LEADER 05735nam 2200757 450 001 9910452791703321 005 20200520144314.0 010 $a981-4436-19-4 035 $a(CKB)2550000001126119 035 $a(EBL)1441476 035 $a(OCoLC)859837238 035 $a(SSID)ssj0000952340 035 $a(PQKBManifestationID)12318000 035 $a(PQKBTitleCode)TC0000952340 035 $a(PQKBWorkID)10902814 035 $a(PQKB)11143901 035 $a(MiAaPQ)EBC1441476 035 $a(WSP)00008623 035 $a(Au-PeEL)EBL1441476 035 $a(CaPaEBR)ebr10775252 035 $a(CaONFJC)MIL526785 035 $a(EXLCZ)992550000001126119 100 $a20131014d2013 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aSpace-time symmetry and quantum Yang-Mills gravity $ehow space-time translational gauge symmetry enables the unification of gravity with other forces /$fJong-Ping Hsu, Leonardo Hsu, authors 210 1$aSingapore :$cWorld Scientific,$d2013. 210 4$d©2013 215 $a1 online resource (289 p.) 225 1 $aAdvanced Series on Theoretical Physical Science ;$vVolume 11 300 $aDescription based upon print version of record. 311 $a981-4436-18-6 311 $a1-299-95534-7 320 $aIncludes bibliographical references and index. 327 $aPreface; Contents; Overview; About the Author; Part I. The Taiji Symmetry Framework Leonardo Hsu and Jong-Ping Hsu; 1. Space-Time Symmetry, Natural Units and Fundamental Constants; 1-1. Underpinnings; 1-2. Physical basis for the system of natural units; 1-3. Nature of the fundamental constants; References; 2. The Taiji Relativity Framework; 2-1. A new space-time framework; 2-2. Taiji relativity; 2-3. Operationalization of taiji time; 2-4. Conceptual difference between taiji relativity and Special Relativity; 2-5. A short digression: The role of a second postulate; References 327 $a3. The Principle of Limiting Continuation of Physical Laws and Coordinate Transformations for Frames with Constant Accelerations3-1. The principle of limiting continuation; 3-2. Constant linear acceleration: The Wu transformations; 3-3. Operational meaning of the space-time coordinates and 'constant-linear-acceleration'; 3-4. Singular walls and horizons in accelerated frames; 3-5. The Wu pseudo-group; 3-6. Relationship between the Wu and Møller transformations; 3-7. Experimental tests of the Wu transformations; References 327 $a4. Coordinate Transformations for Frames with Arbitrary Linear Accelerations and the Taiji Pseudo-Group4-1. Arbitrary Linear Accelerations: The Taiji Transformations; 4-2. Poincare? Metric Tensors for Arbitrary-Linear-Acceleration Frames; 4-3. New Properties of the Taiji Transformations; 4-4. Physical Implications; 4-5. Experimental Tests of the Taiji Transformations; References; 5. Coordinate Transformations for Rotating Frames and Experimental Tests; 5-1. Rotational taiji transformations; 5-2. Metric tensors for the space-time of rotating frames; 5-3. The rotational pseudo-group 327 $a5-4. Physical implications5-5. Experimental tests of the rotational taiji transformations; References; 6. Conservation Laws and Symmetric Energy-Momentum Tensors; 6-1. Conservation laws in the Taiji symmetry framework; 6-2. Symmetric energy-momentum tensors and variations of metric tensors intaiji space-time; 6-3. Integral forms of conservation laws in non-inertial frames; 6-4. Symmetry implications of global and local space-time translations; References; Part II. Quantum Yang-Mills Gravity Jong-Ping Hsu and Leonardo Hsu 327 $a7. The Yang-Mills-Utiyama-Weyl Framework for Internal and External Gauge Symmetries7-1. The Yang-Mills-Utiyama-Weyl framework; 7-2. The Levi-Civita connection and interpretations of Einstein gravity; 7-3. Weyl's parallel transport of scale and electromagnetic fields; 7-4. Curvatures on the connections; 7-5. Taiji symmetry and the space-time translational symmetry group T4; References; 8. Yang-Mills Gravity Based on Flat Space-time and Effective Curved Space-Time for Motions of Classical Objects; 8-1. Translational gauge transformations in taiji space-time 327 $a8-2. Translational gauge symmetry and the field-theoretic origin of effective metric tensors 330 $aYang-Mills gravity is a new theory, consistent with experiments, that brings gravity back to the arena of gauge field theory and quantum mechanics in flat space-time. It provides solutions to long-standing difficulties in physics, such as the incompatibility between Einstein's principle of general coordinate invariance and modern schemes for a quantum mechanical description of nature, and Noether's 'Theorem II' which showed that the principle of general coordinate invariance in general relativity leads to the failure of the law of conservation of energy. Yang-Mills gravity in flat space-time a 410 0$aAdvanced series on theoretical physical science ;$vv. 11. 606 $aSpace and time 606 $aSymmetry (Physics) 606 $aYang-Mills theory 606 $aGauge fields (Physics) 606 $aGravity 608 $aElectronic books. 615 0$aSpace and time. 615 0$aSymmetry (Physics) 615 0$aYang-Mills theory. 615 0$aGauge fields (Physics) 615 0$aGravity. 676 $a530.1435 700 $aHsu$b J. P$g(Jong-Ping)$0858698 701 $aHsu$b Leon$0858699 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910452791703321 996 $aSpace-time symmetry and quantum Yang-Mills gravity$91916774 997 $aUNINA