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The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { i... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { int x,y; x = cilk_spawn fib(n-1); y fib(n 2); 4 cilk_sync; return (x+y);
The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { i... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { int x,y; x = cilk_spawn fib(n-1); y fib(n 2); 4 cilk_sync; return (x+y);
The fork-join parallelism model int fib (int n) { if (n<2) return (n); else { int x,y; x = cil... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); else { int x,y; x = cilk_spawn fib(n-1); y = fib(n-2); 2); cilk_sync; return (x+y);
The asymptotic behavior of the correlator for Polyakov loop operators separated by a large distan... more The asymptotic behavior of the correlator for Polyakov loop operators separated by a large distance R is determined for high temperature QCD. It is dominated by nonperturbative effects related to the exchange of magnetostatic gluons. To analyze the asymptotic behavior, the problem is formulated in terms of the effective field theory of QCD in 3 space dimensions. The Polyakov loop operator is expanded in terms of local gauge-invariant operators constructed out of the magnetostatic gauge field, with coefficients that can be calculated using resummed perturbation theory. The asymptotic behavior of the correlator is exp(−MR)/R, where M is the mass of the lowest-lying glueball in (2 + 1)-dimensional QCD. This result implies that existing lattice calculations of the Polyakov loop correlator at the highest temperatures available do not probe the true asymptotic region in R.One of the basic characteristics of a plasma is the screening of electric fields. The field created by a static charge...
Journal of Systems Architecture, 1999
The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { i... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { int x,y; x = cilk_spawn fib(n-1); y fib(n 2); 4 cilk_sync; return (x+y);
The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { i... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); Example: fib(4)else { int x,y; x = cilk_spawn fib(n-1); y fib(n 2); 4 cilk_sync; return (x+y);
The fork-join parallelism model int fib (int n) { if (n<2) return (n); else { int x,y; x = cil... more The fork-join parallelism model int fib (int n) { if (n<2) return (n); else { int x,y; x = cilk_spawn fib(n-1); y = fib(n-2); 2); cilk_sync; return (x+y);
The asymptotic behavior of the correlator for Polyakov loop operators separated by a large distan... more The asymptotic behavior of the correlator for Polyakov loop operators separated by a large distance R is determined for high temperature QCD. It is dominated by nonperturbative effects related to the exchange of magnetostatic gluons. To analyze the asymptotic behavior, the problem is formulated in terms of the effective field theory of QCD in 3 space dimensions. The Polyakov loop operator is expanded in terms of local gauge-invariant operators constructed out of the magnetostatic gauge field, with coefficients that can be calculated using resummed perturbation theory. The asymptotic behavior of the correlator is exp(−MR)/R, where M is the mass of the lowest-lying glueball in (2 + 1)-dimensional QCD. This result implies that existing lattice calculations of the Polyakov loop correlator at the highest temperatures available do not probe the true asymptotic region in R.One of the basic characteristics of a plasma is the screening of electric fields. The field created by a static charge...
Journal of Systems Architecture, 1999