UCR

Department of Physics & Astronomy



Harry Tom


Harry Tom

Harry W. K. Tom

Professor

Office:
Physics 3033/1021/23/31

Telephone: 951-827-2818
Email: Harry.Tom@ucr.edu
Fax: 951-827-4529

Personal Home Page

Research Interests:

  • Surface nonlinear optics studies of metal, semiconductor and water/solid interface systems
  • Ultrafast physical and chemical processes on surfaces
  • Terahertz spectroscopy of liquid water, confined water, and biomolecules in liquid water
  • Time-resolved imaging of laser-induced damage and of spin torque on magnetic domain walls
  • Optical biosensors
  • Spin dynamics in semiconductors and nanomagnetic materials and devices
  • Laser spectroscopy of positronium atoms and positronium molecules
  • Raman spectroscopy of bone

Education:

Ph.D. University of California, Berkeley

Current Research:

Harry W. K. Tom, Professor of Physics, specializes in nonlinear optics and femtosecond time-resolved laser techniques and is particularly interested in surface dynamics, laser-induced surface chemical reactions, laser-induced phase transitions in bulk materials, nonlinear optics of the water/solid interface, and most recently in terahertz spectroscopy. Tom is Co-Director of the Environmental Physics graduate program, an interdisciplinary program in which condensed matter physicists and environmental scientists collaborate in joint research and graduate training.

1. Coherent Optical Spectroscopy of Surface Phonons and Low Frequency Molecule-Substrate Vibrational Modes and Electronic State Coherence: When a femtosecond laser pulse impinges on a surface, it can excite normal mode vibrations of the surface atoms (ie., phonons), much as striking a bell can excite the normal mode vibrations of a bell. The surface atoms will continue to vibrate at the normal mode frequencies and the mode amplitudes will decay by collisional processes that "dephase" the coherent oscillation. We detect these modes by time-resolved second-harmonic generation: a second "probe" pulse irradiates the surface and the second-harmonic generation from this probe is detected as a function of the pump-probe time-delay. Surface vibrational modes are significant in the study of surface dynamics and reactions because they mediate the transfer of vibrational energy between the bulk material and molecules that may stick or chemically react on the surface. The significance of this new all optical surface phonon technique is that it is the only one that can be used at buried interfaces, ie., gas/solid, liquid/solid, solid/solid interface. We are still investigating the potential of this technique and are using it to investigate surface reactions on clean and adsorbate-covered semiconductor and metal surfaces. We have observed surface phonon at clean and native-oxide covered GaAs (100) and (110). We have seen bulk LO phonon hole-plasmon coupled oscillations. We have also observed phonon changes during Ar+-ion sputtering, insitu oxidation of clean GaAs (100)-(4X6) and laser-induced surface disorder of GaAs (110)-(1X1).

We have also developed a new coherent electronic spectroscopy of surfaces using time-resolved SHG. By measuring both the time-resolved pump-probe cross-correlation and an optical superposition of the SH fields from the probe and autocorrelation, we can deduce the amplitude, frequency, and phase of the induced optical polarization of the surface electronic states and the laser parameters (pulse duration and chirp).

2. Femtosecond surface chemical reactions and physical changes: Femtosecond laser pulses deposit energy into the electronic states of a system on a time scale short compared to electron-phonon relaxation. Femtosecond laser desorption of molecules from surfaces is enhanced by many orders of magnitude over nanosecond laser desorption due to novel energy transfer associated with the electronic excitation. The substrate temperature can be several 1000K while the atomic motion is still cold. Under these conditions multiple electronic excitations must also be considered. For CO desorbed from Cu(111), the yield from a single pulse can be as high as 100%. We are exploring mechanisms of energy transfer to molecules from metals by exploring differences in the isotopic yield of CO desorbed from Cu crystals in UHV. We have also studied laser-induced damage of the reconstructed (1X1) surface of GaAs(110). In both cases, reactions occur due to electronic rather than purely thermal driving mechanisms. The laser intensities are far below the damage threshold for the bulk material. Because we are able to measure the depletion field through DC-field induced SHG, we can also obtain information about the carrier dynamics including surface hole recombination which turns out to be much slower than the so called surface recombination velocity. This work has been partially supported by the National Science Foundation under NSF-CHE-9707143 and Lawrence Livermore National Laboratory under MI-98-013.

3. Femtosecond Laser-Induced Heating, Melting, and Phase Transitions: The absorption of light in semiconductors promotes electronic states that are generally bonding in character to states that are generally anti-bonding. Thus the absorption of light generally weakens the interatomic bonds in a material. During a femtosecond laser pulse, one can promote 5-10% of the electron population all before the lattice acquires much energy. Under those conditions, the bandgap can collapse and the material will disorder spontaneously--within 100 fs. We are exploring mechanisms of energy transfer, bandgap collapse, and electronically induced phase transitions in the regime near and just above damage. We hope to electronically bias these systems close to static high pressure phase transitions by conducting these experiments in diamond anvil cells. These studies are conducted in collaboration with investigators at Lawrence Livermore National Laboratory and is currently funded under LLNL-MI-099-008.

4. Time-Resolved Imaging Studies of Laser-Induced Damage of Optical Crystals: We are able to obtain images of bulk structural changes on a nanosecond timescale after an optical crystal is initially irradiated by a laser pulse. The damage nucleation site absorbs energy and the energy propagates away from the damage site in a shockwave or in dislocation loops. In some cases what we would consider permanent damage does not occur until many 10's of nanoseconds after the laser pulse. Fundamental studies of shockwave propagation, structural phase transitions, and fracture have in general not been conducted in spherical geometry with point like excitation sources. We are thus developing new tools for understanding and predicting structural damage in this geometry. These results are relevant not only to optical damage but also earthquake propagation and structural fatigue of materials. This project is performed in collaboration with several investigators at Lawrence Livermore National Laboratory and is currently funded under LLNL-B346502.

5. Terahertz Spectroscopy of Correlated Electron Materials: Electrons and holes are created when ultrashort laser pulses are absorbed in a semiconductor. Their rapid creation and subsequent motion provide a rapidly varying polarization that radiates in the terahertz frequency range. Spectroscopy based on this terahertz source has favorable signal to noise and frequency range compared to spectroscopy based on globar sources or discrete frequency devices. This femtosecond laser-based source is also more convenient than free electron lasers. Ward Beyermann (UCR) and I are building a femtosecond laser-based terahertz spectrometer that will be used to study correlated electron materials at low temperatures. Correlated electron materials are expected to show interesting spectral features in the terahertz range because their critical temperatures are such that kBTc are comparable to hf where f is in the terahertz range. This work is funded by the National Science Foundation under NSF-DMR-9704032.

5. Environmental Physics: Nonlinear Optical Studies of the Water/Solid Interface: Second-Harmonic Generation and Visible-Infrared Sum-Frequency Generation are two nonlinear optical probes that can provide information about molecular adsorbates at interfaces of environmental importance (such as the water/solid, air/solid, or air/liquid interface). We are currently studying the orientation of water within the double charge layer at water/silica interface on planar and colloidal particle samples. We also study the adsorption of simple molecules at the surface. Our fundamental contribution is the ability to measure the field in the double charge layer in an insitu non-destructive manner. The solid surface charge is effected self-consistently with the adsorbates and pH in the double-charge layer. This work is interesting from the fundamental point of view because chemistry at the water/solid interface is not well understood and certainly not as well studied as chemistry at the vacuum/solid interface. This work is relevant to environment science because current models for pesticide degradation and transport in the environment require microscopic reaction rates. This interdisciplinary research is performed in collaboration with Michael Anderson in the Soil and Environmental Sciences Department. The graduate student who is performing this research will receive both a M.Sc. in Soil Physics and a Ph.D. in Physics. We are currently seeking more graduate students to do related research. Students who are interested in this kind of interdisciplinary research may read more about the Environmental Physics graduate program. Currently 6 graduate students are supported under a National Science Foundation Graduate Research Traineeship program in Environmental Science, NSF-DGE-9554506.

 

Selected Publications (>75 citations): 

  1. T.F. Heinz, H.W.K. Tom and Y.R. Shen, "Determination of Molecular Orientation of Monolayer Adsorbates by Optical Second-Harmonic Generation," Phys. Rev. A28, 1883-1885 (1983).
  2. H.W.K. Tom, T.F. Heinz and Y.R. Shen, "Second-Harmonic Reflection from Silicon Surfaces and its Relation to Structural Symmetry," Phys. Rev. Lett. 51, 1983-1986 (1983).
  3. H.W.K. Tom, C.M. Mate, X.D. Zhu, J.E. Crowell, T.F. Heinz, G.A. Somorjai and Y.R. Shen, "Surface Studies by Optical Second-Harmonic Generation: The Adsorption of O2, CO and Sodium on the Rh(111) Surface," Phys. Rev. Lett 52, 348-351 (1984).
  4. H.W.K. Tom, C.M. Mate, X.D. Zhu, J.E. Crowell, Y.R. Shen and G.A. Somorjai "Studies of Alkali Adsorption on Rh(111) Using Optical Second-Harmonic Generation, Surf. Sci. 172, 466-476 (1986).
  5. H.W.K. Tom and G.D. Aumiller, "Observation of Rotational Anisotropy in the Second-Harmonic Generation from a Metal Surface," Phys. Rev. B33, 8818-8821 (1986).
  6. R.H. Stolen and H.W.K. Tom, "Self-Organized Phase-Matched Harmonic Generation in Optical Fibers," Optics Lett. 12, 585-587, (1987).
  7. H.W.K. Tom, G.D. Aumiller and C.H. Brito-Cruz, "Time-Resolved Study of Laser-Induced Disorder of Si Surfaces," Phys. Rev. Lett. 60, 1438-1441, (1988).
  8. J.A. Prybyla, H.W.K. Tom and G.D. Aumiller, "Direct Time Resolved Observation of Desorption with 100 Femtosecond Resolution," Phys. Rev. Lett. 68, 503-506 (1992).
  9. W.S. Fann, R. Storz, H.W.K. Tom and J. Bokor, "Direct Measurement of Nonequilibrium Electron Energy Distributions in Sub Picosecond Laser Heated Gold Films," Phys. Rev. Lett. 68, 2834-2837 (1992).
  10. W.S. Fann, R. Storz, H.W.K. Tom and J. Bokor, "Electron Thermalization in Gold," Phys. Rev. B46, 13592-13595 (1992).
  11. U. Mohideen, M.H. Sher, H.W.K. Tom, G.D. Aumiller and others, "High Intensity Above-Threshold Ionization of He," Phys. Rev. Lett. 71, 509-512 (1993).
  12. Y.-M. Chang, L. Xu, and H.W.K. Tom, "Observation of Coherent Surface Optical Phonon Oscillations by Time-Resolved Surface Second-Harmonic Generation," Phys. Rev. Lett. 78, 4649-4652 (1997).

Recent Publications:

  1. Y.F. Chiang, J. Wong, X. Tan, Y. Li, K. Pi, W.H. Wang, H.W.K. Tom, R.K. Kawakami, “Oxidation-induced biquadratic coupling in Co/Fe/MgO/Fe(001),” Phys. Rev. B 79, 184410-184414 (2009).
  2. D.B. Cassidy, P. Crivelli, T.H. Hisakado, L. Liszkay, V.E. Meligne, P. Perez, H.W.K. Tom, A.P. Mills, Jr., “Positronium cooling in porous silica measured via Doppler spectroscopy,” Phys. Rev. A 81, 012715-012727 (2010).
  3. D.B. Cassidy, T.H. Hisakado, V.E. Meligne, H.W.K. Tom, A.P. Mills, Jr., ”Delayed emission of cold positronium from mesoporous materials,” Phys. Rev. A 82, 052511-052520 (2010).
  4. D.B. Cassidy, M.W.J. Bromley, L.C. Cota, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., ”Cavity Induced Shift and Narrowing of the Positronium Lyman- Transition,” Phys. Rev. Lett. 106, 023401-023404 (2011).
  5. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “New Mechanism for Positronium Formation on a Silicon Surface,” Phys. Rev. Lett. 106, 133401-133404 (2011).
  6. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Laser Excitation of Positronium in the Paschen-Back Regime,” Phys. Rev. Lett. 106, 173401-173404 (2011).
  7. D.B. Cassidy, M.W.J. Bromley, L.C. Cota, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Cassidy et al. Reply: Cavity Induced Shift and Narrowing of the Positronium Lyman- Transition,” Phys. Rev. Lett. 106, 209302 (2011).
  8. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Photoemission of Positronium from Si,” Phys. Rev. Lett. 107, 033401-033404 (2011).
  9. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Positronium Formation via Excitonlike States on Si and Ge Surfaces,” Phys. Rev. B 84, 195312-195323 (2011).
  10. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Efficient Production of Rydberg Positronium,” Phys. Rev. Lett. 108, 043401-043405 (2012).
  11. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Optical Spectroscopy of Molecular Positronium,” Phys. Rev. Lett. 108, 133402-133406 (2012).
  12. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Positronium Hyperfine Interval Measured via Saturated Absorption Spectroscopy,” Phys. Rev. Lett. 109, 073401-073405 (2012).
  13. D.B. Cassidy, T.H. Hisakado, H.W.K. Tom, A.P. Mills, Jr., “Excitonic positronium emission from n-Si(111),” Phys. Rev. B 86, 155303-155306 (2012).

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