31
v t t
d
,
e
o f
f
³
Z
Z Z
with
V
D
D
Z
Z
Z
Z
ª ¬
º ¼
n T
,
l
d
(2.33)
Here, Eq. (2.18) is simplified to determine the nonequilibrium condition
V
D
Z
Z
Z
n T
,
d
. Under low-temperature conditions on earth surface,
Einstein’s photon energy fluctuation dissipation not only is dynamically viable at the
PB on earth surface, but also connects the photonic energy state which has been measured as the field intensity of solar energy induction n(t) = 〈a
†
(t)a(t)〉 = |u(t, t 0 )|
2
n(t 0 )v(t, t),
where n(t 0 ) represents the primary PB of earth surface. Therefore, in Fig. 2.6, the
plotted net amount of photon energy s versus temperature on earth surface has been
clarified as the nonequilibrium proliferated photon energy generation, as shown by
the solid-blue curve (Fig. 2.6). To be more specific, the first PB of earth surface has
been considered as the Fock state photon number n 0 ,i.e., ρ(t 0 ) = |n 0 ⟩⟨n 0 |, which is
obtained mathematically through the quantum dynamics of the photon energy and
then by solving Eq. (2.36), with respect to the state of net photon energy production
at time t:
U t
t n n
n
n
n
f
¦
0
0 0
0
(2.34)
n
n
n
n
n
k
n
t
v t t
v t t
0
0
0
1
1
1
0
ª ¬
º ¼
ª ¬
º ¼
ª ¬
º ¼ u
,
,
t
,
:
min
n n
k
n
k
n
k v t t
^ `
¦
§
©
¨
·
¹
¸
§
©
¨
·
¹
¸
ª
¬
«
«
º
¼
»
»
0
1
1
,
t
t
:
:
(2.35)
where
: t
,
,
u t t
v t t
0
2
1
. Therefore, the result reveales that an electron-state photon
energy will evolve into different Fock states of | n 0 ⟩ is n
n
t
0
on the earth surface.
The proliferation of net photon energy dissipation n
n
t
0
in the primary state
∣n 0 = 5⟩ and steady-state limit, n
n
t
0
o f
, is thus shown in Fig. 2.7. Therefore,
the generation of net photon energy on earth surface will ultimately reach the thermal nonequilibrium state which is expressed as
n
n
n
n
t
n
T
n
T
0
1
1
o f
ª ¬
º ¼
ª ¬
º ¼
Z
Z
c
c
,
,
(2.36)
To probe this huge photon energy generation on earth surface, a further calculation of the photon energy distribution within the quantum field of earth surface has
Results and Discussion
v t t
d
,
e
o f
f
³
Z
Z Z
with
V
D
D
Z
Z
Z
Z
ª ¬
º ¼
n T
,
l
d
(2.33)
Here, Eq. (2.18) is simplified to determine the nonequilibrium condition
V
D
Z
Z
Z
n T
,
d
. Under low-temperature conditions on earth surface,
Einstein’s photon energy fluctuation dissipation not only is dynamically viable at the
PB on earth surface, but also connects the photonic energy state which has been measured as the field intensity of solar energy induction n(t) = 〈a
†
(t)a(t)〉 = |u(t, t 0 )|
2
n(t 0 )v(t, t),
where n(t 0 ) represents the primary PB of earth surface. Therefore, in Fig. 2.6, the
plotted net amount of photon energy s versus temperature on earth surface has been
clarified as the nonequilibrium proliferated photon energy generation, as shown by
the solid-blue curve (Fig. 2.6). To be more specific, the first PB of earth surface has
been considered as the Fock state photon number n 0 ,i.e., ρ(t 0 ) = |n 0 ⟩⟨n 0 |, which is
obtained mathematically through the quantum dynamics of the photon energy and
then by solving Eq. (2.36), with respect to the state of net photon energy production
at time t:
U t
t n n
n
n
n
f
¦
0
0 0
0
(2.34)
n
n
n
n
n
k
n
t
v t t
v t t
0
0
0
1
1
1
0
ª ¬
º ¼
ª ¬
º ¼
ª ¬
º ¼ u
,
,
t
,
:
min
n n
k
n
k
n
k v t t
^ `
¦
§
©
¨
·
¹
¸
§
©
¨
·
¹
¸
ª
¬
«
«
º
¼
»
»
0
1
1
,
t
t
:
:
(2.35)
where
: t
,
,
u t t
v t t
0
2
1
. Therefore, the result reveales that an electron-state photon
energy will evolve into different Fock states of | n 0 ⟩ is n
n
t
0
on the earth surface.
The proliferation of net photon energy dissipation n
n
t
0
in the primary state
∣n 0 = 5⟩ and steady-state limit, n
n
t
0
o f
, is thus shown in Fig. 2.7. Therefore,
the generation of net photon energy on earth surface will ultimately reach the thermal nonequilibrium state which is expressed as
n
n
n
n
t
n
T
n
T
0
1
1
o f
ª ¬
º ¼
ª ¬
º ¼
Z
Z
c
c
,
,
(2.36)
To probe this huge photon energy generation on earth surface, a further calculation of the photon energy distribution within the quantum field of earth surface has
Results and Discussion