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Atomic emission and absorption spectra are determined by discrete electron energy transitions
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Authoritative scientific references establish that atomic emission and absorption spectra arise from discrete electron transitions between energy states.

Evidence for · 4
2020 · cited by 5
Abstract Fraunhofer, in 1814, was the first to observe spectral lines due to absorption in the solar spectrum almost 150 years after the discovery of the spectrum by Newton. In 1859 Kirchhoff and Bunsen recorded emission and absorption spectra of many elements establishing the fact that each element has its unique line spectrum. Bohr's theory of hydrogen atoms was followed by quantum mechanics to show that an atomic line results from the transition of an atom between a pair of its internal energy states. Atomic emission spectrum results in atomic transition from quantum states of higher energy to those of lower energy. The quantum states of an atom depend on its electronic configuration, and the transitions between any pair of states are governed by dipole selection rules. The periodic table can also be described in terms of the electronic configuration of elements. Each spectral line is characterized by its wavelength and intensity, and these are used in trace detection of various elements in any sample. Spectral intensity plays a major role in the quantitative analysis of elements in an unknown sample.
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are many possible electron transitions for each atom, and each transition has a specific energy difference. This collection of different transitions, The emission spectrum of a chemical element or chemical compound is the spectrum of frequencies of electromagnetic radiation emitted due to electrons making a transition from a high energy state to a lower energy state. The photon energy of the emitted photons is equal to the energy difference between the two states. There are many possible electron transitions for each atom, and each transition h Emission spectroscopy is a spectroscopic technique which examines the wavelengths of photons emitted by atoms or molecules during their transition from an excited state to a lower energy state. Each element emits a characteristic set of discrete wavelengths according to its electronic structure, and by observing these wavelengths the elemental composition of the sample can be determined. Emission spectroscopy developed in the late 19th century and efforts in theoretical explanation of atomic emission spectra eventually led to quantum mechanics. There are many ways in which atoms can be brought to an excited state. Interaction with electromagnetic radiation is used in fluorescence spectroscopy, protons or other heavier particles in particle-induced X-ray emission and electrons or X-ray photons in energy-dispersive X-ray spectroscopy or X-ray fluorescence. The simplest method is to heat the sample to a high temperature, after which the excitations are produced by collisions between the sample atoms. This method is used in flame emission spectroscopy, and it was also the method used by Anders Jonas Ångström when he discovered the phenomenon of discrete emission lines in the 1850s. Although the emission lines are caused by a transition between quantized energy states and may at first look very sharp, they do have a finite width, i.e. they are composed of more than one wavelength of light. This spectral line broadening has many different causes. Emission spectroscopy is often referred to as optical emission spectroscopy because of the light nature of what is being emitted.
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The discrete energy levels of higher harmonics correspond to higher orbitals. Electrons can gain energy to exist in a higher orbital. When this process occurs via interaction with electromagnetic radiation, it is referred to as absorption. Similarly, the regression of an electron into a lower energy orbital results in the release of electromagnetic radiation, and is referred to as emission. Because of the quantized energy levels demanded by a bound system, electrons in a molecule or atom can only absorb or emit light at specific frequencies, which depend on the properties of the system. Certain materials have energy level spacing such that excitation by an energy source can produce a greater number of electrons in an excited state than in the ground state. This is known as population inversion. When this happens for a transition which releases light upon relaxation, light of a specific nature is produced that has great practical importance. This light is monochromatic, and can be channeled back and forth through the medium (gain medium) and allowed only to disperse through a very narrow slit to produce monochromatic, directional, coherent light source.
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that it related the lines in emission and absorption spectra to the energy differences between the orbits that electrons could take around an atom. This In quantum mechanics, an atomic orbital is a function describing the location and wave-like behavior of an electron in an atom. This function describes an electron's charge distribution around the atom's nucleus, and can be used to calculate the probability of finding an electron in a specific region around the nucleus. Each orbital in an atom is characterized by a set of values of three quantum n A…
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  1. Emission spectrumreferencesame source L1no side taken
  2. Atomic emission spectroscopypeer-reviewedno side taken
  3. LibreTexts: 1.5A%3A Wave Mechanics of Electronsreferenceno side taken
  4. Atomic orbitalreferencesame source L1no side taken
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