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Lyman Series of Hydrogen

On the Lyman system of hydrogen
Between heaven and earth, everything has its own reason. In the microscopic domain, the Lyman system of hydrogen atomic spectrum is the key to physical investigation.

Hydrogen atoms, the simplest atoms, contain endless mysteries in their spectra. The Lyman system is a specific series of spectral lines in the spectrum of hydrogen atoms. This spectrum line is generated when the electrons of hydrogen atoms transition from the high energy level to the ground state.

The principle is that electrons have a specific energy level in atoms, and the high energy level is unstable and tends to transition to a low energy level. During this process, energy is released in the form of photons, and the frequency of the photons is related to the energy level difference. The Lyman line corresponds to the transition of the electron from the $n $ ($n\ geq2 $) energy level to the ground state ($n = 1 $).

After many experimental investigations and theoretical deductions, the wavelength of the Lyman line satisfies a specific formula: $\ frac {1} {\ lambda} = R_H (\ frac {1} {1 ^ 2} -\ frac {1} {n ^ 2}) $, $n = 2,3,4,\ cdots $, where $R_H $is the Rydberg constant. This formula accurately describes the law of the wavelength of the Lyman line.

The research of the Lyman line is of great significance to the development of physics. To help us gain a deeper understanding of atomic structure and quantum theory, paving the way for the exploration of the microscopic world. From understanding the behavior of electrons in atoms to promoting progress in many fields of modern physics, it all depends on this.

Viewing the Freeman system, in the microscopic realm, uncovering the mysteries of atoms, developing the subtlety of physics, and leading our generation to constantly pursue the truth of the universe and explore the unknown. This is the charm and mission of science.