A reaction detector system is described which can be used for simultaneous analysis of primary amino groups and sulfhydryl groups in peptides separated by high-performance liquid chromatography. By use of an automatic split valve system, well-defined portions of the effluent are diverted alternately into one of the two reaction detectors, based on the ninhydrin and Ellman assay, respectively. In the latter case the dithioerythritol included in the elution buffers for thiol preservation is eliminated with arsenite. For selective recovery of eluted peptides the amino/thiol group analyser can easily be converted into a high-yield monitoring system compatible with volatile, UV-opaque gradient buffers. In this version an automatic sample valve is used for the thiol assay, removing picomole amounts of material from the effluent destined for collection. In preparative applications there is a progressive net gain in sensitivity with increasing proportion of collected material. Under conditions of optimum recovery ca. 90% of the material could be recovered at a total consumption in the two detectors of less than 100 pmol. Experimental conditions are described which would allow for the additional identification of tryptophan, tyrosine and lysine-containing peptides. The monitoring system may also be used without modification for the assessment of key residues in polypeptides and proteins.
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http://dx.doi.org/10.1016/s0021-9673(01)89047-6 | DOI Listing |
Med Phys
March 2025
Division of Biomedical Physics in Radiation Oncology, German Cancer Research Center (DKFZ), Heidelberg, Germany.
Background: Precise range verification is essential in proton therapy to minimize treatment margins due to the steep dose fall-off of proton beams. The emission of secondary radiation from nuclear reactions between incident particles and tissues stands out as a promising method for range verification. Two prominent techniques are PET and Prompt Gamma-Ray Spectroscopy (PGS).
View Article and Find Full Text PDFAppl Radiat Isot
February 2025
Department of Electrical Power Engineering, Brno University of Technology, Brno, 61600, Czech Republic.
The cross-section measurement of Antimony (Sb) is pivotal to modify or stagnate the rate of neutron flux in nuclear reactors. Neutron induced reaction cross-section data for isotopes of Sb is meagre as per reported in EXFOR. A comprehensive attempt has been made to analyse the reaction cross-section of Sb and Sb at monoenergetic neutron energy of 14.
View Article and Find Full Text PDFRev Sci Instrum
March 2025
Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
The National Ignition Facility (NIF) has 48 Real-Time Nuclear Activation Detectors distributed around the target chamber capable of measuring deuterium-triton reaction neutron yields with high precision. In this work, we extend this functionality to deuterium-deuterium (DD) reaction neutrons using a nuclear reaction that occurs in the detector's scintillator material. The corresponding decay of the activated material has a very short half-life of 5 s, which necessitates rapid data collection immediately following an experiment.
View Article and Find Full Text PDFOral Radiol
March 2025
Department of Prosthodontics and Oral Rehabilitation, Graduate School of Biomedical Sciences, Tokushima University, Tokushima, Japan.
Objectives: Zirconia oral implants produce larger artifacts on computed tomography (CT) compared to titanium oral implants. This study aimed to compare the effectiveness of metal artifact reduction (MAR) software and dual-energy (DE) methods, which are used in multi-detector CT (MDCT) to reduce the artifacts produced by titanium and zirconia oral implants.
Methods: Oral implants were placed in the lower right second premolar and second molar regions of an acrylic mandible model and evaluated using MDCT.
Appl Radiat Isot
March 2025
Institute of Nuclear Physics and Chemistry, China Academy of Engineering Physics, Mianyang, 621900, China.
The cross sections of the Kr(n,p)Br reaction were measured through the secondary decay of the residual nucleus Br at the neutron energies of 13.59, 13.86, 14.
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