General Relativistic Radiative Transfer
... The first part of my thesis investigates the motion of particles in a strong gravitational field (near a black hole). I derive the equations of motion for massive or massless particles acted upon by external forces. Efforts are made to work out self-consistently the structure of the accreting flow a ...
... The first part of my thesis investigates the motion of particles in a strong gravitational field (near a black hole). I derive the equations of motion for massive or massless particles acted upon by external forces. Efforts are made to work out self-consistently the structure of the accreting flow a ...
Schrödinger Cat State Atomic Interferometer with Heisenberg
... In this thesis, we show first how to formulate the properties of all the collective states under various non-idealities, and use this formulation to understand the dynamics thereof. We show that the collective states corresponding to the absorption of a given number of photons can be visualized as a ...
... In this thesis, we show first how to formulate the properties of all the collective states under various non-idealities, and use this formulation to understand the dynamics thereof. We show that the collective states corresponding to the absorption of a given number of photons can be visualized as a ...
... elements and regularized Maxwell equations. The advantages are that, without adding extra unknowns (such as Lagrange multipliers), it provides spurious-free solutions and well-conditioned matrices. Besides, its integral representation involves a less singular kernel (order 1 instead of 3), which mak ...
Electron-hole correlations in semiconductor quantum dots with tight-binding wave functions
... ⫺r兩 ,R) that is assumed to be a function of both the separation 兩 r⬘⫺r兩 of the two particles and the dot radius R. Spinorbit couplings are not included in this work. We use the nearest-neighbor s p 3 s * tight-binding description. The structure of a quantum dot is modeled as an anioncentered zinc-bl ...
... ⫺r兩 ,R) that is assumed to be a function of both the separation 兩 r⬘⫺r兩 of the two particles and the dot radius R. Spinorbit couplings are not included in this work. We use the nearest-neighbor s p 3 s * tight-binding description. The structure of a quantum dot is modeled as an anioncentered zinc-bl ...
... method, in which the system at the thermodynamic equilibrium is simulated considering a propagation in con guration space for a nite imaginary time. However, the same formalism can be extended also to zero temperature calculations, in the so called Path Integral Ground State method, which still pre ...
Stoichiometry: Calculations with Chemical Formulas and Equations
... the operations of art and nature, nothing is created; an equal amount of matter exists both before and after the experiment. Upon this principle, the whole art of performing chemical ...
... the operations of art and nature, nothing is created; an equal amount of matter exists both before and after the experiment. Upon this principle, the whole art of performing chemical ...
Local unitary transformation, long-range quantum
... reversal and parity symmetries but not the spin rotation symmetry.11 However, it was quickly realized that there are many different chiral spin states that have exactly the same symmetry, so symmetry alone is not enough to characterize different chiral spin states. This means that the chiral spin st ...
... reversal and parity symmetries but not the spin rotation symmetry.11 However, it was quickly realized that there are many different chiral spin states that have exactly the same symmetry, so symmetry alone is not enough to characterize different chiral spin states. This means that the chiral spin st ...
