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Quantum number

physical science Maturity 9-11 Next article →

Quantum numbers are quantities used to characterize the possible states of a physical system. In the field of quantum physics and chemistry, they act as a mathematical way to describe the properties of particles. For example, to fully specify the state of an electron in a hydrogen atom, scientists use four specific quantum numbers. These numbers help us understand how particles like electrons behave in space and how they hold energy. Without these values, we could not predict the complex properties of atoms or how they bond together.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates

To understand how these numbers work, we must look at the mechanics of the atom. A system is described by a quantum operator called a Hamiltonian, which represents the system's energy. A quantum number corresponds to an eigenvalue, which is a specific value associated with an observable property. When an observable commutes with the Hamiltonian, the quantum number is called "good." A "good" quantum number acts as a constant of motion during quantum dynamics. This means the value remains precise and predictable even as the system changes over time.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates

In a hydrogen-like atom, there are four distinct types of quantum numbers. The first is the principal quantum number, denoted as $n$. This number describes the electron shell and its energy level. As $n$ increases, the average distance between the electron and the nucleus also increases. The second is the azimuthal quantum number, or $l$, which describes the subshell. This value determines the magnitude of the orbital angular momentum and the shape of the orbital, such as s, p, d, or f shapes. The third is the magnetic quantum number, $m_l$, which identifies the specific orbital within a subshell. It describes how the orbital is oriented along a specific axis. Finally, the spin magnetic quantum number, $m_s$, describes the electron's intrinsic spin. This can result in two states: "spin up" or "spin down."

The history of these numbers is a journey through many decades of discovery. In 1900, Max Planck proposed the concept of quanta to explain blackbody radiation. By 1913, Niels Bohr created an atomic model that relied on a single quantum number. In 1915, Arnold Sommerfeld improved this by adding a second quantum number and using three-dimensional space quantization. Later, researchers like Karl Schwarzschild and Paul Epstein showed that a third number could explain the Stark effect. In 1925, Wolfgang Pauli introduced a new quantum number to solve the mystery of the Zeeman effect. This discovery proved that electrons have an intrinsic spin that is not related to their orbital motion.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates

These numbers carry immense significance for the structure of matter. For instance, in a caesium atom, the outermost valence electron is in the sixth shell. This means its principal quantum number can range from 1 to 6. The azimuthal quantum number $l$ can range from 0 to $n-1$. This mathematical relationship dictates the available shapes for electrons, such as the p orbital appearing in the second shell. Furthermore, the Pauli exclusion principle states that every electron state must have unique quantum numbers. Because of this rule, every single orbital can hold at most two electrons.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates

There are many surprising details regarding how these numbers function in different environments. In some systems, like spin-orbit coupled systems, the standard $l$ and $s$ operators no longer commute with the Hamiltonian. In these cases, scientists must use a different set of numbers, including the total angular momentum quantum number, $j$. These systems also involve parity, which is the eigenvalue under reflection. An orbital can have even parity, or a positive value, or odd parity, with a negative value. Additionally, while atoms use four numbers, subatomic particles like quarks require new numbers, such as "flavour," which have no classical equivalent.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates

Quantum numbers connect to much broader scientific ideas, including the concept of symmetry. As quantum mechanics grew, scientists used group theory to connect conserved quantum numbers to symmetries in field theory. In the 1950s, Chen Ning Yang and Robert Mills developed a non-abelian gauge theory based on the conservation of nuclear isospin. This showed how quantum numbers are deeply tied to the fundamental laws of the universe. Whether describing the nucleus or the electron, these numbers provide the essential framework for modern physics. They allow us to move from simple models to a complete understanding of the subatomic world.

Atomic orbitals n123 m-eigenstates
Atomic orbitals n123 m-eigenstates
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