Stefan Schlamp
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Stefan Schlamp has a total of 31 co-authors. Here are the top co-authors by number of shared publications:
Thomas Rösgen
ETH Zurich
4 shared publicationsEric B. Cummings
S. Schlampand H. G. Hornungare with the Aeronautical Laboratory, California Institute of Technology, Pasadena, California 91125.T. H. Sobotais with Advanced Projects Research, Incorporated, 1925 McKinley Avenue, La Verne, California 91750.E. B. Cummingsis with Sandia National Laboratories, Livermore, California 94551
3 shared publicationsT. Rösgen
3 shared publications- Andreas Kempe
Institute of Fluid Dynamics, ETH Zürich, Zürich, Switzerland
2 shared publications Bryan C. Hathorn
Oak Ridge National Laboratories, Division of Computer Science and Mathematics, Oak Ridge, TN 37831, USA
2 shared publicationsD. Günther
2 shared publications
Latest Publications
- Open Access
- 21 July 2026
- Published by Elsevier in SSRN Electronic Journal
Racing the News: Nanosecond Market Efficiency at Eurex and CME
We propose a Hybrid Piecewise Intensity model linking point-process econometrics to the physical architecture of electronic exchanges, decomposing trade arrivals in the 100 ms around macroeconomic announcements into four latency-aligned phases. Calibrated on nanosecond Eurex and CME data (2019--2025), modal Phase~1 peaks occur at 1.16 μs (Eurex) and 6.64 μs (CME), tracking each venue's network transmission floor. Comparing private embargo-based (PMI) and government-led (NFP, FOMC) releases, we find reaction-speed differences consistent with protocol-induced latency advantages, though confounds remain. The CME concentrates profitability within 200 μs with deteriorating risk-adjusted returns thereafter; Eurex sustains stable Sharpe ratios across longer horizons.
- 21 July 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessRacing the News: Nanosecond Market Efficiency at Eurex and CME
We propose a Hybrid Piecewise Intensity model linking point-process econometrics to the physical architecture of electronic exchanges, decomposing trade arrivals in the 100 ms around macroeconomic announcements into four latency-aligned phases. Calibrated on nanosecond Eurex and CME data (2019--2025), modal Phase~1 peaks occur at 1.16 μs (Eurex) and 6.64 μs (CME), tracking each venue's network transmission floor. Comparing private embargo-based (PMI) and government-led (NFP, FOMC) releases, we find reaction-speed differences consistent with protocol-induced latency advantages, though confounds remain. The CME concentrates profitability within 200 μs with deteriorating risk-adjusted returns thereafter; Eurex sustains stable Sharpe ratios across longer horizons.
- 1 January 2009
- Published by Springer Nature
- p. 43-50
Molecular dynamics of shock waves in dense fluids
- 1 January 2008
- Published by Elsevier in Spectrochimica Acta Part B: Atomic Spectroscopy
- Vol. 63 (1) , 37-41
Expansion phenomena of aerosols generated by laser ablation under helium and argon atmosphere
- 1 January 2008
- Published by Elsevier in Spectrochimica Acta Part B: Atomic Spectroscopy
- Vol. 63 (1) , 37-41
Expansion phenomena of aerosols generated by laser ablation under helium and argon atmosphere
- Open Access
- 22 August 2007
- Published by American Physical Society (APS) in Physical Review E
- Vol. 76 (2) , 026314
Incomplete molecular chaos within dense-fluid shock waves
Large-scale molecular dynamics simulations of an shock in dense argon (, ) and an shock in dense nitrogen (, ) have been performed. The two-point molecular velocity correlation function is calculated within slices in plane with the shock wave. Long-range (ten molecular radii) positive correlations (correlation coefficient ) are observed for the shock-normal velocity component, the in-plane velocity component, and the rotation rates. No correlations are found upstream or downstream of the shock, indicating that this is a nonequilibrium effect. These correlations violate one of the assumptions underlying the Boltzmann equation.- 22 August 2007
- Published by American Physical Society (APS) in Physical Review E
- Vol. 76 (2) , 026314
Open AccessIncomplete molecular chaos within dense-fluid shock waves
Large-scale molecular dynamics simulations of an shock in dense argon (, ) and an shock in dense nitrogen (, ) have been performed. The two-point molecular velocity correlation function is calculated within slices in plane with the shock wave. Long-range (ten molecular radii) positive correlations (correlation coefficient ) are observed for the shock-normal velocity component, the in-plane velocity component, and the rotation rates. No correlations are found upstream or downstream of the shock, indicating that this is a nonequilibrium effect. These correlations violate one of the assumptions underlying the Boltzmann equation. - 21 June 2007
- Published by Springer Nature in Experiments in Fluids
- Vol. 43 (2-3) , 453-461
Non-contact boundary layer profiler using low-coherence self-referencing velocimetry
- 21 June 2007
- Published by Springer Nature in Experiments in Fluids
- Vol. 43 (2-3) , 453-461
Non-contact boundary layer profiler using low-coherence self-referencing velocimetry
- 17 April 2007
- Published by Optica Publishing Group in Optics Letters
- Vol. 32 (10) , 1247-1249
Low-coherence self-referencing velocimetry
Low-coherence self-referencing velocimetry optically measures the relative velocity between a point in a particle-laden fluid and a (potentially moving) reference surface. Low-coherence light scattered off the particles and off the reference surface is coupled into an interferometer with variable optical delay in one arm and an acousto-optical modulator in the second arm. The measurement location is set relative to the reference surface. Its location can be scanned along a line by adjusting the optical delay in the interferometer. The spatial resolution is typically tens of micrometers. Only one low-coherence light beam is required for each component of the velocity vector. Proof-of-principle measurements in Taylor–Couette flow are presented.
- 17 April 2007
- Published by Optica Publishing Group in Optics Letters
- Vol. 32 (10) , 1247-1249
Low-coherence self-referencing velocimetry
Low-coherence self-referencing velocimetry optically measures the relative velocity between a point in a particle-laden fluid and a (potentially moving) reference surface. Low-coherence light scattered off the particles and off the reference surface is coupled into an interferometer with variable optical delay in one arm and an acousto-optical modulator in the second arm. The measurement location is set relative to the reference surface. Its location can be scanned along a line by adjusting the optical delay in the interferometer. The spatial resolution is typically tens of micrometers. Only one low-coherence light beam is required for each component of the velocity vector. Proof-of-principle measurements in Taylor–Couette flow are presented.
- 10 April 2007
- Published by Elsevier in Journal of Computational Physics
- Vol. 223 (1) , 305-315
Higher moments of the velocity distribution function in dense-gas shocks
- 10 April 2007
- Published by Elsevier in Journal of Computational Physics
- Vol. 223 (1) , 305-315
Higher moments of the velocity distribution function in dense-gas shocks
- 1 January 2007
- Published by Elsevier in Spectrochimica Acta Part B: Atomic Spectroscopy
- Vol. 62 (1) , 20-29
Visualization of aerosol particles generated by near infrared nano- and femtosecond laser ablation
- 1 January 2007
- Published by Elsevier in Spectrochimica Acta Part B: Atomic Spectroscopy
- Vol. 62 (1) , 20-29
Visualization of aerosol particles generated by near infrared nano- and femtosecond laser ablation
- 1 September 2006
- Published by AIP Publishing in Physics of Fluids
- Vol. 18 (9)
Molecular alignment in a shock wave
Molecular dynamics simulations of dense nitrogen show that nonspherical molecules have a weak tendency to align their molecular axis such that it lies parallel to the plane of a shock wave front. As a consequence, there is also an even weaker tendency for the molecular rotation axis to align perpendicular to the shock front. The underlying mechanism is discussed and it is argued that this phenomenon can only be observed for dense fluids and only when considering realistic molecular interactions. A single relevant nondimensional parameter is proposed.
- 1 September 2006
- Published by AIP Publishing in Physics of Fluids
- Vol. 18 (9)
Molecular alignment in a shock wave
Molecular dynamics simulations of dense nitrogen show that nonspherical molecules have a weak tendency to align their molecular axis such that it lies parallel to the plane of a shock wave front. As a consequence, there is also an even weaker tendency for the molecular rotation axis to align perpendicular to the shock front. The underlying mechanism is discussed and it is argued that this phenomenon can only be observed for dense fluids and only when considering realistic molecular interactions. A single relevant nondimensional parameter is proposed.
- 1 November 2005
- Published by American Institute of Aeronautics and Astronautics (AIAA) in Journal of Propulsion and Power
- Vol. 21 (6) , 1008-1018
Transient Grating Spectroscopy in a Hot Turbulent Compressible Free Jet
- 1 November 2005
- Published by American Institute of Aeronautics and Astronautics (AIAA) in Journal of Propulsion and Power
- Vol. 21 (6) , 1008-1018
Transient Grating Spectroscopy in a Hot Turbulent Compressible Free Jet