More information on this experiment. |
What are Metastable States?
Atoms can be excited (by lasers, electron collisions, etc.) to energy
levels above their ground states. Normally, these levels are short-lived and
the atoms quickly decay (in 10-7 sec or less) back to the ground state. When
the atom is excited into a level which is not allowed to quickly decay
(i.e., it survives 10-6 sec or longer) it is said to exist in a metastable
level. These metastable atoms contain a lot of energy and are very important in
real-world applications such as gas-discharge lasers and plasma processing of
semiconductors. In our lab we measure cross sections for electron-impact excitation out of the
metastable levels into higher excited levels.
How are Metastable Atoms created?
The study of electron-metastable atom collisions is complicated by
the difficulty of producing targets of metastable atoms in the lab. This
experiment uses a hollow cathode discharge to produce an atomic beam of
metastable atoms. The beam emerging from the hollow cathode discharge has a
metastable atom density of approximately 107 atoms/cm3.
How do we measure the signal?
In this experiment, a low-energy electron beam crosses the atomic
beam at a right angle. The metastables are excited into higher levels, and
when these levels decay, they emit visible radiation. This emitted radiation
is measured using a photomultiplier tube and from this information we can
extract cross sections.
Absolute calibration of cross sections:
We get to use really neat lasers (Ar+ and Ti:Sapphire,
along with some frequency doubling) to obtain absolute values for our
cross sections. We use a laser-induced fluorescence(LIF) technique, which
involves taking the ratio of our electron-excitation signal to a
laser-excitation signal.
Some experimental specs:
Target Density: |
107 to 108 metastables/cm3 |
Energy Range: |
0eV to ground state onset |
Electron Beam current: |
10 µA at 10 eV |
Atoms studied: |
He(21S) and He(23S) metastables (excitation into more than 25 higher levels studied)
Ar( 1s3 ) and Ar( 1s5 ) metastables (excitation into 8 higher levels studied)
Ne( 1s3 ) and Ne( 1s5 ) metastables (excitation into 10 higher levels studied)
Kr( 1s3 ) and Kr( 1s5 ) metastables (excitation into 7 higher levels studied) |
Recent Published Results
- Measurement of electron-impact excitation cross sections out of the neon 3P2 metastable level
-
John B. Boffard, M. L. Keeler, Garrett A. Piech, L. W. Anderson, and Chun C. Lin,
Phys Rev. A 64 (2001) 032708.
- Measurement of Cross Sections for Electron Excitation out of the Metastable Levels of Argon
-
Garrett A. Piech, John B. Boffard, Mark F. Gehrke, L. W. Anderson, and Chun C. Lin,
Phys Rev. Lett. 81 (1998) 309-312.
- Electron excitation out of the 23S metastable level of helium into high-n triplet levels
-
Garrett A Piech, J Ethan Chilton, L W Anderson, and Chun C Lin,
J. Phys. B: At. Mol. Opt. Phys. 31 (1998) 859-872.
- Cross sections for electron excitation of the 23S metastable level of He into higher triplet levels
-
Garrett A. Piech, Mark E. Lagus, L. W. Anderson, Chun C. Lin, and M. R. Flannery,
Physical Review A 55 (1997) 2842-2856.
- A method for measuring cross sections for electron-impact excitation out of metastable levels of atoms
-
Ronald B. Lockwood, L. W. Anderson, and Chun C. Lin,
Z. Phys. D- Atoms, Molecules and Clusters 24 (1992) 155-160.
- Cross sections for electron excitation out of the metastable levels of helium into the higher singlet levels
-
Ronald B. Lockwood, Francis A. Sharpton, L. W. Anderson, and Chun C. Lin,
Physics Letters A 166 (1992) 357-360.
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