I have this itch to swing back to talking about physics after yesterdays more meta thread, much like a pendulum always striving towards the middle position, but constantly overshooting. BTW, pendulums are an excellent representation of how short laser pulses are created!
You have probably heard (or learned) that laser light has a very defined colour (one specific wavelength/frequency), and all photons are in phase with each other, all their waves are perfectly synchronised (coherent).
(Image source: miridiatech.com/news/2014/02/l…)
However, if we only allow one single wavelength, then the laser light is continuous. Only when we add up several slightly different wavelengths (or frequencies) do we get a short and intense pulse, right at the moment when all those different waves happen to align with each other
Before and after, when all the different contributions are not perfectly aligned, their individual troths and peaks partially (or completely) compensate each other.
Obeying the laws of the Fourier Transforms, shorter pulses require a broader spectrum. And ultrashort pulses consequently require a very broad spectrum, which means only very few lasing materials can be used to create these.
[rp-photonics.com/titanium_sapph…]
With Ti:sapphire lasers, the pulse duration can be around 5 - 30 femtoseconds (fs). For the attoclock method, this is fine because one rotation of the field is around 2.7 fs, giving attosecond resolution in the angle.
But for most other methods, we need pulses which are themselves shorter than one femtosecond. We are exploiting an effect which is part of strong-field physics: High Harmonic Generation (HHG), which converts infrared photons of a fs pulse into extreme ultraviolet (XUV) photons.
The key components of HHG are beautifully demonstrated in this video by the Photonics and Laser Applications Group of University of Salamanca, and JILA, University of Colorado
In my own research, I have 1⃣ looked into phase-matching: How coherent are the different XUV photons which are being emitted by all the recombining electrons distributed in the gas cloud?
and 2⃣ also played around with: what happens if the laser field is a mix of two very different frequencies creating a fancy pattern? And if additionally, you have nano-particles nearby, creating a spatial dependence in the laser field?
(second image: doi.org/10.1103/PhysRe…)
(yes, this is me actually talking about something nano finally 😉)
The three-fold symmetry is imprinted onto the typical paths that electrons are taking (first image). But with the spatial dependence on top, that symmetry is completely broken (second image), and the energies with which these electrons are recombining are vastly different.
1. LASER = Light Amplification by Stimulated Emission of Radiation (a) 2. Electron 3. Excited state atom 4. A Photon (I don't think there is a lasing material capable of producing gamma range photons) 5. Diffuse 6. Population Inversion
7. 3 Levels (with just 2 levels, as one approaches population equality, stimulated emission and absorption would start balancing each other out, preventing population inversion and thus there is no amplification of the light) 8. b) The energy gap between excited and ground state
Happy Sunday everyone!
It has been an adventurous week (in many ways 😁).
I recently came across this fun little #laser quiz and thought that would be a nice conclusion to my week here. So take a guess and play along 🤗
1. What does LASER stand for?
a) Light Amplification by Stimulated Emission of Radiation
b) Light Absorption by Simulated Emission of Radiation
c) Latent Absorption of Specified Elliptical Radons
d) Latent Amplification of Stimulated and Elliptical Radons
2. What particle plays the major role in the process of lasing?
Hi everyone :-D
We have reached the weekend already. Over the last few days, I hope I managed to give you a small glimpse into my research field. But one promise I have not yet delivered on: Where will all of this lead? What's the point?
First of all, I don't think I have to convince you that the quantum tunnelling phenomenon is found in all kinds of fields. Recently I came across a paper discussing tunnelling times during a photosynthesis cycle in an organic molecule. doi.org/10.1007/s13538…
Many might be familiar with Scanning Tunnelling Microscope (STM) technique to investigate surface structures with (sub-)atomic spatial resolution (or make an atomic stop-motion movie 😄)
It is evening again, and I finally find a moment to check in here. How are you doing?
I feel like my apartment has turned into a bit of a "sauna for beginners": higher room temperature than I would usually keep in wintertime, and more humid than usual in general (despite having open windows)...
I'm going to switch my plan around a bit. The exciting opportunities for future scientific and technological developments derived from #attoscience (and if I find the time, a project using nano-objects to modify the spatial dependence of my laser fields) will come later.
Good evening! While my fan heater is doing its job, why don't we catch some electrons?
In yesterday's thread, the electrons which have been freed from their bound state by the laser mostly just oscillated around (steered by the electric field) and eventually flew off and away (until they hit a detector).
However, not all electrons are so lucky. For some of them, their trajectory ends up looking almost like that lasso up there. This is if their kinetic energy at the end of the laser pulse is not quite enough to escape from the Coulomb potential of the atom/ion.
Hello everyone!
To talk about my research, I decided to theme it by "studying the ionisation process itself" (today) and "possible things that can happen afterwards" (tomorrow).
I'm going to keep the explanations in the threads fairly colloquial. But I will link the corresponding publications (open access whenever possible) so you can dig into the details there if you wish. Or of course, just ask me any questions you might have and I'll expand on that 😉
Yesterday I have already introduced the idea that the strong electric field of the laser pulse modifies the Coulomb potential which keeps electrons in bound states. The video shows a classical picture of this: