Lauren B Drescher
@lbdrescher.bsky.social
Researching ultrafast dynamics in solids | Attosecond Physics | MSCActions Fellow | Experimental EUV/XUV shenanigans |📍Berlin | she/her 🏳️🌈🏳️⚧️
I thought the emitted signal gets handled via the Qt message loop? But maybe it does so via the call stack, which is why we reach the limit?
I'll see if moving the method call to a QTimer singleShot might solve this 🤔 3/3
I'll see if moving the method call to a QTimer singleShot might solve this 🤔 3/3
January 6, 2026 at 11:41 AM
I thought the emitted signal gets handled via the Qt message loop? But maybe it does so via the call stack, which is why we reach the limit?
I'll see if moving the method call to a QTimer singleShot might solve this 🤔 3/3
I'll see if moving the method call to a QTimer singleShot might solve this 🤔 3/3
The instance gets handed control (method call), performs the sweep and then emits a signal to the UI to indicate it has finished. The UI then saves the data and obtains a new instance, hands control over etc.
But after some iteration, the max recursion depth is reached.
2/3
But after some iteration, the max recursion depth is reached.
2/3
January 6, 2026 at 11:41 AM
The instance gets handed control (method call), performs the sweep and then emits a signal to the UI to indicate it has finished. The UI then saves the data and obtains a new instance, hands control over etc.
But after some iteration, the max recursion depth is reached.
2/3
But after some iteration, the max recursion depth is reached.
2/3
Continued below! 👇
Let's continue! We want to learn how long it takes light to pull the rug out from under a crystal lattice, or to put it closer to jargon, understand how electronic excitation leads to displacive coherent phonon motion. First, how do we model the interaction of light with solids? /1
I've got a new paper out last week in Phys Rev B! We were wondering how quickly light can pull the rug out from under a crystal lattice (so to speak) and lead it to vibrate. How and why? A lengthy thread below! /1
journals.aps.org/prb/abstract...
journals.aps.org/prb/abstract...
September 16, 2025 at 2:32 PM
Continued below! 👇
We believe we observed this in our paper and we shall finally get to it in the next thread!
September 16, 2025 at 2:31 PM
We believe we observed this in our paper and we shall finally get to it in the next thread!
In the 2010s, it was realized that the force originating from the change in carrier density is different depending on the energy of the carriers. So if the carriers relax and change their energies after their excitation, does that change the phase of the phonon oscillation? /16
Ultrafast Relaxation of Symmetry-Breaking Photo-Induced Atomic Forces
We present a first-principles method for the calculation of the temperature-dependent relaxation of symmetry-breaking atomic driving forces in photoexcited systems. We calculate the phonon-assisted de...
journals.aps.org
September 16, 2025 at 2:31 PM
In the 2010s, it was realized that the force originating from the change in carrier density is different depending on the energy of the carriers. So if the carriers relax and change their energies after their excitation, does that change the phase of the phonon oscillation? /16
So in the rug-pull, we would expect a cosine motion, but if we have an impulsive part, we also get a sine motion. The two added together will imprint a phase on the motion.
Where could this phase come from? /15
Where could this phase come from? /15
September 16, 2025 at 2:31 PM
So in the rug-pull, we would expect a cosine motion, but if we have an impulsive part, we also get a sine motion. The two added together will imprint a phase on the motion.
Where could this phase come from? /15
Where could this phase come from? /15
Now the pendulum will be at the extreme end, start to swing to the center and to the other side and then back. We can describe this this with a cosine-function. Giving the kick is called an impulsive excitation, moving the pendulum (which can be described as adding a constant force) displacive /14
September 16, 2025 at 2:31 PM
Now the pendulum will be at the extreme end, start to swing to the center and to the other side and then back. We can describe this this with a cosine-function. Giving the kick is called an impulsive excitation, moving the pendulum (which can be described as adding a constant force) displacive /14
Let's look at our pendulum again and two ways we can start swinging the pendulum. Give it a kick (short force) from the rest position and it will start swinging left and right. We can describe this with a sine-function. Alternatively, we can move where the pendulum is anchored (pull the rug!). /13
September 16, 2025 at 2:31 PM
Let's look at our pendulum again and two ways we can start swinging the pendulum. Give it a kick (short force) from the rest position and it will start swinging left and right. We can describe this with a sine-function. Alternatively, we can move where the pendulum is anchored (pull the rug!). /13
In the semimetal antimony (Sb), which was one of the materials in the original study, the authors observed a unexplained phase difference of the oscillation with respect to their model, which was attributed to an impulsive component in a paper following. Why is the phase so important? /12
Coherent THz Phonons Driven by Light Pulses and the Sb Problem: What is the Mechanism?
Femtosecond laser pulses generate in Sb coherent ${E}_{g}$ phonons at $\ensuremath{\approx}3.4\mathrm{THz}$, in addition to oscillations of ${A}_{1g}$ symmetry accounted for by the phenomenological di...
journals.aps.org
September 16, 2025 at 2:31 PM
In the semimetal antimony (Sb), which was one of the materials in the original study, the authors observed a unexplained phase difference of the oscillation with respect to their model, which was attributed to an impulsive component in a paper following. Why is the phase so important? /12
They noted that either the temperature of the electrons or the number of excited electrons can be taken as the starting point of the derivation, for which they didn't expect any differences. But if the formation of the temperature of the electrons takes some time, will this cause a difference? /11
September 16, 2025 at 2:31 PM
They noted that either the temperature of the electrons or the number of excited electrons can be taken as the starting point of the derivation, for which they didn't expect any differences. But if the formation of the temperature of the electrons takes some time, will this cause a difference? /11
So, using very fast (ultrafast) time-resolved spectroscopy we can observe the thermalizations of electrons. Does it matter for the rug-pull?
Going back to the paper I mentioned yesterday, there is an interesting detail in the derivation of the model the authors provided /10
Going back to the paper I mentioned yesterday, there is an interesting detail in the derivation of the model the authors provided /10
This was observed in the early 90s, and nicely described in this paper. Using femtosecond lasers, a periodic change of reflectivity in several materials is observed which they connected to the "displacive excitation of coherent phonons" - the rug pull. /15 journals.aps.org/prb/abstract...
Theory for displacive excitation of coherent phonons
We report femtosecond time-resolved pump-probe reflection experiments in semimetals and semiconductors that show large-amplitude oscillations with periods characteristic of lattice vibrations. Only ${...
journals.aps.org
September 16, 2025 at 2:31 PM
So, using very fast (ultrafast) time-resolved spectroscopy we can observe the thermalizations of electrons. Does it matter for the rug-pull?
Going back to the paper I mentioned yesterday, there is an interesting detail in the derivation of the model the authors provided /10
Going back to the paper I mentioned yesterday, there is an interesting detail in the derivation of the model the authors provided /10
In metals, this can be very quick, just a few femtoseconds, as we (and others) recently investigated using a similar technique. /9
Initial electron thermalization in metals measured by attosecond transient absorption spectroscopy
Understanding initial electron thermalization has relevance to both fundamental scientific knowledge and application to the construction of novel devices. In this study, attosecond transient absorptio...
journals.aps.org
September 16, 2025 at 2:31 PM
In metals, this can be very quick, just a few femtoseconds, as we (and others) recently investigated using a similar technique. /9
Luckily, the electrons would very much like to be Fermi-Dirac distributed, since it is the most favorable distribution for them. So they are going to quickly exchange energy between each other and the lattice to reach this distribution. How fast depends on the material, temperature and wavelength /8
September 16, 2025 at 2:31 PM
Luckily, the electrons would very much like to be Fermi-Dirac distributed, since it is the most favorable distribution for them. So they are going to quickly exchange energy between each other and the lattice to reach this distribution. How fast depends on the material, temperature and wavelength /8
Microscopically a temperature describes the distribution of states. For the electrons (Fermions) this is described by the Fermi-Dirac distribution, for the phonons (Bosons) by the Boltzmann distribution. So it's hard to assign a temperature if the particles aren't distributed like that /7
September 16, 2025 at 2:31 PM
Microscopically a temperature describes the distribution of states. For the electrons (Fermions) this is described by the Fermi-Dirac distribution, for the phonons (Bosons) by the Boltzmann distribution. So it's hard to assign a temperature if the particles aren't distributed like that /7
Instead it is transferred via quanta of energy (photons). These photons have a frequency and promote electrons from lower to higher energy levels. The distribution of energy after interaction of light therefor represents the available transitions as well as the frequencies of the light used /6
September 16, 2025 at 2:31 PM
Instead it is transferred via quanta of energy (photons). These photons have a frequency and promote electrons from lower to higher energy levels. The distribution of energy after interaction of light therefor represents the available transitions as well as the frequencies of the light used /6
That is if we are working on picosecond (ps) timescales, if we increase the temporal resolution and look on the femtosecond (fs) scale, we see differences appearing. Why? We can go back to Einstein's photoelectric effect to recall that light doesn't continuously depose energy into the solid /5
September 16, 2025 at 2:31 PM
That is if we are working on picosecond (ps) timescales, if we increase the temporal resolution and look on the femtosecond (fs) scale, we see differences appearing. Why? We can go back to Einstein's photoelectric effect to recall that light doesn't continuously depose energy into the solid /5
If our laser is around the visible wavelengths, it is likely exciting electrons and those move fast than the heat of the lattice. So lets consider this: The laser is heating the electrons which are in turn heating the lattice. This is called the two-temperature model. And it works pretty good /4
September 16, 2025 at 2:31 PM
If our laser is around the visible wavelengths, it is likely exciting electrons and those move fast than the heat of the lattice. So lets consider this: The laser is heating the electrons which are in turn heating the lattice. This is called the two-temperature model. And it works pretty good /4
If the light is absorbed and not re-emitted, ultimately we are going to heat up the solid. This is a good description in the long term, but on shorter timescales isn't suffice and wouldn't explain what we see, it doesn't fit with how heat is spreading following laser absorption. We can do better /3
September 16, 2025 at 2:31 PM
If the light is absorbed and not re-emitted, ultimately we are going to heat up the solid. This is a good description in the long term, but on shorter timescales isn't suffice and wouldn't explain what we see, it doesn't fit with how heat is spreading following laser absorption. We can do better /3
While we could start from first-principles and solve the problem numerically, we probably won't learn much. But we can model something from what we know and start with thermodynamics. What happens if we point a laser beam at a solid? /2
September 16, 2025 at 2:31 PM
While we could start from first-principles and solve the problem numerically, we probably won't learn much. But we can model something from what we know and start with thermodynamics. What happens if we point a laser beam at a solid? /2
However, since their temporal resolution (~60fs) was similar to the period of the phonon vibration oscillations (>125fs) one question lingered: How fast is the rug pulled? Tomorrow, I will continue why this question arose and how we use attosecond transient spectroscopy to find out.
September 15, 2025 at 3:11 PM
However, since their temporal resolution (~60fs) was similar to the period of the phonon vibration oscillations (>125fs) one question lingered: How fast is the rug pulled? Tomorrow, I will continue why this question arose and how we use attosecond transient spectroscopy to find out.
This was observed in the early 90s, and nicely described in this paper. Using femtosecond lasers, a periodic change of reflectivity in several materials is observed which they connected to the "displacive excitation of coherent phonons" - the rug pull. /15 journals.aps.org/prb/abstract...
Theory for displacive excitation of coherent phonons
We report femtosecond time-resolved pump-probe reflection experiments in semimetals and semiconductors that show large-amplitude oscillations with periods characteristic of lattice vibrations. Only ${...
journals.aps.org
September 15, 2025 at 3:11 PM
This was observed in the early 90s, and nicely described in this paper. Using femtosecond lasers, a periodic change of reflectivity in several materials is observed which they connected to the "displacive excitation of coherent phonons" - the rug pull. /15 journals.aps.org/prb/abstract...
As we discussed, they can only move in vibrational modes, so a phonon is created. Since the excitation of the electrons is very fast, this is like moving the rug out from under the ions (and moving it to a new place). They all start moving at the same time, creating a motion that we call coherent/14
September 15, 2025 at 3:11 PM
As we discussed, they can only move in vibrational modes, so a phonon is created. Since the excitation of the electrons is very fast, this is like moving the rug out from under the ions (and moving it to a new place). They all start moving at the same time, creating a motion that we call coherent/14
Now what happens if we increase the energy of our system, eg by hitting it with visible light. This leads to the electrons being promoted to higher levels. Since they now sit at a higher level, there is no reason for the ions not be at their favorite position and they start to move. But... /13
September 15, 2025 at 3:11 PM
Now what happens if we increase the energy of our system, eg by hitting it with visible light. This leads to the electrons being promoted to higher levels. Since they now sit at a higher level, there is no reason for the ions not be at their favorite position and they start to move. But... /13