Manik Das1, Somali Mukherjee2, Paula Brandao3, Saikat Kumar Seth4, Santanab Giri5, Soumya Sundar Mati6, Bidhan Chandra Samanta7, Soumik Laha8, Tithi Maity1. 1. Department of Chemistry, P. K. College, Contai, Purba Medinipur, West Bengal 721404, India. 2. Department of Chemistry, University of Calcutta, 92, A. P. C. Road, Kolkata 700009, India. 3. Departamento de Química/CICEC, Universidade de Aveiro, Aveiro, 3810-193, Portugal. 4. Department of Physics, Jadavpur University, Kolkata 700032, India. 5. Department of Chemistry, HIT, Haldia 721657, India. 6. Department of Chemistry, Government General Degree College, Keshiary 721135, West Bengal India. 7. Department of Chemistry, Mugberia Gangadhar Mahavidyalaya, Purba Medinipur 721425, West Bengal, India. 8. IICB, Kolkata 700032, India.
Abstract
Two fluorescence active bromoaniline-based Schiff base chemosensors, namely, (E)-4-bromo-2-(((4-bromophenyl)imino)methyl)phenol (HL1 ) and (E)-2-(((4-bromophenyl)imino)methyl)phenol (HL2 ), have been employed for the selective and notable detection of Cu2+ and Zn2+ ions, respectively, with the simultaneous formation of two new metal complexes [Cu(L1)2] (1) and [Zn(L2)2] (2). X-ray single crystal analyses indicate that complexes 1 and 2 are tetra-coordinated systems with substantial CH...π/π...π stacking interactions in the solid-state crystal structures. These two complexes are exploited for the next step detection of Al3+ and Hg2+ where complex 2 exhibits impressive results via turn-off fluorescence quenching in (DMSO/H2O) HEPES buffer medium. The sensing phenomena are optimized by UV-vis spectral analyses as well as theoretical calculations (density functional theory and time-dependent density functional theory). The combined detection phenomena of the ligand (HL2 ) and complex 2 are exclusively utilized for the first time to construct a molecular memory device, intensifying their multisensoric properties. Furthermore, the DNA- and human serum albumin (HSA)-binding efficacies of these two complexes are examined by adopting electronic and fluorometric titration methods. Complex 2 shows a higher DNA-binding ability in comparison with complex 1, whereas in the case of HSA, the reverse situation is observed. Finally, the binding modes of both the complexes with DNA and HSA have been investigated through molecular docking studies, suggesting good agreement with the experimental results.
Two fluorescence active bromoaniline-based Schiff basechemosensors, namely, (E)-4-bromo-2-(((4-bromophenyl)imino)methyl)phenol (HL1 ) and (E)-2-(((4-bromophenyl)imino)methyl)phenol (HL2 ), have been employed for the selective and notable detection of Cu2+ and Zn2+ ions, respectively, with the simultaneous formation of two new metalcomplexes [Cu(L1)2] (1) and [Zn(L2)2] (2). X-ray single crystal analyses indicate that complexes 1 and 2 are tetra-coordinated systems with substantialCH...π/π...π stacking interactions in the solid-state crystal structures. These two complexes are exploited for the next step detection of Al3+ and Hg2+ where complex 2 exhibits impressive results via turn-off fluorescence quenching in (DMSO/H2O) HEPES buffer medium. The sensing phenomena are optimized by UV-vis spectral analyses as well as theoreticalcalculations (density functional theory and time-dependent density functional theory). The combined detection phenomena of the ligand (HL2 ) and complex 2 are exclusively utilized for the first time to construct a molecular memory device, intensifying their multisensoric properties. Furthermore, the DNA- and humanserum albumin (HSA)-binding efficacies of these two complexes are examined by adopting electronic and fluorometric titration methods. Complex 2 shows a higher DNA-binding ability in comparison with complex 1, whereas in the case of HSA, the reverse situation is observed. Finally, the binding modes of both the complexes with DNA and HSA have been investigated through molecular docking studies, suggesting good agreement with the experimental results.
Fluorescence-based
techniques have gained great momentum in modern-day
research for efficient and ultrafast detection of metal ions having
physiological and environmental pertinences.[1−4] The upsurge of research efforts
for the construction of fluorescence-based chemosensors could be attributed
to their better applicability for the selective and specific recognition
of analytes compared to other analytical methods such as cyclic voltametry,[5] inductively coupled plasma mass spectroscopy,[6] inductively coupled plasma-atomic emission spectroscopy,[7] EPR spectral studies, etc. that are mostly expensive,
single-analyte-driven scrupulous systems. The implementation of metal–organiccomplexes as a possible chemosensory platform attracts much attention
to this end due to their ease of synthesis, large choice of building
precursors, diverse structural features, and most importantly potential
luminescence properties.[8−10] However, to endow a chemosensor
with all such prerequisites, the organic skeleton should be rationally
engineered and synthesized, which demands extensive future studies.Aluminum and mercury are two well-known metals where the former
is largely used in the cosmetics industry, pharmaceutical industry,
food and packaging industry, etc., and the latter is one of the large-scale
heavy metalcontaminants that are discharged with industrial effluents.[11−13] The abnormal accumulation of both these metals may cause several
life-threatening diseases such as Alzheimer’s disease, Minamata
disease, Parkinson’s disease, Hunter–Russel Syndrome,
etc.[14−18] Abnormal chromosomal disorder is also a malicious effect of HgII poisoning, leading to long-term genetic deformities. Hence,
the detection of these two metals is an utmost requirement. However,
due to the inconvenience of the traditional analytical methods, finding
a suitable recognition tool seems more challenging to chemists. According
to our previous discussion, fluorescence spectroscopic techniques
could be an effective alternative, involving the synthesis of fluorescence
active sensors appropriately designed for the recognition of metal
ions of interest. In fact, this process could also be advantageous
for the detection of other physiologically important metals such as
Cu, Zn, etc.[19−27] These two metals play an indispensible role in numerous biological
processes.[28−34] Unfortunately, the industrial revolution has led to critical environmental
problems, which introduce these essential elements in a new perspective
as “pollutants”. The excess release of CuII and ZnII ions in the soil and ground and surface watercauses severe risk to the ecosystem at its current levels of exposure.[35,36] Thus, the detection of these two biologically and environmentally
related metal ions is as an urgent need.Apart from metal sensing,
the fluorometric detection platform can
also be utilized to study the interactions of metal–organiccomplexes with primary macromolecules present within living systems.[37] This investigation is not only important to
establish a relationship between the two disciplines, chemistry and
biology, but at the same time, it is highly interesting in pharmacology
to realize the probable interaction of drug molecules with system
proteins. Designing metalcomplexes having structural and compositional
variations and investigation of their binding efficacy with DNA are
proved to be advantageous for developing effective cancer therapeutic
drugs.[38−40] The determination of different binding modes of DNA
with studied complexes also helps in the systematic modulation of
the drug molecules to have better efficacy. On the other hand, humanserum albumin (HSA), the most abundant circulating protein present
in human blood plasma, binds and transports therapeutic agents, acting
as a potential drug carriage system.[41] The
HSA–drug interactions generally govern the extent of transportation,
distribution, toxic side effects, and finally excretion of drug molecules
in the human body.[42,43] Hence, the exploration of the
interaction of metal-based pharmaceuticals with DNA/HSA is still under
investigation.Addressing all these requirements, primarily,
we have developed
two fluorescence active Schiff base probes HL and HL by coupling of bromoaniline with
salicylaldehyde and 5-bromo salicylaldehyde, respectively (Scheme ). The ligands HL and HL induce remarkable
UV colorimetric and fluorometricchanges, specifically for Cu2+ and Zn2+ among different metalcations, with
the crystallization of two new complexes [Cu(L1)2] (1) and [Zn(L2)2] (2), respectively (Scheme ). The strong emissive nature of complex 2 is
further utilized for the specific and rapid detection of Al3+ and Hg2+ with a low detection limit. Density functional
theory (DFT) and time-dependent density functional theory (TD-DFT)
calculations reveal the probability of formation of a bimetalliccomplex
between Al3+ and complex 2 governing such
efficient sensing phenomena. Considering the two-step detection achieved
by the successive selection of HL and its
complex (2), a molecular memory device is formulated.
Finally, the binding efficacies of both the complexes with ctDNA and
HSA are studied thoroughly. The binding modes as well as the extent
of binding of both the complexes are revealed via the help of combined
experimental and theoretical techniques involving electronic and fluorescence
spectral titration, circular dichroism (CD) analysis, and molecular docking studies.
Scheme 1
Synthesis of the
Ligands HL and HL and Complexes 1 and 2
Results and Discussion
Synthesis and General Characterization
Complexes 1 and 2 are synthesized by
reacting CuCl2 and ZnCl2 solution with HL and HL in respective
solvents and are subjected
to the following spectral analysis. The FT-IR spectral outcomes are
primarily assessed to get an initial idea of the structural skeleton.
The “C=N” stretching is observed in two cases
within 1630–1660 cm–1, suggesting the presence
of an imine bond. The sharp bands ranging from 1410 to 1430 cm–1 could be attributed to the skeleton benzene vibration
in both complexes (Figure S1 in the Supporting
Information). The electronic spectra of complexes 1 and 2 are recorded in DMSO medium (Figure S2 in the Supporting Information). The absorption bands arise
due to charge transfer transition in complexes 1 and 2 appearing at 337 nm and 401 nm, respectively. Unlike complex 2, the absorption band at 568 nm (visible region) for complex 1 is presumably due to the d–d transition. The 1HNMR (d6-DMSO at 25 °C) spectrum of complex 2 shows a signal for two imine protons at δ = 8.6 ppm,
whereas all of the aromatic protons appeared at δ = 7.2–7.5
as a multiplate.
Structure Description of Complexes
Complex 1 [Cu(L1)2]
Complex 1 is a mononuclear Cucomplex that crystallizes
in the monoclinic P21/c space group. The
asymmetric unit comprises one fully occupied L1 ligand
and a half occupied Cu2+ ion located over a crystallographic
inversion center. The centralmetal ion crystallizes in a square planar
geometry in which the four positions are coordinated with two iminenitrogen and two phenoxo oxygen arising from the ligand backbone,
resulting in six-membered chelate rings (Figure a). The obtained O1–Cu1–O1
and N1–Cu1–N1 bond angles are equal to 180°, indicating
the formation of a perfect planar environment around the central atom.
Structural analysis indicates that the phenolic −OH residue
of the ligand undergoes deprotonation during crystallization, producing
phenoxo ions, which further bears the counter charge, maintaining
the electroneutrality of the complex. The crystal packing presumably
takes place, favoring CH...π interactions [CH...centroid 2.874
Å] between the adjacent structural units (Figure b). The observed Cu1–N1 and Cu1–O1
bond lengths are 2.011 and 1.888 Å, respectively. The other relevant
bond lengths and bond angles are tabulated in Table S1 in the Supporting Information.
Figure 1
(a) ORTEP view of complex 1 with 40% ellipsoid probability
(H atoms are not shown for clarity) and (b) crystal packing favoring
CH...π interactions.
(a) ORTEP view of complex 1 with 40% ellipsoid probability
(H atoms are not shown for clarity) and (b) crystal packing favoring
CH...π interactions.
Complex 2 [Zn(L2)2]
Complex 2 crystallizes in the monoclinicC2/c space group with the
centralmetal ion located on a twofold crystallographic axis with
the center of symmetry passing through it. Thus, the asymmetric unit
contains one fully occupied L2 ligand and one Zn2+center situated over a special position (Figure ), as mentioned above. The immediate environment
around the centralmetal is a distorted tetrahedral where the four
positions of the tetrahedron is coordinated with two iminenitrogen
and two phenoxo oxygen arising from the ligand skeleton. Similar to
the previous complex, here also the ligand undergoes deprotonation
during crystallization. The contagious units are stacked with each
other through extensive π....π stacking interactions [centroid...centroid
3.734 Å]. The Zn1–N1 and Zn1–O1 bond distances
are found to be 2.022 and 1.898 Å, respectively. The other required
bond lengths and the bond angles are provided in Table S1 in the Supporting Information.
Figure 2
(a) ORTEP
view with 40% ellipsoid probability (H atoms
are not shown for clarity), (b) polyhedral view around the central
atom, and (c) crystal assembly.
(a) ORTEP
view with 40% ellipsoid probability (H atoms
are not shown for clarity), (b) polyhedral view around the central
atom, and (c) crystal assembly.
Fluorescence and UV–vis Spectroscopic Signature of Ligand
HL1 and HL2
As both the prepared ligands
exhibit potential luminescence features, we commence our work by investigating
the sensing power of HL and HL toward various cations such as Co2+, Fe3+, Na+, Cu2+, Ni2+, Cd2+, Mn2+, Zn2+, and Hg2+ in
DMSO/H2O (9:1) HEPES buffer medium (pH 7.4). Under a UV
lamp (λ = 365 nm), a prominent change in the luminescence of HL and HL was visualized
by the naked eye via the selective addition of Cu2+ and
Zn2+, respectively. No such significant changes were observed
for other analytes, which instigated us to investigate the fluorescence
spectralchanges of the ligand via the addition of the said metal
ions (Figure and Figure S3 in the Supporting Information).
Figure 3
Color changes
visible by the naked eye after addition of (a) Cu2+ in
the HL and (b) Zn2+ in HL ligand; fluorescence emission spectral
change of (c) HL ligand (4 × 10–7 M) at 485 nm in the presence of different cations,
showing considerable fluorescence quenching for Cu2+ ions
and (d) HL ligand (4 ×
10–7 M) at 471 nm in the presence of different cations,
showing considerable fluorescence quenching for Cu2+ ions
in 9:1 (DMSO/H2O) HEPES buffer (pH = 7.4) solution.
Color changes
visible by the naked eye after addition of (a) Cu2+ in
the HL and (b) Zn2+ in HL ligand; fluorescence emission spectralchange of (c) HL ligand (4 × 10–7 M) at 485 nm in the presence of different cations,
showing considerable fluorescence quenching for Cu2+ ions
and (d) HL ligand (4 ×
10–7 M) at 471 nm in the presence of different cations,
showing considerable fluorescence quenching for Cu2+ ions
in 9:1 (DMSO/H2O) HEPES buffer (pH = 7.4) solution.The ligands HL and HL showed emission maxima at 485 and 471 nm, respectively.
To
obtain a quantitative appraisal uniting the change in the fluorescence
intensity of HL and HL with the added amount of Cu2+ and Zn2+, detailed
fluorometric titration experiments were conducted in two cases, and
the titration results are shown in Figure . The figure clearly depicts that after incremental
addition of Cu2+ to HL, the fluorescence
intensity, centered at 485 nm, gradually decreases with a blue shift
of 6 nm (Figure S3 in the Supporting Information),
whereas a considerable enhancement in the fluorescence intensity,
centered at 471 nm, was observed when Zn2+ was added to HL solution (red shift 5 nm). The quenching constant
for HL was determined to be 1.7 × 105 M–1 using the Stern–Volmer equation, F0/F = KSV[Q] +1; where F0 and F denote the emission intensity in the absence
and presence of the analyte, respectively, [Q] stands
for the concentration of the added analyte, and KSV refers to the quenching constant value (Figure S4 in the Supporting Information). The
limit of detection (LOD) was found to be 31.74 × 10–8 M and 39.8 × 10–8 M for HL to Cu2+ and to Zn2+, respectively,
based on LOD = K × σ/S, where K = 3, σ indicates the standard deviation
of the blank solution and S stands for the slope
of the calibration curves (Figure S5 in
the Supporting Information).
Figure 4
(a) HL upon incremental
addition of Cu2+ solution (0.5–10 × 10–7 M)
in (DMSO/H2O) HEPES buffer (pH = 7.4) solution (λex = 360 nm and λem = 485 nm). Inset: visual
color change observed with the addition of Cu2+ to HL solution under UV light (λ = 365 nm)
and (b) HL (3 × 10–7 M) upon incremental addition of Zn2+ solution (0.5–10
× 10–7 M) in (DMSO/H2O) HEPES buffer
(pH = 7.3) solution (λex = 360 nm, λem = 471 nm). Inset: visual color change observed after the addition
of Zn2+ to HL solution under UV
light (λ = 365 nm).
(a) HL upon incremental
addition of Cu2+ solution (0.5–10 × 10–7 M)
in (DMSO/H2O) HEPES buffer (pH = 7.4) solution (λex = 360 nm and λem = 485 nm). Inset: visualcolor change observed with the addition of Cu2+ to HL solution under UV light (λ = 365 nm)
and (b) HL (3 × 10–7 M) upon incremental addition of Zn2+ solution (0.5–10
× 10–7 M) in (DMSO/H2O) HEPES buffer
(pH = 7.3) solution (λex = 360 nm, λem = 471 nm). Inset: visualcolor change observed after the addition
of Zn2+ to HL solution under UV
light (λ = 365 nm).The remarkable quenching constant value for Cu2+–HL and significant enhancement of the fluorescence
intensity for Zn2+–HL along
with the shifting of spectral positions may be considered as the indication
of the complex formation as the ligands contain potential donor centers
that are able to form bonds with metalcores.[44] To investigate and to evaluate the binding constants for HL–Cu2+ and HL–Zn2+ adducts, the UV metric titration was performed
successively. The titration pictorial graph is depicted in Figure S6 in the Supporting Information. The
stability of HL and HL in DMSO/water (9:1) solvent at a fixed pH value (7.4) was confirmed
by means of a time-scan UV–vis experiment (Figure S7, Supporting Information). At the same time, the
stability of the two ligands are also examined at different pH values
and is shown in Figure S7, which justifies
accomplishing the whole study at the fixed pH 7.4. After the addition
of incrementalconcentration of metal ions to ligands, the absorbance
at 353 and 339 nm for HL and HL gradually decreases along with the formation of two
isosbestic points at 382 and 371 nm, as expected, indicating the generation
of single species in HL–Cu2+ solution and HL–Zn2+ solution.
The calculated binding constants for the HL–Cu2+ ion and HL–Zn2+ ion adducts are 1.019 × 105 M–1 and 4.59 × 105 M–1, respectively,
indicating complex formation in two cases. According to the supposition,
we were able to isolate two single crystals and characterize them
accordingly, as we have mentioned in the previous section.
Response
of Complex 2 toward Al3+ and
Hg2+ by Fluorescence and UV–vis Spectroscopy
Among the two complexes, complex 2 possessed a potential
luminescent character, as observed from the fluorescence responses.
It displays a strong emission at 471 nm upon excitation with 360 nm
light in DMSO/H2O (9:1) medium at pH 7.4. Thus, complex 2 can be reutilized for the second-step detection procedure.
Keeping this point in mind, we further exploited complex 2 for the effective detection of metal ions where it showed the selective
recognition of Al3+ and Hg2+ among all (Figure S8 in the Supporting Information). The
fluorometric titration profile of complex 2 was recorded
upon incremental addition of Al3+ and Hg2+ (5–100
μM) solutions to a fixed concentration of complex 2 in DMSO/H2O (9:1) HEPES buffer solution at pH 7.4 (Figure ). In both the cases,
the fluorescence intensity rapidly diminishes with the blue shift
of 13 nm and 22 nm, respectively. The quenching constant values (KSV) are found to be 1.78 × 105 M–1 and 1.19 × 104 M–1 using the Stern–Volmer equation, as mentioned previously
(Figure S9 in the Supporting Information).
The detection limits of complex 2 for Al3+ and Hg2+ ions are found to be 1.78 × 10–8 M and 2.29 × 10–8 M, respectively (Figure S10 in the Supporting Information). From
the quenching constants and detection limit values, it can be further
concluded that the sensing efficacy of complex 2 is higher
in the case of Al3+ than in that of Hg2+ ions.
The quenching constant values are very much comparable with other
Al3+ and Hg2+ sensing organic probes,[45,46] indicating the strong bonding association between the studied analytes
and complex 2.
Figure 5
Fluorescence spectral analyses of complex 2 in (DMSO/H2O) HEPES buffer solution (pH = 7.3)
(a) upon incremental addition
of Al3+ ions (λex = 360 nm and λem = 481 nm) and (b) upon incremental addition of Hg2+ ions (λex = 360 nm and λem = 481
nm). Inset: visual color change observed under UV light (λ =
365 nm) and UV–vis spectral change of complex 2 in DMSO/H2O HEPES buffer solution upon incremental addition
of (c) Al3+ and (d) Hg2+.
Fluorescence spectral analyses of complex 2 in (DMSO/H2O) HEPES buffer solution (pH = 7.3)
(a) upon incremental addition
of Al3+ ions (λex = 360 nm and λem = 481 nm) and (b) upon incremental addition of Hg2+ ions (λex = 360 nm and λem = 481
nm). Inset: visualcolor change observed under UV light (λ =
365 nm) and UV–vis spectralchange of complex 2 in DMSO/H2OHEPES buffer solution upon incremental addition
of (c) Al3+ and (d) Hg2+.This fact is further substantiated by UV–vis spectral titration
via the evaluation of the respective host–guest binding constants
values. The absorbance is recorded after individual addition of Al3+ and Hg2+ (5–100 μM) to complex 2 in DMSO/H2OHEPES buffer solution at pH 7.4 (Figure ). As expected, the
peak at 395 nm of free complex 2 gradually decreases
and two new bands at 339 and 348 nm appeared after the addition of
Al3+ and Hg2+, respectively. An isosbestic point
at 360 and 375 nm, respectively, for Al3+ and Hg2+ appeared on the titration curve, indicating the existence of equilibrium,
which further indicates the conversion of the free chemosensor to
its bimetalcomplexes. The binding constants for complex 2 to Al3+ and complex 2 to the Hg2+ adduct are found to be 1.5 × 106 M–1 and 5.5 × 105 M–1, respectively.
Due to the high binding constant value in Al3+ sensing,
DFT studies and molecular advanced logic gate formation are performed
for Al3+ sensing.
DFT Calculations
The lack of supporting
experimental
evidence regarding the formation of the Zn/Al bimetalcomplex, after
the detection of Al3+ by complex 2, forces
us to perform structure optimization with the help of DFT calculations.
Since we have the crystal structure of complex 2, we
again optimized the same in the B3LYP level of theory with SDD as
a basis set in the gas phase. We observed that this basis set reproduces
the geometrical parameters quite well. Hence, we have modeled the
complex 2–Al3+ adduct and optimized
with the identical level of theory and basis set to obtain the ground-state
geometry. The polarizable continuum model (PCM) embedded in G09w has
been used to create the solvent environment. Furthermore, it has been
observed that CAM-B3LYP, which has the combination of the hybrid qualities
of B3LYP and the long-range correction, can elucidate the UV–vis
spectral properties efficiently.[47,48] The geometry
of the possible binding mode of complex 2 with Al3+ is shown in Scheme . The scheme depicts that after the detection of Al3+, a bimetal is formed where the Al3+center occupies a
distorted octahedral atmosphere. An experimentally performed UV–vis
spectral titration exhibits a gradual decrease in the absorption maxima,
centered at 394 nm, with the formation of a new band at 339 nm after
the incremental addition of Al3+ to complex 2.
Scheme 2
(a) Formation Mechanism and Structure of the Zn/Al Bimetal
Complex
and (b) Major HOMO–LUMO Transitions in the Zn Complex and the
Zn/Al Bimetal Complex
Theoreticalcalculations well supported the experimental results,
indicating a decrease in the absorption maxima at 370 nm with the
formation of a new band at 329 nm. From TD-DFT vertical excited-state
calculations, the strong highest occupied molecular orbital (HOMO)
(π type) to the lowest unoccupied molecular orbital (LUMO; π*
type) transition with an oscillator strength of f = 0.402 (329 nm) (Table ) is observed in the case of the Zn/Al bimetalcomplex, whereas
in complex 2, this energy gap is found to be slightly
lower, with an oscillator strength of f = 0.2907
(370 nm). The energy diagram is shown in Scheme . This lower HOMO–LUMO energy gap
in pure complex 2 in comparison with the bimetalcomplex
may be attributed to the formation of a bimetalcomplex after the
addition of Al3+ to complex 2.
Table 1
Major Transitions with Osc. Strength
and λex of Complex 2 and Complex 2–Al Adduct Calculateda
compound
wavelength
(nm)
osc. strength
major contributions
complex 2
359.37
0.2907
H-1- > LUMO (56%), HOMO-
> L + 1 (40%)
356.88
0.5296
H-1- > L + 1 (43%), HOMO-
> LUMO (54%)
296.44
0.1123
H-1- > L + 1 (29%), HOMO-
> LUMO (22%)
279.35
0.6025
H-3- > LUMO (36%), H-2-
> L + 1 (28%), H-1- > L + 1 (14%), HOMO- > LUMO (14%)
278.52
0.1389
H-3- > L + 1 (27%), H-2-
> LUMO (32%), H-1- > LUMO (14%), HOMO- > L + 1 (20%)
263.67
0.3036
H-9- > LUMO (12%), H-5-
> L + 1 (27%), H-4- > LUMO (24%), H-1- > L + 1 (12%)
complex 2–AlIII adduct(bimetal complex)
451.55
0.1393
HOMO(A)- > L + 6(A) (11%),
HOMO(A)- > L + 8(A) (49%)
367.72
0.3161
HOMO(A)- > L + 8(A) (12%),
HOMO(B)- > L + 1(B) (33%)
363.44
0.3904
HOMO(A)- > L + 1(A) (11%),
HOMO(A)- > L + 11(A) (12%), HOMO(B)- > L + 1(B) (22%)
Bimetal complex
using the CAM-B3LYP/SDD
level of theory in DMSO solvent
Bimetalcomplex
using the CAM-B3LYP/SDD
level of theory in DMSO solvent
Molecular Logic Gate
The photoluminescence experiment
of the receptor HL forced us to investigate
its behavior in numerous logic gates by successive addition of inputs
like various cations such as Zn2+ and Al3+ and
monitoring their photoluminescence changes at 471 nm as an output. HL has showed a much lower potential photoluminescence
intensity than complex 2. Hence, here we investigated
this experiment by considering the incremental photoluminescence properties
of complex 2 and its quenching of emission intensity
via sensing with Al3+. Inputs are contemplated as “1”
in their presence and “0” in their absence. The results
obtained by the instrument are considered as “1” when
the emission intensity crosses the certain emission barrier (25% maximum
of complex 2) and “0” when it failed to
cross the emission barrier (Figure a). In the initial stage, in the absence of any inputs,
no significant emission intensity was observed (ignoring the emission
intensity of HL) and is marked as “0”
(off state). Addition of input A (Zn2+) to probe HL resulted in an output signal at 471 nm, marked
as “1” (on state). With further addition of input B
(Al3+), no significant output signal is obtained. Again,
with the simultaneous addition of both inputs to probe HL, no output signal is observed and is expressed as
“0” (off state). It is observed that HL exhibits a high photoluminescence output signal in this experiment
with addition of input A. Now, we envision the consideration of “AND”
operation and “NOT” operation with input B. Thereafter,
it is noticed that the photoluminescence intensity decreases when
both the inputs were present in the probe, which suggests the off
state by examining the truth table. It can be concluded that this
investigation is related to an “INHIBIT” logic gate,
which consists of a specific arrangement of logical functions “AND”
and “NOT” (Figure b,c).
Figure 6
(a) Emission intensity variation graph of receptor and
complexes,
(b) truth table for advance-level molecular logic gates, and (c) circuit
diagram of logic construction.
(a) Emission intensity variation graph of receptor and
complexes,
(b) truth table for advance-level molecular logic gates, and (c) circuit
diagram of logicconstruction.
Molecular Memory Devices
All of the information gathered
from previous experimentation can further be congregated through successive
logiccircuits. These circuits hold the following response loop. In
this memory device, one input is taken as the “memory element”
by considering the output signal as an input. The memory device works
on a binary logic gate function: either it will be “0”
or “1,” alternatively the two crisp states. In the model
that we have introduced here for the advancement of a significant
mimicking of the memory element, we use Zn2+ and Al3+ designated as the set (S) and reset (R) inputs correspondingly and the photoluminescence was
recorded at 524 nm as the output signal (Figure a). When Zn2+ acts as an input
in this memory function, the device recognizes the binary state “1,”
while under the reset situation Al3+ acts as an input.
As a result, it is found that the device considered the binary state
“0” (Figure b). Hence, it can be concluded that we have successfully constructed
a consecutive logiccircuit on the basis of the “Write–Read–Erase–Read”
property. As a result, one can easily observe that by using the same
solution of the complex, the write–erase cycles can be repeated
many times without a significant decrease in the emission intensity.
In summary, this system can be properly utilized in the technological
field. Hence, molecular successive logic function circuits can be
designed to show a comparable behavior with the logic devices of conventional
semiconductors, and it can be expected that it can be a better technique
for the construction of molecular microprocessors of integrated circuits.
When Hg2+ is used instead of Al3+, the same
result will be obtained.
Figure 7
(a) Consecutive logic circuit of a memory unit
and (b) schematic
presentation of the reversible logic operation for the memory element
with write–read–erase–read properties.
(a) Consecutive logiccircuit of a memory unit
and (b) schematic
presentation of the reversible logic operation for the memory element
with write–read–erase–read properties.
DNA-Binding Studies
In this section,
the photophysical
properties of complex 2 along with the sensing efficacy
to different cations as a metalloreceptor have been discussed. Next,
we evaluate these complexes with respect to their DNA interaction
ability. Several spectroscopic techniques are used to establish the
binding potentiality of the complexes with ctDNA as well as to identify
the mode of interaction. Initially, the electronic absorption spectroscopic
technique has been adopted to determine the binding constant of the
ctDNA–complex moiety. The binding efficacy of complexes 1 and 2 with ctDNA was monitored using a UV spectrophotometer
with regular addition of ctDNA (10–100 and 10–100 μM
for complexes 1 and 2, respectively) in
a fixed concentration of every complex (60 μM for complexes 1 and 2). To eliminate the absorbance of DNA,
the total absorbance is recorded within the 300–400 nm region
to understand the interaction of complexes with ctDNA. The change
in the absorption of complexes 1 and 2 with
an addition of incrementalconcentration of ctDNA is shown in Figure S11 in the Supporting Information. The
absorption titration spectrum clearly indicates that complexes 1 and 2 show the absorption maxima at 374 and
335 nm, respectively, and after the addition of ctDNA, the absorption
maxima gradually decreases along with a blue shift of 2–5 nm.[49] The binding constant Kb of each complex is measured from the ratio of the slope to
the intercept in plots [DNA]/ε –
ε versus [DNA] using eq (Experimental
Section). The best fit of the experimental values for complexes 1 and 2 (using eq ) is also represented in the inset of Figure S11 in the Supporting Information. The binding constant
values of complexes 1 and 2 with ctDNA are
1.87 × 105 M–1 and 3.4 × 105 M–1, respectively, indicating a significant
binding potential of complex 2 in comparison with complex 1. The partial intercalation of complex 2 inside
the base pairs of DNA along with groove binding may be responsible
for its relatively higher binding affinity, whereas complex 1 only showed groove binding with ctDNA due to its more hindered
structure. This is elaborately discussed in the section molecular docking.
Ethidium Bromide (EB) Displacement
Study
The electronic
titration results clearly revealed the effective binding potentiality
of the complexes with the ctDNA. To get a clear idea about the nature
of bonding and also the binding power, EtBr displacement experiments
have been carried out.[50,51] Actually, ethidium bromide (EtBr
= 3,8-diamino-5-ethyl-6-phenyl phenanthridinium bromide) exhibits
strong orange fluorescence whenever it is exposed to ultraviolet radiation.
The luminescence intensity of EtBr increases up to 20-fold in the
presence of ctDNA due to the strong intercalation between the adjacent
base pair of the DNA double helix.[52] This
can be attributed to the fact that the planar phenanthridine ring
is ideally fitted in to the adjoining base pairs of the double helix.
After addition of the complex to the EtBr–DNA domain, the complex
displaces EtBr and as a result of which the fluorescence intensity
decreases. This is the main technique used in this displacement study.[50]Figure S12 in the
Supporting Information shows the emission spectra of the EtBr bonded
with ctDNA in the absence and presence of complexes 1 and 2. It is to be noted that the emission spectra
range between 500 and 700 nm with an excitation of 450 nm, and for
complexes 1 and 2, the emission maxima are
obtained at 618 and 623 nm, respectively. A remarkable decrease in
the emission intensities is observed upon addition of incrementalconcentration of complexes 1 and 2 ( 8–80
μM for complex 1 and 8–80 μM for complex 2) separately to the EB–DNA adduct. This observation
indicates that both the complexes have the ability to bind with ctDNA
by replacing the fluorescence active dye EtBr. The quenching parameters
were determined using the Stern–Volmer equation F0/F = Ksv[Q] + 1, as discussed in the previous section. The Ksv value can be calculated as the slope from
the plot of F0/F versus
[Q]. The quenching constants for complexes 1 and 2 are 6.17 × 104 M–1 and 1.12 × 105 M–1, respectively.Furthermore, the apparent DNA-binding constants
(Kapp) are measured using the equation KEtBr[EtBr] = Kapp[complex], where [complex] stands for the value at 50% decrease in
the fluorescence intensity of EtBr, KEtBr (1.24 × 107 M–1) represents the
DNA-binding constant of EtBr, and [EtBr] is the concentration of EtBr
(5 μM). The Kapp values are found
to be 0.37 × 105 M–1and 1.34 ×
105 M–1 for complexes 1 and 2, respectively. The quenching value and binding parameters
force us to draw a concluding remark regarding the greater interaction
of complex 2 with ctDNA than complex 1.
This is due to the fact that complex 2 interacts with
DNA through the minor groove in addition to partial intercalation,
and this is the main reason behind the higher binding constant of
complex 2 than complex 1.
DAPI Displacement
Study
To determine the concrete support
of minor groove-binding mode of the complexes with ctDNA, 4’,6-diamidino-2-phenylindole
dihydrochloride (DAPI) displacement assay is performed. DAPI is a
highly fluorescence active dye and a good minor binder to DNA.[53] In this study, actually the fluorescence intensity
changes are noted after the gradual addition of the complex to the
DAPI–DNA adduct. The displacement of DAPI from DNA–DAPI
adducts in the presence of a complex decreases the fluorescence intensity,
and this is the main approach used for this displacement study. Figure S13 in the Supporting Information shows
the emission spectralchange of the DAPI–DNA domain in the
absence and presence of complexes 1 and 2 (8–80 μM). It is to be noted that the emission spectra
range between 450 and 535 nm with an excitation of 390 nm. An exceptional
fluorescence quenching is observed after the addition of complex 1 to the DAPI–DNA adduct compared to the addition of
complex 2 to the DAPI–DNA adduct.Figure depicts a
comparison of the fluorescence quenching of the EB–DNA and
DAPI–DNA adduct after the addition of incrementalconcentration
of complexes 1 and 2. The quenching constants
measured using the Stern–Volmer equation for complexes 1 and 2 in the DAPI displacement study are 3.16
× 105 M–1 and 1.62 × 105 M–1, respectively. Based on the fluorescence
quenching bar diagram as well as the quenching constant value (DAPI
displacement), a conclusion can be drawn that complex 1 can bind with DNA via a pure groove-binding mode. However, in the
case of complex 2, there is some partial intercalation
along with groove binding as a result of which complex 2 shows a lower binding constant than 1 in the DAPI displacement
study. This explanation is further highlighted in the section molecular docking.
Figure 8
Fluorescence quenching
of (a) EB–DNA and (b) DAPI–DNA
adduct after the addition of incremental concentration (10–70
μM) of complexes 1 and 2
Fluorescence quenching
of (a) EB–DNA and (b) DAPI–DNA
adduct after the addition of incrementalconcentration (10–70
μM) of complexes 1 and 2
Circular Dichroism Study
After completion of fluorescence
quenching experiments, the circular dichroism study was carried out
to determine the minor groove-minding mode in the interaction of complexes 1 and 2 with ctDNA. The CD spectra of ctDNA in
the presence and absence of the guest (complexes 1 and 2) are shown in Figure S14 in the
Supporting Information. The figure clearly indicates that a positive
lobe and a negative lobe appear at 278 and 248 nm for free DNA, respectively.
These values reveal the presence of the canonical B form of DNA. After
the addition of complexes 1 and 2 to DNA,
very slight increases in the positive lobes occur. This indicates
that after the addition of the guest to DNA, the canonical B form
does not change during interactions. Actually, if the interaction
phenomena of DNA and the guest occur via the minor groove-binding
mode, then the canonical B form will remain more or less unchanged;
however, in the positive zone, a very small peak will appear in the
≫ 300 nm region, and this is observed in the CD spectrum (Figure S14) after the addition of the complex
to DNA.[54,55] This new small peak appears due to the presence
of the guest, which interacts with DNA via groove binding. In the
CD spectrum, this type of new small peak appears in the region of
345–550 nm after the addition of each complex to DNA. This
peak is more prominent in the spectrum of complex 1 than
in that of complex 2, indicating pure groove binding
in the case of complex 1.
Protein-Binding Study
From the foregoing discussion,
we have achieved the first-step success in the biomedical application
of the synthesized complexes, which is the effective binding efficacy
of the complexes with ctDNA. HSA, the most abundant protein in plasma,
is a monomeric multidomain macromolecule, representing the principal
determinant of plasma oncotic pressure and the chief indicator of
fluid distribution in between different body compartments, as it increases
drug solubility in plasma, decreases toxicity, and protects from oxidation.
Hence, as a next target, it is necessary to investigate the binding
potential of complexes 1 and 2 with HSA.
The interaction mechanism of HSA with the metalcomplex is the fundamental
point to realize pharmacodynamics and pharmacokinetics. To understand
the binding mechanism between complexes 1 and 2 with HSA, the electronic titration and fluorescence quenching experiments
have been carried out.
Absorption Titration
In this process,
actually the
change in the absorbance is recorded after the addition of incrementalconcentration of HSA to a fixed concentration of the complex. Prior
to this, we have recorded the UV–vis spectra of complexes 1 and 2 in the Tris buffer medium at different
time intervals (12, 24, 36, and 48 h), which ascertain the extensive
stability of the two complexes in the working buffer medium (Figure S15 in the Supporting Information). The
UV–vis spectralchanges of complexes 1 and 2 with the addition of HSA are shown in Figure . From this experiment, it is noted that
the peak maxima of the UV–vis spectral band (in tris buffer)
appear at 330 nm and 385 nm, respectively, for complexes 1 and 2 ([complex 1] = 80 μM;
[complex 2] = 80 μM), and the absorbance of complexes 1 and 2 is decreased with a blue shift (3 nm
for complex 1 and 5 nm for complex 2) after
gradual addition of HSA (2–16 μM and 2–20 μM
for complexes 1 and 2, respectively). The
apparent binding constants (Kapp) during
the interaction of the compounds with HSA are measured by using eq (Experimental
Section). The association constants for complexes 1 and 2 are found to be 2.07 × 105 M–1 and 1.926 × 105 M–1, respectively. The binding constants indicate that both the complexes
can effectively bind with HSA, but the binding constant is slightly
higher for complex 1. This is clearly discussed in the molecular docking section.
Figure 9
Absorption spectra of
(a) complex 1 and (b) complex 2 after gradual
addition of HSA at 300 K; change in the fluorescence
of HSA (40 μM) upon gradual addition of (c) complex 1 and (d) complex 2 at 300 K.
Absorption spectra of
(a) complex 1 and (b) complex 2 after gradual
addition of HSA at 300 K; change in the fluorescence
of HSA (40 μM) upon gradual addition of (c) complex 1 and (d) complex 2 at 300 K.
Fluorometric Titration Study
HSA shows an inherent
luminescence due to two chromophores, tryptophan (Trp) and tyrosine
(Tyr). Under appropriate conditions, if tyrosine ionizes, then the
emission intensity of HSA decreases, exhibiting the sole contribution
of tryptophan. After analyzing the results obtained from the electronic
titration profile, their interaction ability is checked using fluorometric
analysis. In this procedure, the fluorescence intensity is recorded
upon gradual addition of incrementalconcentration of complexes 1 and 2 to a fixed concentration of HSA. Impressively,
a strong decrease in the emission maxima of HSA (40 μM) centered
at 340 nm is observed after the addition of complex 1 (10–90 μM) and complex 2 (10–90 μM),
adopting a concentration-dependent pathway (Figure ). The titration profile is further utilized
to measure the quenching constant value using the Stern–Volmer
equation. The quenching constants for complexes 1 and 2 are found to be 2.1 × 105 M–1 and 1.4 × 105 M–1, respectively,
which indicates the interaction ability of HSA with the two complexes.
However, we have also calculated the bimolecular quenching rate constant
(Kq) of HSA for both the complexes using
the equation KSV=Kq × τ0, where τ0 stands
for the average decay lifetime of HSA in the absence of a quencher.[56] The Kq values are
found to be 3.91 × 1013 M–1S–1 and 2.60 × 1013 M–1S–1 for complexes 1 and 2, respectively. During the quenching procedure, the titration pictograph
clearly showed that a hypsochromic shift is observed in both the cases.
This could be explained as a result of the association of the complexes
with the Trp residue of HSA mainly in the hydrophobic domain. The
higher binding efficacy of complex 1 to HSA is clearly
explained in the molecular docking section.
Molecular Docking Study
Computer-aided docking techniques
are very useful to measure the binding efficacy and identify the binding
location of biologically active drug molecules in macromolecules.
The mechanistic study of this binding procedure to determine the active
sites of the targeted macromolecules is very essential to render biologically
active drug molecules as therapeutic agents.[57,58] In this perspective, after successful experimental studies with
HSA and ctDNA of our synthesized complex 1 and complex 2, their active binding sites and binding locations have been
interpreted theoretically. The docking space gives a chance to dock
the whole binding sites of HSA and ctDNA molecules individually while
generating the binding location with complexes 1 and 2. In the perspective of HSA, mostly targeted molecules prefer
the binding location either Sudlow site I (subdomain IIA) or Sudlow
site II (sub-domain IIIA), depending on the nature of the functional
groups.[59,60] In our complexes, from Figure a,c it can be seen that both
complexes 1 and 2 are buried inside the
deep hydrophobiccavity between the protein subdomains IIA and IIIA
and below IB. The most reasonable approach to represent the HSA–metalcomplex interaction is only through the residues in the 5 Å range
around complexes 1 and 2, which are shown
in Figure b,d. The
attachment of complex 1 surrounded by the residues ALA-188,
LYS-192, ARG-215, LYS-433, and TYR-449 is through five strong hydrogen
bonds (3 H-bonds 2.4, 2.4, and 2.1 Å with LYS-192; 1 H-bond 3.0
Å with ARG-215; and 1 H-bond 3.4 Å with LYS-433) and two
weak hydrogen bonds (1 H-bond 3.7 Å with LYS-433 and 1 H-bond
4.1 Å with TYR-449). However, binding residues present around
complex 2 are LYS-192, LYS-433, and TYR-449 through three
strong H bonds (1 H-bond 3.2 Å with LYS-192; 1 H-bond 2.3 Å
with LYS-433; and 1 H-bond 3.3 Å with TYR-449). These H-bonding
and van der Waals force of interaction play a major role in the binding
affinity of the complexes inside the HSA domain. From the above investigated
docking results, one can easily interpret that complex 1 binds more strongly with HSA than complex 2, and the
respective docked binding energy values obviously follow similar trends,
as shown in Table S3 (Supporting Information).
The binding energy for the complex 1–HSA adduct
is −8.96 kcal/mol higher than that of the complex 2–HSA adduct, having energy −8.29 kcal/mol. These theoretical
findings are in agreement with UV–vis experimental results.
Figure 10
Minimum
energy docked pose of (a) complex 1 and (c)
complex 2 with close view around complexes within HSA
(b,d).
Minimum
energy docked pose of (a) complex 1 and (c)
complex 2 with close view around complexes within HSA
(b,d).In the case of ctDNA–metalcomplexes, both complexes 1 and 2 are well
fitted preferentially in the
A–T-rich region of ctDNA, as shown in Figure . The docking results reveal that the binding
positions of the metalcomplexes are within three A–T base
pairs (DT8–DA17 to DA6–DT19) and one G–C pair
(DG5-DC20). From the docked structure, it is interesting to see that
complex 2 has the ability to entrap in the groove and
slide between A and T base pairs as partial intercalation (Figure d–f). In
this partial intercalation, the planar heterocyclic portion of complex 2 is present between adenine and thymine base pairs, whereas
the remaining perpendicular part is extended in the minor groove of
ctDNA. Alternatively, complex 1 manages to fit around
the minor groove of DNA only. Decreasing the spatial hindrance around
the sliding moiety increases the intercalative ability of complex 2 compared to that of complex 1. From the binding
energy values (−5.96 kcal/mol for complex 2 and
−5.61 kcal/mol for complex 1), there is a clear
reflection of the spatial hindrance effect, indicating that the partial
intercalating complex 2 has greater binding energy than
complex 1, which has groove-binding ability.
Figure 11
Docking orientations
of (a–c) complex 1 and
(d–f) complex 2 in ctDNA.
Docking orientations
of (a–c) complex 1 and
(d–f) complex 2 in ctDNA.It can be noticed that complex binding is stabilized through H-bonding
with adenine bases (2.8 Å for complex 1 and 4.1
Å for complex 2) and van der Waals interactions
with the functional groups.In partial intercalation, the gap
between base pairs is slightly
increased during the partial tilting[60] of
complex 2, and this orientation favored the possibility
of strong van der Waals interaction in comparison with only the minor
groove-binding complex 1.The experimental results
of UV–vis analysis is completely
in agreement with the computational modeling results. Ligand efficiency
and intermolecular energies are also tabulated in Table S2 in the Supporting Information, and they show the
trends similar to binding energy. Therefore, from the above discussion
on computational modeling, one can understand that Cu-based complex 1 has a high binding efficiency with HSA having strong H-bonding
compared to Zn-based complex 2. In contrast, ctDNA favors
less hindrance complex 2 through partial intercalation
in A–T-rich base pairs compared to complex 1.
Conclusions
In summary, the treatment of bromoaniline with
salicylaldehyde
and 5-bromo salicylaldehyde leads to the formation of two fluorescence
active Schiff base probe (E)-4-bromo-2-(((4-bromophenyl)imino)methyl)phenol
(HL) and (E)-2-(((4-bromophenyl)imino)methyl)phenol
(HL), having specific sensing ability toward
Cu2+ and Zn2+ ions, respectively, through turn-off
and turn-on fluorescence spectralchanges. The electronic titration
method reveals the high binding constant of the aforementioned metal
ions with HL and HL, which is in agreement with the formation of two new complexes,
namely, [Cu(L1)2] (1) and [Zn(L2)2] (2). The sensing ability of complex 2 as a metalloreceptor for Al3+ and Hg2+ ions was tested by using fluorometric and electronic spectral titrations.
DFT calculations have also been carried out to investigate the possible
association of the mentioned analytes with complex 2.
Furthermore, the two-step sensing phenomenon was utilized to formulate
an INHIBIT logiccircuit, which is additionally extended to construct
a molecular memory device. Knowing the ability of the fluorometric
method to determine the association of complexes with biomacromolecules,
the binding efficacies of these two complexes with DNA and HSA are
examined. On the basis of numerous spectroscopic investigations, it
can be concluded that complex 2 has a higher binding
potential toward DNA, whereas complex 1 shows better
affinity toward HSA protein. Theoreticalcalculations and molecular docking studies have finally been performed
to obtain a better view of the interaction region of the macromolecules
with the newly developed complexes (1 and 2).
Experimental Section
Materials and Physical Measurements
All reagents and
solvents used in this synthesis were commercially available. Reagent-grade
chemicals were used in this experiment. Hence, no further purification
was needed. Salicylaldehyde, 5-bromo salicylaldehyde, 4-bromo aniline,
ctDNA, HSA, EB, and DAPI were obtained from Sigma-Aldrich Chemicals.
CuCl2, ZnCl2, and triethyl amine (Et3N) were purchased from Merck. Elemental analyses were performed using
a PerkinElmer 240C elemental analyzer. Electronic absorption spectral
data were collected by using a PerkinElmer UV–vis Lambda 365
spectrophotometer at room temperature. The concentration of ctDNA
per nucleotide was determined by absorption spectroscopy using a molar
extinction coefficient (€) 6600 (M–1 cm–1) at 260 nm. ctDNA interaction studies were performed
in a citrate-phosphate (CP) buffer of 10 mM [Na+] at pH
7.40 containing 0.5 mM Na2HPO4, and HSA interaction
studies were performed in Tris buffer.Caution! Mercury salts are extremely toxic, so proper caution should be taken
before use.
Synthesis of Ligands HL and HL
The ligands HL and HL were prepared
by the condensation reaction
of the corresponding amine and aldehydes following the literature
method[61] and were exploited as sensors
for the first time. Methanol was used as solvent during synthesis. 1HNMR [HL, CDCl3, 25 ° C]: δ
= 6.630–7.524 (m, 7H), 8.604 (s, 1H), 12.988 (s, 1H); 13CNMR [HL, CDCl3, 25
° C]: δ = 161.622 (Ar-C-O), 160.117
(HC=N), 147.042 (Ar–C–N), 135.714 (C, Ar–C), 133.435 (2C, Ar–C),
132.704 (Ar–C), 122.912 (2C, Ar), 121.033 (Ar–C), 120.006
(Ar–C), 119.515 (Ar–C), 110.800 (Ar–C).1HNMR [HL CDCl3,
25 ° C]: δ = 6.951–7.403 (m, 8H), 8.653 (s, 1H),
13.135 (s, 1H); 13CNMR [HL, CDCl3, 25 ° C]: δ = 163.092 (Ar–C–O), 161.117 (HC=N), 147.524
(Ar–C–N), 133.481 (2C, Ar–C),
132.586 (Ar–C), 132.500 (Ar–C), 122.903 (2C, Ar), 120.467
(Ar–C), 119.306 (Ar–C), 119.030 (Ar–C), 117.422
(Ar–C).
Synthesis of [Cu(L1)2] (1)
CuCl2 (0.119 g, 0.7 mmol)
was dissolved in
methanol (30 mL) and was added to 25 mL methanolic solution of the HL ligand (0.248 g, 0.7 mmol) under continuous
stirring conditions. The resulting solution was then refluxed for
additional 3 h. The green colored solution formed was filtered, and
from the filtrate single crystals were obtained within 1 day. Yield
0.462 g (75%).Anal. Calc.: For C26H16Br4CuN2O2 (771.56):
C 40.43; H 2.07; N 3.62%. Found: C 40.39; H 2.10; N, 3.47%, UV: 373
(ε, 9600 CT spectra), 568 (ε, 371 d–d transition).
IR: ν (C=N) 1636 cm–1; ν (skeletal
vibration) 1572 cm–1.
Synthesis of [Zn(L2)] (2)
Complex 2 was synthesized
by adopting exactly the same method used
for the preparation of complex 1. In case of complex 2, ZnCl2 (0.095 g, 0.7 mmol) was dissolved in methanol
and added to the HL solution and by adopting
the same method single crystals were obtained. Yield 0.356 g (72%).Anal. Calc.: For C26H18Br2ZnN2O2 (615.61): C 50.68; H 2.92; N 4.54%. Found: C
50.62; H 2.88; N 4.53%, UV: 401 (ε, 7600 CT spectra), IR: ν
(C=N) 1634 cm–1; ν (skeletal vibration)
1576 cm–1.
Sample Preparation for Fluorescence and UV
Spectral Studies
The stock solutions of HL, HL, and complex 2 (3
× 10–2 M) were prepared in DMSO/H2O (9:1) HEPES buffer medium,
and the stock solution of various metal ions (5 × 10–3 M) were prepared in the same medium by using their chloride salts.
X-ray Crystal Structure Determination
Single-crystal
X-ray diffraction data of the two complexes were collected using a
Bruker APEX-II CCD diffractometer equipped with graphite monochromated
MoKα radiation. Data reduction and structure solution refinement
were carried out using APEX II.[62,63] The structures of complexes 1 and 2 were solved by the direct method and
refined in a routine procedure. All hydrogen atoms were refined isotropically
where the nonhydrogen atoms are treated anisotropically. The summary
of the crystal data and other structure refinement parameters are
provided in Table . Complexes 1 and 2, CCDC 2006526, 2006525,
contain the supplementary crystallographic data for this paper.
Table 2
Crystallographic Data and Refinement
Parameters of Complexes 1 and 2
1
2
CCDC number
2006526
2006525
empirical formula
C26H16Br4CuN2O2
C26H18Br2ZnN2O2
fw
771.56
615.61
crystal size/mm
0.21 × 0.16 ×
0.09
0.17 ×
0.12 ×
0.089
crystal
system
monoclinic
monoclinic
space group
P21/c
C2/c
a/Å
9.8183(6)
21.738(3)
b/Å
10.6368(5)
9.0322(14)
c/Å
12.0379(6)
11.8880(18)
α/°
90
90
β/°
100.785(2)
96.105(7)
γ/°
90
90
V/Å3
1234.98(11)
2320.9(6)
Dcalcd/g cm–3
2.075
1.762
Z
2
4
F(000)
742
1216.0
μ/mm–1Mo Kα radiation
7.384λ =0.71073 Å
4.528λ =0.71073 Å
T/K
296(2)
296(2)
Rint
0.0618
0.0721
range of h,k,l
–12/11,-13/11,-15/15
–30/30,-12/12,-16/16
θmin/max/°
3.120/27.127
2.444/ 30.414
reflections collected/unique/observed
[I > 2σ(I)]
7951/ 2683/2091
28,329/ 3503/ 2552
data/restraints/parameters
2683/0/160
3503/0/152
GOF on F2
1.047
1.065
finalRindices[I > 2σ(I)]
R1 = 0.0538wR2 = 0.1390
R1 = 0.0503wR2 = 0.1574
Rindices(all data)
R1 = 0.0713wR2 = 0.1498
R1 = 0.0717wR2 = 0.1726
Computational
Details
The energies of the optimized
geometries of complex 2 and the Zn–Al bimetalcomplex were determined in the gas phase. For free and oxidized ligands,
the solvent environment was determined by the DFT method with the
Becke, three-parameter, Lee–Yang–Parr (B3LYP)[64,65] hybrid functional for exchange correlation and SDD[66] in the form of a basis set. To study the UV–vis
spectral properties in detail, we have computed the major transitions
by adopting the TD-DFT methodology using the CAM-B3LYP/SDD level of
theory in DMSO solvent. The polarizable continuum model (PCM) has
been used to account for the solvent effect. All of the calculations
were performed using Gaussian 0983[67] and
GaussSum[68] software.
ctDNA/HSA Interaction
Studies
Absorption Spectral Titrations
For the absorption spectral
titration study, a fixed concentration of the metalcomplex was treated
with an incrementalconcentration of ctDNA/HSA. The binding constant
(K) for the association of complexes with ctDNA was
calculated using eq ,[69]where [DNA] stands for the
concentration of ctDNA in the base pairs, ε represents the apparent absorption coefficient corresponding
to Aobs/[complex 1, 2], ε is the extinction
coefficient of the free complex, and ε is the extinction coefficient of the complex, fully bound to ctDNA.
The intrinsic binding constant K could be calculated
from the ratio of the slope to the intercept by using the graph of
[DNA]/(ε – ε) vs [DNA].At the same time, considering
an equilibrium binding system, a quantitative assessment of the association
of HSA was realized by determining the equilibrium constant for complex
formation adopting the double reciprocal equation (eq ,[70]Where ε represents the
extinction coefficient, the subscripts b, f, and T stand for the bound, free, and totalcomplex concentrations. L represents the metalcomplex concentration, M is the concentration of the macromolecule (HSA), and ΔA stands for the absorbance change at a given wavelength.
The association constant for complex formation (Ka) can be evaluated from the ratio of the intercept.
Fluorescence Spectral Studies
EB was used for the displacement
assay study to understand the competitive binding ability of the two
complexes with ctDNA. The fluorescence intensities were noted after
incremental addition of every complex solution to the ctDNA–EB
adduct separately.For proper identification of the interaction
mode, DAPI displacement assay was also performed. In this case, the
change in the fluorescence intensity of the DAPI–ctDNA moiety
was recorded after incremental addition of each complex solution into
the ctDNA–DAPI adduct.In the case of HSA protein, fluorescence
titration was monitored
within the region of 250–450 nm upon excitation at 240 nm.
In this study, after gradual addition of complexes 1 and 2 separately into the HSA solution, an impressive decrease
in the emission intensity was noted.
Circular Dichroism Study
CD titration was carried out
after the addition of incrementalconcentrations of complexes 1 and 2 to a fixed concentration of DNA (60 μM).
The molar ellipticity values [θ] were measured by using the
equation [θ] = 100 × θ/(C × l), where θ stands for the observed ellipticity in
milli degrees, C represents the concentration in
mol/L, and l refers to the cell path length of the
cuvette in cm. The molar ellipticity [θ] (deg.cm–2/dmol) results are presented in terms of base pairs within
the region of 200–400 nm.[71,72]
Molecular
Docking
The crystal structures of Cu-based
complex 1 and Zn-based complex 2 were used
as received from the crystallographic data for the input file of Auto
Dock 4.2 software.[73] Macromolecular crystal
structures of HSA and ctDNA were used as obtained from the Protein
Data Bank (PDB) identifier 1UOR and 1COC, respectively.[74] Polar hydrogen and Gasteiger charges were added
as required. For grid preparation, all domains of the HSA structure
were kept under inspection. In ctDNA, the grid was maintained in such
a way that the A–T and G–C bases were emphasized equally.
Among 20 several docked structures in each category of the complex-macromolecular
adduct, a minimum energy conformer was taken for further analysis.
Other docking parameters were kept as default, as obtained by software
programming. The docked files from Auto Dock were finally analyzed
using the PyMOL and Chimera software package.[75]