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单词 eigen-state
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eigen-state
Used in adoptions or partial translations of German compounds in Mathematics and Physics, as eigentone n., eigenfunction n.; hence employed as combining form in many scientific compounds, as eigenload, eigen-period, eigen-solution, eigen-state, eigen-vector, eigen-vibration (see quots.).
ΚΠ
1930 P. A. M. Dirac Princ. Quantum Mech. iii. 35 The physical meaning of an eigenvalue is that there exists a state, namely, the eigenstate belonging to it, such that a measurement of the observable when the system is in this state will certainly give for result just this eigenvalue.
1940 Chambers's Techn. Dict. 283/1 Eigenperiod, eigenton, frequencies at which acoustic resonance is experienced in rectangular chambers, because of continued reflections between opposite walls.
1947 Jrnl. Royal Aeronaut. Soc. 51 204 A complete theory of the conditions for the existence, and the form of the self-equilibrating orthogonal and load systems (eigenloads)..which vary similarly along all generators, is given.
1951 Rev. Mod. Physics 1 (title) Approximate eigen-solutions.
1955 Electronic Engin. 27 200 An infinite line of similar quadripoles each with matrix A connected in cascade.. must be a vector such that the effect of operating on it with A is to leave it unaltered except for a change in magnitude... Any vector..fulfilling this condition is called an eigen-vector of the operator matrix H.
1955 W. Pauli in W. Pauli Niels Bohr & Devel. Physics 39 The transformation..can be interpreted as replacing every emission operator by an absorption operator of the same eigen-vibration without interchange of particle and anti~particle.
1955 H. B. G. Casimir in W. Pauli Niels Bohr & Devel. Physics 131 The remarkable feature of Bose–Einstein condensation is that a sizable fraction of the particles is forced into the very lowest eigenstate, a state which should have curious and essentially non-classical properties.
1957 L. Fox Numerical Solution Two-point Boundary Probl. vii. 162 Third, if the vector y is an approximation to any eigenvector yk, so that, in 18, αk is much greater than any other αr, then first-order changes in y give rise to second-order changes in λ, and the eigenvalue is determined more accurately than its eigenvector.
1968 C. G. Kuper Introd. Theory Superconductivity ix. 150 Likewise, bϕn is either zero or an eigenstate with energy En − ℏω.
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