Fermions coupled to gauge fields .1in with cond
... of a large system (o(N 2 )). (More on this in a moment.) 2. Too much universality! If this charged black hole is inevitable, how do we see the myriad possible dual states of matter (e.g. superconductivity...)? 3. The charged black hole violates the 3rd Law of Thermodynamics (Nernst’s version): S(T = ...
... of a large system (o(N 2 )). (More on this in a moment.) 2. Too much universality! If this charged black hole is inevitable, how do we see the myriad possible dual states of matter (e.g. superconductivity...)? 3. The charged black hole violates the 3rd Law of Thermodynamics (Nernst’s version): S(T = ...
1 Summary of PhD Thesis It is well known that the language of the
... new branch of science, namely from quantum information theory. We describe some aspects of group-theoretical description of quantum cloning machines, distillation of entanglement and finally construction of new mathematical tools, which help us with above mentioned mathematical modeling, this time i ...
... new branch of science, namely from quantum information theory. We describe some aspects of group-theoretical description of quantum cloning machines, distillation of entanglement and finally construction of new mathematical tools, which help us with above mentioned mathematical modeling, this time i ...
Axiomatic description of mixed states from Selinger`s CPM
... A,B (f : C ⊗ A → C ⊗ B) := λ†B ◦ (p1Cq ⊗ 1B )† ◦ (1C ∗ ⊗ f ) ◦ (p1Cq ⊗ 1A ) ◦ λA : A → B , play a crucial role in quantum information theory. To our knowledge, the need for an abstract notion of internal trace has so far only been indicated by Delbecque in [5], motivated by the fact that while in Se ...
... A,B (f : C ⊗ A → C ⊗ B) := λ†B ◦ (p1Cq ⊗ 1B )† ◦ (1C ∗ ⊗ f ) ◦ (p1Cq ⊗ 1A ) ◦ λA : A → B , play a crucial role in quantum information theory. To our knowledge, the need for an abstract notion of internal trace has so far only been indicated by Delbecque in [5], motivated by the fact that while in Se ...
Quantum Correlations and Fundamental Conservation Laws
... 2) Any theory that has a correlation function different from the ones in QM is incompatible with the fundamental conservation laws and space-time symmetries, and therefore it is unphysical. Local hidden variable theories fall in this class. Bell’s inequalities can be obeyed (in the general case) onl ...
... 2) Any theory that has a correlation function different from the ones in QM is incompatible with the fundamental conservation laws and space-time symmetries, and therefore it is unphysical. Local hidden variable theories fall in this class. Bell’s inequalities can be obeyed (in the general case) onl ...
1.01
... There is a common expression of information, strings of bits, regardless of the object/entity/process it describes. Bits are independent of their physical embodiment. Information is transformed using logic operations. Gates implement logic operations and allow for automatic processing of information ...
... There is a common expression of information, strings of bits, regardless of the object/entity/process it describes. Bits are independent of their physical embodiment. Information is transformed using logic operations. Gates implement logic operations and allow for automatic processing of information ...
Biologic
... A key to this problem certainly lies in the existence of the topoisomerase enzymes that can change the linking number between the DNA strands and also can change the linking number between two DNA duplexes. It is however, a difficult matter at best to find in a tangled skein of rope the just right c ...
... A key to this problem certainly lies in the existence of the topoisomerase enzymes that can change the linking number between the DNA strands and also can change the linking number between two DNA duplexes. It is however, a difficult matter at best to find in a tangled skein of rope the just right c ...
The Physical Implementation of Quantum Computation David P. DiVincenzo
... physical implementation must turn towards these. At least this result says that the required decoherence rate does not become ever smaller as the size and duration of the quantum computation grows. So, once the desired threshold is attainable, decoherence will not be an obstacle to scalable quantum ...
... physical implementation must turn towards these. At least this result says that the required decoherence rate does not become ever smaller as the size and duration of the quantum computation grows. So, once the desired threshold is attainable, decoherence will not be an obstacle to scalable quantum ...
Invite #4 (45minutes), Oral #46 (20+5 minutes)
... [Session 6A: Quantum Gates and Quantum States] 13:40-15:20 New Two-Qubit Gate Library with Entanglement Md Belayet Ali, Takashi Hirayama, Katsuhisa Yamanaka, Yasuaki Nishitani Quantum p-valued Toffoli and Deutsch gates with conjunctive or disjunctive mixed polarity control Claudio Moraga Logic Synth ...
... [Session 6A: Quantum Gates and Quantum States] 13:40-15:20 New Two-Qubit Gate Library with Entanglement Md Belayet Ali, Takashi Hirayama, Katsuhisa Yamanaka, Yasuaki Nishitani Quantum p-valued Toffoli and Deutsch gates with conjunctive or disjunctive mixed polarity control Claudio Moraga Logic Synth ...
QB abstracts compiled 160613
... Conway and Kochen’s free will theorem states that if experimenters have free will in the sense that their choices are not a function of the past, so must some elementary particles. The free will theorem goes beyond Bell’s theorem as it connects the two fundamental resources behind quantum technol ...
... Conway and Kochen’s free will theorem states that if experimenters have free will in the sense that their choices are not a function of the past, so must some elementary particles. The free will theorem goes beyond Bell’s theorem as it connects the two fundamental resources behind quantum technol ...
