Orbit track of electron's motion in constant magnetic field studied via | λ〉 representation
We find that in | λ〉 representation, |λ〉= exp − |λ| 2 2 −iλΠ ++λ ∗K ++iΠ +K + |00〉 , the Hamiltonian H=(Π +Π −+ 1 2 )Ω of an electron in uniform magnetic field displays its differential operation form naturally and directly, and the Landau state with definite energy n and angular momentum number m l...
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Published in | Physics letters. A Vol. 267; no. 2; pp. 194 - 200 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
13.03.2000
|
Online Access | Get full text |
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Summary: | We find that in |
λ〉 representation,
|λ〉=
exp
−
|λ|
2
2
−iλΠ
++λ
∗K
++iΠ
+K
+
|00〉
, the Hamiltonian
H=(Π
+Π
−+
1
2
)Ω
of an electron in uniform magnetic field displays its differential operation form naturally and directly, and the Landau state with definite energy
n and angular momentum number
m
l
can be identified as |
n,
n−
m
l
〉 in the Fock space spanned by (
Π
+,
K
+), where
K
+=
MΩ
2
(x
0−iy
0)
, (
x
0,
y
0) is the guiding center. Based on this the orbit track and the variance of (
x
0,
y
0) as well as its squeezing effect are analysed. |
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ISSN: | 0375-9601 1873-2429 |
DOI: | 10.1016/S0375-9601(00)00045-1 |