If the transition is directly from level 4 to level 1, a single photon - in a single frequency - is emitted. However, it is also possible that an electron falls first from level 4 to level 3, and then from level 3 to level 1, for example. In this case, more than one photon - of different frequencies - can be emitted.
The cause is the transition of electrons after the interaction with a photon.
The range of spectral lines produced during electron transition is determined by the energy difference between the initial and final electronic states. This energy difference corresponds to the photon energy of the emitted light, which dictates the wavelength or frequency of the spectral lines observed in the spectrum. Additionally, the atomic structure and electron configuration of the atom also play a role in determining the specific transitions and resulting spectral lines.
Spectral lines produced by elements are unique to each element due to differences in electron configurations. These lines represent the specific energies emitted or absorbed when electrons transition between energy levels. Analyzing these spectral lines can help identify the presence of specific elements in a sample.
Elements have a specific number of spectral lines because each line corresponds to a specific transition of electrons between energy levels in an atom. The number of spectral lines is determined by the number of energy levels available for electrons to transition between in the atom's electron configuration.
Spectral lines are bright or dark lines in an otherwise continuous or uniform spectrum. They are caused by an excess (emission lines) or deficiency (absorption lines) of observed photons within certain frequency ranges. Absorption lines usually come from a background continuum; photons are absorbed when passing through matter to the observer. Absorption occurs when an electron within an atom absorbs a photons energy and is bumped up to an excited state. Emission lines usually come from hot gases; photons are emitted from these gases and reach the observer. Emission occurs when an electron within an atom falls back down to it's ground state and releases energy in the form of a photon.
Spectral interference occurs when spectral lines overlap. Inductively-coupled plasma mass spectrometry has more spectral interference as its higher energy allows more electron transitions.
Elements with low atomic number can have many spectral lines because their electrons can transition between different energy levels in multiple ways. These transitions result in the emission or absorption of photons with different wavelengths, leading to a variety of spectral lines in the electromagnetic spectrum. In the case of hydrogen, the simple structure of its atom allows for many possible energy level transitions, giving rise to a rich spectrum of spectral lines.
Stars of spectral class M have cooler temperatures compared to stars of other spectral classes, causing their hydrogen lines to weaken and be less prominent in their spectra. The lower temperature results in lower energy levels, making it more difficult for hydrogen atoms to transition between energy levels and emit or absorb light in the hydrogen spectral lines.
A single atom of hydrogen cannot produce all four hydrogen spectral lines simultaneously because each spectral line corresponds to a specific energy transition within the atom's electron configuration. Due to the laws of quantum mechanics, an atom can only emit or absorb energy in discrete amounts, leading to the emission of specific spectral lines corresponding to specific energy transitions.
The spectral lines from distant galaxies do not match those on Earth because of the Doppler effect, cosmic expansion, and differences in elements present in the galaxies. These factors cause the observed spectral lines to be shifted or altered compared to what we see on Earth.
Spectroscopy.
Beryllium spectral lines are specific wavelengths of light emitted or absorbed by beryllium atoms when they undergo transitions between energy levels. These spectral lines are unique to beryllium and can be used in spectroscopic analysis to identify the presence of beryllium in a sample.