Talks

In higher eukaryotic cells, strings of nucleosomes, where long genomic DNA is wrapped around core histones, are irregularly folded into numerous condensed chromatin domains (1,2). Inside these domains, nucleosomes fluctuate and locally behave like a liquid (2,3). While nucleosome behavior is assumed to be highly related to genome functions, it remains unclear how this behavior changes during the cell cycle. During interphase, the nucleus enlarges and genomic DNA doubles. Previous reports have shown that chromatin movements vary during interphase on a minute or longer time-scale. However, using single-nucleosome imaging and tracking (4), we reveal that local nucleosome motion on a second time-scale remains steady throughout the G1, S, and G2 phases in live human cells (4). Combined with Brownian dynamics modeling, our results suggest that this steady-state nucleosome motion is mainly driven by thermal fluctuations. We propose that this observed steady-state nucleosome motion allows cell...

The location of nucleosomes in DNA and their structural stability are critical in regulating DNA compaction, site accessibility, and epigenetic gene regulation. Here, we combine the nanopore platform-based fast and label-free single-molecule detection technique with a voltage-dependent force rupture assay to detect distinct structures on nucleosomal arrays and then to induce breakdown of individual nucleosome complexes. Specifically, we demonstrate direct measurement of distinct nucleosome structures present on individual 12-mer arrays. A detailed event analysis showed that nucleosomes are present as a combination of complete and partial structures, during translocation through the pore. By comparing with the voltage-dependent translocation of the mononucleosomes, we find that the partial nucleosomes result from voltage-dependent structural disintegration of nucleosomes. High signal-to-noise detection of heterogeneous levels in translocation of 12-mer array molecules quantifies the het...

The vast majority (~98%) of the mammalian genome is noncoding but has a vital role in gene regulation. Enhancers are noncoding DNA sequences highly enriched in binding sites for tissue-specific transcription factors. Genes with pleiotropic roles in development often have huge regulatory landscapes (~ 1Mb) with multiple enhancers driving precise gene expression.
The human genome is thought to contain 100s of thousands of enhancers with, as yet, uncharacterised activities and a large proportion of disease-causing and disease-predisposing DNA sequence variants map to potential enhancers. To advance understanding of human disease, massive efforts are currently being directed towards establishing genotype to phenotype correlations for sequence variants. A key pre-requisite to these analyses is defining the precise cell- and tissue-specific activities of the enhancers and the transcription factors that bind them.
Our research focuses on building models for understanding cell-type specific ...

This work investigates the ferroelectric properties of γ − In₂Se₃, a material that uniquely retains its spontaneous polarization at the nano-scale, making it resistant to depolarizing fields. With a direct band gap of 1.8 eV and the ability to switch between insulating and semiconducting phases at room temperature, γ − In₂Se₃ holds promise for next-gen memory devices, where its stable ferroelectricity could revolutionize data storage and processing.

The black hole information paradox is a fundamental conflict between the quantum-mechanical and thermodynamic descriptions of black holes, specifically of their particle-emission process known as the Hawking radiation. The paradox concerns whether the radiation of a black hole is a unitary time evolution or a thermal process that erases most information about the initial state of the black hole. Multiple black hole models (e.g. [1,2]) were shown to exhibit the Page curve behavior, suggesting the unitarity of the Hawking radiation. However, without a verified theory of quantum gravity, the exact structure of black holes remains undetermined, and we need a model-independent way to test black hole unitarity. My project thus aims to develop a general framework for testing black hole unitarity by searching for its physical signatures. In particular, we employ the "hybrid" RST model [3], which possesses a Page-curve behavior, and study whether the unitarity is manifested in the transition rate of the Unruh-DeWitt particle detector. [1] Hong Zhe Chen, Robert C. Myers, Dominik Neuenfeld, Ignacio A. Reyes, Joshua Sandor. Quantum Extremal Islands Made Easy, Part II: Black Holes on the Brane". https://doi.org/10.48550/arXiv.2010.00018. [2] Yohan Potaux, Sergey N. Solodukhin, and Debajyoti Sarkar. "Spacetime Structure, Asymptotic Radiation, and Information Recovery for a Quantum Hybrid State.” Physical Review Letters 130, no. 26 (June 30, 2023): 261501. https://doi.org/10.1103/PhysRevLett.130.261501. [3] Yohan Potaux, Debajyoti Sarkar, and Sergey N. Solodukhin. "Quantum States and Their Back-Reacted Geometries in 2D Dilaton Gravity.” Physical Review D 105, no. 2 (January 12, 2022): 025015. https://doi.org/10.1103/PhysRevD.105.025015.

It may be the case that a spacetime exhibits no asymptotia where gauge invariant observables can be defined in a natural way. On such occasions the introduction of a timeline boundary may be helpful. We therefore discuss the initial boundary value problem in the context of General Relativity.

The theory $S = \int\text{d}^{4-\epsilon}x\left(\frac{1}{2}|\partial\phi|^2 - \frac{m^2}{2}|\phi|^2-\frac{g}{16}|\phi|^4\right)$ exhibits a global $U(1)$ symmetry, and the operators $\phi^n$ ($\bar\phi^n$) have charge $n$ ($-n$) with respect to this symmetry. By rescaling the fields and the coupling constant, it is possible to work in a double limit $n\to\infty$, $g\to 0$ with $\lambda = gn$ kept constant. In this way, it is possible to compute 2-point functions of the form $\langle \phi^n(x) \bar\phi^n(0) \rangle$ in the large $n$ limit, either diagrammatically by a resummation of the leading contribution at all orders in $g$, or using semiclassical methods through the saddle point approximation. This second approach is particularly powerful because it can also be applied to the theory on a curved background. This allows obtaining the form of the 2-point function for an arbitrary metric, and by functionally differentiating with respect to it, it is also possible to obtain, in the flat theory, the 3-point function $\langle T^{ij}(z) \phi^n(x) \bar \phi^n(0) \rangle$ in which an energy-momentum tensor has been inserted. This allows for a non-trivial check of the conformal symmetry of this sector of the theory by verifying the Ward identities that this 3-point function should satisfy.

We discuss the concept of spontaneous symmetry breaking and illustrate it with a general example. We consider Wigner-Weyl and Nambu-Goldstone realisations of symmetry in the quantum theory. Next, we state Goldstone’s theorem and sketch its proof. We discuss why quantum chromodynamics is not realised in the Wigner-Weyl mode.