LETTERS Generation of Fock states in a superconducting quantum circuit
... states, which are states with specific numbers of energy quanta, but such states are hard to create3–7. Here we demonstrate the controlled generation of multi-photon Fock states in a solid-state system. We use a superconducting phase qubit8, which is a close approximation to a two-level spin system, ...
... states, which are states with specific numbers of energy quanta, but such states are hard to create3–7. Here we demonstrate the controlled generation of multi-photon Fock states in a solid-state system. We use a superconducting phase qubit8, which is a close approximation to a two-level spin system, ...
The Rare Two-Dimensional Materials with Dirac Cones
... Since germanene has similar electronic properties to silicene, the growth of germanene is also attractive. In 2014, Gao et al. first reported the fabrication of germanene sheet on Pt(111) which has a distorted (√19×√19) superstructure with respect to the substrate[90]. Calculations have shown that g ...
... Since germanene has similar electronic properties to silicene, the growth of germanene is also attractive. In 2014, Gao et al. first reported the fabrication of germanene sheet on Pt(111) which has a distorted (√19×√19) superstructure with respect to the substrate[90]. Calculations have shown that g ...
Improve The Convergence of Jarzynski Equality through Fast
... by taking the inverse Fourier transform on both sides. Equation (2.14) is know as fluctuation theorem or Crooks relation [3]. If we multiply both side of equation (2.14) by e−βW and take the summation over all possible work, we would obtain the quantum Jarzynski equality: he−βW i = e−β∆F . ...
... by taking the inverse Fourier transform on both sides. Equation (2.14) is know as fluctuation theorem or Crooks relation [3]. If we multiply both side of equation (2.14) by e−βW and take the summation over all possible work, we would obtain the quantum Jarzynski equality: he−βW i = e−β∆F . ...
Analytical Mechanics, Seventh Edition
... magnetism yield observable phenomena that could be understood only from the vantage point of a new space—time paradigm arising from Albert Einstein's special relativity. Hermann Minkowski introduced this new paradigm in a semipopular lecture in Cologne, Germany in 1908 as follows: Gentlemen! The vie ...
... magnetism yield observable phenomena that could be understood only from the vantage point of a new space—time paradigm arising from Albert Einstein's special relativity. Hermann Minkowski introduced this new paradigm in a semipopular lecture in Cologne, Germany in 1908 as follows: Gentlemen! The vie ...
Terahertz driven intraband dynamics of excitons in nanorods Fredrik Sy
... materials such as Silicon, Lead selenide (PbSe), Indium phosphide (InP) and Cadmium selenide (CdSe) to name a few [4,5,6]. Due to their wide array of potential applications, numerous theoretical studies have also been done on the optical and electronic properties of quantum dots with the focus being ...
... materials such as Silicon, Lead selenide (PbSe), Indium phosphide (InP) and Cadmium selenide (CdSe) to name a few [4,5,6]. Due to their wide array of potential applications, numerous theoretical studies have also been done on the optical and electronic properties of quantum dots with the focus being ...
Topological Photonics Lu, John D. Joannopoulos, and Marin Soljaˇci´c
... to the energy gaps of insulators. The sum of the Chern numbers of the dispersion bands below the frequency gap labels the topology of a mirror. This can be understood as the total number of “twists” and “un-twists” of the system up to the gap frequency. Ordinary mirrors like air (total internal refl ...
... to the energy gaps of insulators. The sum of the Chern numbers of the dispersion bands below the frequency gap labels the topology of a mirror. This can be understood as the total number of “twists” and “un-twists” of the system up to the gap frequency. Ordinary mirrors like air (total internal refl ...
Quantum Proofs for Classical Theorems
... where [n] denotes the set {1, . . . , n} and the vectors |i, ji = |ii ⊗ | ji form an orthonormal basis for Cmn . This tensor product of states |φ i and |ψi is also often denoted simply as |φ i|ψi. Note that this new state is a unit vector, as it should be. Not every pure state in Cmn can be expresse ...
... where [n] denotes the set {1, . . . , n} and the vectors |i, ji = |ii ⊗ | ji form an orthonormal basis for Cmn . This tensor product of states |φ i and |ψi is also often denoted simply as |φ i|ψi. Note that this new state is a unit vector, as it should be. Not every pure state in Cmn can be expresse ...
Manipulation and Simulation of Cold Atoms in
... Kantian (who introduced me to real chocolate), Andi Micheli (who has regular coffee breaks at half past one in the morning), Sarah Morrison (who put up with my Australian jokes and linguistic sense of humour), Peter Rabl (who won our Stadtlauf competition for the “Diplom Students”), Alessio Recati ( ...
... Kantian (who introduced me to real chocolate), Andi Micheli (who has regular coffee breaks at half past one in the morning), Sarah Morrison (who put up with my Australian jokes and linguistic sense of humour), Peter Rabl (who won our Stadtlauf competition for the “Diplom Students”), Alessio Recati ( ...
The Casimir Effect: Some Aspects
... data and theory was established. One of the great difficulties was to maintain a perfect parallelism between the plates. Four decades have passed, approximately, until new experiments were made directly with metals. In 1997, using a torsion pendulum Lamoreaux [14] inaugurated the new era of experime ...
... data and theory was established. One of the great difficulties was to maintain a perfect parallelism between the plates. Four decades have passed, approximately, until new experiments were made directly with metals. In 1997, using a torsion pendulum Lamoreaux [14] inaugurated the new era of experime ...