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Related Concept Videos

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

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Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
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A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
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The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
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NMR spectrometers consist of a strong magnet, a radiofrequency transmitter, and a detector attached to a computer console for recording spectra of samples containing NMR-active nuclei. In first-generation NMR instruments called continuous-wave spectrometers, the resonance frequencies of the nuclei are determined by frequency-sweep or field-sweep methods. The magnetic field strength is fixed and the rf signal is swept in the former, while the radiofrequency signal is fixed and the magnetic field...
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AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...
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When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
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Continuous wave electron paramagnetic resonance L-band spectrometer with direct digitalization using time-locked

J Kozioł1, P Rajda2, R Rumian2

  • 1Jagiellonian University, Faculty of Biochemistry, Biophysics and Biotechnology, Department of Molecular Biophysics, 7 Gronostajowa St., 30-387 Krakow, Poland.

Journal of Magnetic Resonance (San Diego, Calif. : 1997)
|November 28, 2020
PubMed
Summary
This summary is machine-generated.

A new digital L-band Electron Paramagnetic Resonance (EPR) spectrometer utilizes direct digital detection with time-locked subsampling (TLSS). This advanced EPR system achieves high signal-to-noise ratios, potentially replacing traditional analog methods.

Keywords:
Direct digital detectionEPRL-band

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Area of Science:

  • Spectroscopy
  • Physical Chemistry
  • Instrumentation

Background:

  • Conventional Continuous Wave (CW) Electron Paramagnetic Resonance (EPR) spectrometers often rely on analog components and magnetic field modulation.
  • Direct digital detection offers potential advantages in terms of signal processing and sensitivity.

Purpose of the Study:

  • To describe a novel digital L-band EPR spectrometer employing direct digital detection with time-locked subsampling (TLSS).
  • To evaluate the performance of this new spectrometer, particularly its phase noise characteristics and signal-to-noise (S/N) ratio.

Main Methods:

  • Development of a microwave source using direct digital synthesis (DDS) with an ultra-low noise master clock.
  • Implementation of a digital receiver with a high-speed Analog-to-Digital Converter (A/D) for direct signal digitalization.
  • Time-locking of the generator and receiver using a common reference source for simultaneous absorption and dispersion signal detection.

Main Results:

  • Achieved exceptionally low phase noise (-140 dBc/Hz at 30.5 kHz from 1.15 GHz carrier).
  • Demonstrated simultaneous detection of absorption and dispersion signals.
  • Obtained a S/N ratio greater than 160 for an 11 µm aqueous TEMPOL solution within 69 seconds.

Conclusions:

  • The developed digital L-band EPR spectrometer represents a significant advancement in EPR instrumentation.
  • The direct digital detection technique, as implemented, shows promise for replacing conventional analog CW spectrometers.
  • The spectrometer's performance, particularly its low phase noise and high S/N ratio, validates the employed methodology.