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# [[Vladislav Shishkov|Владислав Шишков (Vladislav Shishkov)]] - [[Aalto University]], [[Espoo]] | # [[Vladislav Shishkov|Владислав Шишков (Vladislav Shishkov)]] - [[Aalto University]], [[Espoo]] | ||
# [[Juan Camilo López Carreño]] - [[University of Warsaw]], [[Warsaw]] | # [[Juan Camilo López Carreño]] - [[University of Warsaw]], [[Warsaw]] | ||
# [[Yajun Wang]] - [[Shanxi University]], [[ | # [[Yajun Wang|王雅君 (Yajun Wang)]] - [[Shanxi University]], [[Taiyuan]] | ||
# [[Alexandros Spiliotis]] - [[IESL-FORTH]], [[Heraklion]] | # [[Alexandros Spiliotis]] - [[IESL-FORTH]], [[Heraklion]] | ||
# [[Natalia Armaou]] - [[Westlake University]], [[ | # [[Natalia Armaou]] - [[Westlake University]], [[Hangzhou]] | ||
# [[Moritz Meinecke]] - [[University of Würzburg]], [[Würzburg]] | # [[Moritz Meinecke]] - [[University of Würzburg]], [[Würzburg]] | ||
# [[Carlos Antón Solanas]] - {{uam}} | # [[Carlos Antón Solanas]] - {{uam}} | ||
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===== Serge Reynaud ===== | ===== Serge Reynaud ===== | ||
9:00-9:30 | ''Quantum jumps in single-atom resonance fluorescence'' — 9:00-9:30 | ||
:Quantum jumps have been part of the theoretical understanding of interaction processes between atoms and photons since early quantum theory. They play a key role in the description of emission of photons by a single atom excited by a laser tuned near resonance. I will discuss quantum jumps in this resonance fluorescence process for a single two-level atom (with broadband detection).{{cite|reynaud23a}} | |||
===== Kai Müller ===== | ===== Kai Müller ===== | ||
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===== Ahsan Nazir ===== | ===== Ahsan Nazir ===== | ||
12:30-13:00 | ''A Markovian approach to $N$-photon correlations beyond the quantum regression theorem'' — 12:30-13:00 | ||
:We introduce a Markovian framework for computing $N$-photon frequency-resolved correlation functions of quantum emitters in vibrational environments, overcoming the limitations of the quantum regression theorem (QRT). Applying our approach to a driven semiconductor quantum dot renders the investigation of the phonon impact on dot fluorescence tractable beyond the single-photon spectrum. Our method accurately captures the emergence of the phonon sideband—missed by conventional QRT treatments—and reveals rich phonon-induced structure in the filtered two-photon spectrum. Surprisingly, we find that photons emitted via the phonon sideband inherit the second-order coherence properties of the Mollow triplet. | |||
===== Владислав Шишков ===== | ===== Владислав Шишков ===== | ||
''Spectral theory and statistical properties of integrated single-photon sources.'' — 13:00-13:30 | ''Spectral theory and statistical properties of integrated single-photon sources.'' — 13:00-13:30 | ||
:Single-photon light sources are microscopic objects with sizes much smaller than the wavelength of the light they emit. Due to their small sizes, such emitters have a wide emission pattern, requiring special approaches to integrate them into photonic circuits. One of the most common approaches for a single-photon source integration into a photonic integrated circuit is coupling via a resonator in the large Purcell factor regime. This integration method, however, leads to a change in the statistical properties of the resulting light. Indeed, a resonator acts as a spectral filter that distorts the spectrum of the light and, thus, changes its statistical properties. We analyse the applicability of the spectral filtering theory for determining the statistical properties of light emitted by a single-photon source coupled to photonic integrated circuits via resonators in the large Purcell factor regime. | |||
'''''Lunch''''' at | '''''Lunch''''' at | ||
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==== Evening Session <!-- Kai/Eduardo-->==== | ==== Evening Session <!-- Kai/Eduardo-->==== | ||
===== Jake Iles-Smith ===== | ===== Jake Iles-Smith ===== | ||
17:30-18:00 | ''Beyond the Quantum Regression Theorem: Tensor Network Methods for Solid-State Quantum Optics'' — 17:30-18:00 | ||
: Correlation functions are a fundamental theoretical tool in quantum optics; they are used to calculate emission spectra, photon coherence properties, and to assess how well a quantum emitter will operate within a quantum technology. However, calculating these quantities is not always straightforward. While the quantum regression theorem can describe the emission properties of isolated atomic systems, it fails in solid-state environments, where strong coupling to the surrounding lattice leaves crucial features of the optical response unaccounted for. | |||
:In this talk, I will introduce a new family of methods for computing multi-time correlation functions of quantum emitters beyond atomic systems. By combining the process tensor formalism with tensor networks, these techniques provide a numerically exact framework for extracting the emission characteristics of solid-state emitters. I will illustrate their use in quantifying how electron–phonon interactions shape optical coherence, considering both localized and bulk phonon modes. Finally, I will show how these tools can be applied to place rigorous bounds on the indistinguishability and efficiency of quantum emitters in low-dimensional materials, including quantum dots in transition metal dichalcogenides (e.g. WSe₂) and atomic defects in hexagonal boron nitride. | |||
===== Antonio Isaac Fernandez Dominguez ===== | ===== Antonio Isaac Fernandez Dominguez ===== | ||
18:00-18:30 | 18:00-18:30 | ||
===== Yajun Wang ===== | ===== Yajun Wang (王雅君) ===== | ||
18:30-19:00 | ''Squeezed light and lasing'' — 18:30-19:00 | ||
:We focused on the study of technical and quantum noises of a laser source in interferometry. Recently, we have solved the key scientific and technical problems of laser noise characterization and stabilization beyond the quantum noise limit, explored the physical root of noise sources, and developed the key technologies of laser technical and quantum noises stabilization.<ref><u>Quantum-enhanced laser phase noise filter</u>. [[R. Li]], [[N. Jiao]], [[B. An]], [[Y. Wang]], [[S. Shi]], [[L. Tian]], [[W. Li]], [[Y. Zheng]]. {{arXiv|2507.05771}}.<br> <u>Bright squeezed light in the kilohertz frequency band</u>. [[R. Li]], [[B. An]], | |||
[[N. Jiao]], [[J. Liu]], [[L. Chen]], [[Y. Wang]], [[Y. Zheng]]. | |||
{{arXiv|2504.00627}}, to appear in [[LSA|Light: Science & Applications]].</ref> Especially, we have experimentally stimulated a squeezed lasing in the reservoir-engineered optical parametric oscillator (OPO).{{cite|tian25a}} It successfully circumvents the decoherence in the system, and eliminates the undesired noise of spontaneous photon emission in the OPO. As a result, the amplified parametric process simultaneously reserves the coherence and quantum properties in the OPO, and yields a -6.1 dB squeezed laser in optical domain with a 15 kHz linewidth and 2.6 mW optical power. | |||
<dl><dd> | |||
<div class="mw-collapsible mw-collapsed" data-expandtext="Show Figure" data-collapsetext="Hide"> | |||
<center><wz tip="">[[File:Screenshot_20250904_121940.png|480px]]</wz></center> | |||
<div style="width: 480px; margin: 0 auto; font-size: 0.9em; text-align: aligned;">Physical mechanism of the parametric coupling with vacuum or squeezed vacuum reservoir. (a) Parametric down-conversion (PDC) in an above threshold OPO. (b) Mixture of two coherent states with coherence preservation and quantum characteristic deterioration. (c) PDC in a subthreshold OPO. (d) Squeezed vacuum state with quantum characteristic preservation and coherence deterioration. (e) PDC in a subthreshold OPO with squeezing vacuum reservoir. (f) Squeezed lasing with coherence and quantum characteristic preservation.</div> | |||
</div> | |||
</dd></dl> | |||
===== Carlos Sánchez ===== | ===== Carlos Sánchez ===== | ||
19:00-19:30 | ''Quantum metrology through spectral measurements in quantum optics'' — 19:00-19:30 | ||
: A central challenge in quantum metrology from open quantum optical systems is to identify measurement strategies that optimally extract information encoded in the complex quantum state of emitted radiation. Different measurement strategies effectively access distinct temporal modes of the emitted field, and the resulting choice of mode can strongly impact the information available for parameter estimation. While a ubiquitous approach in quantum optics is to select frequency modes through spectral filtering, the metrological potential of this technique has not yet been systematically quantified. We develop a theoretical framework to assess this potential by modeling spectral detection as a cascaded quantum system, allowing us to reconstruct the full density matrix of frequency-filtered photonic modes and to compute their associated Fisher information. We show how this approach allows us to identify optimal filtering strategies for metrology, in terms of frequency selection, detector linewidth, and metrological gain accessible through multiphoton frequency-resolved correlations and mean-field engineering. | |||
20:30 ''''' Dinner ''''' | 20:30 ''''' Dinner ''''' | ||
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===== Alejandro González Tudela ===== | ===== Alejandro González Tudela ===== | ||
12:35-13:05 | ''Controlling propagating photons with chiral, multi-mode waveguide QED | ||
'' — 12:35-13:05 | |||
:Controlling propagating quantum states of light is essential for the development of photonic quantum technologies. In this talk, I will first review how qualitatively new photon-mediated interactions emerge when emitters or resonators couple to chiral, multi-mode waveguides.<ref><u>Topological, multi-mode amplification induced by non-reciprocal, long-range dissipative couplings</u>, [[C. Vega]], [[A.M. Heras]], [[D. Porras]], [[A. González-Tudela]], {{arXiv|2405.10176}}.</ref> I will then show how these interactions enable the implementation of controlled photon-photon phase gates using only two-level systems.{{cite|levyyeyati25a}} In both cases, I will discuss potential implementations in the microwave using circuit QED setups. | |||
'''''Lunch''''' | '''''Lunch''''' | ||
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Participants depart | Participants depart | ||
== Friday 10 October (After) == | |||
Prof. [[S. Reynaud]] will also give an [[INC]] ([https://www.inc.uam.es/ Instituto Nicolás Cabrera]) Colloquium, {{onlinequote|Vacuum fluctuations and Casimir forces}}, at 12:00 in the seminar room of Module 4, Faculty of Sciences (01.04.SS.500). All details can be found [https://www.uam.es/ciencias/facultad/eventos/colloquium-serge-reynaud in this page]. | |||
== Q&A(bstracts) == | == Q&A(bstracts) == | ||
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== One picture is worth a thousand words == | == One picture is worth a thousand words == | ||
[[File:Screenshot_20250903_171405.png|thumb|120px|right]] | [[File:Screenshot_20250903_171405.png|thumb|120px|right]] | ||
For the [[Multiphotonics (2024)]], each participant contributed a formula, meaningful and/or inspiring for them, characteristic of their contribution to the field or merely illustrating their talk. Interestingly, there was no degeneracy: [[Rempe]] provided the [[Jaynes-Cummings Hamiltonian]], someone went for the mere harmonic oscillator (but wasn't [[Dirac]] saying it was enough to understand this?), {{I}} (Fabrice) offered the dissipative Jaynes-Cumming ladder formula, which I still haven't found in any publication earlier to mine{{cite|laussy12e}} | For the [[Multiphotonics (2024)]], each participant contributed a formula, meaningful and/or inspiring for them, characteristic of their contribution to the field or merely illustrating their talk. Interestingly, there was no degeneracy: [[Rempe]] provided the [[Jaynes-Cummings Hamiltonian]], someone went for the mere harmonic oscillator (but wasn't [[Dirac]] saying it was enough to understand this?), {{I}} (Fabrice) offered the dissipative Jaynes-Cumming ladder formula, which I still haven't found in any publication earlier to mine,{{cite|laussy12e}} [[Eduardo]] provided the two-photon spectrum of resonance fluorescence, which produces the logo of the meeting. It was a nice way to make a logo. | ||
For this edition, we'd like to try the same thing but with a figure instead of a formula. This could be a graph, a density plot, the sketch of a concept (artistic or scientific), a diagram, the setup of an experiment, etc., with the same intent of providing a picture—call that a vision if you like—to illustrate the participants' understanding of the topic, ideally with a connection to their talk, even if a remote one. Out of this medley of visual cues to what light-matter interactions is about, we will build the logo of the 2025 meeting. | For this edition, we'd like to try the same thing but with a figure instead of a formula. This could be a graph, a density plot, the sketch of a concept (artistic or scientific), a diagram, the setup of an experiment, etc., with the same intent of providing a picture—call that a vision if you like—to illustrate the participants' understanding of the topic, ideally with a connection to their talk, even if a remote one. Out of this medley of visual cues to what light-matter interactions is about, we will build the logo of the 2025 meeting. | ||
The second MULTIPHOTONICS meeting will take place in Madrid, on 8–9 October (2025) with the support of ICMM—CSIC and IFF—CSIC. It follows the very successful MULTIPHOTONICS (2024) first edition. The workshop will likewise discuss the physics of multiphoton correlations.
If you liked Munich, you'll love Madrid!
Multiphoton generation: Single and $N$-photon emission.
Quantum light generation with properties such as entanglement or squeezing.
Frequency filtering, statistics, coherence and correlation measurements.
Quantum optics, cavity-QED, light-matter interaction and nanophotonics.
ICMM-CSIC on the Cantoblanco Campus:
External attendants will be provided with a two-nights (Tue 7 & Wed 9) hotel room with breakfast at the VP Jardín De Tres Cantos in Tres Cantos. This is a quiet, modern urban-planning city at the north of Madrid, well connected to the site of the meeting and to the Spanish capital itself.
The event is supported by a joint ICMM‒IFF effort:
Participants arrive.
8:50-9:00
Quantum jumps in single-atom resonance fluorescence — 9:00-9:30
Unlocking multiphoton emission from a single-photon source through mean-field engineering — 9:30-10:00
10:00-10:30
10:30-11:00
Coffee break
Quantum noise and squeezing in nanolasers. — 11:30-12:00
12:00-12:30
A Markovian approach to $N$-photon correlations beyond the quantum regression theorem — 12:30-13:00
Spectral theory and statistical properties of integrated single-photon sources. — 13:00-13:30
Lunch at El Goloso — 13:30-15:00
Group photo
Tailoring photon statistics with an atom-based two-photon interferometer — 15:00-15:30
Based on Ref. [5].
15:30-16:00
16:00-16:30
16:30-17:00
Coffee break
Beyond the Quantum Regression Theorem: Tensor Network Methods for Solid-State Quantum Optics — 17:30-18:00
18:00-18:30
Squeezed light and lasing — 18:30-19:00
Quantum metrology through spectral measurements in quantum optics — 19:00-19:30
20:30 Dinner
9:00-9:30
9:30-9:50
Higher-order Fock states for sensing applications. — 9:50-10:20
See Ref. [8].
10:20-10:50
Coffee break
11:15-11:45
11:45-12:15
12:15-12:35
Controlling propagating photons with chiral, multi-mode waveguide QED — 12:35-13:05
Lunch
Tailoring spatial correlations with structured light — 14:00-14:30
14:30-15:00
Spatial correlations of opposite OAM states of light — 15:00-15:20
Liquid time and time liquids — 15:20-15:50
Goodbye coffee & Merienda
Participants depart
Prof. S. Reynaud will also give an INC (Instituto Nicolás Cabrera) Colloquium, «Vacuum fluctuations and Casimir forces», at 12:00 in the seminar room of Module 4, Faculty of Sciences (01.04.SS.500). All details can be found in this page.
At this occasion, we shall try to revive an old format of archiving Scientific debates: instead of publishing proceedings, we will publish the abstract and the (edited) Questions & Answers sessions, which contains information nowhere else to be found.

For the Multiphotonics (2024), each participant contributed a formula, meaningful and/or inspiring for them, characteristic of their contribution to the field or merely illustrating their talk. Interestingly, there was no degeneracy: Rempe provided the Jaynes-Cummings Hamiltonian, someone went for the mere harmonic oscillator (but wasn't Dirac saying it was enough to understand this?), I (Fabrice) offered the dissipative Jaynes-Cumming ladder formula, which I still haven't found in any publication earlier to mine,[17] Eduardo provided the two-photon spectrum of resonance fluorescence, which produces the logo of the meeting. It was a nice way to make a logo.
For this edition, we'd like to try the same thing but with a figure instead of a formula. This could be a graph, a density plot, the sketch of a concept (artistic or scientific), a diagram, the setup of an experiment, etc., with the same intent of providing a picture—call that a vision if you like—to illustrate the participants' understanding of the topic, ideally with a connection to their talk, even if a remote one. Out of this medley of visual cues to what light-matter interactions is about, we will build the logo of the 2025 meeting.