E 1.99:lbnl--57976
|
High Field Magnet R&D in the USA |
1 |
E 1.99:lbnl--57977
|
HD1 Design and Fabrication of a 16 Tesla Nb3Sn DipoleMagnet. |
1 |
E 1.99:lbnl--57978
|
Assessment of Distributed Generation Potential in JapaneseBuildings |
1 |
E 1.99:lbnl--57982
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FastBit An Efficient Indexing Technology For AcceleratingData-Intensive Science. |
1 |
E 1.99:lbnl--57983
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Optimum model-E-GAMS for Distributed Energy System by Using GAMSMethod |
1 |
E 1.99:lbnl--57985
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Microturbine Economic Competitiveness A Study of Two PotentialAdopters. |
1 |
E 1.99:lbnl--57990
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Role of Alcohol on the Fracture Resistance of Dentin |
1 |
E 1.99:lbnl--57994
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Identification of Severe Multiple Contingencies in Electric PowerNetworks |
1 |
E 1.99:lbnl--58000
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Real Options Valuation of U.S. Federal Renewable Energy Research,Development, Demonstration, and Deployment |
1 |
E 1.99:lbnl--58001
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Integrated Performance Monitoring of a Cosmology Application onLeading HEC Platforms |
1 |
E 1.99:lbnl--58002
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Magnetohydrodynamic Turbulence Simulations on the Earth SimulatorUsing the Lattice Boltzmann Method |
1 |
E 1.99:lbnl--58004
|
Performance Evaluation of Plasma and Astrophysics Applications onModern Parallel Vector Systems |
1 |
E 1.99:lbnl--58005
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Data Evaluation for 56Co epsilon + beta+ Decay |
1 |
E 1.99:lbnl--58008
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Comparing Price Forecast Accuracy of Natural Gas Models andFutures Markets |
1 |
E 1.99:lbnl--58009
|
Scenarios for Benefits Analysis of Energy Research, Development,Demonstration and Deployment |
1 |
E 1.99:lbnl--58010
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Design Principles for the Use of Electroactive Polymers forOvercharge Protection of Lithium-Ion Batteries |
1 |
E 1.99:lbnl--58021
|
Heat as a Tracer to Examine Hydraulic Conductance Near the RussianRiver Bank Filtration Facility, Sonoma County, CA |
1 |
E 1.99:lbnl--58024
|
Improvements to the image processing of HST NICMOS observationswith multiple readouts |
1 |
E 1.99:lbnl--58025
|
An Accelerator Control Middle Layer Using MATLAB |
1 |
E 1.99:lbnl--58026
|
Search for b0(s) --> mu+ mu- and b0(d) --> mu+ mu- decays in p anti-p collisions at s**½ = 1.96 tev |
1 |