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{{Short description|Quantum Collection topic on Quantum Hydrogen atom}}
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{{Quantum book backlink|Atomic and spectroscopy}}
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The '''hydrogen atom''' is the simplest atomic system, consisting of a single electron bound to a proton by the Coulomb interaction. It is the only atom in quantum mechanics that admits a fully exact analytical solution of the Schrödinger equation, making it a fundamental model for understanding atomic structure, spectroscopy, and quantum theory.<ref>[https://phys.libretexts.org/Bookshelves/University_Physics/University_Physics_%28OpenStax%29/University_Physics_III_-_Optics_and_Modern_Physics_%28OpenStax%29/08%3A_Atomic_Structure/8.02%3A_The_Hydrogen_Atom The Hydrogen Atom (OpenStax/LibreTexts)]</ref>
'''Hydrogen atom''' the hydrogen atom is the simplest atomic system, consisting of a single electron bound to a proton by the Coulomb interaction. It is the only atom in quantum mechanics that admits a fully exact analytical solution of the Schrödinger equation, making it a fundamental model for understanding atomic structure, spectroscopy, and quantum theory. The hydrogen atom is the simplest atomic system, consisting of a single electron bound to a proton by the Coulomb interaction. It is the only atom in quantum mechanics that admits a fully exact analytical solution of the Schrödinger equation, making it a fundamental model for understanding atomic structure, spectroscopy, and quantum theory. The electron in a hydrogen atom is described by the time-independent Schrödinger equation in a central Coulomb potential:
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{{Author|Harold Foppele}}
{{Author|Harold Foppele}}


{{Sourceattribution|Quantum Hydrogen atom|1}}
{{Sourceattribution|Physics:Quantum Hydrogen atom|1}}

Latest revision as of 11:31, 22 May 2026

← Previous : Atomic structure and spectroscopy
Next : Number →

Hydrogen atom the hydrogen atom is the simplest atomic system, consisting of a single electron bound to a proton by the Coulomb interaction. It is the only atom in quantum mechanics that admits a fully exact analytical solution of the Schrödinger equation, making it a fundamental model for understanding atomic structure, spectroscopy, and quantum theory. The hydrogen atom is the simplest atomic system, consisting of a single electron bound to a proton by the Coulomb interaction. It is the only atom in quantum mechanics that admits a fully exact analytical solution of the Schrödinger equation, making it a fundamental model for understanding atomic structure, spectroscopy, and quantum theory. The electron in a hydrogen atom is described by the time-independent Schrödinger equation in a central Coulomb potential:

Quantum Hydrogen atom.

Schrödinger equation and Coulomb potential

The electron in a hydrogen atom is described by the time-independent Schrödinger equation in a central Coulomb potential:

[22m2e24πε0r]ψ(𝐫)=Eψ(𝐫)

Because the potential depends only on the radial coordinate r, the equation is separable in spherical coordinates.[1]

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Quantum numbers

The solutions are characterized by three quantum numbers:

  • Principal quantum number: n=1,2,3,
  • Orbital angular momentum: =0,1,,n1
  • Magnetic quantum number: m=,,

These arise from the separation of variables into radial and angular parts.[2]

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Energy levels

The allowed energy levels depend only on the principal quantum number:

En=13.6eVn2

This degeneracy is a consequence of the underlying symmetry of the Coulomb potential.[3]

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Wavefunctions and orbitals

The hydrogen wavefunctions are products of radial functions and spherical harmonics:

ψnm(r,θ,ϕ)=Rn(r)Ym(θ,ϕ)

These define the familiar atomic orbitals:

  • s-orbitals (=0) — spherical symmetry
  • p-orbitals (=1) — directional lobes
  • d-orbitals (=2) — more complex structures

[4]

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Angular momentum

The orbital angular momentum is quantized:

L2=2(+1),Lz=m

The hydrogen atom also includes electron spin, introducing total angular momentum when relativistic effects are considered.[5]

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Spectral lines

Transitions between energy levels produce photons with energy:

E=hν=EiEf

This gives rise to discrete spectral series:

  • Lyman series (n1) — ultraviolet
  • Balmer series (n2) — visible
  • Paschen, Brackett, Pfund — infrared

The wavelengths satisfy the Rydberg formula:

1λ=RH(1nf21ni2)

where RH is the Rydberg constant.[6][7]

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Fine and hyperfine structure

More accurate treatments include:

  • Fine structure — relativistic corrections and spin–orbit coupling
  • Hyperfine structure — interaction between electron and nuclear spin

These effects lift degeneracies and produce small spectral splittings.[8][9]

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Importance in quantum mechanics

The hydrogen atom plays a central role because:

  • It provides an exact solution of the Schrödinger equation
  • It explains atomic spectra quantitatively
  • It reveals hidden symmetries (e.g., Runge–Lenz vector)
  • It serves as the starting point for multi-electron approximations

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See also

Table of contents (217 articles)

Index

Full contents

References


Author: Harold Foppele


Source attribution: Physics:Quantum Hydrogen atom