φ
=
1
+
5
2
\varphi = \frac{1+\sqrt{5}}{2}
φ
=
2
1
+
5
i
ℏ
∂
∂
t
Ψ
=
H
^
Ψ
i\hbar\frac{\partial}{\partial t}\Psi = \hat{H}\Psi
i
ℏ
∂
t
∂
Ψ
=
H
^
Ψ
P
V
=
F
V
(
1
+
r
)
n
PV = \frac{FV}{(1+r)^n}
P
V
=
(
1
+
r
)
n
F
V
A
=
P
(
1
+
r
n
)
n
t
A = P\left(1+\frac{r}{n}\right)^{nt}
A
=
P
(
1
+
n
r
)
n
t
∇
⋅
E
=
ρ
ε
0
\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon_0}
∇
⋅
E
=
ε
0
ρ
Δ
x
Δ
p
≥
ℏ
2
\Delta x \, \Delta p \geq \frac{\hbar}{2}
Δ
x
Δ
p
≥
2
ℏ
O
(
n
log
n
)
O(n \log n)
O
(
n
lo
g
n
)
S
=
E
[
R
p
]
−
R
f
σ
p
S = \frac{E[R_p]-R_f}{\sigma_p}
S
=
σ
p
E
[
R
p
]
−
R
f
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