X-ray Pump-Probe Instrument

The X-ray Pump-Probe (XPP) instrument will predominantly use a fast optical laser to generate transient states of matter, and the hard X-ray pulses from the LCLS to probe the structural dynamics initiated by the laser excitation. The laser pump will have the ability to conduct precise optical manipulations, in order to create the desired excited states. The instrument design will emphasize versatility. To maximize the range of phenomena that can be excited, it will be necessary to be able to manipulate the laser pulse energy, frequency, and temporal profile. X-ray scattering will be the dominant tool for probing the laser-induced structural changes. These experiments require the union of four experimental capacities: the generation and delivery of X-ray and laser pulses to the sample, the preparation of the excited state in the sample, and the detection of the X-ray scattering pattern.

Near Experimental Hall, Hutch 3 » complete instrument map

Biological, chemical, and physical processes involve the time-dependent transformation of matter on the atomic scale. Examples of these processes with technological and environmental significance are the photosynthetic generation of chemical energy, the catalytic production of fertilizer, the chemical degradation of pollutants, and the melting of ice. These structural transformations involve the motion of electrons, atoms, and molecules over very short distances (10^-9 m) and very short time scales (10^-12 s). Though much has been learned about these dynamical processes from previous work, particularly studies using X-rays and optical lasers, no existing technology can provide direct observation of atomic motions on ultrafast time scales.

The LCLS will provide transversely-coherent hard X-rays with unprecedented flux and time resolution. These attributes of the LCLS have the potential to revolutionize the experimental investigation of structural dynamics with X-ray techniques by directly following the time evolution of the electron density during the course of a photo-induced biological, chemical, or physical transformation.

The XPP diffraction instrument will enable the study of stimulated changes in the structures of molecules and condensed matter systems. The changes will typically be stimulated by a short pulse of optical laser light, and observed using X-ray scattering techniques. Femtosecond-level synchronization between the optical laser and the LCLS X-ray pulse will allow sub-picosecond time resolution. Some examples of the scientific programs that will be pursued by the XPP instrument are described below.

Dynamics of photo-induced phase transitions
Optical manipulation of solids can lead to photo-induced phase transitions on the ultrafast time scale. For many of these materials, a change in crystal symmetry accompanies a magnetic, ferroelectric, or metal-insulator phase transition. These materials have the potential to be utilized as ultrafast switches in magnetic and electro-optic devices and time-resolved X-ray crystallography provides an ideal tool for tracking the changes in atomic structure. For those systems that undergo a 1st-order photo-induced phase transition, time-resolved X-ray scattering has the potential to provide information about the structure and size of the new phase nucleus with previously unachievable detail.

Figure 1: Femtosecond atomic displacements generated in InSb and Bi in response to ultrafast photoexcitation of charge carriers. The data sets were measured using time-resolved X-ray diffraction at the Sub-Picosecond Pulse Source.
From Fritz et al., SCIENCE 315:633 (2007) and Lindenberg et al., SCIENCE 308:392 (2005). Reprinted with permission from AAAS.*

Studies of intense laser-matter interactions
The structural response of materials to femtosecond laser excitation differs fundamentally from the response to excitation with longer pulses, because the generation of carriers by linear and nonlinear absorption occurs faster than the time scale for carrier diffusion and carrier-phonon scattering. Consequently, the photon field can deposit enormous quantities of energy into electronic degrees of freedom, while the vibrational internal energy remains comparatively unperturbed. Excitation of carriers can alter the ionic potential energy landscape of a material and can lead to atomic motion ^[1,2] (see Figure 1). Identifying the important distinctions between materials and further correlating the material response with material electronic structure remains an important objective for understanding the light-matter interaction. Further knowledge in this field will enhance our ability to manipulate and control material structure with light.

Time-resolved studies of chemical dynamics in solution
The majority of chemical reactions in biological, environmental, and industrial settings occur in disordered media, with liquid water being the ubiquitous example. The development of methods for studying ultrafast time-resolved diffuse scattering in liquids will be an important component of the LUSI project. Pioneering diffuse scattering experiments have been conducted at ID-9 at the ESRF ^[3]. While these studies have demonstrated the viability of transient diffuse scattering measurements in liquids, the technique when applied at a synchrotron has insufficient time resolution for studying chemical dynamics. For these studies the improved time resolution of the LCLS will provide a significant advantage over synchrotron facilities.

Figure 2: Experimentally determined electron densities of the myoglobin molecule before and 100 ps after photolysis.
From Schotte et al., SCIENCE 300:1944 (2003). Reprinted with permission from AAAS.*

Dynamics of photoactive proteins
The variability and efficiency of proteins make them powerful molecular foundries. The size, diversity and complexity of proteins also make them challenging to study and understand with atomic detail. X-ray crystallography helped launch the molecular biology revolution and maintains a position of unique prominence in structural biology as the most powerful tool for determining biomolecular atomic structure. While enormously useful, the equilibrium structure cannot capture the full chemical significance of a protein. To understand how a protein functions at a mechanistic level of detail requires measuring in real time the nuclear motion that accompanies its function. Time-resolved protein crystallography represents the most powerful tool for achieving this experimental objective. While time-resolved crystallographic measurements have been conducted with time resolution as short as 150 ps, Figure 2 demonstrates that global structural changes have already occurred at the earliest time delay ^[4]. To observe and understand how a local perturbation propagates from the epicenter of the distortion to points far removed will require X-ray pulse durations and amplitudes only achievable with linac-based sources. By extending the time resolution of these measurements into the femtosecond regime, the ability to observe how a local distortion can be channeled into a concerted global structural change will be possible for the first time.

1. A. M. Lindenberg et al., Science, 308, 392-395 (2005).
2. D. M. Fritz et al., Science, 315, 633-636 (2007).
3. H. Ihee, M. Lorenc, T.K. Kim, Q.Y. Kong, M. Cammarata, J.H. Lee, S. Bratos and M. Wulff, Science, 309, 1223-636 (2005).
4. F. Schotte, M. Lim, T.A. Jackson, A.V. Smirnov, J. Soman, J.S. Olson, G.N. Phillips, M. Wulff and P.A. Anfinrud, Science, 300, 1944-1947 (2003).