100
n
p
n p n
p
n p
b
b
f
f
−
( )= − + ( )
−
( )= − ( )
1
1
´
´
,
,
(5.59)
whereby n(p) ≡ 1/[eβ(p + μ) ∓ 1] is the suitable antiparticle variable mechanism. As
a result, the function A(p || , k) in this function could be expressed as
A p k
n k p n p
p k p
n k p n p
p
,
scalars
b
b
f
f
( ) ≡
−
(
) ( )
−
(
)
−
(
) ( )
´
´
,
2
2
k k p
p
k p
−
(
)
+ −
(
)
2
2
2 ,
.
fermions
(5.60)
The energy E p of a dynamic photon quantum |p| is therefore expressed as
Fig. 5.9 Heating photon energy formation against the internuclear distance (Bohr) at different
variable frequencies where the photon particle carries out the energy measurements (DQD) by
integrating Higgs boson quantum field
5 Integrated Building Design Technology
n
p
n p n
p
n p
b
b
f
f
−
( )= − + ( )
−
( )= − ( )
1
1
´
´
,
,
(5.59)
whereby n(p) ≡ 1/[eβ(p + μ) ∓ 1] is the suitable antiparticle variable mechanism. As
a result, the function A(p || , k) in this function could be expressed as
A p k
n k p n p
p k p
n k p n p
p
,
scalars
b
b
f
f
( ) ≡
−
(
) ( )
−
(
)
−
(
) ( )
´
´
,
2
2
k k p
p
k p
−
(
)
+ −
(
)
2
2
2 ,
.
fermions
(5.60)
The energy E p of a dynamic photon quantum |p| is therefore expressed as
Fig. 5.9 Heating photon energy formation against the internuclear distance (Bohr) at different
variable frequencies where the photon particle carries out the energy measurements (DQD) by
integrating Higgs boson quantum field
5 Integrated Building Design Technology