Markus Schulz-Weiling
University of British Columbia
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Featured researches published by Markus Schulz-Weiling.
Journal of Physics B | 2011
Nicolas Saquet; J. P. Morrison; Markus Schulz-Weiling; Hossein Sadeghi; J. Yiu; C. J. Rennick; Edward R. Grant
Double-resonant photoexcitation of nitric oxide in a molecular beam creates a dense ensemble of
Journal of Physics B | 2016
Markus Schulz-Weiling; Hossein Sadeghi; Jachin Hung; Edward R. Grant
50f(2)
Journal of Physics B | 2014
Jachin Hung; Hossein Sadeghi; Markus Schulz-Weiling; Edward R. Grant
Rydberg states, which evolves to form a plasma of free electrons trapped in the potential well of an NO
Physical Review A | 2017
R. Haenel; Markus Schulz-Weiling; John Sous; Hossein Sadeghi; M. Aghigh; Luke Melo; J. S. Keller; Edward R. Grant
^+
Journal of Physics B | 2016
Markus Schulz-Weiling; Edward R. Grant
spacecharge. The plasma travels at the velocity of the molecular beam, and, on passing through a grounded grid, yields an electron time-of-flight signal that gauges the plasma size and quantity of trapped electrons. This plasma expands at a rate that fits with an electron temperature as low as 5 K, colder that typically observed for atomic ultracold plasmas. The recombination of molecular NO
Physical Chemistry Chemical Physics | 2011
Hossein Sadeghi; Markus Schulz-Weiling; J. P. Morrison; Julian C. H. Yiu; Nicolas Saquet; Christopher J. Rennick; Edward R. Grant
^+
Journal of Physics: Conference Series | 2011
C. J. Rennick; Nicolas Saquet; J. P. Morrison; J Ortega-Arroyo; P Godin; L Fu; Markus Schulz-Weiling; Edward R. Grant
cations with electrons forms neutral molecules excited by more than twice the energy of the NO chemical bond, and the question arises whether neutral fragmentation plays a role in shaping the redistribution of energy and particle density that directs the short-time evolution from Rydberg gas to plasma. To explore this question, we adapt a coupled rate-equations model established for atomic ultracold plasmas to describe the energy-grained avalanche of electron-Rydberg and electron-ion collisions in our system. Adding channels of Rydberg predissociation and two-body, electron- cation dissociative recombination to the atomic formalism, we investigate the kinetics by which this relaxation distributes particle density and energy over Rydberg states, free electrons and neutral fragments. The results of this investigation suggest some mechanisms by which molecular fragmentation channels can affect the state of the plasma.
NON-NEUTRAL PLASMA PHYSICS IX: 11th International Workshop on Non-Neutral Plasmas | 2015
Markus Schulz-Weiling; Edward R. Grant
This paper offers a toolbox for characterizing the initial conditions and predicting the evolution of the ultracold plasma that forms after resonant laser preparation of a Rydberg gas entrained in a differentially pumped supersonic molecular beam. The conditions afforded by a skimmed free-jet expansion combined with the geometry of laser excitation, determines the phase-space volume of the excited gas. A hydrodynamic shell model, that accounts for the ellipsoidal spatial distribution of this excitation volume in concert with the deforming effects of dissociative recombination, serves to simulate the ambipolar expansion of this molecular ultracold plasma.
Physical Review Letters | 2014
Hossein Sadeghi; A. Kruyen; Jachin Hung; J. H. Gurian; J. P. Morrison; Markus Schulz-Weiling; Nicolas Saquet; C. J. Rennick; Edward R. Grant
A Rydberg gas of xenon, entrained in a supersonic atomic beam, evolves slowly to form an ultracold plasma. In the early stages of this evolution, when the free-electron density is low, Rydberg atoms undergo long-range -mixing collisions, yielding states of high orbital angular momentum. The development of high- states promotes dipole–dipole interactions that help to drive Penning ionization. The electron density increases until it reaches the threshold for avalanche. Ninety μs after the production of a Rydberg gas with the initial state, , a 432 V cm−1 electrostatic pulse fails to separate charge in the excited volume, an effect which is ascribed to screening by free electrons. Photoexcitation cross sections, observed rates of -mixing, and a coupled-rate-equation model simulating the onset of the electron-impact avalanche point consistently to an initial Rydberg gas density of .
Bulletin of the American Physical Society | 2013
Markus Schulz-Weiling; Hossein Sadeghi; Jachin Hung; Edward R. Grant
Spontaneous avalanche to plasma splits the core of an ellipsoidal Rydberg gas of nitric oxide. Ambipolar expansion first quenches the electron temperature of this core plasma. Then, long-range, resonant charge transfer from ballistic ions to frozen Rydberg molecules in the wings of the ellipsoid quenches the centre-of-mass ion/Rydberg molecule velocity distribution. This sequence of steps gives rise to a remarkable mechanics of self-assembly, in which the kinetic energy of initially formed hot electrons and ions drives an observed separation of plasma volumes. These dynamics adiabatically sequester energy in a reservoir of mass transport, starting a process that anneals separating volumes to form an apparent glass of strongly coupled ions and electrons. Short-time electron spectroscopy provides experimental evidence for complete ionization. The long lifetime of this system, particularly its stability with respect to recombination and neutral dissociation, suggests that this transformation affords a robust state of arrested relaxation, far from thermal equilibrium.