![arXiv:1705.06742v1 [cond-mat.quant-gas] 18](http://s1.studyres.com/store/data/015536624_1-695304017ec91e58c90e68ba3242255c-300x300.png)
arXiv:1705.06742v1 [cond-mat.quant-gas] 18
... bilinear-biquadratic spin-1 chain in the presence of a spiral magnetic field. We then solve this effective model using the density matrix renormalization group (DMRG) to map out the zero temperature phase diagram in both the magnetic field (i.e., SOC) strength and the biquadratic interaction. We sho ...
... bilinear-biquadratic spin-1 chain in the presence of a spiral magnetic field. We then solve this effective model using the density matrix renormalization group (DMRG) to map out the zero temperature phase diagram in both the magnetic field (i.e., SOC) strength and the biquadratic interaction. We sho ...
Integral of cos3(2x)
... function with an odd exponent, which we solve using the identity cos2 (u) = 1 − sin2 (u). ...
... function with an odd exponent, which we solve using the identity cos2 (u) = 1 − sin2 (u). ...
Calc Sec 1_1 - Miami Killian Senior High School
... Graphing y=mx+b Using the Slope and y-Intercept • Graphing y = mx + b by Using the Slope and yIntercept • Plot the y-intercept on the y-axis. This is the point (0, b). • Obtain a second point using the slope, m. Write m as a fraction, and use rise over run starting at the y-intercept to plot this p ...
... Graphing y=mx+b Using the Slope and y-Intercept • Graphing y = mx + b by Using the Slope and yIntercept • Plot the y-intercept on the y-axis. This is the point (0, b). • Obtain a second point using the slope, m. Write m as a fraction, and use rise over run starting at the y-intercept to plot this p ...
950 - IACR
... strings (CRS), and that are statistically hiding.1 Yet, when using these commitments to get everlastingly secure OT, we run into the same problem again: We would get an everlastingly secure OT using a CRS, but a generalization of Lo’s impossibility shows that no everlastingly secure OT protocols ex ...
... strings (CRS), and that are statistically hiding.1 Yet, when using these commitments to get everlastingly secure OT, we run into the same problem again: We would get an everlastingly secure OT using a CRS, but a generalization of Lo’s impossibility shows that no everlastingly secure OT protocols ex ...
Real-time evolution for weak interaction quenches in quantum systems
... a generalized Gibbs ensemble [26]. Many of the mentioned results [27,26,30] explicitly agree with this approach and its prerequisites and limitations have been discussed [40,24]. A different notion of local relaxation grounds the examinations of finite subsystems [41,42] which may exhibit thermal sig ...
... a generalized Gibbs ensemble [26]. Many of the mentioned results [27,26,30] explicitly agree with this approach and its prerequisites and limitations have been discussed [40,24]. A different notion of local relaxation grounds the examinations of finite subsystems [41,42] which may exhibit thermal sig ...
Macroscopic Quantum Tunneling in a Josephson Junction Coupled
... superconductors can be thought of as one large “molecule” which traverses the junction. The tunneling of f results in a phase slip (a sudden change of f by 2p) which is observed as a voltage spike, since V is proportional to df/dt. ...
... superconductors can be thought of as one large “molecule” which traverses the junction. The tunneling of f results in a phase slip (a sudden change of f by 2p) which is observed as a voltage spike, since V is proportional to df/dt. ...
Quantum Transport in Nanoscale Devices
... Regarding conventional silicon MOSFETs, the device size is scaled in all dimensions (see Figure 1–2 bottom panel), resulting in smaller oxide thickness, junction depth, channel length, channel width, and isolation spacing. Currently, 65 nm (with a physical gate length of 45 nm) is the state-of-the-a ...
... Regarding conventional silicon MOSFETs, the device size is scaled in all dimensions (see Figure 1–2 bottom panel), resulting in smaller oxide thickness, junction depth, channel length, channel width, and isolation spacing. Currently, 65 nm (with a physical gate length of 45 nm) is the state-of-the-a ...
Overview Andrew Jaramillo Research Statement
... I plan to continue investigating the structure of quantum groups, further generalizing my results. For instance, all of the above results were shown for q not a root of unity. My expectation is that similar results will hold, with the appropriate modifications, for q a root of unity. Moreover, all o ...
... I plan to continue investigating the structure of quantum groups, further generalizing my results. For instance, all of the above results were shown for q not a root of unity. My expectation is that similar results will hold, with the appropriate modifications, for q a root of unity. Moreover, all o ...
How to Construct Quantum Random Functions
... At a high level, implicit in the GGM construction is a binary tree of depth n, where each leaf corresponds to an input/output pair of PRF. To evaluate PRF, we start at the root, and follow the path from root to the leaf corresponding to the input. The security proof consists of two hybrid arguments: ...
... At a high level, implicit in the GGM construction is a binary tree of depth n, where each leaf corresponds to an input/output pair of PRF. To evaluate PRF, we start at the root, and follow the path from root to the leaf corresponding to the input. The security proof consists of two hybrid arguments: ...
Lecture Notes
... What is our goal? We want to be able to take these majoranas - two for a state - and bring them apart. How can we break such an integral object? The two majoranas belong to a single state! We need something like Fig. 4. . . We do habe a magician, though. Kitaev said - what about just removing one of ...
... What is our goal? We want to be able to take these majoranas - two for a state - and bring them apart. How can we break such an integral object? The two majoranas belong to a single state! We need something like Fig. 4. . . We do habe a magician, though. Kitaev said - what about just removing one of ...
PDF 2 Heat Equation
... for an arbitrary constant A. Therefore, for each eigenfunction Xn with corresponding eigenvalue λn , we have a solution Tn such that the function un (x, t) = Tn (t)Xn (x) is a solution of the heat equation on the interval I which satisfies our boundary conditions. Note that we have not yet accounted ...
... for an arbitrary constant A. Therefore, for each eigenfunction Xn with corresponding eigenvalue λn , we have a solution Tn such that the function un (x, t) = Tn (t)Xn (x) is a solution of the heat equation on the interval I which satisfies our boundary conditions. Note that we have not yet accounted ...
FEN FAKÜLTESİ MATEMATİK BÖLÜMÜ Y
... Analysis. Conditioning of boundary value problems. Consistency, stability and convergence for both initial and boundary value problems. Fourier transform tecniques. Fourier analysis, Fourier spectral methods. Geometric integrators. Lie group methods, symplectic methods, Magnus series method. MATH 53 ...
... Analysis. Conditioning of boundary value problems. Consistency, stability and convergence for both initial and boundary value problems. Fourier transform tecniques. Fourier analysis, Fourier spectral methods. Geometric integrators. Lie group methods, symplectic methods, Magnus series method. MATH 53 ...