Femtosecond gas phase electron diffraction with MeV electrons

Author:

Yang Jie123,Guehr Markus45367,Vecchione Theodore453,Robinson Matthew S.123,Li Renkai453,Hartmann Nick453,Shen Xiaozhe453,Coffee Ryan453,Corbett Jeff453,Fry Alan453,Gaffney Kelly453,Gorkhover Tais453,Hast Carsten453,Jobe Keith453,Makasyuk Igor453,Reid Alexander453,Robinson Joseph453,Vetter Sharon453,Wang Fenglin453,Weathersby Stephen453,Yoneda Charles453,Wang Xijie453,Centurion Martin123

Affiliation:

1. University of Nebraska-Lincoln

2. Lincoln

3. USA

4. SLAC National Accelerator Laboratory

5. Menlo Park

6. Physics and Astronomy

7. Potsdam University

Abstract

We present results on ultrafast gas electron diffraction (UGED) experiments with femtosecond resolution using the MeV electron gun at SLAC National Accelerator Laboratory. UGED is a promising method to investigate molecular dynamics in the gas phase because electron pulses can probe the structure with a high spatial resolution. Until recently, however, it was not possible for UGED to reach the relevant timescale for the motion of the nuclei during a molecular reaction. Using MeV electron pulses has allowed us to overcome the main challenges in reaching femtosecond resolution, namely delivering short electron pulses on a gas target, overcoming the effect of velocity mismatch between pump laser pulses and the probe electron pulses, and maintaining a low timing jitter. At electron kinetic energies above 3 MeV, the velocity mismatch between laser and electron pulses becomes negligible. The relativistic electrons are also less susceptible to temporal broadening due to the Coulomb force. One of the challenges of diffraction with relativistic electrons is that the small de Broglie wavelength results in very small diffraction angles. In this paper we describe the new setup and its characterization, including capturing static diffraction patterns of molecules in the gas phase, finding time-zero with sub-picosecond accuracy and first time-resolved diffraction experiments. The new device can achieve a temporal resolution of 100 fs root-mean-square, and sub-angstrom spatial resolution. The collimation of the beam is sufficient to measure the diffraction pattern, and the transverse coherence is on the order of 2 nm. Currently, the temporal resolution is limited both by the pulse duration of the electron pulse on target and by the timing jitter, while the spatial resolution is limited by the average electron beam current and the signal-to-noise ratio of the detection system. We also discuss plans for improving both the temporal resolution and the spatial resolution.

Funder

National Science Foundation

U.S. Department of Energy

Basic Energy Sciences

Publisher

Royal Society of Chemistry (RSC)

Subject

Physical and Theoretical Chemistry

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