Person: Wright, Matthew
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Publication Cold and Slow Molecular Beam
(Royal Society of Chemistry, 2011) Lu, Hsin-I; Rasmussen, Julia; Wright, Matthew; Patterson, Dave; Doyle, JohnEmploying a two-stage cryogenic buffer gas cell, we produce a cold, hydrodynamically extracted beam of calcium monohydride molecules with a near effusive velocity distribution. Beam dynamics, thermalization and slowing are studied using laser spectroscopy. The key to this hybrid, effusive-like beam source is a “slowing cell” placed immediately after a hydrodynamic, cryogenic source [Patterson et al., J. Chem. Phys., 2007, 126, 154307]. The resulting CaH beams are created in two regimes. In one regime, a modestly boosted beam has a forward velocity of (v_f = 65 m s^{−1}), a narrow velocity spread, and a flux of 109 molecules per pulse. In the other regime, our slowest beam has a forward velocity of (v_f = 40 m s{−1}), a longitudinal temperature of (3.6 K), and a flux of (5 \times 10^8) molecules per pulse.
Publication A cold and slow molecular beam
(Royal Society of Chemistry (RSC), 2011) Lu, Hsin-I; Rasmussen, Julia Hege; Wright, Matthew; Patterson, Dave; Doyle, JohnEmploying a two-stage cryogenic buffer gas cell, we produce a cold, hydrodynamically extracted beam of calcium monohydride molecules with a near effusive velocity distribution. Beam dynamics, thermalization and slowing are studied using laser spectroscopy. The key to this hybrid, effusive-like beam source is a ‘‘slowing cell’’ placed immediately after a hydrodynamic, cryogenic source [Patterson et al., J. Chem. Phys., 2007, 126, 154307]. The resulting CaH beams are created in two regimes. In one regime, a modestly boosted beam has a forward velocity of vf=65ms-1, a narrow velocity spread, and a flux of 109 molecules per pulse. In the other regime, our slowest beam has a forward velocity of vf=40ms-1, a longitudinal temperature of 3.6 K, and a flux of 5 x 10 8 molecules per pulse.