A. Schwaighofer, C.K. Akhgar and B. Lendl
Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy 253 (2021) 119563
In this work we employ a commercial broadband laser-based IR
spectrometer for protein secondary structure analysis. The perfor-
mance of the instrument is benchmarked against FTIR spec-
troscopy. Furthermore, we utilize the large available spectral
region (400 cmꢁ1) to follow the enzymatic hydrolysis of triacetin
by lipase.
1. Introduction
Mid-infrared (mid-IR) spectroscopy is a powerful and versatile
technique for the analysis of structure and dynamics of polypeptides
andproteins[1–3]. Vibrationsofthepolypeptiderepeatunitresultin
nine characteristic group frequencies in the mid-IR region that are
referred to as amide bands. Among those, the amide I band (1700–
1600 cmꢁ1) and amide II band (1600–1500 cmꢁ1) were shown to be
most sensitive to protein structure. The sensitivity to individual sec-
ondary structure elements originates in differing patterns of hydro-
gen bonding, dipole–dipole interactions, and geometric
2. Materials and methods
2.1. Reagents and samples
orientations in the a-helices, b-sheets, turns, and random coil struc-
Bovine serum albumin, lysozyme from chicken egg white, and
turesthatinducedifferentfrequenciesoftheC=OandN-Hvibrations.
The resulting characteristic band shapes and positions can be then
correlated with the specific secondary structure folding [4].
c
-globulins from bovine blood (ꢂ97%), lipase from Candida rugosa
(Type VII, ꢂ700 unit/mg solid) were purchased from Sigma-Aldrich
(Steinheim, Germany). Triacetin was purchased from Merck
(Darmstadt, Germany). For protein secondary structure measure-
ments, proper amounts of protein powder were dissolved in water.
For enzymatic activity measurements, stock solutions of 5 mg mLꢁ1
lipase and 250 mM triacetin were prepared. Ultrapure water (resis-
Fourier-transform IR (FTIR) spectroscopy is the established and
most widespread instrumentation in this spectral region. FTIR
spectrometers are commonly equipped with thermal light sources
such as Globars that emit broadband and constant but rather low
power radiation across the mid-IR range. The low emission inten-
sity can lead to limitations regarding measurements of analytes
present in a highly absorbing matrix such as water. For mid-IR
spectroscopy of proteins, there is the pronounced challenge of
the HOH-bending band of water near 1643 cmꢁ1 that overlaps with
the protein amide I band. As a consequence, the optical path is
restricted to < 10 mm for FTIR transmission measurements in order
to avoid total IR absorption [2,3]. These short path lengths lead to
impaired sensitivity because of the lower band absorbances and
limited robustness due to higher probability of cell clogging.
More than two decades ago, quantum cascade lasers (QCLs)
were introduced as a polarized, coherent and high power light
source in the mid-IR region [5]. They allow stable operation at
room temperature and provide spectral power densities higher
than a factor of 104 compared with thermal light sources [6]. Since
the commercial availability of external cavity-QCLs (EC-QCLs),
which offer broadband spectral tuning in the range of several hun-
dred wavenumbers, this type of light source has been increasingly
used for studies of liquid samples [7]. It was shown that the high
available emission power of QCLs enable mid-IR transmission mea-
surements using an optical path 4–5 times larger than with con-
ventional FTIR spectroscopy [8]. For analysis of proteins,
academic setups employing EC-QCLs were reported for investiga-
tion of the amide I region [9,10] as well as amide I + II regions
[11], finally surpassing the performance of FTIR spectroscopy in
terms of limit of detection at similar measurement times [12].
These techniques were employed for analysis of protein structure
after chemical [13], thermal [10] and pH-induced [14] denatura-
tion. Recently there was also introduced a commercially available
QCL-based IR spectroscopy system, (AQS3pro, RedShiftBio) that
covers only the amide I spectral range and provides better perfor-
mance than FTIR spectroscopy in terms of LOD at approximately
10-fold measurement time [15].
tivity: 18 M
pore (Bedford, MA).
X cm) was purified with a Milli-Q system from Milli-
2.2. Laser-based IR spectroscopy
Laser-based IR spectra were recorded with a ChemDetect Ana-
lyzer (Daylight Solutions Inc., San Diego, USA), equipped with a
25 mm diamond transmission flow cell and an EC-QCL providing
a spectral coverage between 1350 and 1770 cmꢁ1. External water
cooling for the laser head was set to 17 °C. For protein secondary
structure measurements, 91 scans were recorded and averaged at
a measurement time of 45 s. For enzymatic activity measurements,
the enzyme and substrate stock solutions were mixed to obtain the
desired concentrations. Subsequently, the resulting solutions were
thoroughly vortexed and injected into the sampling cell. At first, a
reference spectrum was recorded and afterwards sample spectra
were recorded for 20 min. at a time-interval of 20 s (60 scans).
The spectrometer was flushed with dry air to decrease the influ-
ence of water vapor from the atmosphere. If necessary, absorption
bands of water vapor in the atmosphere were subtracted during
post-processing. The recorded spectra were treated by
Savitzky ꢁ Golay smoothing (order: 2, window: 15 points), which
resulted in a spectral resolution of 3.6 cmꢁ1, determined by com-
parison of the band width to FTIR spectra of water vapor. Spectra
recording was performed with the ChemDetect software package.
Data processing and analysis was conducted with in-house code
developed in MatLab R2020b (MathWorks, Inc., Natick, MA, 2014).
2.3. FTIR spectroscopy
FTIR absorption measurements were performed using a Bruker
Vertex 80v FTIR spectrometer (Ettlingen, Germany) equipped with
a liquid nitrogen cooled HgCdTe (mercury cadmium telluride)
detector (D* = 4 ꢃ 1010 cm Hz0.5 Wꢁ1 at 9.2
lm) and a Bruker Ten-
A drawback for laser-based IR setups so far was the limited
accessible spectral range. Even though EC-QCLs with spectral cov-
erages of several hundred wavenumbers are achievable [16,17],
and even larger tuning ranges of>1000 cmꢁ1 provided by a single
device can be obtained by beam combination of multiple EC-QCL
modules, uneven spectral tuning densities of QCLs pose a problem
for implementation of broadband laser-based IR transmission set-
ups [11,12]. For analysis of proteins, a broader spectral range
allows not only to monitor protein structure changes in the amide
I + II bands but also to reveal IR signatures of substrates and prod-
ucts of enzymatic reactions. Furthermore, particularly for chemo-
metric analysis additional and more detailed information can be
gained by analysis of a larger spectral range [14,18–20].
sor 37 FTIR spectrometer equipped with a DLaTGS (deuterated lan-
thanum
a-alanine
doped
triglycine
sulfate)
detector
(D* = 6 ꢃ 108 cm Hz0.5 Wꢁ1 at 9.2
lm). The samples were manually
injected into a flow cell, equipped with two CaF2 windows and an
8
lm-thick spacer. During measurements, the spectrometer was
constantly flushed with dry air for at least 10 min prior to data
acquisition until water vapor absorption was sufficiently constant.
Spectra were acquired with a spectral resolution of 3.6 cmꢁ1 in
double-sided acquisition mode. A total of 341 (Vertex operated at
80 kHz scanner velocity) and 48 (Tensor operated at 10 kHz scan-
ner velocity) scans were averaged per spectrum (acquisition time:
45 s), which was calculated using a Blackman-Harris 3-term
2