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Related Concept Videos

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

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).
There are three main types of inductively coupled plasma atomic emission spectroscopy  (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

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.
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

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...
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...

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High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis
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DAC-board based X-band EPR spectrometer with arbitrary waveform control.

Thomas Kaufmann1, Timothy J Keller, John M Franck

  • 1Department of Chemistry and Biochemistry, University of California Santa Barbara, Santa Barbara, CA, USA.

Journal of Magnetic Resonance (San Diego, Calif. : 1997)
|September 4, 2013
PubMed
Summary

Researchers developed a home-built electron paramagnetic resonance (EPR) spectrometer for precise control of spin systems. This system enables advanced pulse shaping and digital calibration for detailed spin manipulation and analysis.

Keywords:
Arbitrary waveform generationEPRExcitation profilePulse electron paramagnetic resonanceTransfer functionX-band

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Area of Science:

  • Spectroscopy
  • Quantum Control
  • Physical Chemistry

Background:

  • Electron Paramagnetic Resonance (EPR) spectroscopy is a powerful technique for studying systems with unpaired electrons.
  • Precise control over microwave pulse shaping is crucial for advanced EPR experiments and quantum information processing.
  • Existing EPR spectrometers often lack the flexibility for arbitrary waveform generation and precise digital calibration.

Purpose of the Study:

  • To present a home-built, cost-effective EPR spectrometer with arbitrary waveform generation capabilities.
  • To demonstrate precise control over spin systems through tailored microwave pulse shaping.
  • To showcase automated digital calibration and correction routines for enhanced experimental accuracy.

Main Methods:

  • Construction of a simple X-band (8-10 GHz) EPR spectrometer.
  • Integration of a 1 GHz arbitrary waveform generator (AWG) with 14-bit dynamic range.
  • Development of automated digital calibration and feedback routines for pulse shaping and system correction.

Main Results:

  • Demonstrated arbitrary control over a homogenous spin system using shaped X-band pulses.
  • Successfully generated various pulse shapes (rectangular, Gaussian, adiabatic, etc.) with precise amplitude and phase control.
  • Precisely compensated for microwave cavity distortions, yielding optimized, corrected waveforms.

Conclusions:

  • The developed EPR spectrometer offers powerful capabilities for precise spin system manipulation.
  • Automated digital calibration and waveform shaping significantly enhance experimental accuracy and flexibility.
  • This system provides a cost-effective platform for advanced EPR research and potential applications in quantum technologies.