B. M. Patterson
United States Air Force Academy
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Featured researches published by B. M. Patterson.
Optics Letters | 2010
J. F. Sell; M. A. Gearba; B. M. Patterson; T. Genda; B. Naumann; R. J. Knize
Using ultrafast laser excitation and time-correlated single-photon counting techniques, we have measured the collisional mixing rates between the rubidium 5(2)P fine-structure levels in the presence of (4)He gas. A nonlinear dependence of the mixing rate with (4)He density is observed. We find Rb fine-structure transfer is primarily due to binary collisions at (4)He densities of < or = 10(19) cm(-3), while at greater densities, three-body collisions become significant. We determine a three-body collisional transfer rate coefficient (5(2)P(3/2) --> 5(2)P(1/2)) of 1.25(9)x10(-32) cm(6)/s at 22 degrees C.
Optics Letters | 2012
M. A. Gearba; J. F. Sell; B. M. Patterson; R. Lloyd; J. Plyler; R. J. Knize
Employing ultrafast laser excitation and time-correlated single-photon counting, we have measured the fine-structure transfer between Rb 5P states induced by collisions with 4He buffer gas at temperatures up to 150 °C. The temperature dependence of the binary cross section agrees with earlier measurements. Our data show that the temperature dependence of the three-body rate is about the same as that of the binary rate. The three-body rate can be described as arising from the reduction of the rubidium fine-structure splitting due to nearby helium atoms.
Optics Letters | 2003
B. M. Patterson; C. D. Lindstrom; T. Takekoshi; J. R. Lowell; C. Villarreal; R. J. Knize
We present a new technique for measuring atomic lifetimes with a mode-locked laser. A single laser pulse excites the atoms and a subsequent frequency-doubled pulse ionizes the excited-state atoms. The ions are collected and counted. The measurement is repeated using excitation and detection pulses with different time separations, which determines the excited-state decay rate. We demonstrated this technique for the 6P(3/2) state of cesium. The measured lifetime was 30.5 ns and had a statistical uncertainty of 0.1 ns. Systematic effects limited the overall experimental uncertainty to approximately 0.6 ns in this initial experiment.
Physical Review A | 1999
T. Takekoshi; B. M. Patterson; R. J. Knize
Physical Review A | 1999
B. M. Patterson; T. Takekoshi; R. J. Knize
Physical Review A | 2002
J. R. Lowell; T. Northup; B. M. Patterson; T. Takekoshi; R. J. Knize
Physical Review A | 2002
J. R. Lowell; T. Northup; B. M. Patterson; T. Takekoshi; R. J. Knize
Physical Review A | 2011
Jerry Sell; B. M. Patterson; Thomas Ehrenreich; George M. Brooke; James Scoville; R. J. Knize
Physical Review A | 2004
T. Takekoshi; George M. Brooke; B. M. Patterson; R. J. Knize
Archive | 2002
B. M. Patterson; Chadwick D. Lindstrom; T. Takekoshi; J. R. Lowell; Randall James Knize