直流辉光放电与射频辉光放电
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A - B The background ionization stage
During the background ionization stage of the process the electric field applied along the axis of the discharge tube sweeps out the ions and electrons created by ionization from background radiation. Background radiation from cosmic rays, radioactive minerals, or other sources, produces a constant and measurable degree of ionization in air at atmospheric pressure. The ions and electrons migrate to the electrodes in the applied electric field producing a weak electric current. Increasing voltage sweeps out an increasing fraction of these ions and electrons.
直流辉光放电与射频辉光放电
direct current (DC) and radio frequency (RF) glow discharges
By WenQi LU 9/21/2006
1. 气体放电规律
电极间的气体放电
glow-to-arc transition
电源 dc/ac
i
Байду номын сангаас
V
1. Dark Discharge
G – H anormal glow discharge
In the abnormal glow regime above point G, the voltage increases significantly with the increasing total current in order to force the cathode current density above its natural value and provide the desired current.
实验测得的曲线。 注意对应不同 Pd，Vs 有一极小值。
2. Glow Discharge
The glow discharge regime owes its name to the fact that the plasma is luminous. The gas glows because the electron energy and number density are high enough to generate visible light by excitation collisions.
D - E Corona discharges
Corona discharges occur in Townsend dark discharges in regions of high electric field near sharp points, edges, or wires in gases prior to electrical breakdown. If the coronal cuurents are high enough, corona discharges can be technically “glow discharges”, visible to the eye. For low currents, the entire corona is dark, as appropriate for the dark discharges.
E Electrical breakdown（Paschen’s Law）气体的击穿—帕邢定律
击穿电压
Vs
=
BPd ln( APd
)
ln 1
γ
上式称为帕邢定律，表示击穿
电压 Vs 是气压 P 与极间距离 d 乘积 的函数。其中A和B为常数，γ表示一 个正离子撞击阴极表面时平均从阴极 表面逸出的电子数目（二次电子发 射）。
B - C The saturation region
Here radiation induces saturation current change
If the voltage between the electrodes is increased far enough, eventually all the available electrons and ions are swept away, and the current saturates. In the saturation region, the current remain constant while the voltage is increased. This current depends linearly on the radiation source strength, a regime useful in some radiation counters. (e.g. 盖革计数器)
C - D Electron avalanche and the Townsend discharge
If the voltage across the low pressure discharge tube is increased beyond point C, the current will rise exponentially. The electric field is now high enough so the electrons initially present in the gas can acquire enough energy before reaching the anode to ionize a neutral atom. As the electric field becomes even stronger, the secondary electron may also ionize another neutral atom leading to an avalanche of electron and ion production. The region of exponentially increasing current is called the Townsend discharge.
3. Arc Discharges (H – K)
At point H, the electrodes become sufficiently hot that the cathode emits electrons thermoionically. If the DC power supply has a sufficiently low internal resistance, the discharge will undergo a glow-to-arc transition, H-I. The arc regime, from I through K is one where the discharge voltage decreases as the current increases, until large currents are achieved at point J, and after that the voltage increases slowly as the current increases.
电源
i
V
-
+
直流辉光放电区的结构
阳极暗区
电流密度
1. 阴极区
阴极区由Aston暗区，阴极辉区和阴极暗区（或称克罗克斯暗区）三部分组成。 极间电压大部分加在这里，电子被加速与气体原子碰撞，使原子激发或电离。
Aston Dark Space – A thin region to the right of the cathode with a strong electric field. The electrons are accelerated through this space away from the cathode. This region has a negative space charge, meaning that stray initial electrons together with the secondary electrons from the cathode outnumber the ions in this region. The electrons are too low density and/or energy to excite the gas, so it appears dark.
The regime between A and E on the voltage-current characteristic is termed a dark discharge because, except for corona discharges and the breakdown itself, the discharge remains invisible to the eye.
气体放电规律小结
电晕放电，有电子雪崩，自持， 电极附近有微弱发光（电晕）
辉光放电，有电子雪崩， 弧光放电，强电流，
自持，强辉光
低电压，自持
汤生(Townsend)放电， 有电子雪崩，非自持
本底电离， 无电子雪崩，
非自持
2. 直流辉光放电
A general view on the discharge space
H - K Arc Discharges
At point H, the electrodes become sufficiently hot that the cathode emits electrons thermoionically. If the DC power supply has a sufficiently low internal resistance, the discharge will undergo a glow-to-arc transition, H-I. The arc regime, from I through K is one where the discharge voltage decreases as the current increases, until large currents are achieved at point J, and after that the voltage increases slowly as the current increases.
F – G normal glow discharge
After a discontinuous transition from E to F, the gas enters the normal glow region, in which the voltage is almost independent of the current over several orders of magnitude in the discharge current. The electrode current density is independent of the total current in this regime. This means that the plasma is in contact with only a small part of the cathode surface at low currents. As the current is increased from F to G, the fraction of the cathode occupied by the plasma increases, until plasma covers the entire cathode surface at point G.
During the background ionization stage of the process the electric field applied along the axis of the discharge tube sweeps out the ions and electrons created by ionization from background radiation. Background radiation from cosmic rays, radioactive minerals, or other sources, produces a constant and measurable degree of ionization in air at atmospheric pressure. The ions and electrons migrate to the electrodes in the applied electric field producing a weak electric current. Increasing voltage sweeps out an increasing fraction of these ions and electrons.
直流辉光放电与射频辉光放电
direct current (DC) and radio frequency (RF) glow discharges
By WenQi LU 9/21/2006
1. 气体放电规律
电极间的气体放电
glow-to-arc transition
电源 dc/ac
i
Байду номын сангаас
V
1. Dark Discharge
G – H anormal glow discharge
In the abnormal glow regime above point G, the voltage increases significantly with the increasing total current in order to force the cathode current density above its natural value and provide the desired current.
实验测得的曲线。 注意对应不同 Pd，Vs 有一极小值。
2. Glow Discharge
The glow discharge regime owes its name to the fact that the plasma is luminous. The gas glows because the electron energy and number density are high enough to generate visible light by excitation collisions.
D - E Corona discharges
Corona discharges occur in Townsend dark discharges in regions of high electric field near sharp points, edges, or wires in gases prior to electrical breakdown. If the coronal cuurents are high enough, corona discharges can be technically “glow discharges”, visible to the eye. For low currents, the entire corona is dark, as appropriate for the dark discharges.
E Electrical breakdown（Paschen’s Law）气体的击穿—帕邢定律
击穿电压
Vs
=
BPd ln( APd
)
ln 1
γ
上式称为帕邢定律，表示击穿
电压 Vs 是气压 P 与极间距离 d 乘积 的函数。其中A和B为常数，γ表示一 个正离子撞击阴极表面时平均从阴极 表面逸出的电子数目（二次电子发 射）。
B - C The saturation region
Here radiation induces saturation current change
If the voltage between the electrodes is increased far enough, eventually all the available electrons and ions are swept away, and the current saturates. In the saturation region, the current remain constant while the voltage is increased. This current depends linearly on the radiation source strength, a regime useful in some radiation counters. (e.g. 盖革计数器)
C - D Electron avalanche and the Townsend discharge
If the voltage across the low pressure discharge tube is increased beyond point C, the current will rise exponentially. The electric field is now high enough so the electrons initially present in the gas can acquire enough energy before reaching the anode to ionize a neutral atom. As the electric field becomes even stronger, the secondary electron may also ionize another neutral atom leading to an avalanche of electron and ion production. The region of exponentially increasing current is called the Townsend discharge.
3. Arc Discharges (H – K)
At point H, the electrodes become sufficiently hot that the cathode emits electrons thermoionically. If the DC power supply has a sufficiently low internal resistance, the discharge will undergo a glow-to-arc transition, H-I. The arc regime, from I through K is one where the discharge voltage decreases as the current increases, until large currents are achieved at point J, and after that the voltage increases slowly as the current increases.
电源
i
V
-
+
直流辉光放电区的结构
阳极暗区
电流密度
1. 阴极区
阴极区由Aston暗区，阴极辉区和阴极暗区（或称克罗克斯暗区）三部分组成。 极间电压大部分加在这里，电子被加速与气体原子碰撞，使原子激发或电离。
Aston Dark Space – A thin region to the right of the cathode with a strong electric field. The electrons are accelerated through this space away from the cathode. This region has a negative space charge, meaning that stray initial electrons together with the secondary electrons from the cathode outnumber the ions in this region. The electrons are too low density and/or energy to excite the gas, so it appears dark.
The regime between A and E on the voltage-current characteristic is termed a dark discharge because, except for corona discharges and the breakdown itself, the discharge remains invisible to the eye.
气体放电规律小结
电晕放电，有电子雪崩，自持， 电极附近有微弱发光（电晕）
辉光放电，有电子雪崩， 弧光放电，强电流，
自持，强辉光
低电压，自持
汤生(Townsend)放电， 有电子雪崩，非自持
本底电离， 无电子雪崩，
非自持
2. 直流辉光放电
A general view on the discharge space
H - K Arc Discharges
At point H, the electrodes become sufficiently hot that the cathode emits electrons thermoionically. If the DC power supply has a sufficiently low internal resistance, the discharge will undergo a glow-to-arc transition, H-I. The arc regime, from I through K is one where the discharge voltage decreases as the current increases, until large currents are achieved at point J, and after that the voltage increases slowly as the current increases.
F – G normal glow discharge
After a discontinuous transition from E to F, the gas enters the normal glow region, in which the voltage is almost independent of the current over several orders of magnitude in the discharge current. The electrode current density is independent of the total current in this regime. This means that the plasma is in contact with only a small part of the cathode surface at low currents. As the current is increased from F to G, the fraction of the cathode occupied by the plasma increases, until plasma covers the entire cathode surface at point G.