← All parts of this equation

Equation 1 · Part 4 · No Particle Without a Cosigner

Symbol a_k

a~j=∑k(αjkak+βjkak†).\tilde a_j = \sum_k \left( \alpha_{jk} a_k + \beta_{jk} a_k^\dagger \right).
aka_k

What this part means

aka_k is one of the signed contributions combined to compute the quantity on the left.

Its job in the formula

aka_k is one of the signed contributions combined to compute the quantity on the left.

The passage around this formula

The precise, non-negotiable content of the ambiguity is the Bogoliubov transformation. Given two ways of splitting a free field into positive- and negative-frequency modes — two choices of “particle,” in the ordinary sense of excitations above a chosen vacuum — the annihilation operators of one decomposition mix the creation and annihilation operators of the other: a~j=∑k(αjkak+βjkak†)\tilde a_j = \sum_k \left( \alpha_{jk} a_k + \beta_{jk} a_k^\dagger \right). When any of the coefficients βjk\beta_{jk} is nonzero, the vacuum of the a -decomposition is a many-particle state of the a~\tilde a -decomposition, and vice versa: “how many particles are present” is a question whose answer depends on which set of modes was declared fundamental, not on the field configuration by…

Read this part in the article →

Learn the underlying idea

A subscript is a label attached below a symbol. It often selects a time step, component, category, or member of a sequence.

Open the illustrated subscripts: which member of a family? guide →

See this notation across published equations →

Sources cited in the surrounding passage

These citations provide research context; check each source for the exact claim it supports.