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Dr. Alison A. Baski
Silicon Surfaces

One of my primary areas of interest, silicon, is a material that has spawned a multibillion-dollar industry. Properties of silicon which have led to its dominance in the electronics industry include: a nearly perfect SiO2 passivating interface, large wafer size, robustness, and low cost. Although silicon is the material of choice for VLSI technology, it does lack a few highly desirable properties, such as laser action and high mobility. To overcome this limitation, there has been a strong effort to integrate materials having such properties with standard Si integrated circuit technology, i.e. to grow heterostructures on silicon. Recent examples include GaAs grown on Si for optoelectronic and high speed applications, HgCdTe grown on Si for far-infrared detection, and Si/Ge heterostructures for heterojunction bipolar transistors. The challenge of thee systems lies in understanding and controlling the interface between the various materials, where lattice mismatch and different thermal expansion coefficients can lead to misfit dislocations which impair device performance. A number of approaches have been explored to minimize the effect of such dislocations, ranging from manipulation of the growth conditions to the choice of substrate orientation, but much remains to be done.



Dr. John A. Carlisle
Synchrotron-radiation-based materials characterization

After completing my doctoral work in October 1993, I was a postdoctoral research associate in the Chemistry and Materials Science Department at Lawrence Livermore National Laboratory (LLNL). Working under Dr. Louis J. Terminello, and in collaboration with a variety of researchers at LLNL, as well as other national labs, industry, and academia, I have conducted cutting-edge research at the newly commissioned Advanced Light Source (ALS) at Lawrence Berkely National Laboratory. Utilizing the brightest tunable source of soft X-rays available, I have used photoemission, photoabsorption, and soft-x-ray flourescence to probe the geometric and electronic structure of many novel material systems and surfaces. These systems include diamond and diamond-like thin-films, buried monolayers, magnetic multilayers, dopants, polymers, aerogels, and other thin-film systems. In particular, I have been involved in ground-breaking work probing inelastic x-ray scattering processes in several of the above systems, using a technique called resonant soft-x-ray fluorescence

It is this emerging technique of resonant soft-x-ray fluorescence that I wish to develop into a powerful characterization tool of novel surface and material systems. Soft x-ray-fluorescence (SXF) spectroscopy, using synchrotron radiation as a tunable excitation source, offers several advantages for probing the electronic structure of complex, multi-elemental materials [D. L. Ederer et al., Synchrotron Radiat. News 7, 29 (1994)]. As a photon-in, photon-out spectroscopy, SXF is intrinsically bulk-sensitive. This is due to the long mean-free path of photons in solids (~1000A). Also, since core levels are involved in both the photon absorption and emission processes, SXF is both an element- and angular-momentum-selective probe of the occupied electronic structure. Consequently, SXF measures the local particle density of states projected onto each constituent element of the material. Note that this allows one to probe the electronic structure of elements which are buried deeply in a sample, such as dopants, buried thin films, and multilayers. The chief limitatin of SXF has been the low fluorescence yield for photon emission, particularly for light elements. However, third-generation light sources such as the ALS now offer the high brightness that have made high-resolution SXF experiments practical. In particular, this high brightness has enabled detailed studies of the excitation energy dependence of emission spectra when the excitation energy is tuned through a core level binding energy. In these robust resonant SXF experiments, the presence or lack of long-range order, the degree of localization, the energy-separation between the major symmetry points in the band structure, and the crystal momenum-resolved electronic structure, may be determined.

 

 

 

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