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A binuclear silver complex with L-buthionine sulfoximine: synthesis,spectroscopic characterization, DFT studies and antibacterial assays{
Fernando Rodrigues Goulart Bergamini,a Marcos Antonio Ferreira Jr.,a Raphael Enoque Ferraz de Paiva,a
Alexandre Ferreira Gomes,b Fabio Cesar Gozzo,b Andre Luiz Barboza Formiga,c Fabiana Cristina Andrade
Corbi,d Italo Odone Mazali,d Danilo Antonini Alves,e Marcelo Lancellottie and Pedro Paulo Corbi*a
Received 12th July 2012, Accepted 31st August 2012
DOI: 10.1039/c2ra21433d
A binuclear silver(I) complex with the amino acid L-buthionine sulfoximine (BSO) of composition
Ag2C8H16N2O3S was synthesized and characterized by chemical and spectroscopic measurements,
and DFT (density functional theory) studies. Solid-state 13C nuclear magnetic resonance (SSNMR)
and infrared vibrational spectroscopy (IR) analyses indicate the coordination of the nitrogen and
carboxylate groups of the amino acid moiety to one of the silver atoms, while coordination to the
second silver atom occurs through the nitrogen of the sulfoximine group. ESI-QTOF-MS
measurements show the maintenance of the binuclear structure in solution. DFT studies confirm the
proposed structure as a minimum of the potential energy surface (PES) with calculations of the
hessians showing no imaginary frequencies. Raman spectroscopic measurements of the [Ag2(BSO)]
complex led to the assignments of the Ag–N bonds. Biological assays of BSO and [Ag2(BSO)] were
performed by the well-diffusion method over Staphyloccocus aureus (Gram-positive), Escherichia coli
and Pseudomonas aeruginosa (Gram-negative) bacterial strains. The ligand was inactive under the
tested concentration (100 mg mL21). The [Ag2(BSO)] complex was active against the Gram-negative
and Gram-positive bacteria tested, with MIC values of 3.125 mg mL21.
Introduction
Silver compounds have been considered for centuries in the
treatment of infectious diseases.1 Although effective, the use of
silver salts in high concentrations for the treatment of skin
bacterial infections has led to toxic side effects. The fast and
uncontrolled release of the metal ion and its further accumula-
tion in the kidneys and liver are probably the most prominent
causes of silver intoxications.2 The clinical introduction of
sulfonamides in the 1930’s, in addition to the serendipitous
discovery of penicillin by Sir Alexander Fleming, can be
considered a historic event in the treatment of bacterial
infections. The discovery of the biological activities of such
compounds led to the development of new synthetic and semi-
synthetic organic antibacterial drugs.3–5 As a result, the synthesis
and biological applications of new silver-based compounds as
antibacterial agents were drastically reduced.1
Silver nitrate was reconsidered to for clinical use in the 1960’s,
when Moyer et al. proposed that a 0.5% aqueous silver nitrate
solution could be efficiently used on burns against the S. aureus
bacterial strain. According to the authors, the use of silver
nitrate in this concentration does not interfere in epidermal
proliferation.6 This resurgence was closely followed by the
discovery of the antibacterial activities of silver(I)-sulfadiazine in
1968.7 Silver(I)-sulfadiazine presents considerable antibacterial
activity against both Gram-negative and Gram-positive bacterial
strains with reduced adverse effects when compared to silver(I)
nitrate.7
In spite of the antibacterial effect of free sulfadiazine, the
antibacterial activity of silver(I)-sulfadiazine was reported to be
exclusively due to the silver ion, since only it was found inside the
bacterial cells. Sulfadiazine was considered responsible for the
controlled release of the metal ion.7–11
These results have stimulated the search for new active silver(I)
complexes, since silver(I) based antiseptic materials have a low
propensity to induce bacterial resistance in comparison to
common antibiotics.12 In addition, silver also presents low
toxicity when compared to other heavy metals used for the same
purpose, such as gold and platinum.12–14
Nowadays, some bacterial strains have been shown to be
resistant even to the most effective commercially available
aBioinorganic and Medicinal Chemistry Research Laboratory, Institute ofChemistry, University of Campinas—UNICAMP, P.O. Box 6154, 13083-970 Campinas, Sao Paulo, Brazil. E-mail: [email protected] Chemistry Laboratory, Institute of Chemistry, University ofCampinas—UNICAMP, Campinas, Sao Paulo, BrazilcDalton Mass Spectrometry Laboratory, Institute of Chemistry, Universityof Campinas—UNICAMP, Campinas, Sao Paulo, BrazildSolid-State Chemistry Laboratory, Institute of Chemistry, University ofCampinas—UNICAMP, Campinas, Sao Paulo, BrazileLaboratory of Biotechnology, Institute of Biology, University ofCampinas—UNICAMP, Campinas, Sao Paulo, Brazil{ Electronic Supplementary Information (ESI) available. See DOI:10.1039/c2ra21433d
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10372 | RSC Adv., 2012, 2, 10372–10379 This journal is � The Royal Society of Chemistry 2012
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antibiotics. For instance, there are meticillin-resistant Staphylococcus
aureus (MRSA), vancomycin-resistant Enterococcus faecium,
extended-spectrum b-lactamase-producing Enterobacteriaceae and
multi-resistant Pseudomonas aeruginosa and Acinetobacter bauman-
nii.15 The intrinsic or acquired resistance of some bacterial strains,
the latter closely related to the indiscriminate use of antibiotics, led to
the development of new antibacterial compounds to overcome
multiresistant bacterial strains.16–19 Combining bioactive com-
pounds and metal ions which exhibit bacterial activity is one of
the possible approaches against bacterial multiresistance.20,21 The
coordination of molecules such as antibacterial agents or aspecific
enzyme inhibitor compounds with metal ions such as silver and gold
is also desirable due to the possibility to target different bacterial
strains in different phases of bacterial growth.22,23
Two silver(I) complexes derived from N-acetyl-L-methionine
(L-Hacmet) and N-acetyl-DL-methionine (DL-Hacmet), {[Ag(L-
acmet)]}n and {[Ag2(D-acmet)(L-acmet)]}n, were reported to
possess a wide spectrum of antimicrobial activities against the
Gram-negative E. coli and P. aeruginosa bacterial strains (MIC
15.7 mg mL21), and the yeasts Candida albicans (MIC 15.7 mg
mL21) and Saccharomyces cerevisiae (MIC 31.3 mg mL21).24
Cuin et al. recently reported the synthesis of silver(I), gold(I) and
gold(III) complexes with 6-mercaptopurine (MP).25 The Ag(I)-
MP and Au(I)-MP complexes showed good activity against
Mycobacterium tuberculosis, responsible for tuberculosis. In
addition, our research group recently reported the synthesis,
characterization, DFT studies and preliminary antibacterial
assays of Ag(I)-N-acetyl-L-cysteine (Ag-NAC) and Ag(I)-
Nimesulide (Ag-NMS) complexes.26,27 In the case of the Ag-
NAC complex, coordination of the ligand to Ag(I) was through
the sulphur atom, whereas in the Ag-NMS complex coordination
of the ligand was through the nitrogen and oxygen atoms of the
sulfonamide group. Both compounds were tested as antibacterial
agents using the disc diffusion method, being shown to be active
against P. aeruginosa, E. coli and S. aureus bacterial strains.
Besides, the gold(I) complex with N-acetyl-L-cysteine was also
synthesized. Biological studies are in progress in order to
compare its antibacterial activities with the respective silver(I)
complex.28
L-Buthionine sulfoximine (BSO, C8H18N2O3S, M.W.
222.31 g mol21) is a specific and potent inhibitor of c-gluta-
milcysteine synthetase, which decreases the level of glutathione
in tumor cells.29–32 Glutathione is one of the major intracellular
antioxidants with multiple biological functions,33 but has the
negative aspect of also being related to the development of
resistance of several tumors to anti-cancer drugs.34–37 BSO is
used as an adjuvant in treatment with metallodrugs such as cis-
diamminodichloridoplatinum(II) (cisplatin).38 Besides its biolo-
gical properties, BSO is a polyfunctional ligand due to the
presence of two basic nitrogen atoms, the oxygen in the
sulfoximine group and a carboxylic moiety. Here, we describe
the synthesis of a new Ag(I) complex with L-buthionine
sulfoximine [Ag2(BSO)] in aqueous solution, and its full
characterization by elemental, ESI-QTOF mass spectrometric
and thermogravimetric (TG) analyses, infrared (IR), Raman and
solid-state 13C nuclear magnetic resonance (SSNMR) spectro-
scopy. Density functional theory (DFT) studies and antibacterial
activities of the [Ag2(BSO)] complex against Gram-positive and
Gram-negative pathogenic bacterial strains are also described.
Experimental section
Reagents and equipment
L-Buthionine sulfoximine (98%), potassium hydroxide and
silver(I) nitrate (AgNO3) (98%) were purchased from Sigma-
Aldrich Laboratories. Elemental analyses for carbon, hydrogen
and nitrogen were performed using a Perkin Elmer 2400 CHN
analyzer. Infrared spectra from 4000–400 cm21 of BSO and the
silver(I) complex [Ag2(BSO)] were measured using an ABB
Bomen MB Series FT-IR spectrophotometer; samples were
prepared as KBr pellets. The 1H solution-state nuclear magnetic
resonance (1H-RMN), 13C solution-state nuclear magnetic
resonance (13C-NMR), [1H-13C] heteronuclear single-quantum
correlation (HSQC), and [1H-13C] heteronuclear Multiple Bond
Correlation (HMBC) spectra of BSO were recorded on a
AVANCE III 400 MHz spectrometer, using a 5 mm probe at
303 K. The compound was analyzed in a deuterated water
solution. The 13C-{1H} solid-state nuclear magnetic resonance
(SSNMR) spectra of BSO and of the [Ag2(BSO)] complex were
recorded on a Bruker AVANCE II 400 MHz (9.395T) spectro-
meter operating at 100 MHz, using the combination of cross-
polarization, proton decoupling and magic angle spinning (CP/
MAS) at 10 kHz. The 1H radio-frequency field strength was set
to give a 90u pulse. Contact time and recycle delay were 4 ms and
1 s, respectively. Samples were analyzed at room temperature
and the chemical shifts were referenced to TMS.
The 15N NMR chemical shift of BSO was indirectly detected
in the solution-state by a heteronuclear [1H–15N] multiple bond
coherence (HMBC) experiment. The 1H–15N NMR data were
acquired on a Bruker AVANCE III 400 MHz spectrometer,
using a 5 mm probe at 303 K. The compound was analyzed in a
deuterated water solution. Due to the poor solubility and low
percentage of nitrogen in the [Ag2(BSO)] complex composition
the 15N NMR data for the complex could not be obtained either
in the solution or in the solid-state.
Electrospray ionization quadrupole time-of-flight mass spec-
trometry (ESI-QTOF-MS) measurements were carried out in a
Waters Synapt HDMS instrument (Manchester, UK). A sample
of [Ag2(BSO)] was solubilized in 50 : 50 H2O/MeCN (0.1%
formic acid v/v) at a concentration of ca. 4 mg mL21, then
further diluted 100-fold in the same solvent mixture and
immediately analyzed. Resulting solutions were directly infused
into the instruments ESI source at a flow rate of 15 mL min21.
Typical acquisition conditions were capillary voltage: 3 kV,
sampling cone voltage: 20 V, source temperature: 100 uC,
desolvation temperature: 200 uC, cone gas flow: 30 L h21,
desolvation gas flow: 900 L h21, trap and transfer collision
energies: 6 and 4 eV, respectively. ESI{ mass spectra (full scans)
and fragment ion spectra for quadrupole-isolated ions (QTOF-
MS/MS) were acquired in reflectron V-mode at a scan rate of 1
Hz. For fragment ion spectrum experiments by collision-induced
dissociation (argon as collision gas), the desired ion was isolated
in the mass-resolving quadrupole, and the collision energy of the
trap cell was increased until sufficient fragmentation was
observed. Prior to all analyses, the instrument was externally
calibrated with phosphoric acid oligomers (H3PO4 0.05% v/v in
50 : 50 H2O/MeCN) ranging from m/z 99 to 980. Thermal
analysis was performed on a SEIKO EXSTAR 6000 thermo-
analyzer to obtain simultaneous TGA/DTA in the following
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conditions: synthetic air, flow rate of 50 cm3 min21 and heating
rate of 10 uC min21, from 25 uC to 1100 uC.
The Raman spectrum was recorded using a Jobin-Yvon
T64000 single spectrometer system, equipped with a confocal
microscope and a nitrogen-cooled charge-coupled device (CCD)
detector. The spectrum was collected using a 633.0 nm (1.5 mW)
line of He/Ne laser at room temperature. The sample was
analyzed in the solid-state.
Synthesis
The silver(I) complex with BSO was synthesized by the reac-
tion of 2.0 mL of an aqueous solution of silver(I) nitrate (9.0 61024 mol) with 6.0 mL of a freshly prepared aqueous solution of
BSO containing 4.5 6 1024 mol of the ligand. The aqueous
AgNO3 solution was added to the BSO solution under magnetic
stirring at room temperature followed by the addition of 9.0 61024 mol of KOH. After 40 min of constant stirring, the white
solid obtained was vacuum-filtered, washed with cold water and
dried in a desiccator over P4O10. Elemental analysis led to the following
composition: Ag2C8H16N2O3S. Calcd. for Ag2C8H16N2O3S (%): C,
22.0; H, 3.70; N, 6.42; found (%): C, 22.9; H, 3.34; N, 6.60. The
[Ag2(BSO)] complex is insoluble in water, ethanol, methanol,
dimethylsulfoxide, acetonitrile, chloroform, acetone and hexane.
It is slightly soluble in a mixture of water and acetonitrile
(50 : 50 v/v). The composition of the complex has a molar ratio of
2 : 1 metal/ligand. No single crystals of the complex were
obtained, even after several attempts, in order to perform an
X-ray structure determination.
Molecular modeling
Geometry optimizations were carried out using the GAMESS
software39 with a convergence criterion of 1026 a.u. in a
conjugate gradient algorithm. The LANL2DZ40 effective core
potential was used for silver and the atomic 6-31G(d) basis set41
for all other atoms. Density functional theory (DFT) calcula-
tions were performed for BSO and [Ag2(BSO)] using the
B3LYP42 gradient-corrected hybrid functional to solve the
Kohn–Sham equations with a 1025 convergence criterion for
the density charge. For the BSO zwitterions and [Ag2(BSO)]
complex the polarizable continuum model (PCM)43 was used to
simulate the effect of water in the geometry optimization. The
final geometries were confirmed as a minimum of the potential
energy surface (PES) with calculation of the hessians. The
harmonic vibrational frequencies and intensities were calculated
at the same level of theory with the analytical evaluation of the
second derivatives of the energy as a function of the atomic
coordinates. The calculated intensities were used to generate the
theoretical spectra. Frequencies were scaled by a factor of
0.9614, as recommended by Scott and Radom.44 Simulated
vibrational spectra were obtained from the sum of the
Lorentzian functions with 20 cm21 half-bandwidths using the
software MOLDEN 4.7.45 Raman intensities for the [Ag2(BSO)]
complex were simulated by the numerical differentiation
procedure applying an electric field of 2 6 1023 a.u., as
previously reported.46 Frequencies were scaled by a factor of
1.0013, as recommended by Scott and Radom, for low
frequencies.44
Biological assays
Six pathogenic bacterial strains, E. coli ATCC 25922, P.
aeruginosa ATCC 27853, P. aeruginosa 31NM, S. aureus
ATCC 25923, S. aureus BEC9393 and S. aureus Rib1 were
selected. Stock solutions (10.0 mg mL21) of BSO and AgNO3 in
water, and also a 2.0 mL water suspension containing 20.0 mg of
the [Ag2(BSO)] complex were prepared before the experiment.
Sufficient inocula of the bacterial strains were added to a 24
multiwell plate until the turbidity equaled 0.5 McFarland (y1.5
6 1028 CFU mL21). Then, 100 mL of the BSO and AgNO3
solutions and 100 mL of the [Ag2(BSO)] suspension were added
to the plates. The negative control was obtained by leaving one
of the wells of each bacterial strain with no addition of the
considered compounds. The minimal inhibitory concentration
(MIC) of the [Ag2(BSO)] complex was estimated as recom-
mended by the Clinical and Laboratory Standards Institute
(CLSI).47 In this case, the [Ag2(BSO)] complex was submitted to
serial dilutions (1 : 1) in a 96 multiwell plate with 100 mL of each
compound/dilution. Samples were transferred to the plates
containing the respective bacterial strain (0.5 McFarland) in
seven decreasing concentrations.
Results and discussion
Infrared spectroscopic data
The [Ag2(BSO)] infrared (IR) spectrum was analyzed in
comparison to that of free BSO. The IR spectra of BSO and
[Ag2(BSO)] are provided in Fig. 1.
Two bands were related to the asymmetrical and symmetrical
NH2 stretching bands of the amino group and were observed in
the BSO spectrum at 3230 cm21 and 3144 cm21, respectively.
The d(NH2) band is observed in the free ligand spectrum at
1516 cm21. Also, the IR spectrum of the ligand shows a weak
band with a maximum at 2095 cm21, which is assigned to the
combination of the asymmetrical NH3+ bending vibration and
the torsional oscillation of the NH3+ group.48 The asymmetrical
and symmetrical stretching modes of the carboxylate group are
observed at 1618 cm21 and 1447 cm21, respectively. The energy
Fig. 1 Infrared spectra of (A) BSO and (B) the [Ag2(BSO)] complex.
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difference (D) between nas(COO2) and nsym(COO2), which is
used as the parameter to evaluate coordination modes of the
carboxylate group,49,50 is 171 cm21. Moreover, another band
corresponding to NH3+ is also observed in the IR spectrum of
the ligand at 1582 cm21, which reinforces the existence of the
ligand in its zwitterionic form. Characteristic sulfoximine
(HNLSLO) bands are observed in the BSO spectrum at
1210 cm21, and 1012 cm21, and are assigned as the NLS and
SLO stretching vibrations, respectively.51 The combination of the
N–H bending with the SLO and NLS stretching modes is
observed at 1139 cm21. The other characteristic bands for BSO
are the asymmetric and symmetric stretching bands due to the
CH2 group, which are observed at 2962 and 2930 cm21,
respectively.
In the [Ag2(BSO)] spectrum, asymmetrical carboxylate
stretching appears at 1582 cm21, while the symmetrical band is
observed at 1390 cm21. So, in this case, the energy difference (D)
between the nas(COO–) and nsym(COO–) is 192 cm21. According
to the literature, the larger D value for the complex when
compared to the ligand suggests a monodentate coordination of
the carboxylate group to the metal.50
In the [Ag2(BSO)] spectrum, a broad band in the region 3550–
3100 cm21 is observed. This band can be assigned to the
hydrogen bonds between the hydration water molecules and the
NH2 group of the [Ag2(BSO)] complex. Hydrogen bonds lead to
a poor resolution of the asymmetrical and symmetrical N–H
stretching bands. As reported in the literature, the shifting of the
N–H stretching mode in the spectrum of the complex, when
compared to the spectrum of the ligand can be attributed to the
coordination of the amino group of BSO to Ag(I). Moreover, the
band referring to the combination of the asymmetrical NH3+
bending vibration and the torsional oscillation of the NH3+
group, observed for BSO, is not present in the [Ag2(BSO)]
spectrum, which is also indicative of silver(I) coordination to
BSO through the nitrogen of the amino group.
The SLN and SLO stretching bands in the [Ag2(BSO)]
spectrum are observed at 1203 cm21 and at 1012 cm21,
respectively. The shifting of the SLN band suggests the
coordination of BSO to the second silver ion through the
nitrogen of the sulfoximine. The SLN–H bending vibration band
is not present in the [Ag2(BSO)] spectrum, which also indicates
that the other silver ion is coordinated to the nitrogen of the
sulfoximine group. The characteristic bands for the asymmetric
and symmetric stretching modes of the CH2 group are observed
in the same region as for free BSO.
13C and 15N NMR spectroscopic measurements
The structure of BSO with the hydrogen and carbon atoms
numbered is shown in Fig. 2. The solution-state 1H-NMR and13C-NMR for free BSO are presented in the ESI (#1).{ For a
more accurate assignment of the hydrogen and carbon atoms,
the DEPT135, [1H-13C]-HSQC, [1H-13C]-HMBC and [1H-15N]-
HMBC NMR data for the ligand in D2O were also obtained.
The [1H-15N]-HMBC, [1H-13C]-HMBC and DEPT 135 spectra
are shown in the ESI (#2).{ The [1H-13C]-HSQC spectrum is
presented in the ESI (#3).{As observed in the [1H-13C] HSQC spectrum, the triplet at
0.86 ppm in the 1H-NMR spectrum couples with the carbon at
12.7 ppm in the 13C-NMR spectrum. The high field signals in
both the 1H-NMR and 13C-NMR spectra can be respectively
attributed to the hydrogen atoms (H-8) and the carbon atom (C-
8) of the methyl group. The high field carbons at 20.9 ppm and
23.6 ppm can be assigned, respectively, as C-7 and C-6. The C-7
atom couples with the sextet at 1.39 ppm which can be attributed
to the H-7 hydrogen atoms. On the other hand, the C-6 atom
couples with the quintet at 1.70 ppm, which is assigned to the
H-6 hydrogen atoms. With a chemical shift similar to C-6, the
C-3 carbon atom is assigned at 23.6 ppm and couples with
the quartet of the H-3 hydrogen atoms at 2.43 ppm. Due to the
direct bond of the C-4 to the sulfoximine chiral center, the
hydrogen atoms H-4a and H-4b are no longer equivalent and
appear in the spectrum as two quartet signals, in the range 3.27–
3.36 ppm.
The C-2 and C-5 atoms in the 13C-NMR spectrum appear,
respectively, at 53.0 ppm and 53.4 ppm. The C-2 couples with the
quartet at 3.80 ppm. The position of C-2 can be explained by the
direct bonding of this atom to the primary amine. The C-5
carbon couples with a quartet signal at 3.20 ppm which is
assigned to H-5. Finally, the signal that appears at 172.9 ppm is
assigned to carbon C-1.
The [1H-13C]-HMBC and [1H-15N]-HMBC spectra confirm
the HSQC assignment. The DEPT-135 NMR analysis of BSO
confirms C-7, C-6, C-5, C-4 and C-3 as methylenes (CH2).
The NMR spectra of the [Ag2(BSO)] complex were analyzed in
comparison to that of BSO. Due to the low solubility of the
[Ag2(BSO)] complex in both polar and non-polar solvents, the
solid-state nuclear magnetic resonance technique (SSNMR) was
applied. The [Ag2(BSO)] complex and the free ligand 13C-{1H}
SSNMR spectra are provided in Fig. 3, with the respective
carbon assignments.
According to the experimental data, the chemical shift of C-2
in the free ligand spectrum and in the complex spectrum are
observed at 53.8 ppm and at 56.6 ppm, respectively, with a Dd
(d complex˜ d ligand) of 2.8 ppm. Moreover, the C-6, C-3 and
C-5 signals are observed, respectively, at 23.1 ppm, 26.3 ppm and
56.0 ppm in the free ligand spectrum while for the complex the
same carbon atoms appear at 28.9 ppm, 33.7 ppm and 61.6 ppm.
The Dd of the C-6, C-3 and C-5 carbon atoms are DdC-6 =
5.8 ppm, DdC-3 = 7.4 ppm and DdC-5 = 5.6 ppm. As suggested by
the IR data, the NMR data reinforces the coordination of BSO
to one of the silver atoms through the nitrogen of the
sulfoximine. This coordination would lead to changes in the
chemical shift of the carbon C-4. In our case, the DdC-4 was
0.7 ppm.
In the 13C SSNMR spectra of BSO and the [Ag2(BSO)]
complex, C-1 appears as two signals. This phenomenon can be
explained due to the existence of polymorphism for both BSO
and the [Ag2(BSO)] complex in the solid state.52 The chemical
shift for C-1 is observed at 176.6 ppm for the free ligand and at
Fig. 2 The schematic structure of BSO with the carbon and hydrogen
atoms numbered.
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178.7 ppm for the complex (DdC-1 = 2.1 ppm). No substantial
difference was observed in the chemical shifts of the C-7 and C-8
carbon atoms in the complex when compared to the free ligand
(DdC-7 = 1.0 ppm; DdC-8 = 20.1 ppm). The carbon assignments for
BSO and for the [Ag2(BSO)] complex with their respective Dd are
listed in Table 1. According to the NMR data, we suggest that one
of the silver atoms is coordinated to the nitrogen of the amino
group and the oxygen of the carboxylate group, while the other
silver atom is coordinated to the nitrogen of the sulfoximine group.
Thermal analysis
Thermogravimetric (TGA) data for the [Ag2(BSO)] complex is
presented in the ESI (#4).{ Ligand decomposition starts at
170 uC and occurs in two steps, leading to the formation of the
residue of the thermal treatment at 550 uC. Calcd. for loss of
BSO (%) 48.5; found (%) 53.6. The residue represents the
formation of metallic silver. Anal. Calcd. for Ag0 (%) 47.7; found
(%) 43.0. Water content (3.44%) is lost until 100 uC. The presence
of water is most probably due to absorption from the
environment during sample handling before the experiment.
Raman spectroscopic measurements
In order to confirm nitrogen coordination of the sulfoximine and
of the amino groups to the silver atoms, the Raman spectrum of
[Ag2(BSO)] was obtained. The spectrum is provided in the ESI
(#5).{ As observed, the [Ag2(BSO)] spectrum presents two broad
bands with their maxima at 484 cm21 and 668 cm21. According
to the literature, these bands can be assigned to the Ag–N
stretching modes from Ag–N(SO) and Ag–N(H2), respectively.53
Mass spectrometry measurements
The Ag2C8H16N2O3S composition was also confirmed by ESI-
QTOF-MS measurements. The [Ag2(BSO)] spectrum, presented
in Fig. 4, shows the presence of the monoprotonated ion
[Ag2BSO2H]+ at m/z 436.91, as well as the presence of the
[AgBSO]+ ion at m/z 329.00. The spectrum also shows the
presence of the [Ag(BSO)2]+ (m/z 553.11), [Ag2(BSO)2+H]+ (m/z
659.34) and [Ag3(BSO)222H]+ (m/z 764.86) ions. The experi-
mental isotopic pattern for [Ag2BSO2H]+ was compared to the
expected isotopic pattern considering the proposed composition
and was shown to be in good agreement to the latter with an
error of 22.0 ppm (calcd. m/z 434.9062, exp. m/z 434.9053).
To further investigate the structure of the observed ions, the
[Ag2BSO2H]+ and [AgBSO]+ ions, as well as the [BSO+H]+ ion,
were analyzed by ion fragmentation MS/MS spectrometry
(Fig. 5). The energy for the fragmentation of the monoproto-
nated ions was 14 eV for both [BSO+H]+ and [AgBSO]+ and
20 eV for [Ag2BSO2H]+. The [Ag2BSO2H]+ MS/MS spectrum
shows a signal at 216.82 m/z, which corresponds to the
monoprotonated species minus a C8H16N2O3S fragment. This
fragment can be attributed to one BSO ligand with the absence
of two hydrogen atoms. The Ag+ ion is also observed in the
spectrum at 106.90 m/z.
Molecular modeling
The geometries of BSO and [Ag2(BSO)] were obtained by
theoretical calculations using density functional theory (DFT).
Fig. 3 The 13C-SSNMR spectra of (A) [Ag2(BSO)] and (B) BSO.
Table 1 13C NMR assignments for BSO and for the [Ag2(BSO)]complex with the respective Dd
d (ppm) (BSO) d (ppm) (Ag2BSO) Dd (ppm)
C-1 176.6 178.7 2.1C-2 53.8 56.6 2.8C-3 26.3 33.7 7.4C-4 52.6 53.3 0.7C-5 56.0 61.6 5.6C-6 23.1 28.9 5.8C-7 22.1 23.1 1.0C-8 14.5 14.4 20.1
Fig. 4 Mass spectra for the [Ag2(BSO)] complex. (A) The ESI(+)-
QTOF mass spectrum from m/z 150 to 800. The term BSO2H refers to
the BSO ligand minus one hydrogen (C8H17N2O3S, 221.0960 Da). (B)
The isotope pattern comparison for the [Ag2BSO2H]+ ion of m/z 434.90.
The mass error was 22.0 ppm for [Ag2BSO2H]+ ([C8H17Ag2N2O3S]+,
calcd. m/z 434.9062, exp. m/z 434.9053), considering the monoisotopic
ion of the composition.
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The BSO molecule presents a zwitterionic structure. This
structure was optimized and its equilibrium geometry was
confirmed by vibrational analysis. The bond distances found
for the BSO structure are comparable to those previously
reported in the literature for an optimized structure using
DFT.54 The theoretical IR spectrum was obtained by calculation
of the hessians, showing no imaginary frequencies, and
compared to the experimental spectrum, which also confirms
the BSO optimized structure in the solid state. For the
calculations, the polarizable continuum model (PCM) was
employed to account for the effect of water in the description
of the zwitterionic forms. For comparative purposes, the
[Ag2(BSO)] complex structure was optimized at the same level
of theory.
As observed by elemental and thermal analysis, the complex
presents a 2 : 1 metal/ligand ratio, which was also observed by
the ESI-QTOF-MS analysis. The spectroscopic techniques
indicate the coordination of one silver(I) atom through the
nitrogen atom of the amino group and a monodentate
carboxylate, while the other silver(I) ion appears coordinated
to the sulfoximine moiety. So, in the case of the [Ag2(BSO)]
complex, the most stable structure is obtained considering the
coordination number two for the first silver(I) ion, and
coordination number one to the second silver(I) ion, which is
bonded to the nitrogen of the sulfoximine group. Silver(I) ions
can adopt diverse coordination numbers, passing through
coordination numbers one (monodentate) and two to high
coordination numbers and geometries, as reported in the
literature for various silver compounds.55–58 These data permit
us to propose a possible structure for the [Ag2(BSO)] complex,
which was also confirmed as a minimum of PES by calculation
of the hessians.
The optimized structure for the [Ag2(BSO)] complex is
presented in Fig. 6. The calculated Ag–NH2 and Ag–O distances
were 2.075 A and 2.032 A, respectively, while the H2N–Ag–O
angle was 83.0u. The Ag–N and Ag–O distances for the silver
atom bonded to the nitrogen atom of the sulfoximine group are
1.992 A and 2.679 A. The N–Ag–O angle was 83.1u. Detailed
bond distances, angles and dihedrals are reported in the ESI
(#6).{
Fig. 5 The fragment ion mass spectrum (collision-induced dissociation)
for the (A) monoprotonated BSO ligand, [BSO+H]+ of m/z 223.11. The
collision energy of the trap cell was 14 eV. The term BSO refers to the
neutral BSO ligand (C8H18N2O3S, 222.1038 Da). (B) The fragment ion
mass spectrum (collision-induced dissociation) for the [AgBSO]+ ion of
m/z 329.00. The collision energy of the trap cell was 14 eV. The term BSO
refers to the neutral BSO ligand (C8H18N2O3S, 222.1038 Da). (C) The
fragment ion mass spectrum (collision-induced dissociation) for the
[Ag2BSO2H]+ ion of m/z 436.91. The collision energy of the trap cell was
20 eV. The term [BSO22H] refers to the BSO ligand minus two
hydrogens (C8H16N2O3S, 220.0882 Da).
Fig. 6 The [Ag2(BSO)] complex optimized structure obtained by
B3LYP/DFT using LANL2DZ(Ag) and 6-31(d,p). The PCM model
was used to simulate the water effect on the geometric optimizations.
Fig. 7 Simulated infrared spectra of (A) BSO and (C) [Ag2(BSO)]. The
experimental spectra of (B) BSO and (D) [Ag2(BSO)] are presented for
comparison.
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The simulated and experimental IR spectra of BSO and
[Ag2(BSO)] are presented in Fig. 7. The [Ag2(BSO)] IR spectrum
is in good agreement with the experimental spectrum. These
spectra were used to confirm the experimental assignments. The
simulated vibrational spectrum for BSO shows asymmetric
amino group stretching nas(H–N–H) at 3461 cm21 with the
symmetric stretching nsym(H–N–H) observed at 3356 cm21. The
characteristic combination of the asymmetrical NH3+ bend
vibration and the torsional oscillation of the NH3+ group appear
at 2562 cm21. The difference between the simulated and
experimental values for this combination band is larger than
usual, but it can be attributed to intermolecular interactions in
the solid state.50 The n(C–O) appears as a combination mode
with d(NH2) at 1345 cm21. The asymmetric n(C–O) appears at
1699 cm21 whereas the asymmetric d(NH2) appears at
1582 cm21. A combination mode encompassing the sulfoximine
S–N–H bending and the SLO and SLN stretchings appears at
1128 cm21. The d(S–N–H) of the sulfoximine also contributes to
the band at 1072 cm21 whereas the SLN stretching is observed at
913 cm21.
In the simulated [Ag2(BSO)] spectrum, the asymmetric and
symmetric stretching modes nas(H–N–H) and nsym(H–N–H)
appear at 3300 cm21 and 3186 cm21, respectively. These data
reinforce the loss of the hydrogen atom of the NH3+ group and
coordination of the NH2 group to Ag(I).
The bands attributed to the combination mode concerning the
sulfoximine SLO and SLN stretchings appears at 997 cm21 and
1104 cm21. When compared to the free BSO spectrum, these
bands are shifted 224 cm21 and 284 cm1, respectively.
Moreover, the nas(C–O) band is observed at 1660 cm21, being
shifted 239 cm21 when compared to the free ligand.
The calculated values for the stretching modes in the Raman
spectrum, assigned as N–Ag from silver(I)-amine and silver(I)-
sulfoximine are presented in the ESI (#5).{ As observed, the Ag–
N stretching bands are in good agreement with the experimental
data and reinforce the band assignments.
Antibacterial studies
Antibiogram assays were carried out in order to evaluate the
antibacterial activities of the Ag-BSO complex. The activities of
the complex against the considered bacterial strains were
confirmed by MIC values, with concentrations ranging 3.125–
100.0 mg mL21. The results obtained show promising antibacter-
ial activity of the Ag-BSO complex against Gram-negative
bacteria, being comparable to the inhibitory effect of the
standard antibiotic chloramphenicol, used as positive control.
The Ag-BSO complex was less active than the standard
antibiotic vancomycin in the MIC assays for Gram-positive S.
aureus BEC9393, S. aureus Rib 1 and S. aureus ATCC 25923.
The free BSO did not exhibit antibacterial activity under the
same experimental conditions. Antibiotic sensitivity profiles of
the bacterial strains are listed in Table 2. The observed results
show promising potential of application of the Ag-BSO complex
as a cream in skin infections in the case of severe burns, due to
small number of effective antibiotics against some specific Gram-
negative bacterial strains.
Conclusions
A silver(I) complex with BSO was synthesized and structurally
characterized. Elemental, themogravimetric and ESI-QTOF-MS
analyses show a 2 : 1 metal/ligand composition, with the
molecular formula [Ag2(C8H16N2O3S)]. The 13C CP/MAS
SSNMR, IR and Raman spectroscopic data suggest the
coordination of BSO to one silver atom through the amino
and carboxylate groups of the amino acid moiety, and also the
coordination of the ligand to another silver atom through
the nitrogen of the sulfoximine group. DFT studies support the
proposed geometry. Biological studies revealed that the complex
is effective against all the tested bacteria, being more effective
against the tested Gram-negative bacterial strains. Further
studies are intended in order to evaluate the possible mechanism
of action of the [Ag2(BSO)] complex.
Acknowledgements
This study was supported by grants from the Brazilian Agencies
FAPESP (Sao Paulo State Research Foundation, Brazil—proc.
2006/55367-2, 2008/57805-2, 2012/08230-2 and 2009/54066—
Laboratory of Advanced Optical Spectroscopy, LMEOA/IQ—
UNICAMP), CAPES and CNPq (Conselho Nacional de
Desenvolvimento Cientıfico e Tecnologico, Brazil—proc.
573672/2008-3; 472468/2010-3 and 472067/2010-9). The authors
are also grateful to MSc. Helen Graci C. de Meneses for her
valuable contribution in the DFT studies and to Professor Carol
H. Collins for the English revision of the manuscript.
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