增刊
冯劲松：运动光子与原子核外运动电子的相互精确定量调控机理
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表1 氢原子发射光谱——实测的巴尔末线系（可见光波段）的光子调控机理
Tab.1 Actual survey of hydrogen atomic emission spectrum-photon principle adjusting control in the
wavelength of BALMER lines(wave band of light wave) from actual survey
n
λx
Rx
/×107m
ν
r
N
N0
Photons
10
N-N0
×%
0
ξ
-1
-1
/nm
/km·s
/×10-12
m
Photons
10
/nm
3
4
5
656.21
486.074
434.010
1.097 209 735
1.097 226 622
1.097 187 798
5 173.974 0
4 899.416 4
5 510.239 3
9.464
10.554
8.344
6 561.122
6 318.118
6 509.050
13.5
13
3.8
15.119
15
0.79
6
7
8
410.120
386.059
364.581
1.097 239 832
1.097 163 515
1.097 259 605
4 673.408 7
5 860.410 0
4 313.033 0
11.600
7.377
16.000 4
17
16
17
18
0.002 5
0
6 561.122
6 561.748
6561.778
13.620
17.999
0.005
Note：n = natural number;λx = wavelength from actual survey; Rx = Rydberg constant from actual survey; ν= instantaneous velocity of electrons’ motion; r = orbit
radius of electrons’ motion;N = number of photons from actual survey; N0= number of photons from theoretical inference
2.2 氢原子发射光谱的实测——帕邢线系（红外线
波段）的光子调控机理
长[9]，实测波长对应的实测里德伯常数、电子运动瞬
时速度、电子运动轨道半径、实测波长一份光量子内
所含的光子数、以及所对应的常数ξ，结果见表2。
氢原子发射光谱的实测——帕邢线系的实测波
表2 氢原子发射光谱实测—帕邢线系（红外线波段）的光子调控机理
Tab.2 Actual survey of hydrogen atomic emission spectrum-photon principle adjusting
control in the wavelength of paschen series (IR wave band)
n
λx
Rx
/×107m
ν
r
N
N0
Photons
3(4)
5
N-N0
ξ
-1
-1
/nm
/km·s
/×10-12
m
Photons
3.500 5
5.120 7
6.000 8
6.531 5
6.876 0
×%
/nm
4
5
6
7
8
1 875.11
1 281.81
1 093.80
1 004.98
954.62
1.097 078 495
1.097 081 471
1.097 092 704
1.097 036 757
1.097 057 082
6 947.142 0
6 911.978 0
6 777.605 8
7 422.772 4
7 193.949 2
5.258 185 7
5.311 837 2
5.524 605 6
4.605 740 4
4.903 487 8
16.8
2.4
7 498.425
6 407.346
6 561.122
6 028.031
7 032.703
6
0.013
8.8(7.5)
1.8
6(7)
7
2.3 氢原子发射光谱的实测——赖曼线系（远紫外
线波段）的光子调控机理
实测波长对应的实测里德伯常数、电子运动瞬时速
度、电子运动轨道半径、实测波长一份光量子内所含
氢原子发射光谱实测—赖曼线系的实测波长[9]， 的光子数、以及所对应的常数ξ，结果见表3。
表3 氢原子发射光谱实测——赖曼线系的（远紫外线波段）的光子调控机理
Tab.3 Actual survey of hydrogen atomic emission spectrum-photon principle adjusting
control in the wavelength of lyman series (wave band of far ultra-violet rays)
n
λx
Rx
/×107m
ν
r
N
N0
Photons
54
N-N0
ξ
-1
-1
/nm
/km·s
/×10-12
m
Photons
54.008 0
64.009 5
67.510 0
69.130 3
70.010 4
×%
/nm
2
3
4
5
6
121.566
102.583
97.254
94.976
93.782
1.096 797 899
1.096 672 938
1.096 784 365
1.096 768 306
1.096 768 493
9 706.004 4
10 708.099 2
9 819.482 3
9 952.451 2
9 950.913 1
2.693 123 1
2.212 396 3
2.631 204 7
2.561 328 8
2.562 121 2
0.015
0.015
0.76
0.19
0.15
6 561.122
6 561.122
6 512.521
6 549.731
6 561.122
64
67(68)
69
70