dimethyl suberimidate cross-linked pericardium tissue: raman spectroscopic and atomic force...
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Dimethyl suberimidate cross-linked pericardium tissue: Raman
spectroscopic and atomic force microscopy investigations
Maria Jastrzebskaa,*, Justyna Zalewska-Rejdaka, Roman Wrzalikb, Antoni Kocotb,Bogdan Barwinskic, Iwona Mrozc, Beata Cwalinaa
aDepartment of Biophysics, Faculty of Pharmacy, Medical University of Silesia, Ostrogorska 30, 41-200 Sosnowiec, PolandbDepartment of Biophysics and Molecular Physics, Institute of Physics, University of Silesia, Universytecka 4, 40-007 Katowice, Poland
cInstitute of Experimental Physics, University of Wrocław, Plac Maxa Borna 9, 50-204 Wrocław, Poland
Received 7 September 2004; revised 2 November 2004; accepted 2 November 2004
Available online 18 January 2005
Abstract
Chemically stabilized pericardium tissue is widely used as a tissue-derived biomaterial for the preparation of bioprostheses such as heart
valves or vascular grafts. The bifunctional imidoester dimethyl suberimidate (DMS) belongs to the wide class of the cross-linking reagents
and is often used to cross-link a variety of proteins, including collagen matrices and collagen-based tissues. Raman spectroscopy in the wide
frequency range 200–4000 cmK1 and contact mode atomic force microscopy (AFM) have been employed to investigate the structural
changes and chemical bonds in DMS cross-linked porcine pericardium tissue. It has been found, that in addition to the commonly accepted
reaction with the 3-amine groups of lysine or hydroxylysine residues, DMS may interact also with the carbonyl CO and amide NH groups of
the peptide bond in collagen. Our paper presents for the first time spectral evidence for the peptide contribution to the formation of DMS–
collagen cross-links. The results confirm also possible competition between the hydrolysis of the free imidoester group and cross-linking
reaction. Products of the partial alkaline hydrolysis of DMS have been found in the spectra. The observed changes in the surface topography
of the fibrils as well as in their spatial organization in the tissue support the formation of both intra- and interfibrillar cross-links in DMS-
stabilized tissue.
q 2005 Elsevier B.V. All rights reserved.
PACS: 87.14.-g; 87.64.Je; 07.79.Lh
Keywords: Cross-linking; Collagen; Raman spectroscopy; Atomic force microscopy
1. Introduction
Chemically stabilized pericardium tissue is widely used as
bioprostheses in replacement surgery of the vascular system,
e.g. in arterial reconstruction or cardiac valve replacement
[1]. Chemical stabilization with different reagents, e.g.
glutaraldehyde (GA) or dimethyl suberimidate (DMS),
improves the mechanical properties, reduces immuno-
genicity and enzymatic or chemical degradation processes
of the material. However, there are several factors limiting
the functional lifetime of the tissue-based bioprostheses such
0022-2860/$ - see front matter q 2005 Elsevier B.V. All rights reserved.
doi:10.1016/j.molstruc.2004.11.040
* Corresponding author. Tel.: C48 322925541.
E-mail address: [email protected] (M. Jastrzebska).
as calcification, cytotoxicity of the cross-linking reagent or
mechanical fatigue of the material [2].
Pericardium tissue is composed mainly of collagen type I
[3]. Chemical stabilization introduces cross-links into
molecular structure of collagen fibrils. Multiple cross-
linking techniques have been explored in an attempt to find
the ideal procedure to stabilize the collagen-based tissue
[1,2].
The bifunctional imidoester DMS has been employed to
cross-link a variety of proteins and supramolecular
structures, including collagen matrices and collagenous
tissues. Imidoesters are highly specific reagents for amine
groups in proteins, as shown in [4,5]. DMS is widely used as
an alternative fixative reagent to GA because of its lower
cytotoxicity. For example, rat fibrous dermal collagen has
Journal of Molecular Structure 744–747 (2005) 789–795
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M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795790
been cross-linked with DMS for use as dermal implant,
since DMS was found to be less cytotoxic than glutar-
aldehyde. DMS has also been evaluated as a cross-linking
agent for human dermis and porcine aortas for use as
bioprostheses [6].
Mechanisms of the DMS–protein interactions are not
fully understood. It is known, that DMS reacts with the amine
groups of collagen to form diamidine derivative structures
[6]. Another study [6,7] explains, that diimidoesters like
DMS do not polymerize and form cross-links only with free
amine groups from lysine or hydroxylysine residues that are
separated by a distance equivalent to the molecular length of
DMS, i.e. about 11 A. This may restrict the number of cross-
links being introduced into the collagen matrix. DMS cross-
linked collagenous membranes seem to be more biocompa-
tible than glutaraldehyde-treated membranes as revealed by
subcutaneous implantation studies [6]. DMS cross-linked
membranes promote fibroblast migration and proliferation
and act as a scaffold for tissue regeneration.
Raman spectroscopy is a very powerful tool for studying
the structure and molecular interactions of many complex
molecules. This method was successfully used for studying
the mechanism of GA-collagen cross-linking [8]. One of the
greatest advantages of this technique is its ability to provide
information about the structure and interactions of biomo-
lecules in their microenvironment within intact cells and
tissue. The technique is not destructive and does not require
homogenization, extraction or the use of dyes, labels or
other contrast-enhancing agents. As a vibrational technique,
Raman spectroscopy is more advantageous than IR
spectroscopy, e.g. the structural properties of molecules in
aqueous solution are more easily observed [8].
Atomic force microscopy (AFM) is being widely applied
to study surface topography of many biological structures,
at high resolution, in liquid or gaseous environments, so that
materials can be studied in hydrated conditions close to their
native state [9].
The aim of the present work was to study structural
changes and chemical bonds, which are involved in DMS
cross-linking of pericardium tissue, using Raman spec-
troscopy and atomic force microscopy.
2. Experimental
2.1. Materials
Pericardium tissues from hearts of 5–6-month-old pigs
were obtained fresh from slaughter. Fatty tissues and
sections with heavy vasculature or attached ligaments
together with a serosal layer were gently removed from
each pericardium. Three 15!10 mm rectangles were
excised from each pericardium.
2.2. Chemical treatment of pericardium tissue
Stabilization with DMS was performed using 1% DMS
(SIGMA) solution in 0.2 M Tris buffer (pH 9) at 4 8C for 3 h
in dark. After chemical treatment pericardium tissue was
rinsed three times with distilled water and then kept in
phosphate buffer (pH 9) at 4 8C until the measurement could
be made.
2.3. Deuteration
Samples of the pericardium tissue designed for deutera-
tion were transferred into D2O (deuterium oxide 99.8%,
SIGMA). Deuteration was performed in excess of D2O,
5 ml/mg of dry tissue, for 0.5 h.
2.4. Raman spectra
Raman spectra were recorded using a LabRam Raman
spectrometer (Jobin-Yvon-Horiba) comprising an Olympus
BX40 confocal microscope. It was equipped with a grating
monochromator and a charge-coupled device (CCD)
Peltier-cooled detector (1024!256 pixels). The incident
laser excitation was provided by an air-cooled argon laser
source operating at 514.5 nm. The power at the exit of a
50! objective was 50 mW. The spectra were recorded with
resolution of 2.5 cmK1, a collection time of 60 s and an
accumulation of 10 scans. In order to avoid undesirable
Rayleigh scattering, two notch-filters were used cutting the
laser line at 100 cmK1. Pure silica was used to calibrate the
spectrometer.
Baselines of the individual Raman spectra were adjusted
with 20–30 point baseline correction functions using
GRAMS 32.
Spectral intensity was normalized using the CC
vibrational mode of phenylalanine (Phe) aromatic ring
(1004 cmK1) as an internal standard.
Native and DMS cross-linked pericardium tissues are
materials of considerable surface heterogeneity. Raman
spectra were recorded from 10 different points of each
sample surface. The results presented in the paper show
representative records of the Raman spectra.
The measurements were conducted at room temperature
(20 8C) without thermostating.
2.5. Atomic force microscopy
AFM images were obtained in the contact mode, using
the NanoScope E, Digital Instruments, USA, equipped with
the OTR8 probe (Veeco NanoProbee). The length and the
spring constant of the applied V-shaped cantilever were
200 mm and 0.15 N/m, respectively. The constant forces
used were about 10 nN. All measurements were performed
in air, at room temperature. The samples were placed onto
clean surfaces of glass microscope slides. After 20 min,
M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795 791
when the excess of water had evaporated from the sample
surface, the AFM images were recorded.
Two standard AFM signals, i.e. the height and the
differential signal deflection were registered. The height
image corresponds to the topography of the sample, whereas
the deflection image is sometimes more useful in direct
observations. The lateral and height resolutions were 10 and
1 nm, respectively. All AFM images were processed using
the software package WSxM (Spain).
3. Results and discussion
3.1. Raman spectra
Figs. 1 and 2 show the Raman spectra of porcine
pericardium tissue in its native state and after DMS
treatment. The spectra were recorded in two wavelength
ranges, 200–2000 and 2000–4000 cmK1, respectively.
Frequencies and assignments of the bands are collected in
Table 1.
The spectrum in the range 2000–4000 cmK1 has been
recorded for the deuterated tissues. H to D exchange shifts
the OH vibrational mode of bulk water to lower frequencies.
After short equilibration time in D2O (e.g. 0.5 h), the
remaining broad signal in the range 3200–3700 cmK1
Fig. 1. Raman spectra of the native and DMS-stabilized porcine pericardium tiss
Table 1. Peaks, which are discussed in the paper in terms of the DMS–collagen in
inset. Band at 1667 cmK1 is assigned to the CaN stretching vibration [28].
corresponds to the more tightly bound water with the slow
rate of H to D exchange. Following literature data, the
distinct peak at 3328 cmK1 is assigned as an NH vibration
from amides or amines, as shown in Table 1. Because of the
very slow rate (over several days) of the amide- or amine-
proton exchange in collagen, the reduction in the NH
vibrational mode seems to be negligible [10].
Collagen type I is the main component of the fibrous layer
of pericardium tissue. According to the earlier findings [11],
the spectra in Figs. 1 and 2 show bands, which are
characteristic for collagen type I. The basic collagen
molecule consists of a right-handed superhelix formed by
three helical strands. The positions of the amide I
(1655–1667 cmK1) and amide III (1241–1272 cmK1)
bands as well as a strong C–C stretch band around
939 cmK1, support the presence of the helical conformation
in a collagen molecule [12,15]. The observed increase in the
band intensity around 940 cmK1 can point to a stabilizing
effect of the DMS cross-linking on collagen helical structure.
The interactions of the DMS with the collagen from
porcine pericardium tissue result in formation of stable
cross-links. This chemical modification induces changes in
the Raman spectra of the tissue. The analysis of the position
and the intensity of the Raman bands for native and DMS-
stabilized tissues allowed us to recognize the following
types of the DMS–collagen interactions:
ue, in the frequency range 200–2000 cmK1. Peak assignments are given in
teractions are in bold. Raman spectrum of the solid DMS is presented as an
Fig. 2. Raman spectra of the deuterated native and DMS-stabilized porcine pericardium tissue, in the frequency range 2000–4000 cmK1. The inset shows the
repeated measurements in the frequency range 3200–3700 cmK1.
M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795792
3.1.1. Interaction with amine R–NH2 group
According to literature data [6,7], the principal reaction
involves formation of cross-links between the methoxy
group of DMS and 3-amine group of lysine or hydroxylysine
residues in collagen with the release of methanol, as seen in
Scheme 1. Fig. 2 shows Raman spectra for deuterated
tissues with the distinctly seen peak at 3328 cmK1, which is
assigned to the NH vibration from the amines or amides
(Table 1). For more clear presentation, the inset in Fig. 2
shows the repeated measurement in the frequency range
3200–3700 cmK1. Both figures do not show any changes in
the 3328 cmK1 peak after DMS treatment. This result can be
explained by the reaction presented in Scheme 1. According
to the scheme, each molecule of DMS introduces two NH2
groups, simultaneously two amine groups from lysine or
hydroxylysine in collagen are involved in cross-linking
reaction. As a result, there is no change in the amount of
the NH2 groups after DMS treatment and in consequence,
no change in peak intensity at 3328 cmK1.
3.1.2. Interaction of peptide NH group with DMS
The amide III band originates from the NH in plane
deformation around 1270 cmK1 coupled to the CN stretch-
ing mode at 1247 cmK1. As shown in Fig. 1, after DMS
treatment an increase in the CN band intensity and,
simultaneously, a decrease in the NH band intensity are
observed. This effect can be explained by the formation of a
secondary amide type bond between the NH group of
collagen and methoxy OCH3 group from DMS with the
release of methanol, as seen in Scheme 2.
Release of methanol presented in Scheme 2 can be sup-
ported by the increase in the peak intensity at 1319 cmK1,
which is assigned as the OH vibration (Table 1).
3.1.3. Interaction of peptide CO group with DMS
Fig. 1 shows a decrease in the amide I band intensity at
1665 cmK1 for the DMS cross-linked tissue. The main
contribution to the amide I band is the peptide carbonyl
stretching vibration in the range 1655–1667 cmK1. The
observed decrease in the band intensity can be interpreted as
the formation of covalent bond between carbon of the
peptide bond and NH group of the DMS molecule. The
reaction is shown below (Scheme 3).
The observed decrease in band intensity of the carbonyl
bond should be accompanied by the increase in the CaN
bond vibration, according to Scheme 3. In the
Raman spectrum of the solid DMS, the band around
1667 cmK1 is assigned to the CaN stretching vibration
Table 1
Band assignments of Raman spectra of porcine pericardium tissue in native state and after DMS cross-linking treatment
Native pericardium DMS-pericardium Assignment of vibrational mode Ref.
722 719 (CH2) deformation in phase [33]
760 758 (CCO) [34]
772 (PO) stretch [13]
814 814 (COC) deformation [8,33,34]
856 855 (CC) aromatic (Pro, Tyr) [13–15]
875 874 (CC) aromatic (Hyp, Try) [14,15,35]
922 922 (CH2) wagging out of phase [15,34]
939 939 (CC) stretch [8,12,13,36]
965 (PO) sym. stretch [37]
1004 1003 Phe, (CC) ring breathing [13,15,33,38]
1032 1034 (CC) stretch of pyridine ring [20,33]
1065 1065 (COC) deformation [21,22]
1083 1083 (CN)/(CC) deformation [15,23,33]
1102 1099 (COC) stretch asym. [24]
1124 1124 (COC)/ (CN) stretch [15,25,26]
1164 1166 (CC) out of plane/phase [33,34]
1178 1177 (CC) stretch, Tyr [14,15,33–35]
1206 1206 (C–C6H5) stretch [13,15,33,38]
1247 1245 (CN) stretch/Amide III [12,15,26,27,34]
1273 1270 (NH) deformation/Amide III [12,15,26,27,34]
1319 1322 (C–OH) bend [24]
1343 1340 (CH3, CH2) deformation [15,23,28,34]
1397 1395 (CH2) bend [33,34]
1428 1427 (COOK) stretch [15]
1452 1452 (CH) deformation/scissor [26–30,34]
1573 1573 (NH2) scissor/Amide II [8,24]
1665 1664 (CaO) stretch/Amide I [12,26,31,32]
2200–2800 (OD) stretch [10,11]
2800–3000 (CH2, CH3) stretch sym., asym. [30,32–34]
3067 3067 (CaCH) stretch [33,34,38]
3328 3326 (NH) stretch sym. [8,10,30]
sym., symmetric; asym., asymmetric.
Scheme 3.
Scheme 2.
Scheme 1.
M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795 793
Fig. 3. AFM height (A) and deflection (B) images (1.3!1.3 mm) for native
pericardium tissue. The curve (E) shows the axial profile along the line 1 for
the native collagen fibril. AFM height (C) and deflection (D) images (0.7!
0.7 mm) for the DMS-stabilized pericardium tissue. The curve (F) shows the
axial profile along the line 2 for the DMS cross-linked collagen fibril.
M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795794
(inset to the Fig. 1). Conjugation of the CaN with amide
carbon lowers the CaN stretching frequency to a value
below 1667 cmK1 located on the shoulder of the amide I
band. As a result, an increase in the CaN vibration is very
hardly seen on the shoulder of the strong amide I band.
As it was mentioned earlier, the increase in the OH peak
intensity at 1319 cmK1 can also correspond to the formation
of the hydroxyl group, which is attached to the amide
carbon.
The analysis of the Raman spectra shown in Fig. 1
reveals also a spectral evidence for the possible partial
hydrolysis of the DMS. The evidence presented in the
literature points to two major hydrolytic pathways for an
imidoester, giving either oxygen ester and ammonia or
amide and alcohol [4]. Yuthavong et al. [4] found, that at
least 84% of DMS (10 mM) was allowed to hydrolyze in
0.1 M triethanolamine buffer, pH 7.0, with the release of
ammonia. At higher pH values, e.g. pH 9, reaction of DMS
and lysine or hydroxylysine is improved and the yield of
cross-linking products is raising. Under our experimental
conditions, it has been found, that slow alkaline hydrolysis
of DMS can occur. Fig. 1 shows, that after DMS treatment
there is an increase in the 1428 cmK1 peak intensity, which
is assigned to the COOH vibration. At alkaline pH, the
oxygen ester is converted to the suberic acid with the release
of alcohol. The observed increase in the band intensity at
1555–1575 cmK1 for the DMS treated tissue can support
the presence of ammonium ions. The bands visible in the
spectral region 1555–1575 cmK1 are usually assigned to the
amide II band, which is weak or not seen at all in Raman
spectra. The band in the region 1555–1575 cmK1 can also
correspond to the scissoring vibration of the amine NH
group (Table 1).
3.2. AFM images
Fig. 3 shows the height and deflection images for native
(Fig. 3A,B) and DMS-stabilized (Fig. 3C,D) porcine
pericardium tissue. The axial profiles taken from the height
images along the marked lines are also presented in the
figure (Fig. 3E,F). They describe the surface topography of
collagen fibrils.
For the native pericardium tissue, collagen fibrils ran
mostly parallel to each other. A regular transverse
D-banding pattern with a period of about 67 nm, consisting
of high ridges and shallow grooves is distinctly seen
(Fig. 3E). This result is in good agreement with that
previously obtained from the AFM studies for native
collagen type I fibrils [16–18]. The native D-banding
pattern results from the quarter-staggered arrangement of
collagen molecules within the fibril. However, no common
opinion regarding the staggered molecular structure have
been yet presented in the literature. Some recent models
assume not molecular stagger but a staggering of micro-
fibrils made of six or seven non-staggered parallel-aligned
collagen molecules [19].
For the DMS stabilized tissue the D-pattern is signifi-
cantly disturbed (Fig. 3F). As seen in the axial profile, there
are numerous periods that are longer than 70 nm. Moreover,
the spatial organization of fibrils within the tissue is
disturbed, i.e. fibrils are tangled and running in different
directions. The observed considerable changes in the
surface topography of collagen fibrils can confirm formation
of cross-links between collagen molecules within the fibril.
Changes in the spatial organization of fibrils within the
tissue are most probably due to the formation of the inter-
fibrilar cross-links.
4. Conclusions
The analysis of the Raman spectra in the wide frequency
range 200–4000 cmK1, for the native and DMS-stabilized
porcine pericardium tissue, allowed us to recognize different
types of the DMS–collagen interactions. It has been found,
that in addition to the commonly accepted reaction with the
3-amine groups of lysine or hydroxylysine residues, DMS
M. Jastrzebska et al. / Journal of Molecular Structure 744–747 (2005) 789–795 795
may interact also with the carbonyl CO and amide NH
groups of the peptide bond in collagen. Our paper presents
for the first time the spectral evidence for the peptide
contribution to the formation of DMS–collagen cross-links.
The results confirm also possible competition between
the hydrolysis of the free imidoester group and cross-linking
reaction. Products of the partial alkaline hydrolysis of the
DMS molecules have been found in the spectra.
The observed changes in the surface topography of the
fibrils as well as in their spatial organization in the tissue
support the formation of both intra- and interfibrilar cross-
links in DMS-stabilized tissue.
Acknowledgements
Support of the Committee for Scientific Research (KBN)
grant no. NN-5-156/04 is gratefully acknowledged. One of
the authors (IM) thanks Institute of Experimental Physics,
University of Wrocław, for financial support (grant no.
2016/W/IFD/03).
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