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1 ples down to 1 mM using merely a 188 MHz NMR spectrometer.
2 igh mass accuracy and resolution of the mass spectrometer.
3 paper-based SERS substrate by handheld Raman spectrometer.
4 veling-wave ion mobility time-of-flight mass spectrometer.
5 laboratory confocal micro X-ray fluorescence spectrometer.
6 yzed by HPLC combined with DAD and QTOF mass spectrometer.
7 mass spectrometry on a 6600 Triple-TOF mass spectrometer.
8 (n=90), in comparison with a FT-NIR benchtop spectrometer.
9 east 24 h under the vacuum of our MALDI mass spectrometer.
10 its sexual dichromatism distinguishable by a spectrometer.
11 olled by a laser source external to the mass spectrometer.
12 ent made using a standard low-speed infrared spectrometer.
13 nts made using an ion-molecule reaction mass spectrometer.
14 water samples run on a laboratory-based mass spectrometer.
15 ion continuum source flame atomic absorption spectrometer.
16 lution achievable using a given imaging mass spectrometer.
17 ochemical laboratory having access to a mass spectrometer.
18 ring this competitive reaction with a UV-vis spectrometer.
19 matography coupled with high resolution mass spectrometer.
20 y into the trapping cell of an Orbitrap mass spectrometer.
21 proximately 100 cm) and a Q Exactive HF mass spectrometer.
22 ic sector field gas-phase isotope ratio mass spectrometer.
23 er desorption/ionization time-of-flight mass spectrometer.
24 zation interface of a triple quadrupole mass spectrometer.
25 lute solutions with a single pulse of an NMR spectrometer.
26 rences in an inductively coupled plasma mass spectrometer.
27 nsform-ion cyclotron resonance (FT-ICR) mass spectrometer.
28 tting diode (LED) and a microfiber optic USB spectrometer.
29 acid-treated hemoglobin by an accurate mass spectrometer.
30 array detector and a triple-quadrupole mass spectrometer.
31 nization (ESI) interface to an ion-trap mass spectrometer.
32 ately 30 times) compared to the conventional spectrometer.
33 ctance-Fourier transform infrared (ATR-FTIR) spectrometer.
34 for element content using X-ray fluorescence spectrometer.
35 to that obtained with a commercial benchtop spectrometer.
36 ance liquid chromatography coupled to a mass spectrometer.
37 n a quadrupole-Orbitrap high resolution mass spectrometer.
38 sure chemical ionization source on this mass spectrometer.
39 an electrospray can be directed into a mass spectrometer.
40 ed to a high resolution Orbitrap Fusion mass spectrometer.
41 rm electrostatic linear ion trap (ELIT) mass spectrometer.
42 inductively coupled plasma-optical emission spectrometer.
43 rsed and detected using a conventional array spectrometer.
44 on that can be installed on a commercial NMR spectrometer.
45 urier transform ion cyclotron resonance mass spectrometer.
46 etry (LC-MS/MS) using a high-resolution mass spectrometer.
47 ometry (MS/MS) with a triple quadrupole mass spectrometer.
48 lometric detector and a high-resolution mass spectrometer.
49 ring mode and using a triple quadrupole mass spectrometer.
50 VPD for peptide analysis in an ion trap mass spectrometer.
51 de capillary coupled to a Q Exactive HF mass spectrometer.
52 ure and the initial vacuum stage of the mass spectrometer.
53 al from a spatially offset zone to the Raman spectrometer.
54 extracts into a high resolution tandem mass spectrometer.
55 source for subsequent measurement by a mass spectrometer.
56 s was designed to conduct ions into the mass spectrometer.
57 agmentation behavior of peroxy acids in mass spectrometers.
58 rcoming hardware limitations of conventional spectrometers.
59 mid-infrared photodetectors, modulators, and spectrometers.
60 ide-scan data sets from high resolution mass spectrometers.
61 ar ions in various types of widely used mass spectrometers.
62 lticollector inductively coupled plasma mass spectrometers.
63 nstrumentation is coupled with ion trap mass spectrometers.
64 ive and more robust than other types of mass spectrometers.
65 omain, without the need for bulky mechanical spectrometers.
66 of a new class of broadband high-resolution spectrometers.
67 terfaces for coupling the CE devices to mass spectrometers.
68 as [{n(n + 1)}/2]-fold over conventional EEM spectrometers.
69 ratories, equipped with different resolution spectrometers (400 and 500 MHz), using two identical set
70 paration in LC x LC and to use multiple mass spectrometers across both dimensions to perform conventi
71 combined satellite observations from passive spectrometer, active cloud radar, lidar, and wind field
72 ical advances have made high-resolution mass spectrometers affordable to many laboratories, thus boos
73 lux analysis because the resolution of these spectrometers allows for discrimination between (13)C-co
74 that the combination of a miniaturized mass spectrometer, ambient ionization, and statistical analys
77 e consistent with those from an aerosol mass spectrometer (AMS) with a thermal denuder, implying that
81 ansform ion cyclotron resonance (FTICR) mass spectrometer and a time-of-flight (TOF) instrument with
82 rison with a commercially available portable spectrometer and an optical spectrum analyzer shows our
83 nce spectroscopy system using the smartphone spectrometer and demonstrated the capability of hemoglob
84 of fragmentation available on a tribrid mass spectrometer and optimized their collision energies with
85 were measured in situ using a photoacoustic spectrometer and step-scanning a supercontinuum laser so
87 s were obtained using a high-resolution mass spectrometer and the quantitative proteomic software too
88 method at room temperature on a Bruker E500 spectrometer and the results suggested that SO4(.-) was
89 the emitter and the heated inlet to the mass spectrometer and the voltage applied to the emitter sour
90 mass isolated in a quadrupole ion trap mass spectrometer and then irradiated by the tunable infrared
91 ncrease the fraction that can enter the mass spectrometer and with minimum loss of material toward th
92 ssibilities for developing new ultra-compact spectrometers and low-cost hyperspectral imaging sensors
93 n online high-resolution time-of-flight mass spectrometer) and dissolved organic matter in the ocean
94 is also found upon broadband IR light of the spectrometer, and the ratio of the quantum yields of the
95 s, magnetometers, single-particle absorption spectrometers, and microcavity sensors for sizing single
96 roteins within the ICR cell of a FT-ICR mass spectrometer are accomplished through appropriate modula
97 vated dissociation (CAD) in an ion trap mass spectrometer are demonstrated to allow the identificatio
101 on efficiencies were observed with both mass spectrometers as detectors, with about 6 times better si
103 ze makes this Arbitrary Waveform Relaxometer/Spectrometer (AWR) a convenient yet powerfully flexible
105 on of peptides and proteins in ion trap mass spectrometers, but the spectral signal-to-noise ratio (S
106 rbene was generated in situ in a tandem mass spectrometer by decarboxylation of oxo[4-(trimethylammon
107 entation capabilities of the Q Exactive mass spectrometer can be extended with ultraviolet photodisso
109 Multistage fragmentation (MS(n)) in the mass spectrometer can provide sufficient evidence for Ile/Leu
110 Design results demonstrate that this k-space spectrometer can reduce the nonlinearity error in k-spac
111 pproach relies on the advanced Orbitrap mass spectrometer capable of multistage MS analysis across al
112 and reference electrode as mounted in the IR spectrometer cause the formation of a thin electrolyte l
113 g a high-resolution chemical ionization mass spectrometer (CIMS) equipped with an "inlet-less" NO3(-)
115 thodology employing a tandem quadrupole mass spectrometer coupled to a gas chromatograph with headspa
116 ly sensitive inductively coupled plasma mass spectrometer coupled to a scanning flow cell, the activi
117 840 nm were collected using a photoacoustic spectrometer coupled to a supercontinuum laser with a tu
120 e matrix factorization (PMF) of aerosol mass spectrometer data collected in areas dominated by isopre
126 ent a reference drift tube ion mobility mass spectrometer (DTIM-MS) where improvements on the measure
127 e the performance of energy dispersive X-ray spectrometers (EDS) in the low energy range below 1 keV.
128 ectly coupled to an electron ionization mass spectrometer (EI-MS) without any interface or modificati
129 which was coupled to different Orbitrap mass spectrometers (Elite and Q Exactive Plus) and extensivel
130 Recent work has demonstrated that for mass spectrometers employing analog-to-digital converters (AD
131 e describe modifications to an Orbitrap mass spectrometer, enabling high-resolution native MS analysi
132 ce, X-ray spectra were accumulated; the best spectrometer energy resolution (FWHM) achieved at 5.9 ke
133 Using a time-of-flight secondary ion mass spectrometer equipped with an argon cluster ion for sput
135 r and by gas chromatograph coupled with mass spectrometer exhibited the correlation coefficient of 0.
136 ate that the fall-off curve from the k-space spectrometer exhibits much less decay (maximum as -5.20
139 obility, while field asymmetric ion mobility spectrometers (FAIMS) separate them by the change of the
140 field asymmetric time of flight ion mobility spectrometer (FAT-IMS) allows high repetition rates and
141 e we report a linear-in-wavenumber (k-space) spectrometer for an ultra-broad bandwidth (760 nm-920 nm
142 ilities of a laser-coupled ion mobility mass spectrometer for analysis of peptide sequence and struct
143 process including remotely triggering an NMR spectrometer for efficient production of payloads of hyp
144 ulting atomic emissions are recorded using a spectrometer for elemental identification and quantifica
145 ted low-altitude orbits, the Rosetta Orbiter Spectrometer for Ion and Neutral Analysis (ROSINA) on th
146 ual spectroscopic detectors: a near-infrared spectrometer for measuring the organic analyte in the CO
148 xtraction that is directly coupled to a mass spectrometer for the quantitative screening of 12 differ
150 methods available on an Orbitrap Fusion mass spectrometer for three proteins and an E. coli cell lysa
151 etection (flame ionisation detector and mass spectrometer) for quantitative and qualitative purposes.
154 injection period (IT)of low-duty cycle mass spectrometers has been previously shown to improve sensi
155 he popular benchtop Q Exactive Orbitrap mass spectrometer have so far relied exclusively on higher co
157 Recently, laser-based water stable isotope spectrometers have become popular as they enable previou
159 esolution continuum source atomic absorption spectrometer (HR-CS AAS) after leaching Cr(VI) with 0.10
163 tion time-of-flight chemical ionization mass spectrometer (HRToF-CIMS) equipped with an acetate ion s
164 tion chemical ionization time-of-flight mass spectrometer (HRToF-CIMS), operated with two different t
167 n system coupled to a gas chromatograph-mass spectrometer (ILR-CIS-GC-MS) has been explored for the f
168 DESI with the IT of an LTQ Orbitrap-XL mass spectrometer improves spatial resolution by factors of a
169 pressure, dual-gate drift tube ion mobility spectrometer (IMS) to a linear ion trap mass spectromete
171 stem and analyze a single sample on the mass spectrometer in approximately 20 s, with minimal sample
173 ective, and reliable alternative to benchtop spectrometers in fish fillet and patty authentication.
174 ectly to the electrospray source of the mass spectrometer, in order to provide an extremely sensitive
175 he shortcomings of the previous ion mobility spectrometers, in particular (a) diffusional broadening
176 gh-sensitivity proton-transfer reaction mass spectrometer installed at a suburban site in Mohali (Pun
177 70 V (Bruker)) or an isotope ratio infrared spectrometer (IRIS) (in this case a Delta Ray (Thermo Fi
180 ng the microfluidic cell culture to the mass spectrometer is challenging because of geometric and sca
183 ation (UVPD) implemented on an Orbitrap mass spectrometer is used to localize double bond positions w
184 CF-MIMS (Continuous Flow Membrane Inlet Mass Spectrometer) is an innovative tool allowing the investi
185 ike UV-vis, FTIR, Raman, and 2D NMR benchtop spectrometers), is shown to provide a detailed methodolo
186 yphenated to an ion-trap time-of-flight mass spectrometer (IT-TOF-MS) for the separation and identifi
187 ract to the liquid chromatograph-tandem mass spectrometer (LC-MS/MS) or direct coupling of the in-tub
188 chromatography/drift tube ion mobility-mass spectrometer (LC/IM-MS) was evaluated for its utility in
189 spectrometer (IMS) to a linear ion trap mass spectrometer (LIT-MS) via modulation of the ion beam wit
190 ted the application of the LTQ-Orbitrap mass spectrometer (LTQ-Velos Pro, Thermo Fisher) for resolvin
191 lyzer is based on a compact laser absorption spectrometer making use of fiber optics for delivery and
192 (maximum as -5.20 dB) than the conventional spectrometer (maximum as -16.84 dB) over the whole imagi
194 In traditional configurations, Brillouin spectrometers measure only one point of the sample at a
196 with a negative-ion chemical ionization mass spectrometer (methane reagent gas) was used for direct s
197 coupled to a membrane inlet quadrupole mass spectrometer (MIMS) was developed for automated and sens
199 lexity and dynamic range and to utilize mass spectrometer (MS) time efficiently, high chromatographic
200 me, we demonstrate a multichannel smartphone spectrometer (MSS) as an optical biosensor that can simu
201 time (DART) ion source with an ion trap mass spectrometer, native cholesterol in its free alcohol for
202 generation Airborne Visible/Infrared Imaging Spectrometer (near-infrared) and Hyperspectral Thermal E
203 uency deflector in combination with a dipole spectrometer not only allows for single-shot extraction
205 returned by the Visible and InfraRed Mapping Spectrometer on board the Dawn spacecraft show a clear d
206 nlinear-based applications, including mid-IR spectrometer-on-a-chip, all-optical wavelength down/up-c
211 urier transform ion cyclotron resonance mass spectrometer only for situations when the prominent mech
212 andling and low-cost benchtop RGA-based mass spectrometer, opening a new strategy for CO2 capture and
213 e cylindrical ion trap (mini-CIT)-based mass spectrometer operated at >/=1 Torr with air as the buffe
214 nted is based on the use of an Orbitrap mass spectrometer operated at a mass resolution of 100 000 to
215 ion gating operation modes and Orbitrap mass spectrometer parameters with regard to sensitivity and r
216 sional purification" inside an ion trap mass spectrometer paving the way for an improved analysis of
219 proton transfer reaction-time-of-flight mass spectrometer (PTR-TOF) using a new gas inlet and an inno
220 proton transfer reaction time-of-flight mass spectrometer (PTR-ToF-MS) at an engine test facility at
221 proton transfer reaction-time-of-flight-mass spectrometer (PTR-ToF-MS) can be used to enhance specifi
222 proton-transfer-reaction time-of-flight mass spectrometer (PTR-ToF-MS), we investigate the emission f
227 eously, we demonstrate the first untuned MPI spectrometer/relaxometer with unprecedented 400 kHz exci
228 ance liquid chromatography coupled to a mass spectrometer repetition and noncompartmental PKs were an
229 esorption/ionization (LDI) in a bipolar mass spectrometer, revealing elemental constituents and limit
230 servations from the Pluto Energetic Particle Spectrometer Science Investigation (PEPSSI) instrument s
231 er we propose a graphene-based ultra-compact spectrometer (several micrometers in size) that is compa
233 chronized scan mirror placed in front of the spectrometer slit positions the Raman signals onto diffe
235 pling valve and a soot particle aerosol mass spectrometer (SP-AMS) enabled online measurements of the
238 recursor ion is isolated twice with the mass spectrometer switching between CID and UVPD activation m
241 es in chemical sampling using miniature mass spectrometer technology are used to monitor slow reactio
242 iniature, visible to near infrared G-Fresnel spectrometer that contains a complete spectrograph syste
244 infrared) and Hyperspectral Thermal Emission Spectrometer (thermal infrared) imaging spectrometers to
245 by LC-HRMS on an Orbitrap Elite hybrid mass spectrometer (Thermo Fisher Scientific, CA, USA) at reso
247 n mass-selected ions and ozone inside a mass spectrometer to assign sites of unsaturation in complex
248 solariX Fourier transform ion cyclotron mass spectrometer to characterize an IgG1 mAb molecule conjug
249 [(18)O]-labeled O2 and a membrane inlet mass spectrometer to characterize Chlamydomonas reinhardtii f
250 DMS effluent was directly coupled to a mass spectrometer to confirm the elemental identity of the se
251 he feasibility of using the new NIR handheld spectrometer to determine quality parameters in the 'Tom
252 oscopy has been carried out in a tandem mass spectrometer to determine the three-dimensional structur
253 real time (DART) coupled to an Orbitrap mass spectrometer to identify the structure of the species ar
254 soil, and a visible-near-infrared (vis-NIR) spectrometer to measure iron oxides and clay mineralogy.
255 hod utilizes the Orbitrap Fusion tribid mass spectrometer to rapidly assign multiple Xle residues in
256 These abilities allow ion trapping mass spectrometers to be filled to capacity with only ions in
257 sion Spectrometer (thermal infrared) imaging spectrometers to better understand the source of methane
258 lve individual wavelengths constrain current spectrometers to bulky sizes, our nano-3D printed protot
259 MS(3) analysis using an Orbitrap Fusion mass spectrometer, to reliably identify Leu and Ile residues
260 s use a wide variety of high-resolution mass spectrometers under different operating conditions, and
261 ed to an ion trap with a time-of-flight mass spectrometer (UPLC-IT-TOF-MS) that allowed the character
262 a diode array detector (HPLC-DAD) and a mass spectrometer (UPLC-MS), was used to compare the direct i
263 egrated in a SLIM and coupled to a QTOF mass spectrometer using an ion funnel interface to evaluate t
264 enterica were directly infused into the mass spectrometer using static source nanoelectrospray ioniza
265 atography (LC) ESII/MS on two different mass spectrometers using a mixture of drugs, a peptide standa
266 fragmentation patterns of molecules in mass spectrometers using electron impact ionization at 70 eV
267 these species by the Ultraviolet and Visible Spectrometer (UVS) on the Lunar Atmosphere and Dust Envi
269 ime ( approximately 1 s) vapor analysis mass spectrometer was developed to provide tools, techniques,
270 ograph coupled with a triple quadrupole mass spectrometer was employed to quantify BMAA and its inter
271 a newly developed isotope ratio mid-infrared spectrometer was introduced with a precision of x((13)C)
272 n IMS-capable quadrupole time-of-flight mass spectrometer was undertaken to allow the introduction of
273 n inductively coupled plasma atomic emission spectrometer was used for Si ion concentration determina
274 n this study, an aerosol time-of-flight mass spectrometer was used to analyze laboratory generated SS
275 ion mobility quadrupole time-of-flight mass spectrometer was used to examine the gas-phase structure
276 o localized surface plasmon resonance (LSPR) spectrometer was utilized to account for changes in SER
277 Here, using an Orbitrap Fusion Tribrid mass spectrometer, we present an optimized methodology that n
278 eady state deposition conditions in an Auger spectrometer were determined to be PtCl2, free of carbon
279 aboratory and with a classical ion trap mass spectrometer were other remarkable characteristics of ne
280 ansform ion cyclotron resonance (FTICR) mass spectrometers when operated under the selected accumulat
281 first time an ambient pressure ion mobility spectrometer which is able to separate ions both by thei
282 teomics studies utilize high-throughput mass spectrometers which can produce data at an astonishing r
283 ates with a low-noise, line-scanning imaging spectrometer, which allowed pigments and paint binders t
284 were measured using an in-house built Raman spectrometer, which has been optimized for measurements
285 ts, made on traveling wave ion mobility mass spectrometers, which have to be calibrated to extract co
286 polarization-resolved terahertz time-domain spectrometer with a broadband (0.3-2.5 THz), rotatable T
288 a compact ultra-high-resolution ion mobility spectrometer with a resolving power of 250 and an UV ion
289 ion for separation, a benchtop Orbitrap mass spectrometer with HCD-MS/MS for peptide sequencing, and
290 ser at 532nm (4ns, 10Hz) attached to echelle spectrometer with intensified charged coupled device (IC
292 nt a fluorescence excitation-emission-matrix spectrometer with superior data acquisition rates over p
294 observations from the Tropospheric Emission Spectrometer with the GEOS-Chem atmospheric model to bet
295 ve been revolutionized by the advent of mass spectrometers with detectors that afford high mass accur
296 re article we argue that development of mass spectrometers with increasingly high resolution and nove
298 illary cell (LWCC) and miniature fiber optic spectrometer, with detection wavelength set at 690 nm.
300 A recently developed simultaneous-detection spectrometer working in the vacuum ultraviolet (VUV) reg
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