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0
5
10
15
20
25
30
1 3 5
Ga2O3 (mol%)
Dia
met
er (m
m)
E.coli P.aeruginosa S.aureus MRSA C.difficle
Novel quaternary gallium-doped phosphate-based glasses are unique for controlled delivery
of Ga3+ which found to inhibit bacterial growth. The lack of new antibiotics in development
makes these glasses potential new therapeutic agents for pathogenic bacteria including MRSA
and C. difficile.
2
Antimicrobial Gallium-doped Phosphate-based Glasses
Doctor Sabeel P. Valappil1&2, Doctor Derren Ready3, Doctor Ensanya A. Abou Neel1 Doctor
David M. Pickup4, Doctor Wojciech Chrzanowski1,Doctor Luke A. O’Dell 5, Professor
Robert J. Newport4, Professor Mark E. Smith5, Professor Michael Wilson2
and Professor Jonathan C. Knowles1*.
1Division of Biomaterials and Tissue Engineering and 2Division of Microbial Diseases,
University College London, Eastman Dental Institute, 256 Gray’s Inn Road, London.
3Microbiology, Eastman Dental Hospital, UCLH NHS Foundation Trust, 256 Gray’s Inn
Road, London. 4School of Physical Sciences, University of Kent, Canterbury, CT2 7NH,
UK. 5Department of Physics, University of Warwick. Coventry, CV4 7AL, U.K.
*Corresponding Author. Mailing address: Division of Biomaterials and Tissue Engineering,
UCL Eastman Dental Institute, 256 Gray's Inn Road, London WC1X 8LD. UK. Phone: +44
(0)207 915 1189, Fax: +44 (0)207 915 1227, Email:[email protected]
3
Abstract
Novel quaternary gallium-doped phosphate-based glasses (1, 3, and 5 mol% Ga2O3) were
synthesized using a conventional melt quenching technique. The bactericidal activities of the
glasses were tested against both Gram-negative (Escherichia coli and Pseudomonas
aeruginosa) and Gram-positive (Staphylococcus aureus, methicillin-resistant Staphylococcus
aureus, and Clostridium difficile) bacteria. Results of the solubility and ion release studies
showed that these glass systems are unique for controlled delivery of Ga3+. 71Ga NMR
measurements showed that the gallium is mostly octahedrally coordinated by oxygen atoms,
whilst FTIR spectroscopy provided evidence for the presence of a small proportion of
tetrahedral gallium in the samples with the highest gallium content. FTIR and Raman spectra
also afford an insight into the correlation between the structure and the observed dissolution
behaviour via an understanding of the atomic-scale network bonding characteristics. The
results confirmed that the net bactericidal effect was due to Ga3+, and a concentration as low
as 1 mol % Ga2O3 was sufficient to mount a potent antibacterial effect. The dearth of new
antibiotics in development makes Ga3+ a potentially promising new therapeutic agent for
pathogenic bacteria including MRSA and C. difficile.
Key words: phosphate-based glasses; gallium content; bactericide; MRSA; C. difficile
4
Introduction
Recently, much attention has been focused on the need for new antimicrobial agents due to
the increased prevalence of antibiotic-resistant bacteria[1]. The multi-resistant nosocomial
pathogens such as MRSA and Clostridium difficile are the main source of recent increases in
the incidence of hospital-acquired infections (HAIs). Latest figures from the Health Protection
Agency (UK) showed that there were 15,592 cases of C. difficile infection reported in
England in the first quarter of 2007 (January to March). This represents a 22% increase on the
count for the previous quarter (October to December 2006). Similarly, the latest MRSA
bloodstream infection figures showed that there were 1,444 cases reported in England within
the period of January 2007 to March 2007 alone. Despite these trends, only one new
antibacterial drug, called linezolid, with a completely novel mechanism of action has been
introduced in the past 3 decades, and very few new antibiotics are in the advanced stages of
development [1]. Hence there is significant scope to develop novel drugs that combat these
antibiotic-resistant bacteria.
Iron (Fe) metabolism is a key factor in vulnerability of infecting bacteria as they require Fe
for growth and the functioning of key enzymes; such as those involved in DNA synthesis,
electron transport and oxidative stress defenses [2]. Therefore smooth functioning of Fe
metabolism is critical in the pathogenesis of bacterial infections. Gallium (Ga3+) has an ionic
radius nearly identical to that of Fe3+ and can function as a Trojan horse as many biological
systems are unable to distinguish Ga3+ from Fe3+ [3]. More importantly, sequential oxidation
and reduction are critical for many of the biological functions of Fe3+. However,
supplementation of Ga3+ can disrupt Fe3+-dependent processes because, unlike Fe3+, Ga3+
cannot be reduced under the same conditions [3]. Gallium is already approved by FDA to treat
hypercalcemia of malignancy [4] and has recently emerged as a new generation antibacterial
ion that may be useful in treating and preventing localized infections [5]. However, the use of
5
gallium as an antimicrobial agent could be significantly improved by the development of an
effective means of delivery. Chemically-durable materials, that can slowly release gallium
ions for long periods, would be considered desirable materials for medical applications.
Phosphate-based glasses (PBGs) are such durable materials which can act as a unique system
for the delivery of metal ions in a controlled way [6]. Ions incorporated into the glass structures
are not a separate phase, and thus their rate of release is defined by the overall degradation
rate of the glass. Metal ions, such as copper and silver, have been incorporated into PBGs, and
these glasses have then been used as wound dressings to prevent infections[7] and also to
control urinary tract infections in patients needing long-term indwelling catheters [7, 8] .
However, there is an underlying need to improve the properties of existing biomaterials due to
the incidence of HAIs, which often lead to revision surgery. Currently, prophylaxis in the
form of systemically administered antibiotics serves as the main weapon against infection
following implant surgery [9]. Therefore the need for improved antimicrobial agents and better
delivery devices could be met by gallium-doped PBGs. So far gallium has been shown to be
effective against the organisms causing syphilis, trypanosomiasis [10] , tuberculosis [11] and
malaria [12] in humans. It is also effective in the treatment of pneumonia in foals caused by
Rhodococcus equi [13].
The aim of this study was to develop novel gallium-doped PBGs and to investigate the
efficacy of these glasses against bacterial pathogens associated with HAIs such as
Staphylococcus aureus, Escherichia coli, Pseudomonas aeruginosa, methicillin-resistant
Staphylococcus aureus (MRSA) and Clostridium difficile.
2. Results and Discussion
2.1. Glass degradation
As can be seen in Figure.1a, the weight loss data decreased with an increase in the Ga2O3
content of the glasses. However, there were no perceptible differences in the profiles of the 3
6
and 5 mol% Ga2O3 compositions until 48hours. The Gallium free PBGs was found to
dissolve completely by 72hours of incubation. The dissolution rates, obtained by applying a
line of best fit through the data, were 41.70, 23.60, 7.30 and 3.70 µg.mm2.hr-1 for the 0, 1, 3
and 5 mol% Ga2O3 compositions respectively.
6
7
8
9
0 24 48 72 96 120 144
Time (h)
pH
0 1 3 5
Figure 1. Dissolution, determined by weight loss, (a) and pH analysis (b) of the 0, 1, 3 and 5 mol% Ga2O3-doped PBGs as a function of time.
y = 0.0417x
R2 = 0.9792
y = 0.0236x
R2 = 0.9866
y = 0.0073x
R2 = 0.9851
y = 0.0037x
R2 = 0.995
0
1
2
3
4
5
6
0 24 48 72 96 120 144
Time (h)
Wei
gh
t lo
ss (m
g.m
m2 )
0 1 3 5
1 (a)
1 (b)
7
The observed reduction in dissolution rate associated with the increase in Ga2O3 content could
be accounted to the associated increase in the ionic strength of the leaching solution. Glass
degradation has been reported to consist of the three synergistic processes of ion exchange,
hydration, and finally hydrolysis of the phosphate chains while in solution [14]. As a result of
ion exchange, a gel layer usually formed on the glass surface, i.e. hydration, and when it
leached into the surrounding medium it causes an increase in the ionic strength of the solution
with the resultant reduction in the dissolution rate.
2.2. pH Analysis
The pH analysis revealed that its value increased as the Ga2O3 content decreased (Figure 1b).
Gallium free composition displayed the maximum increase (8.61) in pH from the initial value
of 7. However, the pH value for both 3 and 5 mol% Ga2O3 remained close to neutral for the
duration of the study. As is seen from Figure 1b, the pH for compositions with 3 and 5 mol%
Ga2O3 remained neutral for the duration of the study, whereas for the composition with 0 and
1 mol% Ga2O3, the pH increased to about 8.5. The hydrolysis of PBGs exhibit clear pH
dependence as Watanabe et al.[15] stated that the rate of hydrolysis of small ring cyclic
trimeta- and tetrametaphosphates decreased in acidic solutions, and increased in basic
solutions with an increase in the pH value for all solvents.
2.3. Ion release
As expected, the highest levels of cation release, calcium (Ca2+) (Figure. 2a) and sodium ions
(Na+) (Figure. 2b), were observed for the composition with the highest dissolution rate, 0 and
1 mol% Ga2O3 containing glasses. The Ca2+ ion release data correlated with that of the
solubility data obtained. For the Ca2+ release profiles (Figure 2a), the gallium-free
composition released the greatest amount of ions. Also, compositions with higher sodium
mol% released more Na+ ions into solution, and it was directly proportional to the solubility
values, suggesting that sodium ions were released into solution first.
8
It can be seen from Figures 2a and b that greater amounts of Na+ ions than Ca2+ ions were
released from the compositions investigated. However, both Na+ and Ca2+ ion release profiles
showed clear differences between the compositions investigated, with a decrease in Na+ and
Ca2+ ion release seen with increasing Ga2O3 mol%. The greatest Na+ release was seen for the
gallium-free composition, with statistically not significant difference seen between the 3 and 5
mol% Ga2O3 compositions up to 48h. This may be expected as the gallium ions (Ga3+) were
added in place of Na2O, therefore, there was less sodium present in the other two
compositions.
The amounts of phosphorous ions released in this study appear to be linear in nature
(Figure.2c). The release of phosphorous ion decreased as the Ga2O3 content increased in the
glasses, with 5mol% Ga2O3 releasing the least amount of phosphorous. The use of ICP-MS
has enabled the detection of the total amount of phosphorous ions, and this method is found to
be superior to ion chromatography where availability of standards restricts the total detection
of different phosphate species.
0
5
10
15
20
25
30
35
40
45
50
55
60
0 24 48 72 96 120Time (h)
Ca
ion
rel
ease
(pp
m)
0 1 3 5
2 (a)
9
0
50
100
150
200
250
0 24 48 72 96 120Time (h)
Na
ion
rel
ease
(pp
m)
0 1 3 5
0
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
0 24 48 72 96 120Time (h)
P io
n r
elea
se (p
pm
)
0 1 3 5
2 (c)
2 (b)
10
As can be seen from Figure 2d, no Ga3+ was detected from the 0 mol% Ga2O3 composition as
expected, however clear differences are seen between the 1, 3 and 5 mol% Ga2O3
compositions. The 1 mol% Ga2O3 composition released the highest levels of Ga3+ ions, with
the 5 mol% Ga2O3 compositions releasing the least. The release profile of anionic species
mirrored those of the degradation rate, Na+ and Ca2+ ion release.
2.2. Bactericidal tests
This study was conducted to determine an effective range of Ga2O3-doped PBGs that exhibit
bactericidal activity using disk diffusion assay. The zones of inhibition (i.e. zones of no
visible bacterial growth surrounding the disks) were found to be larger in size for the 1mol%
compared to 3 or 5 mol % Ga2O3-doped PBGs when tested against S. aureus, E. coli, P.
aeruginosa, MRSA and C. difficile (Figure.3a).
0
5
10
15
20
25
30
35
40
45
50
55
60
0 24 48 72 96 120Time (h)
Ga
ion
rel
ease
(pp
m)
0 1 3 5
Figure 2. Cumulative ion release (a) calcium, (b) sodium, (c) phosphorous, and (d) gallium as a function of time for 0, 1, 3 and 5 mol% Ga2O3-doped PBGs.
2 (d)
11
In all the experiments, the gallium free PBGs were used as negative controls and the zones of
inhibition presented here is the test values minus that of gallium free PBGs. This result was in
good agreement with the Ga3+ ion release from the glass compositions investigated (Figure
2d). P. aeruginosa was found to be the most susceptible organism to Ga3+. Interestingly,
when gallium free PBGs were tested, a zone of inhibition was seen for S. aureus, MRSA and
C. difficile (data not shown). This could have been due to the change in pH during the glass
degradation as observed in water (Figure.1b).
0
5
10
15
20
25
30
1 3 5
Ga2O3 (mol%)
Dia
met
er (
mm
)
E.coli P.aeruginosa S.aureus MRSA C.difficle
Figure 3. (a) Disc diffusion assay conducted on 0, 1, 3 and 5 mol% Ga2O3-doped PBGs against Staphylococcus aureus, Escherichia coli, Pseudomonas aeruginosa, methicillin-resistant Staphylococcus aureus (MRSA) and Clostridium difficile
3 (a)
12
Initial viable count experiments were conducted on Ga2O3–doped PBGs for P.aeruginosa,
using the most potent Ga2O3 concentrations (1 and 3 mol% Ga2O3) (Figure 3b). Gallium-free
PBGs were used as controls, and initial viable counts were conducted prior to addition of the
PBGs to check the viability of the bacteria. Each point represents the log10 of the mean
number of viable count of three samples. Error bars represent standard deviations. Both
1mol% and 3 mol% Ga2O3–doped PBGs containing glasses showed statistically significant
(p=0.0001) reduction in the log10 of the mean number of viable cells compared to Ga2O3 free
control at 4h (Figure 3b). Moreover, the log10 of the mean number of viable cells on the
1mol% and 3 mol% Ga2O3–doped PBGs (p≤0.0006) displayed maximum effect at 12 h
compared to the control. This effect continued with time as 1mol% and 3 mol% Ga2O3–doped
PBGs, continue to show significant difference (p≤0.0004) to the control at 24h. However,
there were no statistically significant differences (p=0.080) observed between 1mol% and
3mol% Ga2O3–doped PBGs at this time point. These results indicated that the overall killing
Figure 3. (b) The effect of 0, 1 and 3 mol% Ga2O3-doped PBGs on the viability of suspensions of Pseudomonas aeruginosa after 4, 12 and 24h incubation. CFU= colony forming units (mean number of viable cells)
7
7.25
7.5
7.75
8
8.25
4 12 24
Time (h)
Lo
g C
FU
/mm
2
0 1 3
3 (b)
13
of the bacteria beyond this time points is largely due to the nutrient suppression than the
gallium concentration.
Recently, an antimicrobial approach using Ga3+ was reported that targets bacterial Fe3+
metabolism by exploiting the chemical similarities between Fe3+ and Ga3+ [5]. Given the
general ability of Ga3+ to substitute for Fe3+, it could interfere with many Fe-requiring
enzymes, including ribonucleotide reductase, which catalyzes the first step in DNA synthesis
[16]; superoxide dismutase and catalase, which protect against oxidative stress [17]; enzymes
involved in oxidative phosphorylation such as cytochromes; and others. It is also possible that
Ga3+ could act on several targets simultaneously [5], and if this is true, fully defining the
mechanism of action of Ga3+ may be difficult. However, this would also suggest that mutation
of a single intracellular target is unlikely to produce high-level Ga3+ resistance in target
organisms.
In vivo studies reported that the suppression of T cell and macrophage activation by Ga3+
could, however, partially counteract gallium's antimicrobial activities as some dose levels
aggravated progression of tuberculosis in gallium-treated guinea pigs [18]. Therefore, dose
versus response in vivo studies using several different infectious agents would elucidate the
relationship between the antimicrobial and immunomodulating activities of gallium. Results
of such studies would significantly help to determine the therapeutic doses of gallium in
treating infections.
2.3. Structural analysis of the gallium-doped phosphate-based glasses
2.3.1. Thermal analysis
Addition of 1 mol% Ga2O3 in PBGs did not produce a change in Tg; however addition of 3
and 5 mol% Ga2O3 produced a significant increase in Tg as given in Table.1.
14
Increasing Tg temperatures with increasing Ga2O3 mol% was expected as Ga2O3 is known as
a refractory material. This finding suggested that addition of 3 and 5 mol% Ga2O3 resulted in
the formation of more cross-linked glass structure. Such suggestion was also correlated well
with the degradation where the highly cross-linked (5 mol% Ga2O3 containing) glasses
showed lower degradation than gallium-free glasses. Tg is a measure of the bulk as opposed
to parameters such as Tc and Tm which can be used as a measure of a particular phase [19].
Andersson [20] proposed a simpler view of Tg against composition; he stated that the higher
the Na2O content, the lower the Tg. This statement was found to be in accordance with the
values obtained from this investigation as Ga2O3 was used to substitute Na2O.
2.3.2. NMR analysis
Figure 4I shows a stacked plot of the 31P MAS NMR spectra obtained with the frequency
scale expanded to show only the MAS centre bands, and the fitted peak data is given in Table
2. The connectivity of the phosphate network is commonly described by Qn notation, where n
refers to the number of bridging oxygen in the PO43- group. Two peaks are clearly visible at
chemical shifts of around −20 and −5 ppm, representing Q2 and Q1 phosphorous sites
respectively, and Figure 4II shows the fitting of the 0 mol% Ga2O3 spectrum, including fitting
of the spinning sidebands (the spinning sideband intensities were included in calculating the
relative abundance of each Qn species). No Q3 or Q0 sites were observed in any of the spectra.
Glass composition (mol%) Glass code P2O5 CaO Na2O Ga2O3
Density Tg (g.cm-3) (0C)
Ca16Na39P45
Ca16Na38P45Ga1
Ca16 Na36P45Ga3
Ca16 Na34P45Ga5
45 16 39 0 2.59 (±0.01) 341.69 (±0.46) 45 16 38 1 2.61 (±0.01) 341.11 (±2.82) 45 16 36 3 2.61 (±0.02) 359.26 (±1.81) 45 16 34 5 2.66 (±0.01) 369.99 (±0.57)
Table 1. Composition of phosphate-based glasses used in this study with corresponding Density and glass transition temperatures, Tg.
15
The 23Na MAS NMR spectra are shown in Figure 4III(a). The peak moved approximately 1
ppm to a more negative shift as the amount of Ga2O3 increased from 0 to 5 mol%. Figure
4III(b) shows a simulation of the 23Na spectrum of the 0 mol% Ga2O3 sample at two different
fields using a Gaussian distribution in quadrupolar coupling constant CQ to represent the
variation in Na environments present in the sample due to disorder. These simulations
yielded a mean value of CQ = (2.65 ± 0.15) MHz, a FWHM distribution in this parameter of
(2.15 ± 0.15) MHz, and a chemical shift value of δISO = (−3 ± 0.5) ppm. The asymmetry
parameter ηQ was kept at 0 for simplicity, although in reality a distribution in CQ would likely
mean a distribution in this, as well as the isotropic chemical shift. These parameters gave a
good fit to all four 23Na spectra, with only a variation in δISO, which moved 1 ppm downfield
as the Ga2O3 content increased from 0 to 5 mol%. These results imply that although there is
likely to be some association between the sodium and gallium cations, the extent of disorder
of the sodium environment is not significantly affected by the gallium content.
As the mol% of Ga2O3 was increased to 5, the relative abundances of the Q1 and Q2
phosphorous sites remained constant within experimental uncertainty. The 31P MAS NMR
line arising from the Q1 site broadened with increasing Ga2O3 content (Table 2), while the Q2
linewidth remained constant within experimental uncertainty. The chemical shifts of both
sites moved to a more negative value as the Ga2O3 content increased [see Figure 4III(b)], with
a larger change for the Q1 site than for the Q2. This is consistent with a previous study of
Ga2O3-containing sodium phosphate glass [21] and is due to increasing covalency in the
Mol% Q2 Shift Q2 Abundance Q2 Linewidth Q1 Shift Q1 Abundance Q1 Linewidth
Ga2O3 (± 0.2 ppm) / % (± 2 %) (± 0.5 ppm) (± 0.2 ppm) / % (± 2 %) (± 0.5 ppm)
0 −20.2 73 9.5 −3.6 27 8.5
1 −20.4 75 9.6 −4.4 25 9.4
3 −20.8 75 9.7 −6.4 25 10.9
5 −21.0 72 9.9 −7.8 28 11.2
Table 2. 31P MAS NMR fit parameters for the Q1 and Q2 sites.
16
P−O−Ga bonding interaction. A similar trend has been observed in CaO-Na2O-P2O5 glasses
as sodium is replaced by calcium [22]. The fact that the linewidth of the 31P NMR Q1 peak
increased while that of the Q2 remained roughly constant suggests that the gallium cations are
associating with the Q1 chain-end groups and increasing the chemical shift range of these
environments by partially replacing the ionic P−O−Na bonding interactions with more
covalent P−O−Ga bonding.
(ppm) -200 -100 0 100 200
4[I]
4[II]
17
4[III]
4[IV]
Figure 4[I]. 31P MAS NMR spectra obtained (a) 5 mol% Ga2O3, (b) 3 mol% Ga2O3, (c) 1 mol% Ga2O3 and (d) 0 mol% Ga2O3. [II] The fit of the 31P MAS NMR spectrum from the 0 mol% Ga2O3 sample, including the spinning sidebands. [III] (a) The 23Na MAS NMR spectra, and (b) simulation of the 0 mol % Ga2O3 sample at two different fields.[IV] The 71Ga MAS NMR spectra of the samples containing Ga2O3, (a) 5 mol % at 18.8 T, (b) 5 mol % at 14.1 T, (c) 3 mol % at 14.1 T and (d) 1 mol % at 14.1 T. Spectrum (a) took four hours to acquire, (b) and (c) took 24 hours each and spectrum (d) took 48 hours.
18
Figure 4IV shows the 71Ga MAS NMR spectra obtained from the 1, 3 and 5 mol% Ga2O3
samples. Figure 4IV(a) is from the 5 mol% Ga2O3 sample at 18.8 T, and figures 4IV(b),
4IV(c) and 4IV(d) are the 5, 3 and 1 mol% Ga2O3 samples respectively, all at 14.1 T. The
spectra all show a lower signal/noise ratio than the 23Na or 31P spectra due to the lower
amount of gallium present in the sample, the lower natural abundance of the 71Ga isotope
(39.9 % compared with 100 % for both 23Na and 31P), and also the wider lineshape due to
second-order quadrupolar broadening. The relatively large linewidth in these spectra meant
that the spinning sidebands lay very close to the centre-band, although they are not very
clearly visible due to their amplitudes being comparable to that of the noise. Each spectrum
shows a peak centred at approximately −50 ppm. The FWHM linewidth of this peak is
approximately 100 ppm, and for the 5 mol% Ga2O3 sample this width did not appreciably
decrease when the field was increased from 14.1 to 18.8 T. A previous 71Ga MAS NMR
study on Ga2O3-Na2O-P2O5 glasses identified a peak at −60 ppm associated with octahedrally
coordinated gallium and one at 120 ppm due to tetrahedral gallium [23]. This suggests that the
71Ga NMR peak observed here arises from octahedrally coordinated gallium. The fact that the
linewidth does not appreciably decrease between 14.1 and 18.8 T indicates that chemical shift
dispersion is the dominant broadening mechanism at these fields rather than second order
quadrupolar broadening. This suggests a distribution of octahedral gallium sites (i.e. the
gallium exists in a disordered environment). The presence of some tetrahedral gallium cannot
be ruled out since a small peak may be present at around 120 ppm in the spectrum from the
sample containing 5 mol% Ga2O3, but certainly the gallium is mostly octahedral.
2.3.3. Vibrational spectroscopy
Figures 5(I) and 5(II) show the FTIR and Raman spectra of Ga2O3-doped compared to Ga2O3-
free PBGs respectively.
19
1600 1400 1200 1000 800 600 4000.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
νs(O-P-O)
νas
(O-P-O)ν
s(PO
3)-
νas
(PO3)-
νs(PO
2)-ν
as(PO
2)-
(d)
(c)
(b)
Wavenumber / cm-1
Abs
orba
nce
(a)
δ(O-P-O)
1600 1400 1200 1000 800 600 400 200
0
250
500
750
1000
1250
δ(O-P-O)νas
(PO3)-
νas
(PO2)- ν
s(O-P-O)
νs(PO
2)-
Cou
nts
Wavenumber / cm-1
(a)
(b)
(c)
(d)
5 [I]
5 [II]
Figure 5. Structural analysis of the Ga2O3-doped PBGs. [I] FTIR spectra from (a) 0 mol% Ga2O3, (b) 1 mol% Ga2O3, (c) 3 mol% Ga2O3 and (d) 5 mol% Ga2O3. [II] Raman spectra from (a) 0 mol% Ga2O3, (b) 1 mol% Ga2O3, (c) 3 mol% Ga2O3 and (d) 5 mol% Ga2O3.
20
The absorption bands in the vibrational spectra have been assigned according to the literature
[24-27]. The band near 1280 cm−1 is assigned to the asymmetric stretching mode of the two non-
bridging oxygen atoms bonded to phosphorus atoms in the Q2 tetrahedral sites, νas(PO2)–; the
shoulder at 1180 cm−1 is assigned to the symmetric stretch of the same structural unit,
νs(PO2)–. The absorption bands near 1100 and 1000 cm−1 are assigned to the asymmetric and
symmetric stretching modes of chain-terminating Q1 groups (νas(PO3)2– and νs(PO3)
2–),
respectively. The band close to 1100 cm−1 has a component at 1150 cm−1 assigned to Q1 end
groups associated with Na+ ions [25]. The absorption band near 900 cm−1 is assigned to the
asymmetric stretching modes of the P–O–P linkages, νas(P–O–P), and the bands at 770 and
720 cm−1 assigned to the symmetric stretching modes of these linkages, νs(P–O–P). The broad
absorption around 540 cm−1 is attributed to O−P−O deformation modes. The weak shoulder to
the high frequency side of this band at ~610 cm−1, observed in the spectrum from the sample
with the highest gallium content, can be assigned to vibrations localized on GaO4 tetrahedra
[26]. The Raman spectra all exhibit five significant absorption bands. The two most intense
absorptions at 1170 and 670 cm−1 are assigned to νs(PO2)– and νs(P–O–P) modes, respectively.
The weaker bands at 1260 and 1020 cm−1 are due to the antisymmetric νas(PO2) – and νas(PO3)
– vibrations, respectively, and finally, the broad low-energy band with contributions at 380
and 340 cm−1 is attributed to O−P−O deformation modes.
The vibrational spectra shown in Figures 5(I) and 5(II) are quite typical of those from PBGs
close to the metaphosphate composition [24, 27]. Despite this, there are subtle, but significant,
differences between spectra from samples of varying gallium content. The significant change
in the FTIR spectra is the reduction in the intensity of the band at 1150 cm−1 with increasing
gallium content. This band arises from modes involving Q1 end groups associated with Na+
ions [25] and perhaps it is not surprising that its intensity should be reduced as the Na+ ions are
replaced by Ga3+ ions. However, in agreement with the results from the 31P NMR study, this
21
change illustrates that the bonding interaction of the Ga3+ ions with the Q1 end groups is very
different to that of the Na+ ions. The other clear change in the infrared spectra is the gradual
change in the shape of the two νs(P–O–P) bands from two overlapping peaks in the spectrum
from the sample containing no gallium to one broad feature in that from the sample with the
highest concentration of gallium (5 mol% Ga2O3). It is common for the infrared spectra from
CaO-Na2O-P2O5 glasses to exhibit a split νs(P–O–P) absorption band [28], and it is known that
the energy of the νs(P–O–P) mode varies with the P–O–P bond angle because this angle
affects the amount of π bond character of the bridging bonds and hence their vibrational force
constants [26]. In the infrared spectra of Ga2O3-P2O5 glasses, only one νs(P–O–P) band is
observed at 760 cm−1 [26]. Hence, it is probable that the gradual change in the shape of the
νs(P–O–P) band with gallium content in the spectra presented here is caused by the growth of
a peak at 760 cm−1 between the partially overlapping peaks at 770 and 720 cm−1. Again this
change provides evidence for a bonding interaction between the phosphate chains and the
Ga3+ ions. The final and smallest change is the growth of a shoulder observed in the infrared
spectra from the samples with the highest gallium content at ~610 cm−1 on the on the high
frequency side of the broad peak attributed to O−P−O deformation modes . Although this
feature is only very weak, even in the spectrum from the sample containing 5 mol% Ga2O3, its
appearance provides some evidence for the presence of GaO4 tetrahedra in the glass structure.
This result does not contradict the 71Ga NMR result since the vibrations associated with GaO6
octahedra are expected to lie under the broad absorption due to the O−P−O deformation
modes [29] and are not observable here. Both the FTIR and 71Ga NMR spectra are consistent
with most of the gallium present in octahedral coordination with a small proportion
tetrahedrally coordinated.
The Raman spectra, however, shows one significant change, which is the change in shape of
the feature due to O−P−O deformation modes from two overlapping peaks at 380 and 340
22
cm−1 in the spectrum from the sample containing no gallium to one broad peak centred at 350
cm−1 in that from the sample containing 5 mol% Ga2O3. A peak at 350 cm−1 has previously
been observed in the Raman spectra from Ga2O3-P2O5 glasses [26]. The intensity of this peak
grew as a function of gallium content and consequently was assigned to symmetric bending
vibrations of P−O−Ga linkages. The changes in the Raman spectra observed here are
consistent with the growth of a band at 350 cm−1 with increasing gallium content and thus
provide further evidence for P−O−Ga bonding interactions. Furthermore, since the previous
vibrational study on Ga2O3-P2O5 glasses concluded that the nature of the P−O−Ga bonding
was highly covalent, it is likely that the P−O−Ga bonding in the glasses studied here has the
same character.
Thus, the vibrational spectroscopy provides evidence of the covalent nature of the P−O−Ga
interaction. This observation is consistent with the measured degradation rates which showed
a decrease with increasing gallium content, i.e. the Ga2O3-doped PBGs are highly
polymerised with the gallium increasing the covalency of the bonding and leading to a more
durable glass.
3.Conclusion
This paper reports the production of a novel quaternary Ga2O3-doped PBGs (0, 1, 3, and 5
mol% Ga2O3) with their antibacterial properties, physico-thermal properties, solubility, pH
change and ion release. The data obtained from the thermal and solubility analyses were
attributed to the packing density of the 45mol% P2O5 compositions. The solubility was seen to
decrease with increasing Ga2O3 mol%; FTIR and Raman spectroscopy provide some insight
into the likely reason for this via an understanding of the network bonding characteristics.
Both 0 and 1 mol% Ga2O3 compositions showed a gradual increase in pH with time, and this
was due to the depletion of H+ in the solution occurred resulted from its substitution with that
of Na+ and Ca2+ ions released into the solution . The ion release profiles exhibited similar
23
trends to the degradation rates obtained, and a decrease in the rate of release was seen for the
P ions with increasing Ga2O3 content. It was suggested that these ions were branched and
cross-linked with the Ca ions.
In disk diffusion assays, these compositions demonstrated antibacterial effects predominantly
against Pseudomonas aeruginosa, Staphylococcus aureus, and Escherichia coli , along with
small effect on methicillin-resistant Staphylococcus aureus and Clostridium difficile. Overall,
1 mol % Ga2O3-doped PBGs investigated was sufficient to mount a potent antibacterial effect
against the test organisms, and these compositions also gave excellent long-term release of
Ga3+ ions into the medium. Our findings suggested that this Ga2O3 containing glasses, 1
mol% in particular, holds promise as an antimicrobial agent and could offer some advantages
over conventional therapeutic agents as antibiotic-resistant organisms (even those with multi-
drug resistance) are likely to be sensitive to Ga3+. This is likely due to the fact that Ga3+ works
by a completely different mechanism to conventional drugs. Moreover, the fact that Fe3+
levels are so low in human tissues, and that Ga’s activity is increased when Fe3+ is limited [4],
raises the possibility that Ga3+ may be more effective in vivo than our in vitro data indicates.
These data, along with the fact that Ga3+ is FDA approved (for i.v. administration) and there
is a dearth of new antibiotics in development, make Ga3+ a potentially promising new
therapeutic agent for bacterial pathogens especially MRSA and C. difficile. Moreover, Ga3+ is
reported to inhibit bone resorption and stimulate bone formation through its action on
osteoblasts [4] and hence the Ga2O3 doped novel glass composition reported in this study
might well have applications in bone tissue engineering.
4. Experimental
4.1.Preparation of gallium-doped phosphate-based glasses
Phosphate-based glasses were produced using NaH2PO4 (BDH), P2O5 (Sigma), and CaCO3
(BDH). For the production of gallium containing PBGs, Ga2O3 (Sigma) was also used as
24
shown in Table I. The required amount of chemicals were weighed and placed into a
Pt/10%Rh crucible (Johnson Matthey, Royston, UK). The crucible was then placed in a
preheated furnace at 1100°C for 1hour. The molten glass was then poured into graphite
moulds, which had been preheated to 350°C. The glass samples were allowed to cool to room
temperature, and the resulting glass rods were cut into discs by using a rotary diamond saw
(Testbourne Ltd., Basingstoke, UK). Density measurements were conducted on triplicate
samples using Archimedes’ Principle.
4.2.Degradation study
Ga2O3-doped PBGs rods (5 mm diameter and 2 mm thickness) with different contents of
gallium ions were placed in plastic containers, filled with 50 ml of deionised water (pH 7±0.5),
and then placed in a 37°C incubator. At various time points (6, 24, 48, 72 and 120h), the
three disks were taken out of their respective containers, and excess moisture was removed by
blotting the samples dry with tissue prior to weighing them. All the disks were placed into a
fresh solution of deionised water and placed back into the 37°C incubator. To obtain the rate
of weight loss, the initial weight (M0) of each sample was measured as well as the weight at
time t (Mt) to give a weight loss per unit area thus: weight loss=(M0–Mt)/A, where A is the
surface area (mm2). The measurements were carried out in triplicate, and the weight loss per
unit area were plotted against time. The slope of this graph gave a degradation rate value in
terms of mg.mm-2 h-1, which was determined by fitting a straight line of the form y = mx
through the origin.
4.3. pH measurements
The pH measurements of the degrading medium were taken at each time point (6, 24, 48, 72
and 120h) using a Hanna Instruments pH 211 Microprocessor pH meter (BDH, UK) with an
attached glass combination pH electrode (BDH, UK). The pH electrode was calibrated using
pH calibration standards (Colourkey Buffer Solutions, BDH, UK).
25
Both dissolution studies and standards, for ion release study, were prepared using high purity
water. This was obtained from a PURELAB UHQ-PS system (Elga Labwater, UK), which
polished the water obtained from an existing water purification system, to a purity level of
18·2 MΩcm-1 resistivity.
4.4. Ion release study
Ion release studies were simultaneously conducted, and the medium was analysed for Na+ and
Ca2+ using ion chromatography (Dionex, UK). Both Gallium and Phosphorous ion release
was measured using inductively coupled plasma mass spectrometry, ICP-MS, which is an
analytical technique that determines the elements content in the samples. It is accomplished
by counting the number of ions at a specific mass of the element and detects only elemental
ions and can determine the individual isotopes of each element. The ICP-MS (Spectromass
2000 by SPECTRO) was used to determine amounts of both gallium and phosphorous ions
released from all tested glass compositions at the previously mentioned time points. The
instrument detection limit of the gallium and phosphorous is in the range 1-10 ppt. However,
instrument was calibrated for the predicted concentration in the range 0.1-1000ppb by mixing
single element standards obtained from Sigma and diluted in ultra pure water.
4.5. Inhibition of microbial growth by gallium-doped PBGs
Ga2O3-doped PBGs (1, 3, and 5 mol % Ga2O3) were investigated for their ability to inhibit
microbial growth using a disk diffusion methodology (BSAC Disk Diffusion Method for
Antimicrobial Susceptibility Testing, Version 4, 2005). Isosensitest agar (Oxoid, Basingstoke,
UK) plates were inoculated with a standardized culture of S. aureus (NCTC 6571), E. coli
(NCTC 10418) and P. aeruginosa (PA01). Columbia agar (Oxoid, Basingstoke, UK) with 2%
NaCl plates were inoculated with MRSA-16. In the case of the anaerobic bacterium C.
difficile, Wilkins-Chalgren agar plates supplemented with 5% horse blood (E & O
Laboratories, UK) were used. Ga2O3-doped PBGs disks of 5 mm diameter and 2 mm
26
thickness were then placed on the inoculated plates. Disks not containing any gallium were
used as negative controls. These plates were then incubated overnight in air at 37°C except C.
difficile which was incubated for 48 hours in an anaerobic chamber. The diameters of any
zones that had formed around the disks were measured in triplicate using calipers.
P. aeruginosa (PA01) which showed the highest susceptibility to the Ga2O3-doped PBGs
were inoculated into 10mL of nutrient broth and incubated overnight at 370C with 200 rpm
agitation in an Orbital Shaker (Stuart Scientific, UK). The overnight cultures were used to
inoculate 5mL volume of phosphate buffer saline (PBS; Oxoid) to a standardized optical
density of 0.03 at a wavelength of 600 nm (OD600). Ga2O3-doped PBGs disks of 5 mm
diameter and 2 mm thickness were added to each tube, with the gallium free disk (0 mol%
Ga2O3) used as controls. The tubes were then incubated at 370C. At various time intervals (1,
12 and 24 h) serial dilutions of the suspensions were carried out in PBS. 50 µl volumes of the
suspension and each dilution were spread onto McConkey agar (Oxoid, Basingstoke, UK)
plates. The plates were then incubated aerobically at 30°C for 48 h. For each type of disc,
viable counts (colony forming units; CFUs) were conducted in triplicate.
4.6. Thermal and Structural analysis of the gallium-doped phosphate-based glasses
4.6.1. Thermal Analysis
A portion of each glass sample was crushed into powder using a vibratory agate mill, and the
glass transition temperature (Tg) was determined using a Pyris Diamond Differential Scanning
Calorimetry (Perkin-Elmer Instruments, UK). The instrument was calibrated using the
manufacturer’s instructions, with indium and zinc as standards, and all tests were carried out
under nitrogen purge. Samples (n=3) of 5mg were heated, cooled and reheated from 25 to
550 °C at 100°C.min-1. Tg was calculated by the onset of change in the endothermic direction
(upwards) of the heat flow.
27
4.6.2.NMR
23Na MAS NMR experiments were conducted using a 3.2 mm diameter rotor spinning at 30
kHz. Spectra were acquired using a Bruker Avance II spectrometer attached to a 14.1 T
magnet (23Na Larmor frequency 158.7 MHz). Aqueous NaCl was used as a reference, with
the sharp resonance from this set to 0 ppm. The liquid 90° pulse length was determined as 2.5
µs, although a much shorter pulse length (0.5 µs) was used on the solid samples. A one-pulse
sequence was used, with a recycle delay of 5 seconds. Certain 23Na spectra were also
recorded at 7.05 T under similar conditions.
31P MAS NMR experiments were conducted using a 4 mm diameter rotor spinning at 10 –
12.5 kHz. Spectra were acquired using a Chemagnetics Infinity Plus spectrometer attached to
a 7.05 T magnet (31P Larmor frequency 121.5 MHz). NH4H2PO4 was used as a secondary
reference compound, the signal from this set to 0.9 ppm. A pulse length of 1.5 µs was used
(corresponding to a ~30° tip angle), with a recycle delay of 5 seconds.
71Ga MAS NMR experiments were conducted at 14.1 T (71Ga Larmor frequency 183.0 MHz)
using a Bruker Avance II spectrometer and a 3.2 mm rotor, spinning at approximately 18 kHz.
A one-pulse sequence was used with a pulse length of 0.75 µs corresponding to a tip angle of
~30°, and a recycle delay of 2 seconds. Spectra were references to aqueous Ga(H2O)63+ at 0
ppm. The 5 molar % Ga2O3 sample was also investigated at 18.8 T using a 2.5 mm probe
spinning at 22 kHz and similar experimental parameters.
All spectra were processed using TOPSPIN 2.0 or Spinsight and fitted using either dmfit2007
[29] or QuadFit [30].
4.6.3.Vibrational Spectroscopy
Infrared spectra were recorded in transmission mode on a Biorad FTS175C spectrometer
controlled by Win-IR software. Samples were diluted in dry KBr and scanned in the range
4000-400 cm−1. Each spectrum was the result of summing 64 scans.
28
The Raman data were collected using a Jobin Yvon microRaman module attached to an
Olympus microscope (BX40). The illuminating laser line was at 632.8 nm (HeNe). The
spectrometer had a 1200 gr/mm grating. The spectra were recorded on a liquid nitrogen
cooled CCD. Typical sample exposure times were 10x10 secs.
Acknowledgements
This work was supported by the EPSRC, UK grant no. GR/T21080/01, EP/C000714/1 and
EP/C000633/1. The authors would like to thank Nick Foster for his help with the collection of
the Raman data. This work was undertaken at UCLH/UCL which received a proportion of
funding from the department of health’s NIHR Biomedical Research Centres Funding
Scheme, UK.
29
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