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NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

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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Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He mathematically...
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The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this particular...
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An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
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The Discrete Fourier Transform (DFT) is a fundamental tool in signal processing, extending the discrete-time Fourier transform by evaluating discrete signals at uniformly spaced frequency intervals. This transformation converts a finite sequence of time-domain samples into frequency components, each representing complex sinusoids ordered by frequency. The DFT translates these sequences into the frequency domain, effectively indicating the magnitude and phase of each frequency component present...
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The Fourier series is a powerful mathematical tool for representing periodic signals as an infinite sum of complex exponentials. In practice, this infinite series is truncated to a finite number of terms, yielding a partial sum. This truncation makes the approximation of the signal feasible but introduces certain challenges, particularly near discontinuities, known as the Gibbs phenomenon.
The Gibbs phenomenon refers to the persistent oscillations and overshoots that occur near discontinuities...

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Updated: Jun 10, 2026

Measurements of Long-range Electronic Correlations During Femtosecond Diffraction Experiments Performed on Nanocrystals of Buckminsterfullerene
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Why projection-based WF-in-DFT cannot be exact, even with the exact exchange-correlation functional. Formal and

Enzo Monino1, Daria Drwal2, Michał Hapka3

  • 1J. Heyrovský Institute of Physical Chemistry, Academy of Sciences of the Czech Republic, v.v.i., Dolejškova 3, 18223 Prague 8, Czech Republic.

The Journal of Chemical Physics
|June 9, 2026
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Summary

This study develops theoretical foundations for embedding quantum wavefunctions within density functional theory (DFT) environments. It identifies errors in embedding methods, primarily stemming from the interface between the active system and its environment.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Materials Science

Background:

  • Embedding correlated wavefunctions in environmental fields is crucial for accurate molecular simulations.
  • Density functional theory (DFT) provides a computationally efficient framework for electronic structure calculations.
  • Accurate treatment of subsystem-environment interactions is essential for reliable predictions.

Purpose of the Study:

  • Establish theoretical foundations for wavefunction-in-DFT embedding.
  • Analyze error sources in projection-based density matrix renormalization group-in-DFT.
  • Improve the accuracy of quantum embedding methods for chemical systems.

Main Methods:

  • Developed an approximate kinetic-energy functional for embedding.
  • Formulated a projection-based wavefunction-in-DFT embedding functional.
  • Analyzed errors using molecules with dissociating covalent bonds.
  • Investigated the impact of approximate exchange-correlation (xc) functionals.

Main Results:

  • The derived embedding functional is nonvariational, with its minimum bounded above by the exact ground-state energy.
  • The primary error source in density matrix renormalization group-in-DFT embedding is the nonadditive xc energy at the subsystem-environment interface.
  • Employing pair-density xc functionals does not resolve inaccuracies due to self-interaction effects at the interface.

Conclusions:

  • The theoretical framework reveals inherent limitations in current wavefunction-in-DFT embedding approaches.
  • Self-interaction errors at the subsystem-environment interface are a key deficiency in approximate embedding functionals.
  • Further development is needed to address these errors for more accurate quantum simulations.