88
L
v
F F
v
qA
heat = ∂
( ) − ∗ −
+ ∗
+∂
(
)
1
2
2
1
4
2
2
2
2
2
2
µ
µ ν
µν
µ
µ
σ
λ
σ
Θ
(5.20)
Evidently, to start high heating in the quantum field of the curtain wall, the free
particles (with Lagrangian L free ) should be real scalar particles with affirmative
m
2
= λv
2
(in which m represents the particle mass; check Fig. 5.4).
Fig. 5.4 (a) The consideration of heating photon (GHz-fs2) energy regarding wavelength (ym).
(b) A photon’s transformation mechanism at the level of energy from the electrons’ quantum intensity spectra. The photon absorbance is demonstrated taking wavelength into consideration
5 Integrated Building Design Technology
L
v
F F
v
qA
heat = ∂
( ) − ∗ −
+ ∗
+∂
(
)
1
2
2
1
4
2
2
2
2
2
2
µ
µ ν
µν
µ
µ
σ
λ
σ
Θ
(5.20)
Evidently, to start high heating in the quantum field of the curtain wall, the free
particles (with Lagrangian L free ) should be real scalar particles with affirmative
m
2
= λv
2
(in which m represents the particle mass; check Fig. 5.4).
Fig. 5.4 (a) The consideration of heating photon (GHz-fs2) energy regarding wavelength (ym).
(b) A photon’s transformation mechanism at the level of energy from the electrons’ quantum intensity spectra. The photon absorbance is demonstrated taking wavelength into consideration
5 Integrated Building Design Technology