TY - JOUR
T1 - Evaluation of the mean excitation energies of gaseous and liquid argon
AU - Strait, M.
N1 - Publisher Copyright:
© 2024 The Author(s)
PY - 2024/1/1
Y1 - 2024/1/1
N2 - Current and future experiments need to know the stopping power of liquid argon. It is used directly in calibration, where commonly the minimum-ionizing portion of muon tracks is used as a standard candle. Similarly, muon range is used as a measure of muon energy. More broadly, the stopping power figures into the simulation of all charged particles, and so uncertainty propagates widely throughout data analysis of all sorts. The main parameter that controls stopping power is the mean excitation energy, or I-value. Direct experimental information for argon's I-value come primarily from measurements of gaseous argon, with a very limited amount of information from solid argon, and none from liquid argon. A powerful source of indirect information is also available from oscillator strength distribution calculations. We perform a new calculation and find that from oscillator strength information alone, the I-value of gaseous argon is (187 ± 5) eV. In combination with the direct measurements and other calculations, we recommend (187 ± 4) eV for gaseous argon. For liquid argon, we evaluate the difference in central value and uncertainty incurred by the difference of phase and recommend (197 ± 7) eV. All uncertainties are given to 68% C.L.
AB - Current and future experiments need to know the stopping power of liquid argon. It is used directly in calibration, where commonly the minimum-ionizing portion of muon tracks is used as a standard candle. Similarly, muon range is used as a measure of muon energy. More broadly, the stopping power figures into the simulation of all charged particles, and so uncertainty propagates widely throughout data analysis of all sorts. The main parameter that controls stopping power is the mean excitation energy, or I-value. Direct experimental information for argon's I-value come primarily from measurements of gaseous argon, with a very limited amount of information from solid argon, and none from liquid argon. A powerful source of indirect information is also available from oscillator strength distribution calculations. We perform a new calculation and find that from oscillator strength information alone, the I-value of gaseous argon is (187 ± 5) eV. In combination with the direct measurements and other calculations, we recommend (187 ± 4) eV for gaseous argon. For liquid argon, we evaluate the difference in central value and uncertainty incurred by the difference of phase and recommend (197 ± 7) eV. All uncertainties are given to 68% C.L.
KW - Interaction of radiation with matter
KW - Neutrino detectors
UR - http://www.scopus.com/inward/record.url?scp=85182517642&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85182517642&partnerID=8YFLogxK
U2 - 10.1088/1748-0221/19/01/P01009
DO - 10.1088/1748-0221/19/01/P01009
M3 - Article
AN - SCOPUS:85182517642
SN - 1748-0221
VL - 19
JO - Journal of Instrumentation
JF - Journal of Instrumentation
IS - 1
M1 - P01009
ER -