On conjugate complex time. III: Superstrings and complex Lorentz transformation
From MaRDI portal
Publication:1862301
DOI10.1016/S0960-0779(00)00060-6zbMath1019.83015OpenAlexW2079913845MaRDI QIDQ1862301
Publication date: 19 March 2003
Published in: Chaos, Solitons and Fractals (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1016/s0960-0779(00)00060-6
String and superstring theories in gravitational theory (83E30) Equations of motion in general relativity and gravitational theory (83C10)
Related Items
On the intrinsic gravitational repulsion ⋮ On Cantorian spacetime over number systems with division by zero ⋮ Cantor and generalized continuum hypotheses may be false ⋮ Elie Cartan and pan-geometry of multispatial hyperspace ⋮ On El Naschie's complex time, Hawking's imaginary time and special relativity ⋮ On the universe's missing mass
Cites Work
- Clifford algebra to geometric calculus. A unified language for mathematics and physics
- New foundations for classical mechanics
- On conjugate complex time and information in relativistic quantum theory
- On the nature of complex time, diffusion and the two-slit experiment
- A note on quantum gravity and Cantorian spacetime
- Orthogonality of matrices and some distance problems
- Is the principle of equivalence a principle?
- On conjugate complex time. I: Complex time implies existence of tangential potential that can cause some equipotential effects of gravity
- On conjugate complex time. II: Equipotential effect of gravity retrodicts differential and predicts apparent anomalous rotation of the sun.
- Energy-nonconservation in physics?
- New non-zero photon mass interpretation of the Sagnac effect as direct experimental justification of the Langevin paradox.
- Die Lorentz-Kraft auf pseudo-Riemannschen Mannigfaltigkeiten
- Trigonometry in Lorentzian Geometry
- Generalized Hyperbolic Functions
- Bakerian Lecture, 1975: Global geometry
- Measurement of the effect of Coriolis and centrifugal forces on the trajectory of a body in a rotating frame
- Can Quantum-Mechanical Description of Physical Reality be Considered Complete?
- General Relativity
- Causality and the Lorentz group
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item