Spectroscopy in Plasma Physics

Princeton Plasma Physics Laboratory, July 18–20, 2017

(One set-up for up to 2 participants)

Host and Mentor

Photo of Dr. Zwicker

Andrew Zwicker received his B.A. in physics from Bard College and his Ph.D. in physics from Johns Hopkins University. He was a post-doctoral fellow at Oak Ridge National Laboratory and the Princeton Plasma Physics Laboratory where he performed impurity transport measurements on fusion-relevant plasmas both in the U.S. and Europe. He joined PPPL’s Science Education Department in 1998 and is currently the Head where he performs plasma physics experiments on dusty plasmas, plasma speakers and develops new plasma demonstrations for educational use. A Fellow of the American Physical Society, he is also a Lecturer in the Writing Program at Princeton University and mentors undergraduate students on plasma physics experiments.

Andrew Zwicker, Head of Science Education, Princeton Plasma Physics Laboratory, P.O. Box 451, Princeton, NJ 08543. Email: azwicker@pppl.gov.

Plasmas are the most common form of matter in the visible universe but remain one of the least studied topics in the undergraduate physics curriculum. While a fascinating multi-variable system on its own, the study of plasmas also has connections to a significant number of topics in an undergraduate physics curriculum, from classical mechanics to atomic physics.

Photo of PPPL experiments

In this Immersion, participants will first build a DC glow discharge, a simple plasma source that is understandable to undergraduate students yet flexible enough to be used in a variety of experiments (see our recent article in the Sept. 2013 edition of AJP for more details). This type of source is relevant to fluorescent lighting, plasma televisions, and surface treatment of materials. The dc glow discharge is composed of two conductors separated by some distance and electrical potential inside an evacuated vessel at moderately low pressures (between a few and a hundred Pascals). The electrical potential needs to be high enough (hundreds to thousands of Volts) to breakdown the gas into a plasma. The characteristics of the plasma are controlled by four variables: potential difference and distance between the electrodes as well as the type of gas used and its pressure. In our device, we evacuate glass vessels that house stainless steel electrodes. Each has a two-stage direct-drive vacuum pump, an inlet valve system, and a pressure sensor. The vessels can be filled with any gas (including air) through one fine and one coarse valve. These valves also enable fine control of the gas pressure from 3 to 300 Pa. We use power supplies that provide a potential difference of up to 2000 V and 20 mA.

Spectroscopy is one of the standard experiments in atomic physics courses. It is also one of the methods of evaluating plasma parameters such as electron density and temperature. An analysis of dc glow optical emission is readily accessible to undergraduate students. In a dc glow discharge, light is typically emitted by neutral atoms that are excited by electron collisions. If we further assume that electrons collide with atoms in their ground states, then the distribution of the excited levels depends on the electron energy distribution. Experimentally observed line intensities are therefore related to the electron energy, and therefore the observed intensities can be used to estimate the electron temperature of the plasma (under the assumption that the electrons follow a Maxwell-Boltzmann distribution). We use a survey spectrometer for a broad spectrum of argon in a dc glow discharge and a higher resolution instrument with a high enough spectral resolution to distinguish individual lines which are used to infer the electron temperature via a Boltzmann-type plot.

This Immersion will be 3 days long. We will cover building the plasma source, vacuum techniques, calibration of the diagnostics, data acquisition and analysis, as well as all safety aspects of the device. We have several versions of this plasma source, the simplest costs only $2K, the largest approximately $10K which assumes that participants do not have any equipment available for use at their home laboratory. A full parts list will be available so that participants can easily recreate the laboratory setup at their home institution. The survey spectrometer is approximately $3,000 and the high resolution spectrometer is approximately $10,000.

Please note that the Jonathan F. Reichert Foundation has established a grant program (ALPhA webpage; Foundation website) to help purchase apparatus used in Laboratory Immersions. Limitations and exlusions apply, but generally speaking the foundation may support up to 40% of the cost of the required equipment.