M. Hortaçsu
Istanbul Technical University
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Featured researches published by M. Hortaçsu.
Nuclear Physics | 1980
M. Hortaçsu; K.D. Rothe; Bert Schroer
Abstract As an alternative to the method of spherical compactification for the Dirac operator in instanton background fields we study the correct method of “box-quantization”: the Atiyah-Patodi-Singer spectral boundary condition. This is the only self-adjoint boundary condition which respects the charge conjugation property and the γ5 symmetry, apart from the usual breaking due to zero modes. We point out the relevance of this approach to the computation of instanton determinants and other problems involving Dirac spinors.
General Relativity and Gravitation | 2003
M. Hortaçsu; Hasan Tuncay Özçelik; Barış Yapışkan
We solve the Einstein equations for the 2 + 1 dimensions with and without scalar fields. We calculate the entropy, Hawking temperature and the emission probabilities for these cases. We also compute the Newman-Penrose coefficients for different solutions and compare them.
Journal of Mathematical Physics | 2007
Tolga Birkandan; M. Hortaçsu
We study the solutions of the Dirac equation in the background of the Nutku helicoid metric. This metric has curvature singularities, which necessitates imposing a boundary to exclude this point. We use the Atiyah-Patodi-Singer [Math. Proc. Cambridge Philos. Soc. 77, 43 (1975)] nonlocal spectral boundary conditions for both the four and the five dimensional manifolds.
Classical and Quantum Gravity | 1999
Alikram N. Aliev; M. Hortaçsu; J. Kalayci; Yavuz Nutku
Physical properties of gravitational instantons which are derivable from minimal surfaces in three-dimensional Euclidean space are examined using the Newman-Penrose formalism for Euclidean signature. The gravitational instanton that corresponds to the helicoid minimal surface is investigated in detail. This is a metric of Bianchi type , or E(2), which admits a hidden symmetry due to the existence of a quadratic Killing tensor. It leads to a complete separation of variables in the Hamilton-Jacobi equation for geodesics, as well as in Laplaces equation for a massless scalar field. The scalar Green function can be obtained in closed form, which enables us to calculate the vacuum fluctuations of a massless scalar field in the background of this instanton.
Physics Letters B | 1982
K.G. Akdeniz; M. Arik; M. Durgut; M. Hortaçsu; S. Kaptanoǧlu; N.K. Pak
Abstract The Gursey model, a conformally invariant pure spinor model in four dimensions, is quantized to result in an asymptotically free theory.
Physics Letters B | 1982
K.G. Akdeniz; M. Arik; M. Durgut; M. Hortaçsu; S. Kaptanoǧlu; N.K. Pak
Abstract A pure spinor model with a non-polynomial interaction with global SU ( n ) symmetry is quantized in the path integral formalism. The model is found to be asymptotically free.
General Relativity and Gravitation | 1999
M. Hortaçsu; B. C. Lutfuoglu
We show spurious effects in perturbativecalculations due to different orderings of inhomogeneousterms while computing corrections to Green functions fortwo different metrics. These effects are not carried over to physically measurable quantities likethe renormalized value of the vacuum expectation valueof the stress-energy tensor.
Classical and Quantum Gravity | 1997
A N Aliev; M. Hortaçsu; N. Ozdemir
We study the interaction of a massless quantized spinor field with the gravitational field of N parallel static cosmic strings by using a perturbative approach. We show that the presence of more than one cosmic string gives rise to an additional contribution to the energy density of vacuum fluctuations, thereby leading to a vacuum force of attraction between two parallel cosmic strings.
Physics Letters B | 1983
K.G. Akdeniz; M. Arik; M. Hortaçsu; N.K. Pak
Abstract Non-abelian gauge theories are obtained as effective theories of certain models which at the lagrangian level contain only spinor fields.
Journal of Mathematical Physics | 1993
M. Hortaçsu
It is shown that quantum fluctuations, in particular vacuum polarization, vanish in the background of a spherical impulsive wave solution of the Einstein field equations, recently found by Nutku and Penrose. The calculation is done in first‐order perturbation theory but arguments are given why it should persist to all orders.