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Related Concept Videos

Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

632
The underlying principle of Raman spectroscopy is based on the interaction between light and matter, specifically molecules' inelastic scattering of photons. When a monochromatic beam of light, typically from a laser source, interacts with a sample, most scattered light has the same frequency as the incident light. This is known as Rayleigh scattering.
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
632
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

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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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Chemical Shift: Internal References and Solvent Effects01:17

Chemical Shift: Internal References and Solvent Effects

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In an NMR sample, precise measurement of the absolute absorption frequencies of nuclei is difficult. A standard internal reference compound is added, and the frequency difference between the reference signal and sample signals is measured.
The internal reference compound generally used in NMR spectroscopy is tetramethylsilane (TMS). TMS is preferred because it is chemically inert, soluble in NMR solvents, and easily removable. Also, the highly shielded methyl protons in TMS yield an intense...
826
Inductive Effects on Chemical Shift: Overview01:27

Inductive Effects on Chemical Shift: Overview

1.3K
The protons in unsubstituted alkanes are strongly shielded with chemical shifts below 1.8 ppm. Methine, methylene, and methyl protons appear at approximately 1.7, 1.2 and 0.7 ppm, while the proton signal from methane appears at 0.23 ppm. An electronegative substituent, such as chlorine, withdraws the electron density from the protons, increasing their chemical shift. Progressive substitution of the hydrogens in methane by chlorine shifts the proton signals increasingly downfield, to 3.05 ppm in...
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Hybridization of Atomic Orbitals II03:35

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sp3d and sp3d 2 Hybridization
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The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Transfer-Learning Deep Raman Models Using Semiempirical Quantum Chemistry.

Jawad Kamran1,2, Julian Hniopek1,2, Thomas Bocklitz1,2

  • 1Institute of Physical Chemistry, Friedrich Schiller University Jena, Helmholtzweg 4, 07743 Jena, Germany.

Journal of Chemical Information and Modeling
|June 18, 2025
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Summary
This summary is machine-generated.

Researchers generated simulated Raman spectra to pretrain deep learning models, overcoming data limitations in biophotonics. This approach enhances model generalizability and reduces computational costs for spectral analysis.

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Area of Science:

  • Biophotonics
  • Spectroscopy
  • Computational Chemistry

Background:

  • Raman spectroscopy provides specific molecular information with minimal sample preparation.
  • Its application is widespread, often enhanced by chemometrics, machine learning (ML), and deep learning (DL).
  • A key challenge is the lack of large, independent Raman spectra databases, hindering model training and generalizability.

Purpose of the Study:

  • To address the data scarcity issue in Raman spectroscopy for deep learning model training.
  • To develop a scalable framework for spectral analysis using synthetic data.
  • To improve the generalizability and reduce the computational cost of deep Raman models.

Main Methods:

  • Generating simulated vibrational spectra using semiempirical quantum chemistry methods.
  • Pretraining deep learning models on large synthetic spectral datasets.
  • Fine-tuning pretrained models on smaller, experimental bacterial Raman spectra datasets.
  • Employing transfer learning techniques.

Main Results:

  • Synthetic data enabled efficient pretraining of deep learning models.
  • Transfer learning achieved performance comparable to models trained from scratch.
  • The approach significantly reduced computational costs.
  • Validated the utility of synthetic data for deep Raman model development.

Conclusions:

  • Synthetic data generation is a viable strategy for pretraining deep Raman models.
  • Transfer learning offers a scalable and cost-effective framework for spectral analysis.
  • This method is particularly beneficial for resource-limited settings in biophotonics.