Closed lapofran closed 5 years ago
Hi, there is a straight forward way to do it: Create a TMM source with Air|Gold|Quartz|Air, that provides the complex refractive index of every layer, the refractive index of Quartz is real, so no light will be deposited if you heat your material. However, there will be a diffusion process of the heat from Gold -> Quartz. With ´addLayer(length,heat_Conductivity,heat_Capacity, density,coupling_Constant)´ you can add the layers and then start the simulation.
Note, the TTM mainly takes thermodynamical parameters into consideration. band gap and optical parameters are considered only through the refractive index of every layer. The main focus lies on how much of the light is absorbed in every layer. The rest is relaxation between the systems and diffusion into the material.
A reference on |Gold|Glass| thin film measurements
Femtosecond pump–probe nondestructive examination of materials
by Pamela M. Norris,a)Andrew P. Caffrey, and Robert J. StevensDepartment et al. in Review of Scientific Instruments, Volume 74 Number 1. (January 2003) In specific Fig. 5)
Hi, there is a straight forward way to do it: Create a TMM source with Air|Gold|Quartz|Air, that provides the complex refractive index of every layer, the refractive index of Quartz is real, so no light will be deposited if you heat your material. However, there will be a diffusion process of the heat from Gold -> Quartz. With ´addLayer(length,heat_Conductivity,heat_Capacity, density,coupling_Constant)´ you can add the layers and then start the simulation.
Thanks for your quick answer. I see how using a transfer matrix in this multilayer case can be useful to compute the energy deposited. If I would define a simulation with 2 temperatures and then add a metal and dielectric layer, I would still be faced with the problem that I have to provide values for the electron thermal conductivity, electron heat conductivity and electron-phonon coupling of the dielectric layer, which are not readily available or defined for dielectrics:
sim = simulation(2, s)
#add layers (Length [m], conductivity [W / cm . K], heatCapacity [J / (m^3 . K^2)], density [kg / m^3], coupling [W/(m^3.K)])
sim.addLayer(200e-9, [317, 1], [lambda Te: 3.6e-3*Te, 129], 19300, 2.2e16) # Au Layer
sim.addLayer(4e-3, [???, 12], [???, 730], 2648, ???) # Quartz layer
With this simulation, I am seeking to get some insight on the evolution of the temperature with respect to depth in the dielectric layer upon excitation of the metal layer.
Finding the physically right input for those parameters is a current topic of research and also one reason why we are interested in this software. Not only to verify results, once parameters are known, but also to test different parameters on this model and check with experimental results. Not specifically for Quarz, but for a range of other materials I can recommend
Electron-phonon coupling and electron heat capacity of metals under conditions of strong electron-phonon nonequilibrium
by Zhibin Lin and Leonid V. Zhigilei in Physical Review Vol 77 (2008)
Note, that the coupling between the two systems is considered to be linear in our model.
Thank you for the reference. I was thinking that maybe a working approach could be to compute the dynamics in the metal layer with a two-temperature model, but to fall back to a single-temperature model in the case of the dielectric.
That would be an excellent idea in principle but can not be easily realized with the current code. You could try to set the coupling constant of the second layer to 0, i.e. the two systems in the second layer will evolve individually. One more thing considering the heat capacity: One approach can be to go to Nist webbook and look for the total heat capacity of Quarz, then subtract the lattice contribution. This should give you a good approximation to the electron heat capacity of Quarz.
Hi, I would like to know whether there is a straightforward way to simulate a multilayer system where a metal thin film (e.g. gold) would be deposited on a dielectric (e.g. glass, quartz). The dynamics of the metal layer are easy solved as a single layer, two-temperature case, but in my understanding, the two-temperature model is not relevant to a large-gap dielectric.