Fractional Fourier–Kravchuk transform
... but still three dimensional; all their sensor points [Eq. (1.2)] are on the x axis. We regard the Newton equations (1.6) as the fundamental dynamical definition of a waveguide; they are satisfied (of course) by the Schrödinger differential operator (1.5) but also by a difference operator [see Eq. ( ...
... but still three dimensional; all their sensor points [Eq. (1.2)] are on the x axis. We regard the Newton equations (1.6) as the fundamental dynamical definition of a waveguide; they are satisfied (of course) by the Schrödinger differential operator (1.5) but also by a difference operator [see Eq. ( ...
An important problem, not discussed so far by other authors, is the
... This paper is organized as follows. Section 2 presents the minimal background in quantum circuit design necessary to understand the paper. Examples are used to illustrate the most important notions. Section 3 describes the general problem of synthesis of quantum circuits (called also quantum arrays) ...
... This paper is organized as follows. Section 2 presents the minimal background in quantum circuit design necessary to understand the paper. Examples are used to illustrate the most important notions. Section 3 describes the general problem of synthesis of quantum circuits (called also quantum arrays) ...
Reply to criticism of the ‘Orch OR qubit’ – ‘Orchestrated... reduction’ is scientifically justified
... (Section 5.6 in our review [2]). Here we respond point-by-point to the issues they raise. Reimers et al. . . . For quantum information processing one must have quantum information storage units such as qubits . . . the involvement of quantum gravity in the manifestation of consciousness would need t ...
... (Section 5.6 in our review [2]). Here we respond point-by-point to the issues they raise. Reimers et al. . . . For quantum information processing one must have quantum information storage units such as qubits . . . the involvement of quantum gravity in the manifestation of consciousness would need t ...
Post-quantum Security of the CBC, CFB, OFB, CTR
... 2 . Thus, all we need to show is that replacing one block of the challenge ciphertext by randomness leads to a negligible change in the advantage of the adversary. The situation is depicted in Figure 1 (b). – Say we want to show that c2 = H(m2 ⊕ c1 ) is indistinguishable from random (the situation i ...
... 2 . Thus, all we need to show is that replacing one block of the challenge ciphertext by randomness leads to a negligible change in the advantage of the adversary. The situation is depicted in Figure 1 (b). – Say we want to show that c2 = H(m2 ⊕ c1 ) is indistinguishable from random (the situation i ...
Topological quantum memory
... assumption—measurement requires the amplification of a microscopic quantum effect to a macroscopic signal, which may take a while. But by measuring a classical error syndrome for each code block, we can improve the efficiency of error recovery. Furthermore, if we can measure qubits and perform quant ...
... assumption—measurement requires the amplification of a microscopic quantum effect to a macroscopic signal, which may take a while. But by measuring a classical error syndrome for each code block, we can improve the efficiency of error recovery. Furthermore, if we can measure qubits and perform quant ...
Review - Sociedade Brasileira de Química
... of AB or S = s chains. Those represent usual quantum AF Heisenberg chains, which are known to follow Haldane’s conjecture,59 i.e. half-integer spin chains are critical with no long-range order and integer spin chains are disordered. Moreover, the addition of the relevant Wess-Zumino term to the quan ...
... of AB or S = s chains. Those represent usual quantum AF Heisenberg chains, which are known to follow Haldane’s conjecture,59 i.e. half-integer spin chains are critical with no long-range order and integer spin chains are disordered. Moreover, the addition of the relevant Wess-Zumino term to the quan ...
Fabrication and characterization of single luminescing quantum dots
... the case in lighting technology, since due to its indirect bandgap nature bulk silicon is an inherently poor light emitter. With the discovery of efficient light emission from silicon nanostructures, great new interest arose and research in this area increased dramatically. However, despite more tha ...
... the case in lighting technology, since due to its indirect bandgap nature bulk silicon is an inherently poor light emitter. With the discovery of efficient light emission from silicon nanostructures, great new interest arose and research in this area increased dramatically. However, despite more tha ...
Chapter 7 Spin and Spin–Addition
... as strong to the magnetic moment as its orbital angular momentum, is called the anomalous magnetic moment of the electron. The constant µB is known as Bohr’s magneton 1 . ...
... as strong to the magnetic moment as its orbital angular momentum, is called the anomalous magnetic moment of the electron. The constant µB is known as Bohr’s magneton 1 . ...
Circuit Quantum Electrodynamics with Transmon Qubits in
... concerning plagiarism, including those regulations concerning disciplinary actions that may result from plagiarism. ...
... concerning plagiarism, including those regulations concerning disciplinary actions that may result from plagiarism. ...
Quantum Computation and Quantum Information
... defined to be a unit vector in H. Let |ψ(t) be the state of the quantum system at time t, which is also referred to as a wave function. The states |ψ(t1 ) and |ψ(t2 ) at t1 and t2 are connected through |ψ(t2 ) = U(t1 , t2 )|ψ(t1 ), where U(t1 , t2 ) is a unitary operator depending only on time ...
... defined to be a unit vector in H. Let |ψ(t) be the state of the quantum system at time t, which is also referred to as a wave function. The states |ψ(t1 ) and |ψ(t2 ) at t1 and t2 are connected through |ψ(t2 ) = U(t1 , t2 )|ψ(t1 ), where U(t1 , t2 ) is a unitary operator depending only on time ...
Experimental generation of single photons via active multiplexing
... the electro-optic material. This design of the router has several advantages: (1) It can route incoming photons independent of their polarizations, which is crucial for certain tasks. In the schemes of polarization-entanglement-based quantum cryptography [24] and quantum computation with polarizatio ...
... the electro-optic material. This design of the router has several advantages: (1) It can route incoming photons independent of their polarizations, which is crucial for certain tasks. In the schemes of polarization-entanglement-based quantum cryptography [24] and quantum computation with polarizatio ...
