The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal conductivity of solids under conditions of laser cooling has been converted to a form that contains on its right-hand side an expression for the load power and the removed power. Numerical and analytical solutions are presented for this equation under conditions far from saturation. They give the time-dependent temperature distribution inside a sample for laser cooling of optical fibers and extended crystals. © 2003 Optical Society of America
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
A fundamental limit for the scaling of the output power of fiber lasers is the heat generated in the...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
A fundamental limit for the scaling of the output power of fiber lasers is the heat generated in the...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The equation obtained earlier by the authors from a starting model Hamiltonian for the thermal condu...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
In the framework of nonequilibrium statistical operator, the equations are derived for number of pho...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The method of the nonequilibrium statistical operator is employed to derive the kinetic equations fo...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
The optimum conditions for laser cooling of solids are studied. By way of example, a system of impur...
A fundamental limit for the scaling of the output power of fiber lasers is the heat generated in the...