The Schrodinger equation for an m-mass and q-charged particle, interacting with an electromagnetic field, is expressed as follows (−ih▼ — qA(r, t))² + gó(r,t)] v(r,t). (1) 2m According to the tera transformation, the electromagnetic potential and state of that particle at Eq. (1) changed as follows: A(r, t)→ A'(r, t) = A(r, t) - Vg(r, t) ih (r, t) = (2) (3) (r, t) → (r, t) = e-iqg(r.)/(r,t). (4) By working starting from Eq. (1), Show that transformation in Eqs. (2)-(4) gives the Schrodinge A'(r, t), o'(r. t), and (r. t),, whose shape is the same with Eq. (1). ə o(r, t) → o' (r, t) = o(r, t) + (r, t) equation in In other words, the Schrodinger equation is invariant tera.

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The Schrodinger equation for an m-mass and q-charged particle,
interacting with an electromagnetic field, is expressed as follows
ih(r, t)
—ih▼ — qA(r,t))² + qó(r,t)] v(r,t).
(1)
According to the tera transformation, the electromagnetic potential and state of that particle at
Eq. (1) changed as follows:
A(r, t) → A'(r, t) = A(r, t) - Vg(r, t)
Ә
o(r, t) → o'(r, t) = o(r, t) +
at
g(r, t)
(2)
(3)
(r, t) →
(r, t) = e-igg(r.)/(r, t).
By working starting from Eq. (1), Show that transformation in Eqs. (2)-(4) gives the Schrodinger
A'(r, t), o'(r, t), and (r, t),, whose shape is the same with Eq. (1).
equation in
In other words, the Schrodinger equation is invariant tera.
Transcribed Image Text:The Schrodinger equation for an m-mass and q-charged particle, interacting with an electromagnetic field, is expressed as follows ih(r, t) —ih▼ — qA(r,t))² + qó(r,t)] v(r,t). (1) According to the tera transformation, the electromagnetic potential and state of that particle at Eq. (1) changed as follows: A(r, t) → A'(r, t) = A(r, t) - Vg(r, t) Ә o(r, t) → o'(r, t) = o(r, t) + at g(r, t) (2) (3) (r, t) → (r, t) = e-igg(r.)/(r, t). By working starting from Eq. (1), Show that transformation in Eqs. (2)-(4) gives the Schrodinger A'(r, t), o'(r, t), and (r, t),, whose shape is the same with Eq. (1). equation in In other words, the Schrodinger equation is invariant tera.
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