Designed especially for neurobiologists, FluoRender is an interactive tool for multi-channel fluorescence microscopy data visualization and analysis.
Deep brain stimulation
BrainStimulator is a set of networks that are used in SCIRun to perform simulations of brain stimulation such as transcranial direct current stimulation (tDCS) and magnetic transcranial stimulation (TMS).
Developing software tools for science has always been a central vision of the SCI Institute.

SCI Publications

1999


C.L. Bajaj, V. Pascucci, G. Zhuang. “Single Resolution Compression of Arbitrary Triangular Meshes with Properties,” In Proceedings of DCC: Data Compression Conference 1999, IEEE Computer Society, Snowbird, Utah March, 1999.



C.L. Bajaj, S. Cutchin, V. Pascucci, A. Paoluzzi, C. Morgia. “Web Based Collaborative CAAD,” In Proceedings of the 5th Symposium on Solid Modeling and Applications, 1999.



C. Bajaj, V. Pascucci, E. Petajan, G. Zhuang. “Polygonal Model Coding Evaluation for Low bit-rate Communication,” In Proceedings of the International Workshop on Synthetic - Natural Hybrid Coding and Three Dimensional Imaging, September, 1999.



M. Berzins, L.J.K. Durbeck. “Unstructured Mesh Methods Applied to Hyperbolic PDEs with Source Terms: Error Estimates and Mesh Quality,” In Godunov Methods: Theory and Applications Conference and Short Course, Oxford. numeritek Ltd.URL, October, 1999.



M. Berzins, J. Nash, P. Selwood. “Parallel Solution of Reacting Flow Problems using Unstructured Tetrahedral Meshes,” In Proceedings of 9th SIAM Parallel Processing for Scientific Computing, Philadelphia, PA, 1999.
ISBN: 0-89871-435-4



M. Berzins. “A Solution Based H1 Norm Triangular Mesh Quality Indicator,” In Grid Generation and Adaptive Algorithms, Edited by Marshal W. Bern, Joseph E. Flaherty, Mitchell Luskin, Springer, pp. 77-88. 1999.

ABSTRACT

The issue of mesh quality measures for triangular (and tetrahedral) meshes is considered. A new mesh quality measure is based both on geometrical and solution information and is derived by considering the error in the H 1 norm when linear triangular elements are used to approximate a quadratic function. The new measure is then compared with the recent mesh quality measure based on the L 2 norm. Simple examples are used to show that the choice of norm is critical in deciding what is a good triangulation



M. Berzins. “Mesh Quality - Geometry, Error Estimates or Both?,” In Engineering and Computers, Vol. 15, pp. 236--247. 1999.



D. Botstein, L. Smarr, D. Agard, M. Levitt, D. Lippman, D. Herrington, C.R. Johnson, G Rose, G. Rubin, A. Levison, M. Spence, H. Smith, C. Peskin, G. Jacobs. “NIH Biomedical Information Science and Technology Initiative (BISTI),” Note: Prepared by the Working Group on Biomedical Computing Advisory Committee to the Director, National Institutes of Health, July, 1999.

ABSTRACT

The biomedical community is increasingly taking advantage of the power of computing, both to manage and analyze data, and to model biological processes. The working group should investigate the needs of NIH-supported investigators for computing resources, including hardware, software, networking, algorithms, and training. It should take into account efforts to create a national information infrastructure, and look at working with other agencies (particularly NSF and DOE) to ensure that the research needs of the NIH-funded community are met.

It should also investigate the impediments biologists face in utilizing high-end computing, such as a paucity of researchers with cross-disciplinary skills. The panel should consider both today's unmet needs and the growing requirements over the next five years (a reasonable horizon for extrapolating the advances in the rapidly changing fields of computing and computational biology).

The result of deliberations should be a report to the NIH Director, which will be presented to the Advisory Committee to the Director. The report should include recommendations for NIH actions to support the growing needs of NIH-funded investigators for biomedical computing.



J.D. Brederson. “The I3Stick: An Inexpensive, Immersive, Interaction Device,” School of Computing Technical Report, No. UUCS-99-014, University of Utah, November, 1999.



D.H. Brooks, G.F. Ahmad, R.S. MacLeod, G.M. Maratos. “Inverse Electrocardiography by Simultaneous Imposition of Multiple Constraints,” In IEEE Trans Biomed. Eng., Vol. 46, No. 1, pp. 3--18. 1999.



O.G. Byutner, G.D. Smith. “Conformational Properties of Poly(vinylidene fluoride). A Quantum Chemistry Study of Model Compounds,” In Macromolecules, Vol. 32, No. 25, pp. 8376--8382. 1999.
DOI: 10.1021/ma9902605

ABSTRACT

The molecular geometries and conformational energies of model molecules of poly(vinylidene fluoride) (PVDF) have been determined from high-level quantum chemistry calculations and have been used in parametrization of a six-state rotational isomeric state (RIS) model for PVDF. The model molecules investigated were 1,1,1,3,3-pentafluorobutane, 1,1,1,3,3,5,5,5-octofluoropentane, 2,2,4,4-tetrafluoropentane, and 2,2,4,4,6,6-hexafluoroheptane (HFH). Analysis of the conformations of these molecules revealed split trans minima (t+ = 195°, t- = 165°), as was seen in previous studies of perfluoroalkanes. In contrast, the gauche minima, which split in perfluoroalkanes, did not do so in the PVDF model compounds. The lowest energy conformer of HFH, g+g+g+g+, was found to be at least 0.4 kcal/mol lower in energy per backbone dihedral than any of the conformers of HFH resembling crystalline polymorphs of PVDF, indicating that intermolecular interactions are important in stabilizing conformations of PVDF in the crystalline phases. A six-state RIS model was able to accurately reproduce the conformer energies of the PVDF model compounds. The RIS analysis revealed that, as in n-alkanes and perfluoroalkanes, the trans conformation of the backbone dihedral is intrinsically lower in energy than the gauche conformation in the PVDF model compounds. However, very large unfavorable second-order interactions between fluorine atoms occur in −CH2− centered t+t+ sequences and, to a lesser extent, t+g+ and t+g- sequences. The quantum chemistry based RIS model yielded a characteristic ratio for PVDF in good agreement with experiment, but with significantly different conformer populations than predicted by earlier RIS models, including a much higher gauche probability. The high gauche probability of 65% for unperturbed PVDF chains (at 463 K), greater than that for poly(ethylene) and much greater than that for poly(tetrafluoroethylene), is a consequence of the unfavorable second-order interactions occurring in −CH2− centered sequences containing trans conformations.



T.H.C. Childs, M. Berzins, G.R. Ryder, A. Towtoni. “Selective Laser Sintering of an Amorphous Polymer-Simulations and Experiments,” In Proceedings of the Institution of Mechanical Engineers Part B: Journal of Engineering Manufacture, Vol. 213, No. B4, pp. 333--349. 1999.


Matched: evap.zip


L. Durbeck. “Evaporation: A Technique for Visualizing Mesh Quality,” In 8th International Meshing Roundtable, Sandia National Laboratories, pp. 259--265. Oct, 1999.



C. Guerra, V. Pascucci. “On Matching Sets of 3D Segments,” In Proceedings of SPIE Vision Geometry VIII, Denver, USA pp. 157-167. 1999.



C. Guerra, V. Pascucci. “3D Segment Matching Using the Hausdorff Distance,” In Proceedings of the IEEE Conference on Image Processing and its Applications, IPA99, pp. 18--22. 1999.



C. Guerra, V. Pascucci. “Segment Matching for Protein Secondary Structure Comparison,” In Proceedings of the Third International Conference on Computational Molecular Biology, RECOMB'99, ACM, Lyon, France pp. 30. 1999.



C.D. Hansen, T. Udeshi, S.G. Parker, P. Shirley. “Parallel Methods for Isosurface Visualization,” In Ninth SIAM Conference on Parallel Processing for Scientific Computing, Note: extended abstract, 1999.



R.E. Hogan, K.E. Mark, L. Wang, S.C. Joshi, M.I. Miller, R.D. Bucholz. “MR Imaging Deformation-Based Segmentation of the Hippocampus in Patients with Mesial Temporal Sclerosis and Temporal Lobe Epilepsy,” In Epilepsia, Vol. 40, No. 7, 1999.



M.A. Johnson, T.N. Truong. “High Level Ab Initio and Density Functional Theory Evaluation of Combustion Reaction Energetics: NO2 and HONO Elimination from Dimethylnitramine,” In Journal of Physical Chemistry, A, Vol. 103, No. 44, pp. 8840--8846. October, 1999.
DOI: 10.1021/jp9925029

ABSTRACT

Dimethylnitramine (DMNA) is used as a model system for investigating accurate and efficient electronic structure methods for nitramines. Critical points on the potential energy surfaces of DMNA, CH3NCH3, CH3NCH2, NO2, HONO, and the transition state to HONO elimination were located through geometry optimizations using the B1LYP, B3LYP, MPW1PW91, and BH&HLYP density functional methods, in addition to MP2, G2(MP2), and QCISD ab initio theories using the cc-pVDZ basis set. For cost-effective determination of nitramine reaction energetics, highly correlated single-point calculations at DFT geometries are recommended. Our best estimated reaction enthalpies for N-N bond scission and HONO elimination are 41.6 and −0.9 kcal/mol, respectively, determined at the QCISD(T)//QCISD level of theory. These numbers can be reproduced to within 1.3 kcal/mol for the N-N bond and to within 0.5 kcal/mol for the HONO reaction by calculating QCISD(T) energies at B1LYP geometries, thus saving considerable computational cost without sacrificing accuracy. Using the same strategy, the transition state energy for HONO elimination can be modeled to within 0.1 kcal/mol of the QCISD(T)//QCISD result.



M.A. Johnson, T.N. Truong. “Importance of Polarization in Simulations of Condensed Phased Energetic Materials,” In Journal of Physical Chemistry, B, Vol. 103, No. 44, pp. 9392--9393. October, 1999.
DOI: 10.1021/jp992514u

ABSTRACT

An embedded cluster model is used to estimate the molecular dipole moment of crystalline dimethylnitramine (DMNA). The electrostatic potential due to the crystal is included in the calculation via the SCREEP (surface charge representation of the electrostatic embedding potential) approach. The resulting dipole moment for DMNA in the crystalline environment is 6.69 D. This number is more than 40% greater than the gas-phase value and 15% greater than the estimated dipole moment in the liquid phase, thus providing evidence of a strong polarization effect in condensed phases of DMNA.