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[Fizinfo] Szemináriumok - Seminars: Thiering Gergő


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  • From: Szeminárium koordinátor <sem-admin AT szfki.hu>
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  • Subject: [Fizinfo] Szemináriumok - Seminars: Thiering Gergő
  • Date: Thu, 6 Mar 2025 06:00:01 +0100 (CET)
  • Authentication-results: smtp012.wigner.hu (amavis); dkim=pass (1024-bit key) reason="pass (just generated, assumed good)" header.d=szfki.hu

Habilitation lectureThiering GergőHUN-REN Wigner RCP SZFIAb-initio theory of
orbital and phonon driven relaxation pathways in quantum defects of
semiconductorsTuesday, 11 March 2025, 10:00, KFKI Campus, Bldg. 1, 2nd floor,
Conference RoomIn the past decades, various crystallographic point defects
were identified in two- and three-dimensional host materials such as diamond,
silicon, silicon carbide, and 2D-boron-nitride. Initially, the
characterization of defects started from the materials science point of view
to unravel and understand their physics in various hosts. However, within the
past decades, new proposed applications have been emerged mainly for quantum
applications [1,2]. However, there are various technological challenges to
overcome for defect-based qubits and quantum emitters that still limit the
defect qubit applications "en masse". Mainly, these challenges are related to
the loss of coherence within qubits which is especially important when the
qubits are entangled together as a solid-state spin register.Therefore, in my
talk I will show various processes [3,4,5,6] that can ultimately lead to
relaxation of electronic orbital "L" states, electronic "S" spin or nuclear
"I" spin degrees of freedom. For example, both the electronic and 14N nuclear
spin of NV(-) (nitrogen vacancy) in diamond are proposed for applications as
NV in general as been both measured extensively and theoretically modelled by
vast number of studies in the past decades [1,2]. We modelled by ab-initio
DFT (density functional theory) calculations that all SDS (zero-field), SAI
(hyperfine) and IPI (quadrupolar) 3×3 tensors acting in |³E⟩ optical excited
upper triplet state of NV are entangled with the 2× orbital degeneracy
("mL=±1") that of |e±⟩ electronic orbitals localized on the defect. In most
studies, ¹⁴N "I" spins are usually treated devoid from any relaxation during
of optical cycles. However, we show [3,4] both experimentally and
theoretically that the traditional "green laser (532-nm)" optical pumping
into the upper |³E⟩ spin triplet excited state leads to additional "ΔmI=±2"
double jump relaxation channels for ¹⁴N via orbital coupling of the
quadrupolar (Q) tensor by means of a "Q₂(L₊²I₋²+L₋²I₊²)"
Hamiltonian.Nevertheless, the lower spin triplet of NV(-) is an orbitally
non-degenerate |³A2⟩ multiplet and thus exempt from orbitally assisted
relaxation. However, phonons of diamond can still relax the electronic spin
via the "spin-phonon" on which we developed [5] an ab-initio framework that
can predict the temperature dependence of rates acting between |mS = 0⟩↔|mS =
+1⟩↔|mS = -1⟩ spin states of NV(-). We find that our ab-initio tools and
experimental measurements depict that two distinct quasilocal phonons centred
at 68.2(17) and 167(12) meV are involved in the relaxation of "S" spin
between the 9-474 K temperature range in high-purity diamond samples.
Additionally, in conjunction with experimental work [6] we develop the key
elements of orbital and spin flipping processes induced by thermal phonons
for the SiV(-) centre of diamond. We find that group theory considerations
and selection rules are crucial to understand the observed anisotropy and
thus we were able to distinguish the strength of pure orbital-phonon
("ΔmL=±2") relaxation and various other weaker diagonal and off-axis
spin-orbit-phonon relaxation pathways. In summary, in the present talk I will
try to depict a general spin-orbit-phonon theory that can be used to model
the processes acting in defect qubits that may highlight the limitations and
caveats of quantum technology applications of point defects in solids. [1]
Wolfowicz, et al. "Quantum guidelines for solid-state spin defects." Nat Rev
Mater 6, 906–925 (2021). [2] I. B. W. Harris and D. Englund, Phys. Rev. B
109, 085414 (2024) [3] R. Monge, T. Delord, G. Thiering, Á. Gali, and C. A.
Meriles, Phys. Rev. Lett. 131, 236901 (2023) [4] G. Thiering, Á. Gali,
arXiv:2402.19418 [quant-ph] (2024) [5] M. Cambria, ... G. Thiering, ... S.
Kolkowitz, Physical Review Letters 130 (25), 256903 (2024) [6] G. Thiering,
A. Gali, F. Jelezko, K Senkalla, F. Frank, B. Koslowski (APS global meeting
2025) https://summit.aps.org/events/MAR-T19/2[6] G. Thiering, A. Gali, F.
Jelezko, K Senkalla, F. Frank, B. Koslowski (APS global meeting 2025)
https://summit.aps.org/events/MAR-T19/2 &nbsp;Minden érdeklődőt szívesen
látunk! - Everyone is welcome to attend.Attila Nagysem-admin AT szfki.hu

  • [Fizinfo] Szemináriumok - Seminars: Thiering Gergő, Szeminárium koordinátor, 03/06/2025

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