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- In the theory of [[linear operator]]s, for some operator \(f\), the [[eigenfunction]] with eigenvalue4 KB (574 words) - 18:26, 30 July 2019
- '''Fourier transform''' is linear integral transform with the exponential [[kernel]]. The Fourier operator is [[linear operator|linear]]: for complex constants \(\alpha\) and \(\beta\),11 KB (1,501 words) - 18:44, 30 July 2019
- ...bservable [[physical quantities]] as [[Hermitian operator]]s acting on the linear space of [[vector of state|vectors of state]]. ...m]] is characterized with an element \(\psi\) of the [[linear space]]; any linear combinaiton of the states of a physical system is also interpreted as the s7 KB (1,006 words) - 18:26, 30 July 2019
- </ref>. In order to avoid numbers in the names of operators, they are called using the Roman numeral system: [[DCTIV]]. All these operators are discrete analogies of the intergal [[CosFourier]] operator, and all use10 KB (1,689 words) - 18:26, 30 July 2019
- J. S. Levinger. The linear no-threshold theory: Readers weigh in. Physics Today, July 2016, page 10. http://www.guardian.co.uk/environment/blog/2013/mar/11/nuclear-reactor-operators-financially-liable-disasters125 KB (3,105 words) - 08:04, 26 December 2019
- ...m; the Hamiltonian is [[Hermitian operator]] acting on the elements of the linear space mentioned in the Axiom Q1; in one of representations, the evolution o Q3. The measurable quantities of classical mechanics correspond to the linear [[Hemitian operator]]s acting on the space of the states; the Hamiltonian6 KB (913 words) - 16:02, 26 July 2019
- the linear combination Linear operations on the space of wave functions are called "operators".4 KB (618 words) - 18:44, 30 July 2019