query: Independents fields and the Lagrange Density of Schrodinger equation
positive_passages.docid: 29505
positive_passages.text: Why treat complex scalar field and its complex conjugate as two different fields?
negative_passages.docid: 30152
negative_passages.text: Derivation of time-dependent Schrödinger equation from De Broglie hypothesis
negative_passages.docid: 121574
negative_passages.text: Schrödinger equation derivation and Diffusion equation
negative_passages.docid: 108242
negative_passages.text: Quantum mechanics scattering theory
negative_passages.docid: 87951
negative_passages.text: Normalizable wavefunction that does not vanish at infinity
negative_passages.docid: 159017
negative_passages.text: Bohr-Sommerfeld quantization condition from the WKB approximation
negative_passages.docid: 32209
negative_passages.text: Labeling solutions of an Eigenvalue equation involving Bessel functions
negative_passages.docid: 8450
negative_passages.text: Classical field limit of the electron quantum field
negative_passages.docid: 150081
negative_passages.text: Deriving Lagrangian density for electromagnetic field
negative_passages.docid: 157191
negative_passages.text: Conjugate Variables, Noether's Theorem and QM
negative_passages.docid: 29329
negative_passages.text: Does a four-divergence extra term in a Lagrangian density matter to the field equations?
negative_passages.docid: 79094
negative_passages.text: Perturbation expansion with path integrals
negative_passages.docid: 69481
negative_passages.text: Classical limit of the path integral formulation of quantum mechanics
negative_passages.docid: 7555
negative_passages.text: Why do we consider Lagrangian densities in field theory (as opposed to Lagrangians as in point mechanics)?
negative_passages.docid: 45559
negative_passages.text: Why we use $L_2$ Space In QM?
negative_passages.docid: 114317
negative_passages.text: Cauchy-Schwarz inequality in Shankhar's Quantum Mechanics
negative_passages.docid: 76845
negative_passages.text: Cauchy's Theorem on Path Integrals