Mass spectrometry has become an increasingly important tool of high accuracy, efficiency, and speed for the routine analysis of nucleic acids. To make it useful for large-scale sequencing of genomic material as required for example in genotyping and clinical diagnosis, it is necessary to find approaches that allow the analysis of sequences much larger than the 100 nucleotides currently possible. Matrix-assisted laser desorption/ionization (MALDI) mass spectra of synthetic DNA, restriction enzyme fragments of plasmid DNA, and RNA transcripts up to a size of 2180 nucleotides are reported. The demonstrated mass accuracy of 1 percent or better and the sample requirement of a few femtomoles or less surpass all currently available techniques for the analysis of large nucleic acids. DNA and RNA can be analyzed with only a limited investment in sample purification.

The nine C-terminal amino acids of the respiratory syncytial virus protein P are necessary and sufficient for binding to ribonucleoprotein complexes in which six ribonucleotides are contacted per N protein protomer The respiratory syncytial virus (RSV) phosphoprotein (P) is a major polymerase co-factor that interacts with both the large polymerase fragment (L) and the nucleoprotein (N). The N-binding domain of RSV P has been investigated by co-expression of RSV P and N proteins in Escherichia coli. Pull-down assays performed with a series of truncated forms of P fused to glutathione S-transferase (GST) revealed that the region comprising the last nine C-terminal amino acid residues of P (233-DNDLSLEDF-241) is sufficient for efficient binding to N. Site-directed mutagenesis shows that the last four residues of this peptide are crucial for binding and must be present at the end of a flexible C-terminal tail. The presence of the P oligomerization domain (residues 100-160) was an important stabilizing factor for the interaction. The tetrameric full-length P fused to GST was able to pull down both helical and ring structures, whereas a monomeric Cterminal fragment of P (residues 161-241) fused to GST pulled down exclusively RNA-N rings. Electron-microscopy analysis of the purified rings showed the presence of two types of complex: undecamers (11N) and decamers (10N). Mass-spectrometry analysis of the RNA extracted from rings after RNase A treatment showed two peaks of 22 900 and 24 820 Da, corresponding to a mean RNA length of 67 and 73 bases, respectively. These results suggest strongly that each N subunit contacts 6 nt, with an extra three or four bases further protected from nuclease digestion by the ring structure at both the 59 and 39 ends.

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Lasers emitting in the ultraviolet wavelength range of 260-360 nm are almost exclusively used for matrixassisted laser desorption/ionization mass spectrometry (MALDI-MS) of macromolecules. Reports about the use of lasers emitting in the infrared first appeared in 1990/1991. In contrast to MALDI in the ultraviolet, a very limited number of reports on IR-MALDI have since been published. Several matrices have been identified for infrared MALDI yielding spectra of a quality comparable to those obtained in the ultraviolet. Water (ice) was recognized early as a potential matrix because of its strong 0-H stretching mode near 3 ,m.Interest in water as matrix derives primarily from the fact that it is the major constituent of most biological tissues. exceeding that of typical MALDI conditions by three orders of magnitude. The laser energy is assumed to be absorbed by the copper substrate; sodium, resonantly excited by the 589-nm photons, is believed to assist in the ionization process. Interestingly, they also encountered the problem of very limited reproducibility and reported that good spectra are obtained from the sample rim only. This paper reports the rather unexpected and surprising results of a series of systematic, experiments designed to assess the utility of ice as a MALDI-matrix in the infrared. EXPERIMENTAL PROCEDURESAn in-house built reflectron time-of-flight instrument of 3.5 m equivalent flight length and a 12 kV acceleration potential was used for all experiments (3). Working pressure in the sample chamber is 3 x 10-4 Pa. Ions are detected by a conversion dynode (ion impact energy 20-27 kV, depending on ion mass) mounted 1 cm in front of a venetian blind secondary electron multiplier (EMI R2362

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