Болдырев Алексей Сергеевич
Факультет компьютерных наук
Профессиональные интересы
Должности
- Научный сотрудник — Факультет компьютерных наук, Институт искусственного интеллекта и цифровых наук, Научно-учебная лаборатория методов анализа больших данных
- Доцент — Факультет компьютерных наук, Департамент больших данных и информационного поиска
- Приглашенный преподаватель — НИУ ВШЭ в Нижнем Новгороде, Факультет менеджмента, Департамент маркетинга и предпринимательства
Био
- · Начал работать в НИУ ВШЭ в 2018 году.
- · Научно-педагогический стаж: 13 лет.
Образование
- 2013 · Кандидат физико-математических наук
- 2010 · Специалитет: Московский государственный университет им. М.В. Ломоносова, специальность «Физика атомного ядра и частиц», квалификация «Физик»
Опыт работы
- · 2020: Научный сотрудник Научно-учебной лаборатории методов анализа больших данных НИУ ВШЭ ( настоящее время)
- · 2020: Доцент Департамента больших данных и информационного поиска ( настоящее время) Постдок НИУ ВШЭ (2018–2020) Старший научный сотрудник Института ядерной физики им. Д.В. Скобельцына, МГУ им. М.В. Ломоносова (2017–2018)
- · Младший научный сотрудник Физического института им. П.Н. Лебедева РАН (2006-2017) Научный сотрудник Института ядерной физики им. Д.В. Скобельцына МГУ им. М.В. Ломоносова (2016) Стипендия TRIL, Международный центр теоретической физики Абдуса Салама (ICTP) (2015–2016) Научный сотрудник Института ядерной физики им. Д.В. Скобельцына МГУ им. М.В. Ломоносова (2014–2015)
Награды и поощрения
- · Благодарность НИУ ВШЭ (май 2024)
- · Благодарственное письмо проректора НИУ ВШЭ (сентябрь 2022)
- · Надбавка за публикацию в журнале из Списка А (и приравненном к нему научном издании) (2023–2024)
- · Надбавка за публикацию в международном рецензируемом научном издании (2022–2023, 2021–2022, 2020–2022)
- · Надбавка за регулярные публикации в международных рецензируемых научных изданиях (2024–2029)
Гранты и проекты
- — · Факультет компьютерных наук НИУ ВШЭ, Сколтех и Физический институт им. П. Н. Лебедева РАН провели Московскую международную школу физики 2024
Конференции (3)
Показать все
- · 2022: Second MODE Workshop on Differentiable Programming for Experiment Design (Колумбари, Крит). Доклад: LHCb ECAL optimization
- · 2021: First MODE Workshop on Differentiable Programming (Лувэн-ла-Нёв). Доклад: Optimization of LHCb calorimeter
- · 2020: Instrumentation for Colliding Beam Physics (Новосибирск). Доклад: ML-assisted versatile approach to Calorimeter R&D
Идентификаторы исследователя
- ORCID:
0000-0002-7872-6819 - ResearcherID:
K-6303-2012 - SPIN РИНЦ:
2497-2125 - Google Scholar: https://scholar.google.ru/citations?&user=VD-s9u4AAAAJ&hl=en
- Scopus AuthorID:
35222997400
Публикации (274)
Progress in end-to-end optimization of fundamental physics experimental apparata with differentiable programming
2025 · ARTICLE · en
In this article we examine recent developments in the research area concerning the creation of end-to-end models for the complete optimization of measuring instruments. The models we consider rely on differentiable programming methods and on the specification of a software pipeline including all factors impacting performance — from the data-generating processes to their reconstruction and the inference on the parameters of interest — along with the careful specification of a utility function well aligned with the end goals of the experiment. Building on previous studies originated within the MODE Collaboration, we focus specifically on applications involving instruments for particle physics experimentation, as well as industrial and medical applications that share the detection of radiation as their data-generating mechanism. This report illustrates the most recent advancements in the area, and outlines, for each of the discussed applications as well as for automatic differentiation itself, ongoing and future work.
An Approach to Finding a Robust Deep Learning Model
2025 · ARTICLE · en
The rapid development of machine learning (ML) and artificial intelligence (AI) applications requires the training of a large numbers of models. This growing demand highlights the importance of training models without human supervision, while ensuring that their predictions are reliable. In response to this need, we propose a novel approach for determining model robustness. This approach, supplemented with a model selection algorithm designed as a meta-algorithm, is versatile and applicable to any machine learning model, provided that it is appropriate for the task at hand. This study demonstrates the application of our approach to evaluate the robustness of deep learning models. To this end, we study small models composed of a few convolutional and fully connected layers, using common optimizers because of their ease of interpretation and computational efficiency. We address the influence of training sample size, model weight initialization, and inductive bias on the robustness of deep learning models.
Branching fraction measurement of the decay 𝐵+ →𝜓(2𝑆)𝜙(1020)𝐾+
2025 · ARTICLE · en
The branching fraction of the decay 𝐵+ →𝜓(2𝑆)𝜙(1020)𝐾+, relative to the topologically similar decay 𝐵+ →𝐽/𝜓𝜙(1020)𝐾+, is measured using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8, and 13 TeV, corresponding to an integrated luminosity of 9 fb−1. The ratio is found to be 0.061 ±0.004 ±0.009, where the first uncertainty is statistical and the second systematic. Using the world-average branching fraction for 𝐵+ →𝐽/𝜓𝜙(1020)𝐾+, the branching fraction for the decay 𝐵+ →𝜓(2𝑆)𝜙(1020)𝐾+ is found to be (3.0 ±0.2 ±0.5 ±0.2) ×10−6, where the first uncertainty is statistical, the second systematic, and the third is due to the branching fraction of the normalization channel.
Angular analysis of B0 → K*0e+e− decays
2025 · ARTICLE · en
An angular analysis of B0 → K*0e+e− decays is presented using proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of 9 fb−1. The analysis is performed in the region of the dilepton invariant mass squared of 1.1–6.0 GeV2/c4. In addition, a test of lepton flavour universality is performed by comparing the obtained angular observables with those measured in B0 → K*0μ+μ− decays. In general, the angular observables are found to be consistent with the Standard Model expectations as well as with global analyses of other b → sℓ+ℓ− processes, where ℓ is either a muon or an electron. No sign of lepton-flavour-violating effects is observed.
Search for resonance-enhanced 𝐶𝑃 and angular asymmetries in the Λ+𝑐 →𝑝𝜇+𝜇− decay at LHCb
2025 · ARTICLE · en
The first measurement of the 𝐶𝑃 asymmetry of the decay rate (𝐴𝐶𝑃) and the 𝐶𝑃 average (Σ𝐴FB) and 𝐶𝑃 asymmetry (Δ𝐴FB) of the forward-backward asymmetry in the muon system of Λ+𝑐 →𝑝𝜇+𝜇− decays is reported. The measurement is performed using a data sample of proton-proton collisions, recorded by the LHCb experiment from 2016 to 2018 at a center-of-mass energy of 13 TeV, which corresponds to an integrated luminosity of 5.4 fb−1. The asymmetries are measured in two regions of dimuon mass near the 𝜙-meson mass peak. The dimuon-mass integrated results are 𝐴𝐶𝑃 =(−1.1 ±4.0 ±0.5)%, Σ𝐴FB =(3.9 ±4.0 ±0.6)%, Δ𝐴FB =(3.1 ±4.0 ±0.4)%, where the first uncertainty is statistical and the second systematic. The results are consistent with the conservation of 𝐶𝑃 symmetry and the Standard Model expectations.
Evidence for 𝐵− →𝐷**0𝜏−𝜈_𝜏 Decays
2025 · ARTICLE · en
The first evidence for the decay 𝐵−→𝐷**0𝜏−‾𝜈𝜏 is obtained using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb−1, at centre-of-mass energies of 7, 8, and 13 TeV. Here, the 𝐷**0 meson represents any of the three excited charm mesons 𝐷1(2420)0, 𝐷*2(2460)0, and 𝐷′1(2400)0. The 𝐵− →𝐷**0𝜏−¯𝜈𝜏 signal is measured with a significance of 3.5𝜎, including systematic uncertainties. The combined branching fraction ℬ(𝐵−→𝐷**01,2𝜏−¯𝜈𝜏)×ℬ(𝐷**01,2→𝐷*+𝜋−), where 𝐷**01,2 denotes both 𝐷1(2420)0 and 𝐷*2(2460)0 contributions, is measured to be [0.051±0.013(stat)±0.006(syst)±0.009(ext)]%, where the last uncertainty reflects that of the branching fraction of the normalization channel 𝐵− →𝐷**01,2𝐷−𝑠(*). The ratio between the tauonic and muonic semileptonic 𝐵 decays, with the latter taken from world average values, is also determined and found to be ℛ(𝐷**01,2)=0.13±0.03(stat)±0.01(syst)±0.02(ext).
Measurement of the multiplicity dependence of Υ production ratios in pp collisions at sqrt(s) = 13 TeV
2025 · ARTICLE · en
The Υ(2S) and Υ(3S) production cross-sections are measured relative to that of the Υ(1S) meson, as a function of charged-particle multiplicity in proton-proton collisions at a centre-of-mass energy of 13 TeV. The measurement uses data collected by the LHCb experiment in 2018 corresponding to an integrated luminosity of 2 fb−1. Both the Υ(2S)-to-Υ(1S) and Υ(3S)-to-Υ(1S) cross-section ratios are found to decrease significantly as a function of event multiplicity, with the Υ(3S)-to-Υ(1S) ratio showing a steeper decline towards high multiplicity. This hierarchy is qualitatively consistent with the comover model predictions, indicating that final-state interactions play an important role in bottomonia production in high-multiplicity events.
Search for charge-parity violation in semileptonically tagged D0 → K+π− decays
2025 · ARTICLE · en
An analysis of the flavour oscillations of the charmed neutral meson is presented. The ratio of D0 → K+π− and D0 → K−π+ decay rates is measured as a function of the decay time of the D0 meson and compared with the charge-conjugated system to search for charge-parity violation. The meson flavour at production is double-tagged by the charges of the muon and pion in the preceding and D∗(2010)+ → D0π+ decays, respectively. These decays are selected from proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 5.4 fb−1. The flavour oscillation parameters, relating to the differences in mass and width of the mass eigenstates, are found to be y′ = (5.8 ± 1.6) × 10−3 and (x′)2 = (0.0 ± 1.2) × 10−4. No evidence for charge-parity violation is seen either in the flavour oscillations or in the decay, where the direct charge-parity asymmetry is measured to be AD = (2.3 ± 1.7) %.
Study of light-meson resonances decaying to 𝐾0S𝐾𝜋 in the 𝐵 →(𝐾0S𝐾𝜋)𝐾 channels
2025 · ARTICLE · en
A study is presented of 𝐵+ →𝐾0S𝐾−𝜋+𝐾+ and 𝐵+ →𝐾0S𝐾+𝜋−𝐾+ decays based on the analysis of proton-proton collision data collected with the LHCb detector at center-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of 9 fb−1. The 𝐾0S𝐾𝜋 invariant-mass distributions of both 𝐵+ decay modes show, in the 𝑚(𝐾0S𝐾𝜋)
Measurement of CP asymmetry in B0s→D∓sK± decays
2025 · ARTICLE · en
A measurement of the CP-violating parameters in B0s→D∓sK± decays is reported, based on the analysis of proton-proton collision data collected by the LHCb experiment corresponding to an integrated luminosity of 6fb−1 at a centre-of-mass energy of 13TeV. The measured parameters are obtained with a decay-time dependent analysis yielding Cf=0.791±0.061±0.022, AΔΓf=−0.051±0.134±0.058, AΔΓf⎯⎯⎯=−0.303±0.125±0.055, Sf=−0.571±0.084±0.023 and Sf⎯⎯⎯=−0.503±0.084±0.025, where the first uncertainty is statistical and the second systematic. This corresponds to CP violation in the interference between mixing and decay of about 8.6σ. Together with the value of the Bs mixing phase −2βs, these parameters are used to obtain a measurement of the CKM angle γ equal to (74±12)∘ modulo 180∘, where the uncertainty contains both statistical and systematic contributions. This result is combined with the previous LHCb measurement in this channel using 3fb−1 resulting in a determination of γ=(81+12−11)∘.
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