Results 11  20
of
81
Soft CP breaking and the strongCP problem
, 2008
"... I put forward a model with vectorlike isosinglet quarks in which soft breaking of CP leads to strong CP violation only arising at twoloop level. Nonperturbative effects in Quantum Chromodynamics (QCD) may lead to P and CP violation, characterized by a parameter θ, in strong interactions. The exper ..."
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. The experimental upper bound on the electric dipole moment of the neutron requires θ< ∼ 2 × 10 −10 [1]. (Electric dipole moments of elementary particles are both Pand Tviolating; in normal field theory, T violation is equivalent to CP violation.) The presence of this unnaturally small number in QCD is known
CERTIFICATE OF APPROVAL
, 2014
"... Treatment plan optimization for rotatingshield brachytherapy ..."
A framework for the storage and retrieval of continuous media data
 IN PROCEEDINGS OF THE IEEE INTERNATIONAL CONFERENCE ON MULTIMEDIA COMPUTING AND SYSTEMS, WASHINGTON D.C
, 1995
"... Continuous media applications require a guaranteed transfer rate of data, which conventional storage servers are not designed to provide. The aim of this paper is to provide a general framework for the design of storage servers that deal with both continuous and noncontinuous media data. We present ..."
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Cited by 22 (10 self)
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present several algorithms for the concurrent transfer of continuous media data for multiple requests with di erent rates. The algorithms provide high throughput by reducing the seek latency time and by eliminating rotational latency incurred when accessing data on disks. Each of these algorithms
Enhanced Todd Podd Electromagnetic Moments in Reflection Asymmetric Nuclei
, 1996
"... Collective P and T odd moments produced by parity and time invariance violating forces in reflection asymmetric nuclei are considered. The enhanced collective Schiff, electric dipole and octupole moments appear due to the mixing of rotational levels of opposite parity. These moments can exceed sin ..."
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Cited by 3 (0 self)
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Collective P and T odd moments produced by parity and time invariance violating forces in reflection asymmetric nuclei are considered. The enhanced collective Schiff, electric dipole and octupole moments appear due to the mixing of rotational levels of opposite parity. These moments can exceed
UW/PT972 Hot B violation, the lattice, and hard thermal loops
, 1997
"... It has recently been argued that the rate per unit volume of baryon number violation (topological transitions) in the hot, symmetric phase of electroweak theory is of the form η α5 wT 4 in the weakcoupling limit, where η is a nonperturbative numerical coefficient. Over the past several years, there ..."
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It has recently been argued that the rate per unit volume of baryon number violation (topological transitions) in the hot, symmetric phase of electroweak theory is of the form η α5 wT 4 in the weakcoupling limit, where η is a nonperturbative numerical coefficient. Over the past several years
New Facets of the Linear Ordering Polytope
, 1995
"... The linear ordering problem has many applications and was studied by many authors (see [5, 9, 12] for survey). One approach to solve this problem, the socalled cutting plane method [8, 14] derives facetdefining inequalities, which are violated by current nonfeasible solution and adds them to the ..."
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Cited by 13 (1 self)
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The linear ordering problem has many applications and was studied by many authors (see [5, 9, 12] for survey). One approach to solve this problem, the socalled cutting plane method [8, 14] derives facetdefining inequalities, which are violated by current nonfeasible solution and adds them
ROLE OF TRANSVERSE POLARIZATION IN CONSTRAINING NEW PHYSICS
, 2004
"... Transverse polarization (TP) can be used to study interference of (S, P) or T type couplings from new physics with SM contribution. In e + e − → t¯t, a CPodd azimuthal asymmetry can constrain the scale Λ of new (S, P) or T contact interactions to be higher than about 7 TeV for √ s = 500 GeV, ∫ Ldt ..."
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Transverse polarization (TP) can be used to study interference of (S, P) or T type couplings from new physics with SM contribution. In e + e − → t¯t, a CPodd azimuthal asymmetry can constrain the scale Λ of new (S, P) or T contact interactions to be higher than about 7 TeV for √ s = 500 Ge
Explicit Actions for Electromagnetism with Two Gauge Fields with Only one Electric and one Magnetic Physical Fields
, 2006
"... We extend the work of Mello et al. based in Cabbibo and Ferrari concerning the description of electromagnetism with two gauge fields from a variational principle, i.e. an action. We provide a systematic independent derivation of the allowed actions which have only one magnetic and one electric physi ..."
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physical fields and are invariant under the discrete symmetries P and T. We conclude that neither the Lagrangian, nor the Hamiltonian, are invariant under the electromagnetic duality rotations. This agrees with the weakstrong coupling mixing characteristic of the duality due to the Dirac quantization
Floorplanning with Abutment Constraints and Lshaped/Tshaped Blocks based on Corner Block List
 in Proc. DAC, 2001
, 2001
"... The abutment constraint problem is one of the common constraints in practice to favor the transmission of data between blocks. Based on Comer Block List(CBL), a new algorithm to deal with abutment constraints is developed in this paper. We can obtain the abutment information by scanning the intermed ..."
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Cited by 3 (0 self)
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the intermediate solutions represented by CBL in linear time during the simulated annealing process and fix the CBL in case the constraints are violated. Based on this algorithm, a new method to deal with Lshaped/Tshaped blocks is proposed. The shape flexibility of the soft blocks and the rotation and reflection
Collective T and P Odd Electromagnetic Moments in Nuclei with Octupole Deformations
, 1996
"... Parity and time invariance violating forces produce collective P and T odd moments in nuclei with static octupole deformation. Collective Schiff moment, electric octupole and dipole and also magnetic quadrupole appear due to the mixing of rotational levels of opposite parity and can exceed singlep ..."
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Parity and time invariance violating forces produce collective P and T odd moments in nuclei with static octupole deformation. Collective Schiff moment, electric octupole and dipole and also magnetic quadrupole appear due to the mixing of rotational levels of opposite parity and can exceed
Results 11  20
of
81