Treatise on Materials Science and TechnologyHerbert Herman |
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Page 55
... is not much need for compression if most data cannot be compressed , so users need a general - purpose compression algorithm that compresses most data with a good compression 55 Selecting a General-Purpose Data Compression Algorithm.
... is not much need for compression if most data cannot be compressed , so users need a general - purpose compression algorithm that compresses most data with a good compression 55 Selecting a General-Purpose Data Compression Algorithm.
Page 100
... compression time te on the sending side and the decompression time ta on the receiving side ( where the sender is not necessarily the server ) ; 2. the compression ... compression algorithms 100 CHAPTER 3. COMPRESSION ENGINE ARCHITECTURE.
... compression time te on the sending side and the decompression time ta on the receiving side ( where the sender is not necessarily the server ) ; 2. the compression ... compression algorithms 100 CHAPTER 3. COMPRESSION ENGINE ARCHITECTURE.
Page 100
Ross N. Williams. Paper Value Description Williams88 βια Compression Bahl74 α / β Compression Jakobsson82 α / β Compression gain Pratt80 α / β Compression ratio Teuhola78 α / β Compression gain Turner75 a / B Compression ratio Bentley86 ...
Ross N. Williams. Paper Value Description Williams88 βια Compression Bahl74 α / β Compression Jakobsson82 α / β Compression gain Pratt80 α / β Compression ratio Teuhola78 α / β Compression gain Turner75 a / B Compression ratio Bentley86 ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray