-test (2.306)b | P value | F-value (6.338)b | P value | θLc | θUc | 
|---|---|---|---|---|---|---|---|---|
| a Average of five determinations.b The values in parenthesis are tabulated values of “t”and “F” at (P = 0.05).c Bias of ± 2% is acceptable. | ||||||||
| Developed method | 100.03 | 0.724 | 0.523 | 0.628 | 0.549 | 1.873 | 0.558 | −0.920 | 
| Reported method | 99.69 | 0.99 | ||||||
Recovery studies were also conducted using drug-free human plasma spiked with known concentrations of lisinopril to evaluate the method's performance in biological matrices (Table S3). The method demonstrated excellent recovery across the tested concentration range (0.05–1.5 μg mL−1) with recovery percentages ranging from 97.46% to 103.64%. At the lowest concentration (0.05 μg mL−1), the method achieved 97.46% recovery with 3.454% RSD, demonstrating satisfactory performance near the quantification limit. Mid-range concentrations (0.1 and 0.5 μg mL−1) showed optimal performance with recoveries of 103.64% and 102.36%, respectively, and improved precision (RSD < 3%). At the highest concentration (1.5 μg mL−1), the method maintained excellent accuracy (97.81% recovery) with the best precision (1.353% RSD). The consistent recovery values across the concentration range and acceptable precision (RSD < 5%) confirm the method's suitability for bioanalytical applications.
The MoGAPI assessment, which combines the visual impact of GAPI with quantitative total scoring, yielded a score of 80% classifying the method as excellent green (Fig. 5B). The high score reflected (1) off-line sample collection with no preservation requirements and minimal transport considerations, (2) simple analytical procedures without complex extraction requirements operating at room temperature, (3) readily available reagents with B,N CQDs synthesized from commercially available precursors including citric acid, boric acid, and urea using standard laboratory equipment, (4) accessible instrumentation utilizing standard fluorescence spectroscopy equipment available in most analytical laboratories, and (5) minimal environmental impact through reduced waste generation and low energy consumption. The MoGAPI assessment confirmed the method's superior environmental performance compared to conventional analytical approaches for lisinopril determination, particularly highlighting the advantages of green solvent usage and simplified analytical procedures.
The CACI assessment, emphasizing simplicity, efficiency, and reliability inspired by click chemistry principles, resulted in a score of 70 indicating highly practical method performance (Fig. 5D). The evaluation demonstrated excellent alignment with click analytical chemistry principles through (1) simplified sample preparation, (2) excellent feasibility with all reagents commercially available, standard fluorescence instrumentation accessible in most laboratories, and estimated cost less than $10 per sample analysis, (3) quantitative determination capability applicable to pharmaceutical formulations and biological matrices demonstrating analytical versatility, (4) acceptable sensitivity with detection limit of 6.21 ng mL−1 representing less than 1% of pharmaceutical concentrations, and (6) rapid analysis time. The CACI assessment confirmed the method's practical advantages including simplicity, cost-effectiveness, and rapid implementation suitable for routine analytical applications.
The comprehensive multi-metric assessment demonstrates that the developed B,N CQDs fluorescence method exhibits excellent environmental traits with high practical applicability. All four metrics consistently identified the method's strengths in environmental sustainability through minimal reagent consumption, absence of organic solvents, low energy requirements, and reduced waste generation, combined with practical implementation advantages including simple procedures, readily available reagents and instrumentation, and rapid analysis times. The assessment scores of AGREE (0.77), MoGAPI (80%), BAGI (77.5), and CACI (70) collectively establish the method as a sustainable and practical alternative for routine lisinopril determination, demonstrating significant improvements over conventional analytical approaches and supporting the transition toward more environmentally responsible analytical practices in pharmaceutical quality control and bioanalytical applications.
Despite the promising analytical performance and practical advantages, several limitations warrant consideration for future development. The primary limitation concerns selectivity challenges when analyzing complex biological matrices containing structurally similar compounds with amino and carboxylic acid functional groups. While the method demonstrated excellent selectivity against tested interferents, the fluorescence quenching mechanism relies on specific interactions between B,N CQDs and lisinopril's functional groups, which may not provide absolute selectivity in the presence of structurally related pharmaceuticals. Future research should focus on enhancing method selectivity through advanced recognition strategies, particularly the development of molecularly imprinted polymers (MIPs) combined with B,N CQDs. MIP-CQDs composite materials could provide dual recognition mechanisms, combining the fluorescence properties of B,N CQDs with the selective binding cavities of molecularly imprinted polymers, thereby significantly improving selectivity against structurally similar interferents. Additionally, surface modification of B,N CQDs with specific recognition elements or aptamers could enhance selectivity while maintaining excellent analytical performance. Integration with advanced separation techniques such as capillary electrophoresis or microfluidic devices could provide additional selectivity dimensions, while extending the method to simultaneous determination of multiple ACE inhibitors through multivariate calibration approaches would increase practical applicability. This work represents a significant advancement in pharmaceutical analysis, offering a sustainable, cost-effective, and sensitive alternative for lisinopril determination with promising potential for further development in bioanalytical applications.
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