Bloch equations are phenomenological equations that were introduced by Felix Bloch in 1946.
2.
They are analogous to the Maxwell-Bloch equations.
3.
Terahertz transitions in solids can be systematically approached by generalizing the semiconductor Bloch equations and the related many-body correlation dynamics.
4.
In 1956, H . C . Torrey mathematically showed how the Bloch equations for magnetization would change with the addition of diffusion.
5.
The observability of quantum jumps was predicted by Hans Dehmelt in 1975, and they were first observed using optical Bloch equations are not consistent with quantum jumps.
6.
The SLR algorithm simplifies the solution of the Bloch equations to the design of two polynomials, which can be solved using well-known digital filter design algorithms.
7.
A direct solution to the pulse design problem was independently proposed by Shinnar and Le Roux based on a discrete approximation to the spin domain version of the Bloch equations.
8.
Bloch equations are " macroscopic " : they describe the equations of motion of macroscopic nuclear magnetization that can be obtained by summing up all nuclear magnetic moment in the sample.
9.
Structurally, the SLEs resemble the semiconductor Bloch equations ( SBEs ) if the \ Pi _ { \ omega, \ mathbf { k } } are compared with the microscopic polarization within the SBEs.
10.
Only if one sets V _ { \ mathbf { k } } to zero, one finds isolated transitions within each { \ mathbf { k } } state that follow exactly the same dynamics as the optical Bloch equations predict.
मोबाइल