A ball-pen probe is novel technique used to measure directly the plasma potential in strongly as well as weakly magnetized plasmas. The probe was invented by Jiří Adámek in the Institute of Plasma Physics  AS CR in 2004. The ball-pen probe balances the electron saturation current to the same magnitude as that of the ion saturation current. In this case, its floating potential becomes identical to the plasma potential. This goal is attained by a ceramic shield, which screens off an adjustable part of the electron current from the probe collector due to the much smaller gyro–radius of the electrons. First systematic measurements have been performed on the CASTOR tokamak. The probe has been already used at different fusion devices as ASDEX Upgrade, COMPASS, ISTTOK, MAST, TJ-K, RFX , H-1 Heliac, IR-T1  as well as low temperature devices as DC cylindrical magnetron in Prague and linear magnetized plasma devices in Nancy and Ljubljana.
How the ball-pen probe measures the plasma potential
If a Langmuir probe (electrode) is inserted into a plasma, its potential generally lies considerably below the plasma potential due to what is termed a Debye sheath. Thus, the potential of Langmuir probe is named as floating potential . Therefore, it is impossible to measure directly the plasma potential by simple Langmuir probe. The difference between plasma and floating potential is given by the electron temperature [eV]:
and the coefficient . The coefficient is given by the ratio of the electron and ion saturation current density ( and ) and collecting areas for electrons and ions ( and )
The ball-pen probe, in magnetized plasma, modifies the collecting areas for electrons and ions and makes the ratio equal to one. Thus, the coefficient is equal to zero and floating potential of ball-pen probe is equal to the plasma potential independently on electron temperature
The ball-pen probe inserted into the magnetized plasma is directly on the plasma potential without additional power supplies or electronics.
The ball-pen probe design
The design of the ball-pen probe is shown in the schematic picture. The probe consists of a conically shaped collector (non-magnetic stainless steel, tungsten, copper, molybdenum), which is shielded by an insulating tube (boron nitride, Alumina). The collector is fully shielded and the whole probe head must be oriented perpendicularly to the magnetic field lines. It is necessary to find the sufficient retraction of the ball-pen probe collector in order to reach , which strongly depends on the magnetic field's value. The physics of the ball-pen probe are not yet fully understood, but the collector retraction should be roughly below the ion's Larmor radius. This "calibration" can be done in two different ways:
1) the ball-pen probe collector is biased by swept voltage (low frequency) to provide the I-V characteristics and see the saturation current of electrons as well as ions. The ball-pen probe collector is systematically retracted until the I-V characteristics become symmetric. In this case, the ratio is close to one. However, the experimental observation at different fusion devices confirmed that the ratio is close, but not equal, to one. The I-V characteristics remain symmetric for deeper positions of the ball-pen probe collector too.
2) the ball-pen probe collector is fully floating. The ball-pen probe collector is systematically retracted until its potential saturates at some value, which is above Langmuir probe potential. The floating potential of the ball-pen probe remains almost constant for deeper positions too.
The electron temperature measurements without power supply
The electron temperature can be measured by using ball-pen probe and common Langmuir probe with high temporal resolution in magnetized plasma without any external power supply. The electron temperature can be obtain from previous equation, assuming Maxwellian plasma
The value of coefficient is given by the Langmuir probe geometry, plasma gas (Hydrogen, Deuterium, Helium, Argon, Neon,...) and magnetic field. It can be partially effected by other features like secondary electron emission, sheath expansion etc. The coefficient can be calculated theoretically, and its value is around 3 for non-magnetized hydrogen plasma. This value is obtained under assumption that the ion and electron temperatures are equal and there are no other above mentioned effects (sheath expansion, ...). It should be also taken into account that ratio of ball-pen probe is close to one, but not equal to one as it is assumed in previous chapter. Therefore, the difference between ball-pen probe and Langmuir probe potential is given by the electron temperature, coefficient of Langmuir probe and empirical value of the ratio  of ball-pen probe (if there is no empirical value of it can be used an approximation ). Therefore, the electron temperature can be simply measured by using formula
The coefficient for different plasma condition:
|ASDEX Upgrade||1.9 T (on LFS)||Deuterium||2.2|
|H-1 Heliac||< 1 T||Helium||3.76|
|Linear magnetized plasma device, Ljubljana||0.01 T||Argon||5.2|
|DC cylindrical magnetron, Prague||0.02 T - 0.04 T||Argon||5.2|
|Linear device Mirabelle, Nancy||0.08 T||Argon||4.1|
|Linear device Mirabelle, Nancy||0.08 T||Helium||2.9|
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