Research Article | | Peer-Reviewed

Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes

Received: 11 March 2026     Accepted: 23 March 2026     Published: 10 April 2026
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Abstract

The spectral characteristics of 2-aminophenol (2AP) in various solvents, α-cyclodextrin (α-CD) and β-cyclodextrin (β-CD) at pH~3, pH~7, and pH~11, were investigated using UV-visible, fluorescence, time-resolved fluorescence measurements, and PM3 computational methods. The Ag: 2AP: CD nanomaterials were synthesized and characterized by SEM, FTIR, and XRD techniques. In all the pH conditions, 2AP exhibited distinct absorption and emission shifts upon complexation with α-CD and β-CD. In various solvents, the absorption and emission maxima of 2AP were similar to those of 2-anisidine. 2AP showed a single broad emission band in all solvents, whereas dual emission observed in CD solutions indicates the presence of an intramolecular proton transfer (IPT) process in the 2AP molecule. The lifetimes of the inclusion complexes were longer than that of the free 2AP molecule. The geometrical restriction of the α-CD cavity likely limits the free rotation of the amino and hydroxyl groups, thereby enhancing the intensity of the IPT emission. The calculated HOMO-LUMO energy gap, total energy, free energy, enthalpy, entropy, dipole moment, and zero-point vibrational energy of the CD: 2AP complex differed significantly from those of the isolated 2AP, α-CD and β-CD molecules, and both the vertical and horizontal bond lengths between the amino and hydroxy groups are smaller than the β-CD cavity size confirming the formation of an inclusion complex. SEM-EDX data confirmed the presence of 5.5% silver in the nanomaterials.

Published in American Journal of Physical Chemistry (Volume 15, Issue 2)
DOI 10.11648/j.ajpc.20261502.11
Page(s) 22-32
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2026. Published by Science Publishing Group

Keywords

2-aminophenol, Cyclodextrin, Silver Nano, pH Effects, Excimer

1. Introduction
The ability of cyclodextrins (CDs) to accommodate guest molecules of suitable size within their cavities has been widely utilized to control the photophysical and photochemical properties of various molecules, such as fluorescence enhancement and intramolecular excimer/exciplex formation . Kim et al. , Jiang et al. , and others demonstrated that the twisted intramolecular charge transfer (TICT) emission of 4-(N, N-diethylamino) and 4-(N, N-dimethylamino) benzoic acids is enhanced upon complexation with β-CD. This enhancement has been attributed to the reduced polarity of the microenvironment rather than to restricted molecular motion inside the CD cavity. From this point of view, it is interesting to examine how CD systems influence the intramolecular charge transfer (ICT) emission and the excited-state geometry of different types of ICT molecules.
Over the past two decades, we have investigated the solvent, pH, and CD dependences of the photophysical properties of various molecules in both the ground and excited states. Since different organic molecules exhibit remarkable behavior depending on pH and microenvironmental conditions, it is worthwhile to study some substituted phenols under diverse conditions. In this context, the present work analyze: (i) the absorption and fluorescence spectral shifts and the first excited singlet-state lifetime of 2-aminophenol (2AP) in α-CD, β-CD, solvents of different polarities, and at various pH values; (ii) the proton transfer reaction of 2AP in aqueous, α-CD, and β-CD media; (iii) the structures and geometries of the inclusion complexes by molecular modeling (PM3) methods; and (iv) the doping effect of 2AP: CD on silver nanomaterials characterized by DSC, FTIR, ¹H NMR, and SEM techniques .
2. Materials and Methods
2.1. Preparation of CD Solution
The concentration of the stock solution of 2-aminophenol (2AP) was 2 × 10⁻² mol/dm³. Aliquots of the stock solution (0.1 or 0.2 mL) were transferred into 10 mL volumetric flasks. Varying concentrations of α-CD or β-CD solutions (0.2, 0.4, 0.6, 0.8, and 1.0 × 10⁻² mol/dm³) were added. The mixed solutions were diluted to the mark with triply distilled water and shaken thoroughly. The final concentration of 2AP in all flasks was 4 × 10⁻⁴ mol/dm³. All experiments were carried out at room temperature (298 K).
2.2. Preparation of Ag: 2AP: CD Nanomaterials
A 0.01 M solution of silver nitrate was prepared in 50 mL of deionized water and warmed at 50-60°C for 30 minutes. Then, 1-2 mL of 1% trisodium citrate solution (1 g dissolved in 100 mL of deionized water) was added with vigorous stirring. The appearance of a pale yellow color confirmed the formation of silver nanoparticles .
Cyclodextrin (1 mmol) was dissolved in 40 mL of distilled water, and 2AP (1 mmol) dissolved in 10 mL of ethanol was slowly added to the CD solution. The mixture was stirred at 50°C for 2 hours using a magnetic stirrer. Subsequently, the silver nanoparticle solution was added and stirred for an additional 2 hours. The resulting dilute solution was gently warmed at 40-50°C until its volume was reduced by approximately 50%. The solution was then refrigerated overnight at 5°C.
The precipitated Ag-2AP-CD nanomaterials were collected by filtration and washed several times with small amounts of ethanol and water to remove uncomplexed 2AP, silver, and CD, respectively. The product was dried under vacuum at room temperature and stored in an airtight container. The resulting powder samples were used for further characterization and analysis .
2.3. Instruments Used
Absorption spectra were recorded using Shimadzu UV-Visible spectrophotometers (Models 1650 PC and UV-2600 PC), while fluorescence measurements were carried out on a Shimadzu RF-5301 fluorimeter.
FTIR: Using an Avatar FTIR spectrometer, FTIR analysis was conducted, which is a typical method for determining molecular structures and detecting functional groups. Pellets were formed by combining 4 mg of sample with 120 mg of KBr. A resolution of 4 cm-1 (256 scans) was used to capture spectra spanning the 4000-400 cm-1 range.
DTA: An analysis of the nanomaterials' and components' thermal behaviour was conducted using STRe software and a Mettler Toledo DSC1 equipment. Under a nitrogen environment, samples ranging from 2 to 5 mg were scanned at a temperature of 10°C/min from 25 to 280°C in pans made of aluminium. The instrument was calibrated with indium.
XRD: XRD patterns were recorded using a BRUKER D8 Advance diffractometer (Bruker AXS GmbH, Karlsruhe, Germany) equipped with Cu Kα₁ radiation (λ = 1.5406 Å), operated at 40 kV and 20 mA. The diffraction data were collected over a 2θ range of 5°-80°, with a scan rate of 5°/min and a step size of 0.03°, using dry powdered samples.
FE-SEM: Imaging surface morphology and microstructure using a scanning electron microscope (SEM) is a multipurpose approach. The SEM scans the surface of a solid sample using a concentrated stream of high-energy electrons, and the signals it emits reveal the material's topography, composition, crystallinity, and electrical characteristics. An XL ESEM machine was used to obtain SEM pictures for this investigation. The samples that had been pulverised were attached to brass stubs using conductive tape that had two sides. A vacuum sputter coater was used for 30 seconds at 30 W to coat the samples with a thin conductive coating (carbon, gold, silver, or platinum) that was around 200 thick before imaging. The conductivity, resolution, and prevention of charge buildup are all improved by this coating. With an excitation voltage of either 15 or 25 kV, imaging was carried out at magnifications of 200×, 500×, and 5000×.
Molecular Modeling Studies: PM3 semiempirical approach was used to study the inclusion behaviour of the compounds containing α-CD and β-CD because it is computationally efficient and can efficiently represent complex molecular systems, particularly those with non-covalent interactions like hydrogen bonding. Spartan 08 was used to build the guest molecules' and CDs' initial geometries, and then we optimised them using the PM3 technique in the Gaussian 09W package. While optimising, no symmetry restrictions were enforced.
3. Result and Discussion
3.1. Effect of α-CD and β-CD with pH on 2-aminophenol
To analyze the inclusion behavior of the monocationic, neutral, and monoanionic forms of 2AP with α-CD and β-CD, the absorption and emission spectra (Table 1, Figure 1, and Figure 2) were recorded in solutions of approximately pH~3, pH~7, and pH~11. The absorption and emission maxima of 2AP in these pH conditions (in the absence of CD) appear at the following wavelengths: pH ~3: λabs = 272, 212 nm; λflu = 300 nm; pH ~7: λabs = 283, 232 nm; λflu = 337 nm; pH ~11: λabs = 286, 216 nm; λflu = 338 nm. These results indicate that the monocationic species is predominant at pH ~3, the neutral species at pH ~7, and the monoanionic species at pH ~11. At pH ~7, the emission maximum at 337 nm resembles that observed in non-aqueous solvents and can therefore be assigned to the molecular form of 2AP.
The spectral maxima of 2AP in selected solvents are as follows: cyclohexane: λabs= 286, 236 nm; λflu = 320 nm; acetonitrile: λabs= 289, 240 nm; λflu = 326 nm; methanol: λabs= 284, 235 nm; λflu = 330 nm; water: λabs= 282, 229 nm; λflu = 335 nm. These results show that in different solvents, the absorption and emission maxima of 2AP are similar to those of 2-anisidine (2AS) : cyclohexane: λabs= 285, 235 nm; λflu = 309 nm; acetonitrile: λabs= 288, 240 nm; λflu = 323 nm; methanol: λabs= 286, 237 nm; λflu = 327 nm; water: λflu = 284, 230 nm; λflu = 334 nm. 2AP exhibits a single broad emission band in all solvents. The absence of longer-wavelength emission indicates that intramolecular charge transfer (ICT), exciplex, or excimer formation does not occur in any of the solvents .
When compared with aniline (cyclohexane: λflu = 283, 235 nm; λflu = 320 nm; acetonitrile: λflu = 286, 238 nm; λflu = 329 nm; methanol: λflu = 284, 232 nm; λflu = 334 nm; water: λflu = 278, 230 nm; λflu = 335 nm) , no significant spectral changes are observed for 2AP. However, relative to phenol (cyclohexane: λflu = 277-271 nm; λflu = 300 nm; acetonitrile: λflu = 278-272 nm; λflu = 302 nm; methanol: λflu = 275-272 nm; λflu = 305 nm; water: λflu = 272-278 nm; λflu = 305 nm) , a red shift is observed for 2AP, indicating delocalization between the amino and hydroxyl groups.
Table 1. Absorption and fluorescence maxima of 2-aminophenol (2AP) with different α-CD and β-CD concentrations.

Concentration of α-CD x10-3 M

pH - 3.0

pH - 7

pH - 11

abs

flu

IF

abs

flu

IF

abs

flu

IF

2AP only (without CD)

281 228

303

0.32

283 229

302 341

0.34

284 230

338

0.29

0.2 M α-CD

269 211

303

0.41

281 229

302 341

0.40

284 230

363

0.36

1.0 M α-CD

269 211

303

0.53

281 229

302 341

0.49

284 230

365

0.51

0.2 M β-CD

270 209

301

0.43

277 229

303

0.46

283 228

337 300

0.48

1.0 M β-CD

270 210

302

0.56

273 229

303

0.57

283 228

337 300

0.61

K (1: 1) x105 M-1 α-CD

60

114

500

201

55

314

G (kcalmol-1) α-CD

-10.32

-22.35

-9.53

-40

-15

-22.0

K (1: 1) x105 M-1 β-CD

86.3

85

70.7

213

220

195

G (kcalmol-1) β-CD

11.2

-13

-10.7

-10.0

-18.6

-15.0

Excitation wavelength (nm)

270

270

270

In solvents, the absorption maximum of 2AP is red-shifted from cyclohexane to acetonitrile but blue-shifted in alcohol and water, whereas the emission maximum is progressively red-shifted from cyclohexane to water. 2AP exhibits a single broad fluorescence band in all solvents, and the absence of longer-wavelength emission in polar solvents further confirms the absence of excimer or exciplex formation. In all solvents, 2AP displays a single emission band, whereas in CD solutions dual emission is observed. The dual emission can be explained as follows: one band appears in the shorter-wavelength region (300 nm, SW) and the other in the longer-wavelength region (360 nm, LW). As the CD concentration increases, both SW and LW emission bands undergo red shifts, with the LW band showing a larger shift.
Figure 1. Absorbance spectra of PTD in different α-CD and β-CD concentrations (M): 0, (2) 0.002, (3) 0.004, (4) 0.006, (5) 0.008, (6) 0.01.
Figure 2. Fluorescence spectra of PTD in different α-CD and β-CD concentrations (M): 0, (2) 0.002, (3) 0.004, (4) 0.006, (5) 0.008, (6) 0.01.
In both α-CD and β-CD solutions, the absorption and emission maxima, as well as the spectral profiles of 2AP at pH~3, pH~7, and pH~11, differ from one another. In α-CD, the absorption maximum is blue-shifted at pH ~3 and shows no significant change at pH~7 and pH ~11. In β-CD, the absorption is red-shifted at pH~3, blue-shifted at pH~7, and shows no notable shift at pH~11. In α-CD, the absorbance of 2AP decreases at pH ~3 but increases at pH ~7 and pH ~11. In β-CD, the absorbance decreases at pH~3 and pH ~7 but increases at pH ~11.
In the excited state, in α-CD solutions, the emission intensity increases in all three pH values, whereas in β-CD the emission intensity decreases at pH ~3 but increases at pH~7 and pH~11 (Figure 2). In all the pH conditions, dual emission bands are observed in both CDs. In aqueous CD-free solutions, the emission maxima at pH~3, pH~7, and pH~11 differ from each other. In α-CD at pH~3, 2AP shows an emission maximum at 300 nm, while at pH~7 and pH~11, it appears at 337 nm. Increasing α-CD concentration enhances the single emission intensity at pH ~3 and induces dual emission at pH~7 and pH~11. The effect of β-CD on the emission spectra of 2AP differs from that of α-CD. With increasing β-CD concentration, emission intensity decreases at pH~3 but increases at pH~7 and pH~11. In β-CD, a single emission band is observed at pH~3 and pH~7, while dual emission appears at pH~11. Further, at pH~11, the intensity of the shorter-wavelength band (SW, normal emission) decreases, whereas the longer-wavelength (LW) emission increases .
The observed variations in absorbance, emission intensity, and spectral maxima arise from the encapsulation of 2AP molecules within the α-CD and β-CD cavities. No significant change in absorbance was observed even after 12 hours, indicating the stability of the inclusion complexes. The presence of an isosbestic point in the absorption spectra at all pH values suggests the formation of 1: 1 inclusion complexes, though the orientation of the guest molecule inside the CD cavity may differ . The binding constant (K, Table 1) values were obtained from the slope and intercept of the Benesi-Hildebrand plots. The negative ΔG values (Table 1) indicate that the inclusion process is spontaneous and exothermic at 303 K.
In the excited state, as the concentration of α-CD and β-CD increases, the emission intensity of 2AP either increases or decreases depending on the pH. In CD-free solutions, 2AP exhibits a single broad emission band, whereas upon addition of CD, a longer-wavelength emission band appears. In the excited state, the amino and hydroxyl groups become more conjugated with the aromatic π-system, resulting in a marked charge separation within the molecule. The large Stokes shift and broad emission suggest the presence of intramolecular proton transfer (IPT) between the amino and hydroxyl groups .
Among the neutral, monocationic, and monoanionic species, CDs preferentially include the neutral form due to the hydrophobic nature of their cavities . The red or blue shifts observed in the ground state in CD/pH solutions further indicate IPT involvement. Because the inclusion of 2AP depends on both the CD cavity size and pH, the absorption and emission spectra vary with pH and CD type. The spectral changes observed with CD addition at different pH values suggest that IPT interactions play a major role in the inclusion complexation. At higher α-CD and β-CD concentrations, differences in emission maxima and spectral profiles of 2AP at pH ~3, pH ~7, and pH ~11 confirm the formation of distinct inclusion complexes .
3.2. Intramolecular Proton Transfer Emission (IPT)
At pH ~7, 2AP exhibits a single broad emission in solvents but dual emission in both α-CD and β-CD. The dual emission, which is characteristic of IPT is clearly observed. Compared to pH ~3, the IPT emission is stronger at pH ~7 and pH ~11. This behavior may be attributed to variations in polarity, viscosity, and CD cavity size, which play a significant role in influencing the IPT behavior of 2AP. To confirm the dual emission of 2AP in the presence of CDs, solvent-induced changes in the absorption and emission spectra were also studied for this molecule in selected solvents. Both short-wavelength (SW) and long-wavelength (LW) emission intensities increased with increasing CD concentration and pH . The emission intensities of both SW and LW bands also increased with excitation wavelength (λexci ~260-300 nm). These results suggest the presence of IPT in the 2AP molecule, similar to that observed in aminobenzoic acid and hydroxy derivatives . The appearance of the LW emission at higher CD concentrations clearly indicates the presence of IPT emission in the 2AP molecule.
A question may arise as to why the 2AP molecule exhibits different IPT emission intensities at pH ~3, pH ~7, and pH ~11? It is well known that the strength of interaction depends on the polarity, CD cavity size, and guest molecular size in the inclusion complex. This implies that the interaction is highly sensitive to the relative sizes of the guest and the CD. The interaction between the amino/hydroxy group and the phenyl ring with the CD cavity plays an important role, as these polar groups can have maximum contact with the internal surface of the CD cavity. Further, the increased absorbance in CD solutions suggests that the aromatic ring is encapsulated within the non-polar region of the CD cavity.
At pH ~3 and pH ~11, protonation and deprotonation occur at the amino and hydroxy groups, respectively, leading to variations in the orientation of the 2AP molecule inside the CD cavity. Since the interior of the CD cavity is nonpolar, the neutral amino/hydroxy groups may penetrate more deeply into the cavity compared to their protonated (NH₃⁺) or deprotonated (hydroxyl anion) forms. Additionally, the amino group and the hydroxyl anion may interact with the CD - hydroxyl groups. Inside the CD cavity, the guest molecule experiences a much less polar environment, which enhances the IPT band. The geometrical constraint imposed by the α-CD cavity restricts the free rotation of the amino or hydroxy group, hindering IPT-state formation and thereby enhancing normal emission .
3.3. Excited Singlet State Lifetimes
The fluorescence lifetimes of 2AP in aqueous and CD media were determined from decay curves and are listed in Table 1. The lifetimes of the inclusion complexes were longer than that of free 2AP. The lifetime of 2AP increased in the following order: water < α-CD < β-CD. This trend indicates that the β-CD: 2AP complex is more stable than the α-CD: 2AP complex. The increase in lifetime with increasing CD concentration is attributed to the encapsulation of the molecule within the CD cavity. These results demonstrate the greater complexation ability of β-CD, indicating higher encapsulation efficiency.
3.4. Molecular Modelling
The ground-state geometries of 2AP, α-CD, β-CD, and their inclusion complexes were optimized using the PM3 method (Figure 3). The HOMO-LUMO energies, thermodynamic parameters (energy, enthalpy, entropy, and free energy), dipole moments, zero-point vibrational energies, and Mulliken charge values are summarized in Table 2. Both CDs have the same height (7.8 Å). The internal cavity diameter of α-CD is 4.7-5.3 Å, and that of β-CD is 6.0-6.5 Å; the external diameters are 8.8 Å and 10.8 Å, respectively.
In 2AP, the vertical and horizontal distances between the NH₂ and OH groups are 6.72 Å and 5.44 Å, respectively (Figure 3). Both these dimensions are smaller than the β-CD cavity size, hence 2AP molecule freely entrapped in this CD cavity, however, the 2AP molecule is tightly encapsulate in the α-CD or 2AP molecule cannot be completely encapsulated within the α-CD cavity. These observations indicate that 2AP forms different types of inclusion complexes with α-CD and β-CD.
All thermodynamic parameters of the CD: 2AP complexes differ significantly from those of the isolated guest molecule, confirming complex formation. The negative values of energy, enthalpy, and Gibbs free energy indicate that the inclusion processes are both energetically and enthalpically favorable. The binding energies (ΔE) of the inclusion complexes are higher than that of the isolated 2AP molecule, suggesting enhanced stability of the complexes.
Table 2. Binding energies and HOMO, LUMO energy of 2-aminophenol (2AP) with α-CD and β-CD by PM6 method.

Properties

2AP

α-CD

β-CD

2AP-α-CD A

2AP-α-CD B

2AP-β-CD A

2AP-β-CD B

EHOMO (eV)

-8.93

-10.05

-9.99

-8.93

-9.20

-8.55

-8.91

ELUMO (eV)

0.02

0.14

0.12

0.05

-0.14

0.20

0.13

EHOMO - ELUMO (eV)

-8.95

-10.19

-10.11

-8.99

-9.05

-8.76

-9.04

µ (eV)

-4.45

-4.95

-4.93

-4.44

-4.67

-4.17

-4.39

χ (eV)

4.45

4.95

4.93

4.44

4.67

4.17

4.39

η (eV)

4.47

5.09

5.05

4.49

4.53

4.37

4.52

S (eV)

2.23

2.54

2.52

2.24

2.26

2.18

2.26

ω (eV)

4.43

4.81

4.81

4.39

4.81

3.97

4.26

Dipole (D)

2.55

9.92

10.52

8.97

7.40

9.51

5.52

E*

-20.32

-1353.95

-1577.74

-1387.13

-1384.81

-1609.83

-1609.15

ΔE*

-12.85

-10.53

-11.76

-11.08

G*

50.03

510.13

606.37

578.29

577.62

672.66

672.29

ΔG*

18.11

17.45

15.88

16.26

H*

74.50

599.76

704.03

671.85

672.34

776.56

776.60

ΔH*

-2.41

-1.91

-1.93

-1.98

S**

82.07

300.59

327.58

313.80

317.70

348.46

349.86

ΔS**

-68.86

-64.96

-59.79

-61.19

* kcal mol-1), ** kcal/mol-Kelvin
Figure 3. PM3 optimized structures of (a, b) 2AP (c, d) HOMO, LUMO of 2AP.
3.5. Nanomaterials Studies
3.5.1. Scanning Electron Microscope
The copper nano, 2AP, Ag: 2AP: α-CD, and Ag: 2AP: β-CD nanomaterials were investigated by SEM (Figure 4). The SEM images clearly show that Ag nanoparticles are present in a clustered spherical form, 2AP appears in a rod-like shape, Ag: 2AP: α-CD exhibits a micro-rod morphology, and Ag: 2AP: β-CD displays a rod-shaped structure. SEM-EDX data confirm the presence of approximately 5.5% silver nanoparticles in the nanomaterials. These morphological differences support the formation of the Ag: 2AP: CD nanomaterials.
Figure 4. SEM images for a) Ag nano, b) 2AP, c) Ag: 2AP: α-CD and d) Ag: 2AP: β-CD.
3.5.2. Infrared Spectral Studies
FTIR spectra was used to analyze Ag nano, 2AP, Ag: 2AP: α-CD, and Ag: 2AP: β-CD nanomaterials . In the isolated 2AP molecule, the N-H, O-H, and C-H stretching frequencies appear at 3361, 3296, and 3043 cm-1, respectively. The N-H bending and aromatic ring C=C stretching vibrations are observed at 1699, 1606, and 1509 cm-1, respectively. The aromatic C-C, C-OH, and C-O stretching vibrations occur at 1468, 1304, and 1180 cm-1, respectively. The C-O-C and C-N stretching bands appear at 1259, 1180, and 1360 cm-1, respectively, while the O-H out-of-plane bending vibration is seen at 696 and 690 cm-1 in the 2AP molecule.
In the nanomaterials, the NH₂ and OH stretching bands appear at 3230 and 2912 cm-1, respectively, while the aromatic C=C and C-O stretching vibrations are observed at 1608 and 1336 cm-1. The aromatic ring deformation band appears at 584 cm-1. A noticeable decrease in intensity in the spectra of nano Ag: 2AP: CD complexes suggests that the 2AP molecule strongly interacts with the silver nanoparticles.
3.5.3. Differential Scanning Colorimeter
The DSC profiles of α-CD, β-CD, 2AP and the corresponding inclusion complexes are also analysed. The DSC curves of α-CD shows three endothermic peak at 79.2 ºC, 109.1 ºC and 137.5°C and β-CD shows a broad endothermic peak at 128.6 ºC and, these endothermic peaks are attributed to crystal water loss from CDs. The melting and boiling point of 2AP shows a sharp peak at 120 and 164 ºC respectively. A broader endothermic effect was recorded for α-CD, β-CD and respective inclusion complexes as a consequence of water loss from the CDs. The DSC thermogram of Ag-2AP-CD complexes did not show peaks corresponding to pure 2AP and CD, instead new peaks appeared at 274 ºC and 291 ºC for Ag: 2AP: α-CD and Ag: 2AP: β-CD respectively.
3.5.4. X RD Spectral Studies
The crystallinity of all nanoparticles was determined from their XRD patterns . Based on JCPDS data, the mineral name (3C) and face-centered cubic (FCC) structure were identified. The standard Ag FCC structure corresponds to JCPDS card number 87-0717, with hkl values at 111, 200, 220, and 311Pure Ag nano had strong powder peaks at 38.11º, 44.30º, 64.45º, and 77.40º. These peaks correspond to the reflection of the face centered cubic structure of metallic silver. The XRD pattern of α-CD shows a crystalline nature approximately at 11.94°, 14.11°, 21.77° and 𝛽-CD shows 11.49°, 17.58°, however, the intensity and presence of these can vary depending on the sample and preparation. 2AP shows orthorhombic system and the peaks appears at 7.253º, 7.833º, and 19.641º. The XRD pattern of Ag/2AP: β-CD nanomaterials shown that a clear distinct diffraction patterns at 12.13°, 19.26°, 27.25°, 31.76°, 37.63°, 45.86°, 65.04°, and 76.75°. The variation in the peak intensities of the nanomaterials and the pure components suggest that new nanomaterials are formed.
4. Conclusion
The absorption and emission spectral maxima of 2-aminophenol (2AP) in different concentrations of α-cyclodextrin (α-CD) and β-cyclodextrin (β-CD) at pH ~3, pH ~7, and pH ~11 were investigated. In both α-CD and β-CD solutions, distinct absorption and emission shifts were observed at all pH conditions. In all solvents, the absorption and emission maxima of 2AP were similar to those of 2-anisidine. 2AP exhibited a single broad emission band in the solvents, while a dual emission was observed in the CD solutions, indicating the presence of intramolecular proton transfer (IPT) in the 2AP molecule. The geometrical restriction of the α-CD cavity likely limits the free rotation of the amino and hydroxyl groups, thereby enhancing the intensity of the IPT emission. The lifetimes of the inclusion complexes were longer than that of the free 2AP molecule. The calculated HOMO-LUMO energy gap, total energy, free energy, enthalpy, entropy, dipole moment, and zero-point vibrational energy of the CD: 2AP complex differed significantly from those of the isolated guest molecule, confirming the formation of an inclusion complex. SEM images and FTIR, XRD spectra clearly reveal the differences among Ag nanoparticles, 2AP, and the Ag: 2AP: CD nanomaterials. SEM-EDX data confirm the presence of approximately 5.5% silver nanoparticles in the nanomaterials.
Abbreviations

FTIR

Fourier Transform Infrared Spectroscopy

DTA

Differential Thermal Analysis

XRD

X-ray Diffraction

SEM

Scanning Electron Microscopy

HOMO

Highest Occupied Molecular Orbital

LUMO

Lowest Unoccupied Molecular Orbital

2AP

2-aminophenol

Ag NPs

Silver Nanoparticles

α-CD

Alpha Cyclodextrin

β-CD

Beta Cyclodextrin

PM3

Parametric Method 3

ΔE

Iinternal Energy Change

ΔH

Enthalphy Change

ΔG

Free Energy Change

ΔS

Entropy Change

Author Contributions
Narayanasamy Rajendiran: Supervision, Resources, Methodology, Software, Writing – original draft, Writing – review & editing
Ayyadurai Mani: Formal Analysis, Investigation
Palanichamy Ramasamy: Data curation
Sengamalai Senthilmurugan: Validation
Conflicts of Interest
The authors declare no conflict of interest.
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    Rajendiran, N., Mani, A., Ramasamy, P., Senthilmurugan, S. (2026). Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes. American Journal of Physical Chemistry, 15(2), 22-32. https://doi.org/10.11648/j.ajpc.20261502.11

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    Rajendiran, N.; Mani, A.; Ramasamy, P.; Senthilmurugan, S. Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes. Am. J. Phys. Chem. 2026, 15(2), 22-32. doi: 10.11648/j.ajpc.20261502.11

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    AMA Style

    Rajendiran N, Mani A, Ramasamy P, Senthilmurugan S. Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes. Am J Phys Chem. 2026;15(2):22-32. doi: 10.11648/j.ajpc.20261502.11

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  • @article{10.11648/j.ajpc.20261502.11,
      author = {Narayanasamy Rajendiran and Ayyadurai Mani and Palanichamy Ramasamy and Sengamalai Senthilmurugan},
      title = {Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes},
      journal = {American Journal of Physical Chemistry},
      volume = {15},
      number = {2},
      pages = {22-32},
      doi = {10.11648/j.ajpc.20261502.11},
      url = {https://doi.org/10.11648/j.ajpc.20261502.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajpc.20261502.11},
      abstract = {The spectral characteristics of 2-aminophenol (2AP) in various solvents, α-cyclodextrin (α-CD) and β-cyclodextrin (β-CD) at pH~3, pH~7, and pH~11, were investigated using UV-visible, fluorescence, time-resolved fluorescence measurements, and PM3 computational methods. The Ag: 2AP: CD nanomaterials were synthesized and characterized by SEM, FTIR, and XRD techniques. In all the pH conditions, 2AP exhibited distinct absorption and emission shifts upon complexation with α-CD and β-CD. In various solvents, the absorption and emission maxima of 2AP were similar to those of 2-anisidine. 2AP showed a single broad emission band in all solvents, whereas dual emission observed in CD solutions indicates the presence of an intramolecular proton transfer (IPT) process in the 2AP molecule. The lifetimes of the inclusion complexes were longer than that of the free 2AP molecule. The geometrical restriction of the α-CD cavity likely limits the free rotation of the amino and hydroxyl groups, thereby enhancing the intensity of the IPT emission. The calculated HOMO-LUMO energy gap, total energy, free energy, enthalpy, entropy, dipole moment, and zero-point vibrational energy of the CD: 2AP complex differed significantly from those of the isolated 2AP, α-CD and β-CD molecules, and both the vertical and horizontal bond lengths between the amino and hydroxy groups are smaller than the β-CD cavity size confirming the formation of an inclusion complex. SEM-EDX data confirmed the presence of 5.5% silver in the nanomaterials.},
     year = {2026}
    }
    

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  • TY  - JOUR
    T1  - Synthesis of Silver-2-Aminophenol-Cyclodextrin Nanomaterials and pH Dependent of 2-Aminophenol-Cyclodextrin Inclusion Complexes
    AU  - Narayanasamy Rajendiran
    AU  - Ayyadurai Mani
    AU  - Palanichamy Ramasamy
    AU  - Sengamalai Senthilmurugan
    Y1  - 2026/04/10
    PY  - 2026
    N1  - https://doi.org/10.11648/j.ajpc.20261502.11
    DO  - 10.11648/j.ajpc.20261502.11
    T2  - American Journal of Physical Chemistry
    JF  - American Journal of Physical Chemistry
    JO  - American Journal of Physical Chemistry
    SP  - 22
    EP  - 32
    PB  - Science Publishing Group
    SN  - 2327-2449
    UR  - https://doi.org/10.11648/j.ajpc.20261502.11
    AB  - The spectral characteristics of 2-aminophenol (2AP) in various solvents, α-cyclodextrin (α-CD) and β-cyclodextrin (β-CD) at pH~3, pH~7, and pH~11, were investigated using UV-visible, fluorescence, time-resolved fluorescence measurements, and PM3 computational methods. The Ag: 2AP: CD nanomaterials were synthesized and characterized by SEM, FTIR, and XRD techniques. In all the pH conditions, 2AP exhibited distinct absorption and emission shifts upon complexation with α-CD and β-CD. In various solvents, the absorption and emission maxima of 2AP were similar to those of 2-anisidine. 2AP showed a single broad emission band in all solvents, whereas dual emission observed in CD solutions indicates the presence of an intramolecular proton transfer (IPT) process in the 2AP molecule. The lifetimes of the inclusion complexes were longer than that of the free 2AP molecule. The geometrical restriction of the α-CD cavity likely limits the free rotation of the amino and hydroxyl groups, thereby enhancing the intensity of the IPT emission. The calculated HOMO-LUMO energy gap, total energy, free energy, enthalpy, entropy, dipole moment, and zero-point vibrational energy of the CD: 2AP complex differed significantly from those of the isolated 2AP, α-CD and β-CD molecules, and both the vertical and horizontal bond lengths between the amino and hydroxy groups are smaller than the β-CD cavity size confirming the formation of an inclusion complex. SEM-EDX data confirmed the presence of 5.5% silver in the nanomaterials.
    VL  - 15
    IS  - 2
    ER  - 

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    1. 1. Introduction
    2. 2. Materials and Methods
    3. 3. Result and Discussion
    4. 4. Conclusion
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