Ice As a Matrix for IR-Matrix-Assisted Laser Desorption/Ionization

Ice As a Matrix for IR-Matrix-Assisted Laser Desorption/Ionization

Proc. Natl. Acad. Sci. USA Vol. 93, pp. 7003-7007, July 1996 Biochemistry Ice as a matrix for IR-matrix-assisted laser desorption/ionization: Mass spectra from a protein single crystal STEFAN BERKENKAMP, MICHAEL KARAst, AND FRANz HILLENKAMPt Institute for Medical Physics and Biophysics, University of Munster, Robert-Koch Strasse 31, D-48149 Muenster, Germany Communicated by Fred W. McLafferty, Cornell University, Ithaca, NY, March 6, 1996 (received for review November 13, 1995) ABSTRACT Lasers emitting in the ultraviolet wavelength ated with the vast majority of biological molecules. If func- range of 260-360 nm are almost exclusively used for matrix- tional, it might allow the in situ analysis of macromolecular assisted laser desorption/ionization mass spectrometry constituents in frozen cell sections without extraction or (MALDI-MS) of macromolecules. Reports about the use of exchanging the water with another suitable matrix. However, lasers emitting in the infrared first appeared in 1990/1991. In attempts to obtain spectra from samples of bulk, frozen contrast to MALDI in the ultraviolet, a very limited number aqueous protein solutions failed (6). Sporadic protein signals of reports on IR-MALDI have since been published. Several of poor signal-to-noise-ratio and reproducibility were obtained matrices have been identified for infrared MALDI yielding exclusively from the very rim of the sample. The latter spectra of a quality comparable to those obtained in the observation is in agreement with results reported by Williams ultraviolet. Water (ice) was recognized early as a potential and coworkers (7, 8) who also used frozen solutions of DNA matrix because ofits strong 0-H stretching mode near 3 ,m. as well as a few proteins for laser ablation time-of-flight MS. Interest in water as matrix derives primarily from the fact that Their experimental approach and rational is, however, very it is the major constituent of most biological tissues. If a functional as matrix, it might allow the in situ analysis of different from the standard MALDI technique. They placed macromolecular constituents in frozen cell sections without layer of the frozen sample solution of a few micrometers extraction or exchanging the water. We present results that thickness onto a corroded copper surface and irradiated with show that IR-MALDI of lyophilized proteins, air dried protein a wavelength of 589 nm and an irradiance of about 109 W/cm2, solutions, or protein crystals up to a molecular mass of30 kDa exceeding that of typical MALDI conditions by three orders of is possible without the addition of any separate matrix. magnitude. The laser energy is assumed to be absorbed by the Samples must be frozen to retain a sufficient fraction of the copper substrate; sodium, resonantly excited by the 589-nm water of hydration in the vacuum. The limited current sensi- photons, is believed to assist in the ionization process. Inter- tivity, requiring at least 10 pmol of protein for a successful estingly, they also encountered the problem of very limited analysis needs to be further improved. reproducibility and reported that good spectra are obtained from the sample rim only. Matrix-assisted laser desorption/ionization mass spectrometry This paper reports the rather unexpected and surprising (MALDI-MS) has become a widely used technique for the results of a series of systematic, experiments designed to assess analysis oflarge biological molecules (1). Lasers emitting in the the utility of ice as a MALDI-matrix in the infrared. ultraviolet (UV) wavelength range of 260-360 nm and matri- ces absorbing strongly in this range are almost exclusively used in MALDI instruments. First reports about the use of lasers EXPERIMENTAL PROCEDURES emitting in the infrared (IR) at wavelengths around 3 ,um [erbium-yttrium-aluminium garnet laser] and 10.6 p.m (CO2 An in-house built reflectron time-of-flight instrument of 3.5 m laser) appeared as early as 1990 (2, 3). A host of potential equivalent flight length and a 12 kV acceleration potential was matrices are available with a strong absorption at these wave- used for all experiments (3). Working pressure in the sample lengths, mainly resulting from 0-H and N-H vibrational chamber is 3 x 10-4 Pa. Ions are detected by a conversion modes at 3 ,um. Several of them, such as succinic acid, glycerol, dynode (ion impact energy 20-27 kV, depending on ion mass) or urea, have been proven to be functional matrices yielding mounted 1 cm in front of a venetian blind secondary electron spectra of a quality comparable to those obtained in the UV multiplier (EMI R2362). Signals are processed by a transient (4). The IR absorption, even though a factor of at least 10 recorder with a time resolution of 10 ns (LeCroy 9400A) and weaker than those encountered in the UV, leads to enough then transferred to a personal computer for storage and deposition of energy into the sample to make plausible the further evaluation. Single pulses of an erbium-yttrium- desorption of molecules. In addition, the fact that the spectral aluminum garnet laser (SEO 1-2-3, Schwartz Electro Optics, essential features recorded with either UV or IR wavelengths Orlando, FL) of - 150 ns duration at a wavelength of 2.94 gm are virtually identical suggests that the mechanisms of desorp- are focused to a spot diameter of 180 gm with a 450 angle. The tion and the function of the matrix are essentially identical in instrument is equipped with a liquid nitrogen cooling stage. both cases. However, the ionization step in IR-MALDI is still The temperature of the stainless steel substrate is monitored unknown, in contrast to the UV for which credible models with a thermocouple with an absolute accuracy of ±5 K, but have been suggested (5). Water in the frozen state (to provide it may be possible that the actual temperature of the top layer, compatibility with the vacuum requirements of the spectrom- even of very thin samples, is slightly higher than the measured eter) was recognized early as a potential matrix because of its substrate temperature. strong 0-H stretching mode near 3 ,um. Interest in water as matrix derives primarily from the fact that it is the major constituent of most biological tissues and is naturally associ- Abbreviation: MALDI-MS, matrix-assisted laser desorption/ ionization mass spectrometry. tPresent address: Division of Instrumental and Analytical Chemistry, The publication costs of this article were defrayed in part by page charge University of Frankfurt, Theodor-Stern-Kai 7, D-60590 Frankfurt, payment. This article must therefore be hereby marked "advertisement" in Germany. accordance with 18 U.S.C. §1734 solely to indicate this fact. *To whom reprint requests should be addressed. 7003 Downloaded by guest on September 23, 2021 7004 Biochemistry: Berkenkamp et al. Proc. Natl. Acad. Sci. USA 93 (1996) RESULTS to the very thin sample layer. Three temperature ranges can be differentiated for the analysis: For temperatures below about All attempts to improve quality and reproducibility of protein 170 K no useful protein signals are observed, presumably spectra obtained from samples of bulk, frozen aqueous solu- because the is still tions (typically 3-10 ,ul) by variation of all accessible param- sample covered by frost, which accumulates eters, in particular, the concentration of analyte solution from primarily during the sample introduction into the vacuum. 10-6 M to saturation (which for most biomolecules is about Very good spectra can be obtained in the range of 170-220 K 10-4 M-10-3 M), source pressure, addition of salts (sodium, for several hours after sample introduction into the vacuum. potassium), magnitude of irradiance from 2 x 106 W/cm2 to For some proteins this temperature range extends as high as 5 x 107 W/cm2, variation of substrate material (copper, 240-270 K. Mass resolution (FWHM) of 300-350 is routinely stainless steel, silver, aluminum, etc.) gave very unsatisfactory obtained for proteins up to a molecular mass of 20 kDa in this results: either no signal or only those of water clusters up to a temperature range; selected spectra exhibit a mass resolution mass of "5000 Da were obtained. Protein signals of poor of up to 700 as demonstrated for cytochrome c in Fig. 2. This signal-to-noise-ratio (typically s/n ' 10) were obtained only contrasts with a resolution of 150-200 obtainable with the from the very rim of the sample and only in 10-30% of the given instrument for standard preparations of the same pro- exposures, depending on the sample temperature. Fig. 1 shows teins under optimal conditions in UV- and IR-MALDI. Above a spectrum that was obtained from a 3 x 10-3 M solution of these temperatures the sample loses its water of hydration by lysozyme at T = 160 K. Resolution of the MI is only =40 full sublimation or evaporation on a time scale too short for useful width at half maximum (FWHM) with the doubly charged mass spectrometry. Good spectra of molecules above 10 kDa lysozyme as the base peak. typically require a protein concentration of 10-3 M; however, The situation changes dramatically if the samples (typically spectra have been obtained from 10-5 M solutions, although 3-5 Al of a 10-3 M solution) are first "dried" under ambient with a substantially decreased signal-to-noise-ratio and a conditions before being frozen to liquid nitrogen temperature. strong low mass signal background. For sample solutions below Similar results are obtained if a few flakes of lyophilized 10-5 M, analysis is also possible if several layers of sample are protein are applied directly to the substrate and frozen. All prepared on top of each other.

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