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Direct Biological Sample Analyses by Laserspray Ionization Miniature Mass Spectrometry Yanbing Zhai, Siyu Liu, Lijuan Gao, Lili Hu, and Wei Xu Anal. Chem., Just Accepted Manuscript • DOI: 10.1021/acs.analchem.7b05366 • Publication Date (Web): 21 Mar 2018 Downloaded from http://pubs.acs.org on March 21, 2018
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Analytical Chemistry
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Direct Biological Sample Analyses by Laserspray
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Ionization Miniature Mass Spectrometry
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Yanbing Zhai,1# Siyu Liu,1# Lijuan Gao,2 Lili Hu,1 and Wei Xu1*
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School of Life Science, Beijing Institute of Technology, Beijing 100081, China
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Beijing Center Physical and Chemical Analysis, Beijing, 100089, China
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*Corresponding Author: Wei Xu School of Life Science Beijing Institute of Technology Haidian, Beijing, 100081, China Email:
[email protected] Website: http://www.escience.cn/people/weixu
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#Equal Contribution
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Abstract
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With improved performances, miniature mass spectrometers are becoming
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suitable for more practical applications. At the same time, the coupling of an
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approximate ionization source is essential in terms of minimizing sample preparation
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and broadening the range of samples that could be analyzed. In this study, an
6
atmospheric pressure laserspray ionization (AP-LSI) source was coupled with our
7
home developed miniature ion trap mass spectrometer. The whole system is compact
8
in size, and biological samples could be directly analyzed with minimum sample
9
preparation. Direct detections of peptides, proteins, drugs in whole blood and urine
10
could be achieved with high sensitivity. The analyses of tissue sections were
11
demonstrated, and different regions in a tissue section could be differentiated based
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on their lipid profiles. Results suggest that the coupling of AP-LSI with miniature
13
mass spectrometer is a powerful technique, which could potentially benefit target
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molecule analysis in biological and medical applications.
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Analytical Chemistry
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1. Introduction
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Mass spectrometry (MS) is a powerful analytical technique, which has been
3
widely applied in the analyses of chemical and biological molecules.1-5 Conventional
4
laboratory MS instruments have high analytical performances in terms of sensitivity,
5
mass range and mass resolution. However, these instruments are also typically
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large-in-size and high in power consumption. Miniature MS systems have then been
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developed to meet the increasing demands of on-site chemical analysis.6-8 Based on
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membrane inlet9-11 or ultra-low gas intake techniques,12,13 various portable gas
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chromatography MS (GC-MS) systems become available for volatile sample analysis
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in the field.14-16 To handle non-volatile samples, atmospheric pressure interfaced (API)
11
miniature mass spectrometers were also developed.17-22 An atmospheric pressure
12
interface enables the coupling of atmospheric pressure ionization sources with a
13
miniature mass spectrometer, so that non-volatile samples such as biomolecules could
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be analyzed. At the same time, great efforts have also been made to improve the
15
performances of a miniature mass spectrometer, especially in the past five years. For
16
example, sensitivity of the continuous atmospheric pressure interfaced (CAPI)
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miniature mass spectrometer have been improved by ~ 100 times from ~1 µg/mL to
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~10 ng/mL when analyzing peptides.17,19,23
19
With enhanced performances, miniature mass spectrometers are ready and have
20
been used in more applications, such as from toxic gas and explosive detection to
21
point-of-care testing.13,24-29 When using a miniature mass spectrometer, it is expected
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to be easy-to-operate and fast-in-analysis, which is essentially different from
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laboratory applications. In practical application scenarios, there are minimum sample
24
pretreatment resources. Instruments, such as centrifugal and chemical dryer devices,
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will not be available. Therefore, a miniature mass spectrometer is normally facing
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samples in complex matrices directly, and there is a higher requirement in terms of
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handling complex matrix. The coupling of ambient or atmospheric pressure ionization
28
methods30-32 with miniature mass spectrometer is a perfect marriage, which could
29
effectively solve this problem. Indeed, several ambient ionization techniques have 3
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been coupled with miniature mass spectrometers and demonstrated powerful in
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different applications. Up to now, electrospray33-36 and plasma18,37-39 based ionization
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methods as well as matrix assisted ionization (MAI)40 have been coupled with
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portable mass spectrometers. Easy in sample preparation, powerful in analyte
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desorption and ionization, atmospheric pressure matrix assisted laser desorption
6
ionization (AP-MALDI)41,42 method has also been coupled with a medium-size,
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field-deployable mass spectrometer.43,44 Even so, a conventional AP-MALDI source
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is not the best choice for miniature mass spectrometers. One reason is that the mass
9
range of a miniature mass spectrometer is limited (typically < 2000 Th). A
10
conventional AP-MALDI source typically generates ions with single charge, and
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mass spectrometers with higher mass ranges may be necessary. As another laser based
12
ionization method, laserspray ionization (LSI)45,46 is a variant of MAI. In LSI, a laser
13
is applied to desorb solid samples from a substrate followed by an ionization process,
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which is believed to be assisted by vacuum, matrix and heated capillary. LSI is easy
15
to operate and even could be performed at a normal AP-MALDI or MALDI setup
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under their operating conditions.47,48 More importantly, LSI could produce highly
17
charged gas-phase ions directly from solid samples,45,49,50 which is the significant
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difference from conventional MALDI. As a result, LSI would be favorable when
19
coupling with miniature mass spectrometers.
20
In this study, an IR pulsed laser was used for an atmospheric pressure LSI
21
(AP-LSI) and coupled with our home-developed CAPI mini mass spectrometer. Prior
22
to this study, IR lasers have been used in conventional MALDI and LSI but coupled
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with lab-scale instruments.49,51,52 Herein, the direct analyses of biological samples
24
were demonstrated using this AP-LSI mini MS system. By choosing appropriate
25
matrix and sample preparation method, this AP-LSI source could generate ions with
26
multiple charges, especially for peptides and proteins. As a result, proteins, such as
27
cytochrome C and myoglobin could be detected within a mass range below 1500 Th.
28
When analyzing pure samples, tens of picogram detection sensitivity was achieved for
29
drugs and peptides. This system shows high tolerance to complex matrices. Drugs in 4
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Analytical Chemistry
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whole blood and urine could be detected with a limit of detection (LOD) on the level
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of couple hundreds of ng. The analysis of tissue samples was also demonstrated. High
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throughput MS analysis using this standalone fieldable mass spectrometer could be
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achieved by working with a moving stage and optimized matrices, which could
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potentially facilitate targeted biomarker detections in point-of-care testing.
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2. Experimental sections
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2.1 Instrumentation
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In this study, an AP-LSI source was coupled with our home developed miniature mass
4
spectrometer, which has a continuous atmospheric pressure interface.17,19 As shown in
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Figure 1a, a pulsed diode-pumped solid-state (DPSS) laser was chosen to be used in
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the AP-LSI source. This DPSS laser source (Wedge 1064, Brightness Solutions, Italy)
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is relatively small-in-size, and it can output a pulsed infrared laser beam with a
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wavelength of 1064 nm and a pulse width of 1 ns. Its pulse frequency could be
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adjusted ranging from 1 Hz to 1000 Hz, and energy of each pulse is also adjustable up
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to 4 mJ per pulse energy. A series of optical lens were used to guide the laser beam to
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the sample holder placed right below the MS inlet. To ensure stability of the laser path,
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all optical components were integrated onto a steel plate. The laser beam was finally
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focused by a focusing lens with a focal length of 25 mm, and a laser spot size of ~0.6
14
mm (in diameter) is used in this study. All optics lenses were purchased from Daheng
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Optics Inc. (Beijing, China). For safety consideration, protection goggles and a
16
laboratory coat must be worn during experiments.
17
The miniature mass spectrometer was developed in house, details about the
18
instrument setup could be found in our previous publications.17-19 Briefly, the mini
19
MS was based on a differential pumping system with two vacuum chambers, which
20
were connected to each other with a skimmer, and a stainless steel capillary was used
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to the connect the first vacuum chamber with the atmosphere environment. This
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capillary also served as sample inlet and had an inner diameter of 0.25 mm and a
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length of 20 cm. As one type of inlet ionization method,40,45,53,54 the ionization process
24
of LSI in this study occurred in the inlet capillary, and laser ablation helps in terms of
25
analyte desorption. During experiments, the inlet capillary was grounded and exposed
26
in room temperature. A linear ion trap with hyperbolic electrodes was placed in the
27
second vacuum chamber and served as the mass analyzer. An electron multiplier
28
(model 2500, Detech Inc.) integrated with a dynode was used as the ion detector.
29
Established in this work, the whole instrument, including the laser source, was around 6
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Analytical Chemistry
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60 × 45 × 26 cm in dimensions (38 × 26 × 24 cm when leaving out the laser source)
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and less than 20 kg in total weight. The system was pumped by the combination of a
3
turbo pump (10 L/s, Hipace 10, Pfeiffer Inc., Germany) and a diaphragm pump (50
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L/min, SVF-E0-50, Scroll Tech Inc., China), which maintain an operational pressure
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of ~6 mTorr for the ion trap. In addition, the mass range of the instrument was
6
adjusted up to around 2000 Th by lowering the RF frequency. Experiments were
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carried out in a repetitive laser shot mode with a pulse frequency of 10 Hz, unless
8
otherwise specified. In this study, the laser pulse was not synchronized with the
9
mini-MS. No voltage was applied to the sample plate. The optimized mini-MS
10
operating parameters were found according to a standard tuning procedure using
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nano-ESI. The ion injection time was typically set to 500-1000 ms depending on the
12
analyte amount or concentration. The experiments presented in this work were all
13
performed in a positive ion mode.
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2.2 Chemical reagents and samples
15
Chemical reagents. Reserpine (MW 608.68) was purchased from Acros
16
Organics (Geel, Belgium), Ciprofloxacin (MW 331.34) was purchased from Aladdin
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industrial. Inc (Shanghai, China). High-performance liquid chromatography
18
(HPLC)-grade methanol and acetonitrile were purchased from Fisher Scientific
19
(Fairlawn, NJ). 3-nitrobenzonitrile (3-NBN) was purchased from Acros Organics
20
(Geel, Belgium), 1,2-dicyanobenzene (1,2-DCB) was purchased from Sigma-Aldrich
21
(St. Louis, MO). 3-NBN and 1,2-DCB are two common matrices used in LSI and inlet
22
ionization. Standard samples used in experiments were all diluted in methanol−water
23
(1:1 v/v). 3-NBN and 1,2-DCB were dissolved in acetonitrile, NFR was dissolved in
24
water. All matrixes were prepared to a concentration of 0.1 mg/µL.
25
Biological samples and materials. Met-Arg-Phe-Ala (MRFA, MW 523.65),
26
Gly-Pro-Arg-Pro (GPRP, MW 425.48), angiotensin I (MW 1374.54), angiotensin II
27
(MW 1046.18) and bradykinin (MW 1060.22), cytochrome c and myoglobin were all
28
purchased from Sigma-Aldrich (St. Louis, MO). All peptides and proteins were
29
diluted in methanol-water (1:1 v/v) with addition of 1% acetic acid. Urine was 7
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donated by a healthy volunteer in our lab. Blood and brain slices were obtained from
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experimental mice (C57BL/6 mice, 2 to 3 months old) in our university. The mice
3
experimental studies were approved by Animal Care and Use Committee of Beijing
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Institute of Technology. Mice were decapitated and whole blood was collected in
5
heparinized tubes, while its whole brain was harvested and flushed with saline for 5
6
minutes to remove blood cells. The clean brain was stored in solution of 4%
7
paraformaldehyde (PFA) for two days and then transferred to 30% sucrose solution at
8
4 ℃. The dehydrated brains were sliced into 30 µm thick sections from coronal brain
9
section in sequence using a Leica CM1850 cryostat (Leica Microsystems Inc.,
10
Bannockburn, IL).
11 12
2.3 Sample preparation
13
Prior to the AP-LSI mass spectrometry analysis, a simple sample preparation
14
step was needed. As shown in Figure 1b, a stainless-steel plate was used as the sample
15
holder in this work. Glass slides were also tested, but no obvious differences were
16
observed. Matrix solution in a volume of 10 µL was firstly loaded on the substrate
17
plate using a pipette, followed by dropping 10 µL analyte solution into the matrix
18
solution. After dried at room temperature, the analyte-matrix mixture was subjected to
19
the laser ablation, and then analyzed by the miniature mass spectrometer.
20
To prepare tissue sections, 10 µL purified water was firstly dropped onto the
21
sample plate, and then a piece of brain section was laid onto it. After relaxing and
22
tiling the tissue section in water condition, absorbent paper was then used to dry out
23
the section. Finally, 10 µL matrix solution was spread over the tissue section and
24
waited to dry at room temperature.
25
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Analytical Chemistry
1
3. Results and discussion
2
3.1 Optimization and characterization of the AP-LSI
3
As an atmospheric pressure ionization source, AP-LSI here involves analyte
4
desorption, molecule transfer to the MS inlet, and ionization in the capillary inlet.
5
Desorption and transfer efficiency of analytes depends on the choice of matrix, laser
6
pulse energy and frequency, as well as the distance between the laser focus spot and
7
the MS inlet (d and h shown in Figure 1b). The ionization efficiency of LSI is relevant
8
to many factors, including the choice of matrix, temperature of the inlet capillary,
9
vacuum pressure. In this study, LSI was performed on an miniaturized mass
10
spectrometer, which has fixed inlet capillary and vacuum pressure. To transfer
11
samples as much as possible into the capillary inlet and achieve a higher ionization
12
efficiency, the choice of matrix, the relative position of sample spot to MS inlet, laser
13
energy and frequency were optimized, and details could be found in the supporting
14
information. After optimization, 3-NBN was selected as the LSI matrix, laser pulse
15
energy and frequency were chosen to be 1.2 mJ/pulse and 10 Hz. Since 3-NBN does
16
not have strong absorption in the IR region, it is believed that thermal heating might
17
be the key effect of the IR laser on sample desorption. The vertical (h) and horizon (d)
18
distance between laser spot and the mini-MS inlet were optimized as 5 mm and 6 mm,
19
respectively. These optimized parameters were used in later studies in this work,
20
otherwise specified.
21
After optimization, sensitivity of the system was characterized using reserpine
22
and MRFA. In the experiments, Samples of different concentrations were loaded on
23
the sample holder, ion intensities were recorded in terms of analyte absolute amounts.
24
Analyte absolute amount was defined and calculated as the absolute amount of
25
analyte distributed in the ablated laser spot (details could be found in the Supporting
26
Information). Figure 2a and 2c plot the linear range of quantitation curves of reserpine
27
and MRFA, respectively. Seven parallel experiments were carried out in each
28
measurement to minimize the sample non-uniform distribution effects. As shown in
29
Figure 2b and 2d, limit of detections (LOD) of 50 pg and 200 pg in absolute amount 9
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were obtained for reserpine and MRFA, respectively. A signal-to-noise ratio (SNR) of
2
SNR>5 was maintained in the LOD experiments.
3
The capability of this AP-LSI mini MS in analyzing larger biomolecules were
4
then explored. First, peptides including GPRP, bradykinin, angiotensin I and
5
angiotensin II were tested. The amount of sample loaded in a laser spot area was ~1
6
ng for each of these peptides. Mass spectra of these peptides were obtained and
7
plotted in Figure 3. The mass spectrum of GPRP (Figure 3a) was dominated by singly
8
charged protonated ion ([M+H]+); while multiply charged ions ([M+2H]2+ and/or
9
[M+3H]3+) could also be observed or even dominated in the mass spectra of
10
bradykinin, angiotensin I and angiotensin II. Similar to MAI, multiply charged ions
11
were produced by AP-LSI in this system, which is believed to be attributed to the
12
matrix and conditions the matrix particles experience in traversing the inlet tube.45,50
13
Similar phenomenon was also observed by Sarah Trimpin group in their matrix
14
assisted ionization (MAI) methods using 3-NBN as matrix.40,55-57 Experiments have
15
also been carried out by applying different extraction voltages on the sample holder,
16
and no obvious differences in terms of intensity and multiply charged ions were
17
observed. Results confirm that ions were not formed during the laser ablation (refer to
18
Supporting Information for details). In addition, a few fragment ions (b- and y- ions)
19
were also observed in the mass spectra of bradykinin, angiotensin I, and angiotensin II
20
with relative low abundance. Laser pulse energy and frequency were also tuned in this
21
experiment, and it was found that the appearance and relative intensity ratios of these
22
fragment ions were independent of laser parameters. Similar results were obtained
23
when using different matrices. It is concluded that these fragment ions were not
24
resulted from laser ablation, but very likely a consequence of in source fragmentation
25
happened during ion transfer in the MS inlet.
26
The multiple charged ions observed in our AP-IR-LSI mass spectra are similar to
27
those acquired using electrospray ionization (ESI) sources, which is especially
28
beneficial for our miniature mass spectrometer. Typically, the mass range of a
29
miniature mass spectrometer is not as wide as lab-scale MS instruments, and larger 10
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Analytical Chemistry
1
biomolecules could be analyzed by lowering their mass-to-charge ratios (m/z) with
2
multiple charges. Therefore, larger molecules, for example proteins, were expected to
3
be able to be analyzed within the mass range of our mini-MS. Cytochrome c and
4
myoglobin were used to demonstrate instrument capability of protein analyses.
5
Following the same sample preparation procedures, 10 µL sample solutions (100
6
µg/mL) were loaded onto the sample plate and mixed with the matrix. After the
7
sample mixture dried, pulsed laser was then applied to conduct MS analysis. Figure 4
8
shows the mass spectra of these two proteins. Multiply charged ions were well
9
observed in the mass spectra, which show similar feature as that of conventional ESI
10
mass spectra.
11
3.2 Direct analyses of drugs in blood and urine
12
Biological samples, such as blood and urine, have very complex matrix. Direct
13
analysis of urine and blood is a great challenge for ESI-MS. Therefore, complicated
14
sample pretreatment procedures are conventionally performed before MS or LC-MS
15
analysis. However, in a typical application scenario of a miniature mass spectrometer,
16
the sample pretreatment procedure or equipment are not desired and available.
17
Therefore, a mini mass spectrometer normally needs to handle these complex samples
18
directly. The capability of analyzing target analyte in complex biological samples
19
with minimum sample pretreatment is then demonstrated using this AP-IR-LSI mini
20
mass spectrometer. In the experiments, ciprofloxacin and reserpine were spiked into
21
urine and whole blood, respectively. Prior to analysis, the urine stock solution was
22
diluted two times and the blood stock solution was diluted four times in volume using
23
methanol-water (1:1 v/v) as solvent. Then these samples were loaded onto sample
24
plates and suspected to laser ablation after dried. Ciprofloxacin in urine and reserpine
25
in blood could be directly detected with the mass spectra shown in Figure 5. Figure 5a
26
and 5b are mass spectra obtained from ciprofloxacin in urine with an absolute amount
27
of 100 ng and reserpine in blood with an absolute amount of 400 ng, respectively.
28
Tandem MS was also performed using collision induced dissociation (CID) as shown
29
in Figure 5c and 5d to confirm the results. 11
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3.3 Tissue analysis
2
As a solid sample, tissue is another important type of biological sample. Lab scale
3
MALDI-MS has been widely applied in tissue analysis, especially for tissue imaging
4
in biomedical applications.58-60 By coupling with high-resolution mass spectrometers,
5
LSI has also been used for imaging of mouse brain and other tissues samples.48,61,62 In
6
this study, mouse brain tissue slices were analyzed using the AP-LSI mini MS system.
7
Under the optimized working condition with a laser energy of 1.4 mJ/pulse, lipids in
8
mouse brain were observed as shown in Figure 6. In the experiments, mass spectra
9
with different relative abundances of m/z 735 and 789 were observed when analyzing
10
different points on the tissue section. By exploring the relative abundance difference
11
of mass peaks with their corresponding positions of tissue section, we found that
12
higher relative abundance of m/z 735 (PC 32:0) resulted from grey matter and higher
13
relative abundance of m/z 789 (PC 36:1) abundance was responsible for white matter.
14
The results are consistent with that reported by other groups previously,63,64 who also
15
revealed that PC 32:0 abundance is responsible for grey matter and PC 36:1
16
abundance is associated with white matter. As noticed, the spatial resolution of the
17
current AP-LSI is only about 0.6 mm. Issues, such as spatial resolution, MS resolution
18
and carryover effects need to be solved, before this system is ready to perform MS
19
imaging experiments.
20
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Analytical Chemistry
1
4. Conclusions
2
In this study, an AP-IR-LSI miniature mass spectrometer was developed. Using
3
3-NBN as matrix and under optimized working conditions, an LOD of 200 pg in
4
absolute amount could be achieved for standard samples. The rapid analyses of
5
biological samples, including peptides, proteins, drugs in urine and blood, tissue
6
sections were demonstrated using the system with minimum sample preparations. By
7
coupling with an IR laser, the instrument would actually lose portability. However,
8
this laserspray ionization method could greatly simplify the ionization and sample
9
preparation procedure, especially for complex samples. The AP-IR-LSI mini-MS has
10
capability of direct analyzing complex samples on spot and is potentially feasible for
11
environmental monitoring, point-of-care diagnostic testing and rapid MS imaging.
12 13 14 15 16 17 18
Acknowledgements This work was supported by NNSF (21475010, 61635003), BNSF (16L00065) and State Key Laboratory of Explosion Science and Technology (YBKT16-17).
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References (1) Aebersold, R.; Mann, M. Nature 2003, 422, 198-207. (2) Beckey, H.-D. Principles of Field Ionization and Field Desorption Mass Spectrometry: International Series in Analytical Chemistry; Elsevier, 2016. (3) Covey, T. R.; Lee, E. D.; Bruins, A. P.; Henion, J. D. Anal. Chem. 1986, 58, 1451A-1461A. (4) Kostiainen, R.; Kotiaho, T.; Kuuranne, T.; Auriola, S. J. Mass Spectrom. 2003, 38, 357-372. (5) Rosenstock, H.; Krauss, M.; McLafferty, F. by FW McLafferty, Academic Press, New York 1963, 1. (6) Snyder, D. T.; Pulliam, C. J.; Ouyang, Z.; Cooks, R. G. Anal. Chem. 2015, 88, 2-29. (7) Ouyang, Z.; Cooks, R. G. Annual Review of Analytical Chemistry 2009, 2, 187-214. (8) Guo, Q.; Gao, L.; Zhai, Y.; Xu, W. Chin. Chem. Lett. 2017. (9) Ketola, R. A.; Kotiaho, T.; Cisper, M. E.; Allen, T. M. J. Mass Spectrom. 2002, 37, 457-476. (10) Johnson, R.; Cooks, R.; Allen, T.; Cisper, M.; Hemberger, P. Mass Spectrom. Rev. 2000, 19, 1-37. (11) Janfelt, C.; Frandsen, H.; Lauritsen, F. R. Rapid Commun. Mass Spectrom. 2006, 20, 1441-1446. (12) Janfelt, C.; Talaty, N.; Mulligan, C. C.; Keil, A.; Ouyang, Z.; Cooks, R. G. Int. J. Mass spectrom. 2008, 278, 166-169. (13) Contreras, J. A.; Murray, J. A.; Tolley, S. E.; Oliphant, J. L.; Tolley, H. D.; Lammert, S. A.; Lee, E. D.; Later, D. W.; Lee, M. L. J. Am. Soc. Mass Spectrom. 2008, 19, 1425-1434. (14) Riter, L. S.; Peng, Y.; Noll, R. J.; Patterson, G. E.; Aggerholm, T.; Cooks, R. G. Anal. Chem. 2002, 74, 6154-6162. (15) Frandsen, H.; Janfelt, C.; Lauritsen, F. R. Rapid Commun. Mass Spectrom. 2007, 21, 1574-1578. (16) Janfelt, C.; Graesboll, R.; Lauritsen, F. R. Int. J. Mass spectrom. 2008, 276, 17-23. (17) Zhai, Y.; Zhang, X.; Xu, H.; Zheng, Y.; Yuan, T.; Xu, W. Anal. Chem. 2017, 89, 4177-4183. (18) Zhai, Y.; Jiang, T.; Huang, G.; Wei, Y.; Xu, W. Analyst 2016, 141, 5404-5411. (19) Zhai, Y.; Feng, Y.; Wei, Y.; Wang, Y.; Xu, W. Analyst 2015, 140, 3406-3414. (20) He, M.; Xue, Z.; Zhang, Y.; Huang, Z.; Fang, X.; Qu, F.; Ouyang, Z.; Xu, W. Anal. Chem. 2015, 87, 2236-2241. (21) Wei, Y.; Bian, C.; Ouyang, Z.; Xu, W. Rapid Commun. Mass Spectrom. 2015, 29, 701-706. (22) Gao, L.; Cooks, R. G.; Ouyang, Z. Anal. Chem. 2008, 80, 4026-4032. (23) Meng, X.; Zhang, X.; Zhai, Y.; Xu, W. Instruments 2018, 2, 2. (24) Ferreira, C. R.; Yannell, K. E.; Jarmusch, A. K.; Pirro, V.; Ouyang, Z.; Cooks, R. G. Clin. Chem. 2016, 62, 99-110. (25) Li, L.; Chen, T.-C.; Ren, Y.; Hendricks, P. I.; Cooks, R. G.; Ouyang, Z. Anal. Chem. 2014, 86, 2909-2916. (26) Sanders, N. L.; Kothari, S.; Huang, G.; Salazar, G.; Cooks, R. G. Anal. Chem. 2010, 82, 5313-5316. (27) Hendricks, P. I.; Dalgleish, J. K.; Shelley, J. T.; Kirleis, M. A.; McNicholas, M. T.; Li, L.; Chen, T.-C.; Chen, C.-H.; Duncan, J. S.; Boudreau, F. Anal. Chem. 2014, 86, 2900-2908. (28) Dalgleish, J. K.; Hou, K.; Ouyang, Z.; Cooks, R. G. Anal. Lett. 2012, 45, 1440-1446. (29) Smith, J. N.; Keil, A.; Likens, J.; Noll, R. J.; Cooks, R. G. Analyst 2010, 135, 994-1003. 14
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(30) Alberici, R. M.; Simas, R. C.; Sanvido, G. B.; Romão, W.; Lalli, P. M.; Benassi, M.; Cunha, I. B.; Eberlin, M. N. Anal. Bioanal. Chem. 2010, 398, 265-294. (31) Peacock, P. M.; Zhang, W.-J.; Trimpin, S. Anal. Chem. 2016, 89, 372-388. (32) Klampfl, C. W.; Himmelsbach, M. Anal. Chim. Acta 2015, 890, 44-59. (33) Hu, B.; So, P.-K.; Chen, H.; Yao, Z.-P. Anal. Chem. 2011, 83, 8201-8207. (34) Kuo, C.-P.; Shiea, J. Anal. Chem. 1999, 71, 4413-4417. (35) Liu, J.; Wang, H.; Cooks, R. G.; Ouyang, Z. Anal. Chem. 2011, 83, 7608-7613. (36) Wang, H.; Liu, J.; Cooks, R. G.; Ouyang, Z. Angew. Chem. 2010, 122, 889-892. (37) Wiley, J. S.; Shelley, J. T.; Cooks, R. G. Anal. Chem. 2013, 85, 6545-6552. (38) Kumano, S.; Sugiyama, M.; Yamada, M.; Nishimura, K.; Hasegawa, H.; Morokuma, H.; Inoue, H.; Hashimoto, Y. Anal. Chem. 2013, 85, 5033-5039. (39) Wang, X.; Zhou, X.; Ouyang, Z. Anal. Chem. 2015, 88, 826-831. (40) Devereaux, Z. J.; Reynolds, C. A.; Fischer, J. L.; Foley, C. D.; DeLeeuw, J. L.; Wager-Miller, J.; Narayan, S. B.; Mackie, K.; Trimpin, S. Anal. Chem. 2016, 88, 10831-10836. (41) Laiko, V. V.; Baldwin, M. A.; Burlingame, A. L. Anal. Chem. 2000, 72, 652-657. (42) Laiko, V. V.; Moyer, S. C.; Cotter, R. J. Anal. Chem. 2000, 72, 5239-5243. (43) Doroshenko, V. M.; Laiko, V. V.; Misharin, A. S.; Google Patents, 2013. (44) Misharin, A.; Novoselov, K.; Laiko, V.; Doroshenko, V. M. Anal. Chem. 2012, 84, 10105-10112. (45) Trimpin, S.; Inutan, E. D.; Herath, T. N.; McEwen, C. N. Molecular & Cellular Proteomics 2010, 9, 362-367. (46) Nyadong, L.; Inutan, E. D.; Wang, X.; Hendrickson, C. L.; Trimpin, S.; Marshall, A. G. J. Am. Soc. Mass Spectrom. 2013, 24, 320-328. (47) McEwen, C. N.; Larsen, B. S.; Trimpin, S. Anal. Chem. 2010, 82, 4998-5001. (48) Inutan, E. D.; Wager-Miller, J.; Mackie, K.; Trimpin, S. Anal. Chem. 2012, 84, 9079-9084. (49) Trimpin, S.; Wang, B.; Inutan, E. D.; Li, J.; Lietz, C. B.; Harron, A.; Pagnotti, V. S.; Sardelis, D.; McEwen, C. N. J. Am. Soc. Mass Spectrom. 2012, 23, 1644-1660. (50) Trimpin, S.; Inutan, E. D.; Herath, T. N.; McEwen, C. N. Anal. Chem. 2009, 82, 11-15. (51) Niu, S.; Zhang, W.; Chait, B. T. J. Am. Soc. Mass Spectrom. 1998, 9, 1-7. (52) Zhang, W.; Niu, S.; Chait, B. T. J. Am. Soc. Mass Spectrom. 1998, 9, 879-884. (53) Peacock, P. M.; Zhang, W. J.; Trimpin, S. Anal. Chem. 2017, 89, 372. (54) Pagnotti, V. S.; Chubatyi, N. D.; Mcewen, C. N. Anal. Chem. 2011, 83, 3981-3985. (55) Trimpin, S.; Inutan, E. D. J. Am. Soc. Mass Spectrom. 2013, 24, 722-732. (56) Inutan, E. D.; Trimpin, S. Molecular & Cellular Proteomics 2013, 12, 792-796. (57) Chakrabarty, S.; Pagnotti, V. S.; Inutan, E. D.; Trimpin, S.; McEwen, C. N. J. Am. Soc. Mass Spectrom. 2013, 24, 1102-1107. (58) Andersson, M.; Groseclose, M. R.; Deutch, A. Y.; Caprioli, R. M. Nat. Methods 2008, 5, 101-108. (59) Chen, S.; Xiong, C.; Liu, H.; Wan, Q.; Hou, J.; He, Q.; Badu-Tawiah, A.; Nie, Z. Nature nanotechnology 2015, 10, 176-182. (60) Kompauer, M.; Heiles, S.; Spengler, B. Nat. Methods 2017, 14, 90-96. (61) Harron, A. F.; Hoang, K.; McEwen, C. N. Int. J. Mass spectrom. 2013, 352, 65-69. (62) Richards, A. L.; Lietz, C. B.; Wager-Miller, J.; Mackie, K.; Trimpin, S. J. Lipid Res. 2012, 53, 1390-1398. 15
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(63) Trim, P. J.; Atkinson, S. J.; Princivalle, A. P.; Marshall, P. S.; West, A.; Clench, M. R. Rapid Commun. Mass Spectrom. 2008, 22, 1503-1509. (64) Woods, A. S.; Jackson, S. N. The AAPS journal 2006, 8, E391-E395.
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Figure 1
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Figure 1. AP-LSI miniature mass spectrometer setup. Three-dimensional setup of the
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instrument (top); Schematic plot of sample preparation and laser ablation.
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Figure 2
Reserpine (LOD 50 pg)
75 50 25 0
y = 6.0943x + 1253.3 R² = 0.9943 0
1000
1500
2000
2500
absolute amount (pg)
(c)
2
500
MRFA (LOD 200 pg)
50
y = 0.6726 x + 3.6949 R² = 0.9973
25 0
0
1000
2000
3000
4000
609
100
Reserpine (50 pg) 75 50
S/N > 5
25 0 200
300
400
5000
500
600
700
800
m/z
(d)
100 75
relative abundance (%)
(b)
100
relative abundance (%)
relative abundance (%)
(a)
relative abundance (%)
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100
MRFA (200 pg) 524 75 50
S/N > 5
25 0 200
300
absolute amount (pg)
400
500
600
700
800
m/z
3
Figure 2. Standard sample analysis using the AP-LSI miniature mass spectrometer. (a)
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Linear range of quantitation for reserpine; (b) mass spectrum of reserpine, 50 pg of
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reserpine was presented in the laser spot; (c) Linear range of quantitation for MRFA;
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(b) mass spectrum of MRFA, 200 pg of MRFA was presented in the laser spot;
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Figure 3
[M+H]+ 426
100
GPRP
(b)
relative abundance (%)
relative abundance (%)
(a)
75 50 25 0 200
300
400
500
100
[M+2H]2+ 531
Bradykinin
75 50
710
0 400
600
2
100
Angiotensin I
25
[M+3H]3+
75 50
0 400
[M+H]+ 1296
b 6+ 784
433
600
800
800
1000
1200
m/z (d)
[M+2H]2+ 648
1000
1200
1400
relative abundance (%)
(c)
y8+ [M+H]+ 904 1061
y6+
25
m/z
relative abundance (%)
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[M+2H]2+ 524
Angiotensin II [M+H]+ 1047
75 50
b6+ 784
25 0 400
600
800
1000
m/z
m/z
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Figure 3. Peptide analyses using the AP-LSI miniature mass spectrometer. Mass
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spectra of (a) GPRP, (b) bradykinin, (c) angiotensin I and (d) angiotensin II.
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Figure 4
100
relative abundance (%)
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
12+ 13+ 1031 951
Cytochrome c
75
11+ 1125
15+ 825 14+ 884
50
(a)
10+ 1237
9+ 1374
16+ 17+ 773 728
25 0 100
14+ 1212
Myoglobin
15+ 16+ 1131 1061
75 17+ 19+ 18+ 998 883 21+ 943 80820+ 849
50 25 0 600
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700
800
13+ 1305
(b) 12+ 1414
900 1000 1100 1200 1300 1400 1500
m/z
3
Figure 4. Protein analyses using the AP-LSI miniature mass spectrometer. Mass
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spectra of (a) cytochrome c and (b) myoglobin.
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Figure 5
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Figure 5. Detection of drugs in complex matrices using the AP-LSI miniature mass
4
spectrometer. (a) Mass spectrum of ciprofloxacin in urine, 100 ng of ciprofloxacin
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was presented in the laser spot; (b) the corresponding tandem mass spectrum of 100
6
ng ciprofloxacin in urine; (c) mass spectrum of reserpine in blood, 400 ng of reserpine
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was presented in the laser spot; (b) the corresponding tandem mass spectrum of 400
8
ng reserpine in blood.
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Figure 6
100
relative abundance (%)
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735 [PC(32:0)+H]+
75 50
761 [PC(34:1)+H]+ 773 [PG(36:3)+H]+ 789 [PC(36:1)+H]+ 799 [PG(38:4)+H]+
grey matter 833 [PI(34:3)+H]+
25 0 100 75 50
[PC(34:1)+H]+ 761 789 [PC(36:1)+H]+ 799 [PG(38:4)+H]+ [PC(32:0)+H]+ 735 833 [PI(34:3)+H]+
white matter
25 0 300 400 500 600 700 800 900 1000
2
m/z
3
Figure 6. Tissue section analyses using the AP-LSI miniature mass spectrometer. (a)
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Mass spectrum of grey matter in a mouse brain tissue section; (b) mass spectrum of
5
white matter in a mouse brain tissue section.
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