TJ-II:Heavy Ion Beam Probe

TJ-II disposes of Heavy Ion Beam Probe systems.

HIBP 1

HIBP probe diagram

The advanced Heavy Ion Beam Probe can simultaneously measure the plasma electric potential φ, the electron density n_e, and a poloidal magnetic field component B_p at a point inside the plasma. This point can be scanned through the plasma cross-section by varying the deflection potentials (active beam control). A multiple cell array detector (MCAD) has been developed to investigate the spatial structure of plasma turbulence. The system is located in sector B4.

HIBP probe composite photo (taken around 2002)

HIBP 2

A second, similar system has been installed in sector A4 (see photo). The purpose of this second system is to study plasma potential asymmetries and long range correlations of turbulence.

Installation of the second HIBP probe (March, 2011)

Operation principle

The Heavy Ion Beam Probe (HIBP) is a unique diagnostic for its ability to measure plasma electric potential well inside the plasma column, where no material probes can be inserted. The operating principle is as follows: heavy ions $I^{q}$ with charge $q$ (Cs$^{+}$ in the case of TJ-II) are accelerated to high energies (several hundred keV) and injected as a continuous jet into the plasma column. The interaction with the plasma yields a fan of secondary ions $I^{q'}$ that are more strongly deflected by the magnetic field. Those secondary ions produced in the so-called `sample volume' are collected in an energy analyser. Their energy contains information on the electric potential in the sample volume. Trajectory reconstruction codes allow us to measure the position and reltive potential of the sample volume.

Formal expression of the electric potential φ

Refering to the figure, we will denote as $A$, $B$ and $C$ the injection, ionization and detection points respectively. The Hamiltonian of a charge in an electromagnetic field is

Schematic HIBP operation principle.

${\mathcal {H}}(\mathbf {p} ,\mathbf {x} ,t)={\frac {1}{2m}}(\mathbf {p} -q\mathbf {A} )^{2}+q\phi ={\frac {1}{2}}m\mathbf {v} ^{2}+q\phi =E_{k}+E_{p}$

From the Hamiltonian equations we obtain the ion trajectory $\mathbf {x} (t)$. The ion's energy variation from $A$ to $B$ is given as

$\Delta {\mathcal {H}}(A\rightarrow B)=\int _{t_{A}}^{t_{B}}{\frac {d{\mathcal {H}}}{dt}}dt=\int _{t_{A}}^{t_{B}}{\frac {\partial {\mathcal {H}}}{\partial t}}dt~$

and using the above expression for the Hamiltonian we obtain

${\frac {\partial {\mathcal {H}}}{\partial t}}=q{\frac {\partial \phi }{\partial t}}-q\mathbf {v} \cdot {\frac {\partial \mathbf {A} }{\partial t}}~,$

and thus

$\Delta {\mathcal {H}}(A\rightarrow B)=q\int _{t_{A}}^{t_{B}}{\frac {\partial \phi }{\partial t}}dt-q\int _{t_{A}}^{t_{B}}\mathbf {v} \cdot {\frac {\partial \mathbf {A} }{\partial t}}dt~.$

We use the notation

$\Delta {\mathcal {H}}(A\rightarrow B)=q\Omega _{AB}~.$

In the range of ion energies and plasma temperatures commonly found in magnetic fusion experiments the main ionizing collision is electron impact $I^{+}+e^{-}\to I^{2+}+2e^{-}$. Because of the large mass ratio between the heavy ions and light electrons ($\sim 10^{5}$) we can regard the collision as an ionizing process with no change in the ion momentum and kinetic energy.

The extra positive charge after the ionization gives the ion an energy increment

$\Delta {\mathcal {H}}_{ioniz.}=(q'-q)\phi (B,t_{B})~,$

and therefore the total energy change between $A$ and $B$ is

$\Delta {\mathcal {H}}(A\to B)\equiv {\mathcal {H}}_{B}-{\mathcal {H}}_{A}=q\Omega _{AB}+(q'-q)\phi (B)~.$

Similarly, the energy change between $B$ and $C$ is

$\Delta {\mathcal {H}}(B\to C)\equiv {\mathcal {H}}_{C}-{\mathcal {H}}_{B}=q'\Omega _{BC}~.$

Summing the above energy variations gives

$\phi (B)={\frac {{\mathcal {H}}_{C}-{\mathcal {H}}_{A}-(q\Omega _{AB}+q'\Omega _{BC})}{q'-q}}~.$

In most situations, the energy difference (or the electric potential energy inside the plasma) is much larger than the energy increment caused by the fluctuating electromagnetic fields $q\Omega$ which tends to cancel out along the ion's trajectory. The electric potentials of the injection and detection points are both close to the vacuum vessel potentials so that ${\mathcal {H}}_{C}-{\mathcal {H}}_{A}\approx E_{k,C}-E_{k,A}$. Therefore this simplifies to

$\phi (B)={\frac {E_{k,C}-E_{k,A}}{q'-q}}~.$

Operational expression for the electric potential φ

The energy analyser of the HIBP diagnostic at TJ-II is of the Proca-Green type. The kinetic energy of the secondary ions entering the analyser is given by

$E_{k}=q'\phi _{ana}(F\delta i+G)~,\quad \delta i={\frac {i_{u}-i_{d}}{i_{u}+i_{d}}}~,$

where $\phi _{ana}$ is the deflecting electric potential in the analyser gird, $i_{(u,d)}$ are the currents measured on the up and down plates of the analyser and $F$ and $G$ are adimensional geometric factors depending on construction parameters and on the entrance angle of the ions entering the analyser. The kinetic energy of the ions at the injection point $E_{k,A}$ can be written as their charge times the accelerating potential in the injector, i.e., $E_{k,A}=q\phi _{inj}$

Substituting this and the Proca-green expression for the enery into the formula for the electtric potential and inserting, for the particular case of TJ-II, $q'({\textrm {Cs}}^{2+})=2$ y $q({\textrm {Cs}}^{+})=1$, one gets

$\phi (B)=2\phi _{ana}(F\delta i+G)-\phi _{inj}~.$

In a stellarator it is possible to calibrate the measurement of the plasma electric potential. After the end of the plasma discharge but still during the flat-top of the machine currents the injection of a short pulse of neutral gas provides a zero-potential signal

$0=2\phi _{ana}(F\delta i_{0}+G)-\phi _{inj}~.$

Subtracting the above equations a simplified expression for the electric potential is obtained

$\phi (B)=2\phi _{ana}F(\delta i-\delta i_{0})~.$

The ionization rate of primary ions in a plasma volume is approximately proportional to the local electron density. For the high energy neutral beam and the low density plasmas, as found in the TJ-II device, the attenuation of the secondary beam along its trajectory from the ionization or sample volume to the analyser is negligible. In this situation, the total current on the analyser plates $i=i_{u}+i_{d}$ is approximately proportional to the electron density in the sample volume

$i=i_{u}+i_{d}\propto n_{e}(B)~.$