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Introduction to Spectroscopy and Astronomical Observations

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Laboratory Astrophysics

Part of the book series: Astrophysics and Space Science Library ((ASSL,volume 451))

Abstract

This chapter presents an introduction to the techniques and tools used in astronomy and astrophysics research, mainly focused on spectroscopy. The basic concepts of spectroscopy are first described, from the Schrödinger equation to the Lambert–Beer’s law. The spectroscopy of solid systems, widely found in astronomical media, is studied in more detail. An introduction is provided also to the basic concepts of astronomical observations, and the information that can be obtained from them, both in the gas phase and in solid systems. An appendix is included with conversion factors for some of the many magnitudes and units employed in this area.

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Notes

  1. 1.

    There might arise some confusion with the i and f nomenclature for energy levels in Sect. 3.3 above, which is more usually employed in spectroscopy. Subindices i and f refer to the initial and final states of a transition, whereas l and u refer to the lower and upper states. They coincide for absorptions but have the opposite meaning for emissions.

References

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SIESTA:

CASTEP:

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Specific References:

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Acknowledgments

We gratefully acknowledge financial support from Projects FIS2016-C331P, AYA2014-60585-P and AYA2015-71975-REDT of the Spanish MINECO. We are grateful to Angel González Valdenebro for help with the figures.

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Correspondence to Rafael Escribano .

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Appendix: Units and Conversion Factors

Appendix: Units and Conversion Factors

Several units are used in spectroscopy which are especially suitable for specific spectral regions, or traditionally used by spectroscopists or astrophysicists. Some of them are listed below, where <> means equivalent to, and c = 2.99792458 × 1010 cm s−1, Avogadro’s number NA = 6.0221367 × 1023 molec mol−1, Boltzman’s constant k = 1.38064852 × 10−23 m2 kg s−2 K−1 (1.38064852 × 10−16 erg K−1 in cgs units) and Planck’s constant h = 6.6260755 × 10−34 J s:

Frequency ν (microwave region) to wavenumber \( \overline{\nu} \): 1 GHz = 109 Hz <> 1/c cm−1= 3.33564 ×10 −2 cm−1; 1 kHz = 103 Hz <> 3.33564 × 10−8 cm−1.

Wavenumber \( \overline{\nu} \) (infrared region) to wavelength λ: mid-IR region: 1000 cm−1 <>10 μm; 3000 cm−1 <> 3.333 μm; near-IR region: 6000 cm−1 <> 1.6 μm.

Wavelength λ (visible and UV regions) to energy E: 1 μm <> (hc/λ) 1.986447 × 10−19 J <> (hcNA) 11.96266 × 104 J mol−1; 665 nm (approx. red light) <> 17.98899 × 104 J mol−1.

Other energy units (X-ray region): 100 eV <> 9.64853 × 106 J mol−1 <> 1.23984× 10−2 μm.

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Escribano, R., Muñoz Caro, G.M. (2018). Introduction to Spectroscopy and Astronomical Observations. In: Muñoz Caro, G., Escribano, R. (eds) Laboratory Astrophysics . Astrophysics and Space Science Library, vol 451. Springer, Cham. https://doi.org/10.1007/978-3-319-90020-9_3

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