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Check it out now to nanolux online instruction hello welcome to lecture 5 in the characterization series and week 3 today we are going to talk about laser characterization for thermal conductivity that's an important method for thin films that have been used in the last 10-15 years here is a typical experimental setup and a typical experimental result it's the idea is simple whatever is the film I want to measure its thermal conductivity I can put a transducer a piece of aluminum or another metal that absorbs a fast laser for example 100 times a second laser light is absorbed and then the aluminum heats up and the heat decays here is the change in surface reflection versus time and this surface reflection is proportional to temperature as we saw in previous lecture and the decay you can see it is in this case two different super lattices with different germanium concentration and by just looking at it by RI you can say one of them decays faster than the other and if you feed it with the 48 law you can get a thermal conductivity and in this case is 2.8 vs. 8.1, so this is a technique that has been around for about 20 years or so and the basic idea is the metal film is heated did act as a heat source there are also tiny pics you see in the decay this has to do with the fact this metal as it heats up it creates acoustic wave that propagates inside the materials, so you can measure something about interfaces inside, and even you can measure the thickness of this using this acoustic waves about 10 years ago there was a detailed study of this technique time domain term reflectance that actually told us taught us that we really have much more information in such signal let's see how an experimental setup works I told you a fem laser is policies coming but in reality what you have is often an oscillator that has a frequency on the order of mega Hertz so in this case will be 12 nanosecond repetition rate you have a pump that comes and heat the sample that create the impulse heating and a probe that comes a little later in this case I guess pump is delayed, but it's symmetric you can consider it both ways and probes the surface reflection or temperature data later on often because the change in affliction is a small we need to do lock in and this locking is done in this case by putting a function generator and modulating the pump and this frequency of this modulation could be on the order of point 12 let's say n megahertz and these are parameters that previously when people analyze this decay we're not we're not as prominent but if you really look at what happens in the device here is a graph timing the horizontal axis the power of the impulse pump in this case modulated sinusoidally and the probe is coming a little delay with respect to the pump create a temperature profile that goes up and the decays this is the exponential life decay that I mentioned and the probe takes this curve at a given delay and pull and basically sample it and this is a signal...
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