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M. Goncharov

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DOI: 10.1103/physrevlett.88.091802
2002
Cited 520 times
Precise Determination of Electroweak Parameters in Neutrino-Nucleon Scattering
The NuTeV Collaboration has extracted the electroweak parameter sin(2)theta(W) from the measurement of the ratios of neutral current to charged current nu and (-)nu cross sections. Our value, sin(2)theta((on-shell))(W) = 0.2277 +/- 0.0013(stat) +/- 0.0009(syst), is 3 standard deviations above the standard model prediction. We also present a model independent analysis of the same data in terms of neutral-current quark couplings.
DOI: 10.1103/physrevd.64.112006
2001
Cited 217 times
Precise measurement of dimuon production cross sections in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi mathvariant="normal">Fe</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mover><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:…
We present measurements of the semi-inclusive cross sections for νμ- and ν¯μ-nucleon deep inelastic scattering interactions with two oppositely charged muons in the final state. These events dominantly arise from the production of a charm quark during the scattering process. The measurement was obtained from the analysis of 5102 νμ-induced and 1458 ν¯μ-induced events collected with the NuTeV detector exposed to a sign-selected beam at the Fermilab Tevatron. We also extract a cross-section measurement from a reanalysis of 5030 νμ-induced and 1060 ν¯μ-induced events collected from the exposure of the same detector to a quad-triplet beam by the Chicago Columbia Fermilab Rochester (CCFR) experiment. The results are combined to obtain the most statistically precise measurement of neutrino-induced dimuon production cross sections to date. These measurements should be of broad use to phenomenologists interested in the dynamics of charm production, the strangeness content of the nucleon, and the Cabibbo-Kobayashi-Maskawa matrix element Vcd. Received 21 February 2001DOI:https://doi.org/10.1103/PhysRevD.64.112006©2001 American Physical Society
DOI: 10.1103/physrevd.74.012008
2006
Cited 155 times
Precise measurement of neutrino and antineutrino differential cross sections
The NuTeV experiment at Fermilab has obtained a unique high statistics sample of neutrino and anti-neutrino interactions using its high-energy sign-selected beam. We present a measurement of the differential cross section for charged-current neutrino and anti-neutrino scattering from iron. Structure functions, F_2(x,Q^2) and xF_3(x,Q^2), are determined by fitting the inelasticity, y, dependence of the cross sections. This measurement has significantly improved systematic precision as a consequence of more precise understanding of hadron and muon energy scales.
DOI: 10.1103/physrevlett.83.4943
1999
Cited 136 times
Search for Neutral Heavy Leptons in a High-Energy Neutrino Beam
A search for neutral heavy leptons (NHLs) has been performed using an instrumented decay channel at the NuTeV (E-815) experiment at Fermilab. The data were examined for NHLs decaying into muonic final states ( μμν, μeν, μπ, and μρ); no evidence has been found for NHLs in the 0.25–2.0 GeV mass range. This analysis places limits on the mixing of NHLs with standard light neutrinos at a level up to an order of magnitude more restrictive than previous search limits in this mass range.Received 4 August 1999DOI:https://doi.org/10.1103/PhysRevLett.83.4943©1999 American Physical Society
DOI: 10.1103/physrevlett.90.239902
2003
Cited 120 times
Erratum: Precise Determination of Electroweak Parameters in Neutrino-Nucleon Scattering [Phys. Rev. Lett.<b>88</b>, 091802 (2002)]
Received 17 April 2003DOI:https://doi.org/10.1103/PhysRevLett.90.239902©2003 American Physical Society
DOI: 10.1103/physrevlett.99.192001
2007
Cited 105 times
Measurement of the Nucleon Strange-Antistrange Asymmetry at Next-to-Leading Order in QCD from NuTeV Dimuon Data
We present a new measurement of the difference between the nucleon strange and antistrange quark distributions from dimuon events recorded by the NuTeV experiment at Fermilab. This analysis is the first to use a complete next to leading order QCD description of charm production from neutrino scattering. Dimuon events in neutrino deep inelastic scattering allow direct and independent study of the strange and antistrange content of the nucleon. We find a positive strange asymmetry with a significance of 1.6σ. We also report a new measurement of the charm mass.Received 25 March 2007DOI:https://doi.org/10.1103/PhysRevLett.99.192001©2007 American Physical Society
DOI: 10.1103/physrevd.65.111103
2002
Cited 97 times
Effect of asymmetric strange seas and isospin-violating parton distribution functions on<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>θ</mml:mi></mml:mrow><mml:mrow><mml:mi>W</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>measured in the NuTeV experiment
The NuTeV Collaboration recently reported a value of ${\mathrm{sin}}^{2}{\ensuremath{\theta}}_{W}$ measured in neutrino-nucleon scattering that is 3 standard deviations above the standard model prediction. This result is derived assuming that (1) the strange sea is quark-antiquark symmetric, $s(x)=\overline{s}(x),$ and (2) up and down quark distributions are symmetric under the simultaneous interchange of $u\ensuremath{\leftrightarrow}d$ and $p\ensuremath{\leftrightarrow}n.$ We report the impact of violations of these symmetries on ${\mathrm{sin}}^{2}{\ensuremath{\theta}}_{W}$ and discuss the theoretical and experimental constraints on such asymmetries.
DOI: 10.1103/physrevlett.86.2742
2001
Cited 97 times
Measurements of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="italic">F</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msubsup><mml:mrow><mml:mi mathvariant="italic">xF</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi></mml:…
We report on the extraction of the structure functions F2 and DeltaxF(3) = xF(nu)(3)-xF(nu;)(3) from CCFR nu(mu)-Fe and nu;(mu)-Fe differential cross sections. The extraction is performed in a physics model-independent (PMI) way. This first measurement of DeltaxF(3), which is useful in testing models of heavy charm production, is higher than current theoretical predictions. The ratio of the F2 (PMI) values measured in nu(mu) and mu scattering is in agreement (within 5%) with the predictions of next-to-leading-order parton distribution functions using massive charm production schemes, thus resolving the long-standing discrepancy between the two sets of data.
DOI: 10.1103/physrevlett.89.011804
2002
Cited 43 times
Search for<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>→</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mover><mml:mrow><mml:mi>ν</mml:mi></mml:mrow…
Limits on nu(mu)-->nu(e) and nu(mu)-->nu(e) oscillations are extracted using the NuTeV detector with sign-selected nu(mu) and nu(mu) beams. In nu(mu) mode, for the case of sin(2)2alpha = 1, Delta(m)(2)>2.6 eV(2) is excluded, and for Delta(m)(2)>>1000 eV(2), sin(2)2alpha>1.1 x 10(-3). The NuTeV data exclude the high Delta(m)(2) end of nu(mu)-->nu(e) oscillation parameters favored by the LSND experiment without the need to assume that the oscillation parameters for nu and nu are the same. We present the most stringent experimental limits for nu(mu)(nu(mu))-->nu(e)(nu(e)) oscillations in the large Delta(m)(2) region.
DOI: 10.48550/arxiv.2403.13697
2024
Rota-Baxter operators of non-scalar weights, connections with coboundary Lie bialgebra structures
In the paper, we introduce the notion of a Rota-Baxter operator of a non-scalar weight. As a motivation, we show that there is a natural connection between Rota-Baxter operators of this type and structures of quasitriangular Lie bialgebras on a quadratic finite-dimensional Lie algebra. Moreover, we show that some classical results on Lie bialgebra structure on simple finite-dimensional Lie algebras can be obtained from the corresponding results for Rota-Baxter operators.
DOI: 10.48550/arxiv.2404.09261
2024
Formal integration of complete Rota-Baxter Lie algebras
In this paper, first we revisit the formal integration of Lie algebras, which give rise to braces in some special cases. Then we establish the formal integration theory for complete Rota-Baxter Lie algebras, that is, we show that there is a Rota-Baxter group with the underlying group structure given by the Baker-Campbell-Hausdorff formula, associated to any complete Rota-Baxter Lie algebra.
DOI: 10.1016/j.nima.2006.06.011
2006
Cited 27 times
The timing system for the CDF electromagnetic calorimeters
We report on the design and performance of the electromagnetic calorimeter timing readout system (EMTiming) for the Collider Detector at Fermilab (CDF). The system will be used in searches for rare events with high-energy photons to verify that the photon is in time with the event collision, to reject cosmic-ray and beam-halo backgrounds, and to allow direct searches for new, heavy, long-lived neutral particles that decay to photons. The installation and commissioning of all 862 channels were completed in Fall 2004 as part of an upgrade to the Run II version of the detector. Using in situ data, including electrons from W→eν and Z→ee decays, we measure the energy threshold for a time to be recorded to be 3.8±0.3GeV (1.9±0.1GeV) in the central (plug) portion of the detector. Similarly, for the central (plug) portion we measure a timing resolution of 600±10ps (610±10ps) for electrons above 10 GeV (6 GeV). There are very few system pathologies such as recording a time when no energy is deposited, or recording a second, fake time for a single energy deposit.
DOI: 10.1016/s0168-9002(99)01304-2
2000
Cited 29 times
Precision calibration of the NuTeV calorimeter
NuTeV is a neutrino-nucleon deep-inelastic scattering experiment at Fermilab. The detector consists of an iron-scintillator sampling calorimeter interspersed with drift chambers, followed by a muon toroidal spectrometer. We present determinations of response and resolution functions of the NuTeV calorimeter for electrons, hadrons, and muons over an energy range of 4.8 to 190 GeV. The absolute hadronic energy scale is determined to an accuracy of 0.43%. We compare our measurements to predictions from calorimeter theory and GEANT3 simulations.
DOI: 10.1103/physrevd.67.119902
2003
Cited 28 times
Erratum: “Effect of asymmetric strange seas and isospin-violating parton distribution functions on<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>θ</mml:mi></mml:mrow><mml:mrow><mml:mi>W</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>measured in the NuTeV experiment” [Phys. Rev. D<b>65…
The NuTeV collaboration recently reported a value of sin2thetaW measured in neutrino-nucleon scattering that is 3 standard deviations above the standard model prediction. This result is derived assuming that (1) the strange sea is quark-antiquark symmetric, s(x)=sbar(x), and (2) up and down quark distributions are symmetric under the simultaneous interchange of u<->d and p<->n. We report the impact of violations of these symmetries on sin2thetaW and discuss the theoretical and experimental constraints on such asymmetries.
DOI: 10.1088/2632-2153/ac7198
2022
Cited 5 times
Pile-up mitigation using attention
Abstract Particle production from secondary proton-proton collisions, commonly referred to as pile-up, impair the sensitivity of both new physics searches and precision measurements at large hadron collider (LHC) experiments. We propose a novel algorithm, Puma , for modeling pile-up with the help of deep neural networks based on sparse transformers. These attention mechanisms were developed for natural language processing but have become popular in other applications. In a realistic detector simulation, our method outperforms classical benchmark algorithms for pile-up mitigation in key observables. It provides a perspective for mitigating the effects of pile-up in the high luminosity era of the LHC, where up to 200 proton-proton collisions are expected to occur simultaneously.
DOI: 10.1103/physrevlett.87.041801
2001
Cited 27 times
Observation of an Anomalous Number of Dimuon Events in a High Energy Neutrino Beam
A search for long-lived neutral particles ( N0's) with masses above 2.2 GeV/c(2) that decay into at least one muon has been performed using an instrumented decay channel at the NuTeV experiment at Fermilab. Data were examined for particles decaying into the final states mumu, mu(e), and mu(pi). Three mumu events were observed over an expected standard model background of 0.069+/-0.010 events; no events were observed in the other modes.
DOI: 10.1103/physrevlett.87.251802
2001
Cited 24 times
Extraction of R=σL/σT from CCFR νμ-Fe and ν¯μ-Fe Differential Cross Sections
We report on the extraction of R = sigma(L)/sigma(T) from CCFR nu(mu)-Fe and nu(mu)-Fe differential cross sections. The CCFR differential cross sections do not show the deviations from the QCD expectations that are seen in the CDHSW data at very low and very high x. R as measured in nu(mu) scattering is in agreement with R as measured in muon and electron scattering. All data on R for Q(2)>1 GeV(2) are in agreement with a NNLO QCD calculation which uses NNLO parton distribution functions and includes target mass effects. We report on the first measurements of R in the low x and Q(2)<1 GeV(2) region (where an anomalous large rise in R for nuclear targets has been observed by the HERMES Collaboration).
DOI: 10.1103/physrevlett.86.5430
2001
Cited 24 times
First Measurement of the Low-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="italic">x</mml:mi></mml:math>, Low-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="italic">Q</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Structure Function<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><…
A new structure function analysis of CCFR deep inelastic nu-N and nu-N scattering data is presented for previously unexplored kinematic regions down to Bjorken x = 0.0045 and Q(2) = 0.3 GeV(2). Comparisons to charged lepton scattering data from NMC and E665 experiments are made and the behavior of the structure function F(2)(nu)2 is studied in the limit Q(2)-->0.
DOI: 10.1016/j.nima.2003.11.098
2004
Cited 11 times
Selection of tau leptons with the CDF Run 2 trigger system
We have implemented triggers for hadronically decaying tau leptons within a framework of the CDF Run 2 trigger system. We describe the triggers, along with their physics motivations, and report on their initial performance.
DOI: 10.1103/physrevlett.84.4043
2000
Cited 13 times
Search for a<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>33.9</mml:mn><mml:mi /><mml:mi>MeV</mml:mi><mml:mi>/</mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Neutral Particle in Pion Decay
The E815 (NuTeV) neutrino experiment has performed a search for a 33. 9 MeV/c(2) weakly interacting neutral particle produced in pion decay. Such a particle may be responsible for an anomaly in the timing distribution of neutrino interactions in the KARMEN experiment. E815 has searched for this particle's decays in an instrumented decay region; no evidence for this particle was found. The search is sensitive to pion branching ratios as low as 10(-13).
DOI: 10.1016/s0920-5632(02)01777-2
2002
Cited 11 times
Nuclear effects and the NuTeV sin2 θW measurement
NuTeV measures sin2 θW by comparing neutral and charged current cross-sections on a heavy nuclear target, and finds a value of sin2 θW(on-shell) = 0.2277 ± 0.0013(stat) ± 0.0009(syst), approximately 3σ from the predicted value. We discuss the possibility that nuclear effects on parton distribution functions or cross-sections may be responsible for the discrepancy.
DOI: 10.1103/physrevd.64.012002
2001
Cited 11 times
Observation of neutral current charm production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi mathvariant="normal">Fe</mml:mi></mml:math>scattering at the Fermilab Tevatron
We report on the first observation of open charm production in neutral current deep inelastic neutrino scattering as seen in the NuTeV detector at Fermilab. The production rate is shown to be consistent with a pure gluon-$% Z^{0}$ boson production model, and the observed level of charm production is used to determine the effective charm mass. As part of our analysis, we also obtain a new measurement for the proton-nucleon charm production cross section at $\sqrt{s}=38.8$ GeV.
DOI: 10.1088/1742-6596/784/1/012053
2017
Cited 4 times
Spectrophotometric method for quantitative measuring essential oil in aromatic water and distillate with rose smell
In this connection, we improved the express methods of determining the mixture of volatile aromatic substances by the spectrophotometry of aromatic water and steam distillate of essential oil raw materials (traditional or biotechnological with rose smell). Direct spectrophotometry of distillation water is impossible because it is a colloid of liquid oil and law is not observed. Therefore, it is necessary to dissolve 1 ml of distillate in ethanol in the ratio 1:4, in this case we take real solution with no lipophilic fall-out on the walls of cuvette, also the light absorption law is observed. There are stable maximums in spectrums of studied oils. Optical density of these maximums is a result of summary absorption of terpenoid components (aromatic and monoterpene alcohols, its ethers). Optical density of tested and standard solutions is measured in appropriate wavelengths. Spectrophotometric method of determination of essential oil quantity in aromatic water with rose smell differs with high sensitivity (10-5-10-6 gmol/l) and allows to determine oil concentration from 0,900 to 0,008 mg with an error less than 1%. At that, 1 ml is enough for analysis. It's expedient to apply this method while operating with small quantity of water distillate in biochemical and biotechnological researches and also as express control for extraction and hydrodistillation of essential oil raw material (rose petals and flowers from different origin, eremothecium cultural liquid etc.).
2012
Cited 4 times
Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV
DOI: 10.1103/physrevlett.87.071803
2001
Cited 8 times
Search for the Lepton Family Number Violating Process<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mover><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="italic">e</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mi /><mml:mo>→</mml:mo><mml:mi /><mml:mrow><…
The NuTeV experiment at Fermilab has used a sign-selected neutrino beam to perform a search for the lepton number violating process nu(mu)e(-)-->mu(-)nu(e), and to measure the cross section of the standard model inverse muon decay process nu(mu)e(-)-->mu(-)nu(e). NuTeV measures the inverse muon decay asymptotic cross-section slope sigma/E to be (13.8 +/- 1.2 +/- 1.4) x 10(-42) cm(2)/GeV. The experiment also observes no evidence for lepton number violation and places one of the most restrictive limits on the cross-section ratio sigma(nu(mu)e(-)-->mu(-)nu(e))/sigma(nu(mu)e(-)-->mu(-)nu(e)) < or = 1.7% at 90% C.L. for V-A couplings and < or = 0.6% for scalar couplings.
2013
Cited 3 times
Energy calibration and resolution of the CMS electromagnetic calorimeter in pp collisions at √s = 7 TeV
DOI: 10.1016/s0920-5632(03)01314-8
2003
Cited 6 times
High energy neutrino scattering results from NuTeV
The NuTeV experiment at Fermilab has obtained a unique high statistics sample of neutrino and antineutrino interactions using a novel high-energy sign-selected neutrino beam. Recent results from this sample are presented including a precision measurement of the electroweak parameter sin2≡W, which is observed to be three standard deviations above the standard model prediction.
DOI: 10.12737/25059
2017
Cited 3 times
To Improve Accuracy of Radionuclide Therapy Dosimetry Planning Using Monte Carlo Method
Purpose: Development and clinical testing of methodology dosimetry planning of radionuclide therapy based on Monte Carlo simulation of radiation transfer process.&#x0D; Material and methods: The method of determination in absolute units of radiopharmaceutical (RP) activity accumulated in tumor lesions. The technique is based on scintigraphy syringe containing diagnostic RP activity, biplane patient scintigraphy after injection of the RP and determination of the RP accumulation when administered calculated using the Monte Carlo method for the absorption and scattering of radiation in the patient’s body and in the collimator of the gamma camera. Code MCNP Monte Carlo simulation was used. The layout of determination of the value of accumulated RP activity in the patient’s tumor site implies successive implementation of the following three steps.&#x0D; 1. Scintigraphic images are obtained of the vial containing already known activity of the RP placed at the fixed source-to-collimator distance, following&#x0D; which estimation of the detector count rate within the specified region of interest of the vial image is undertaken.&#x0D; 2. Therapeutic activity A0 is introduced in the patient’s body, scintigraphic examination of the patient is performed. Estimation of the detector count rate in the region where the tumor is located and the value of tissue background in the close enough vicinity to the tumor is performed using the tools for contouring the region of interest on the obtained planar image provided using the software imbedded in the scintigraphic equipment.&#x0D; 3. Value of accumulated activity RP in the affected tumor is determined according to the correction factor which is calculated using Monte-Carlo method for specific clinical case for the geometry used in obtaining scintigraphic images which is identical to the conditions of measurement of activity in the vial and in the patient’s body. The technique has been tested in the study, with an injection of 30 MBq of 123I-MIBG child with neuroblastoma.&#x0D; Results: The level of accumulation of radiopharmaceutical in the tumor of the adrenal gland was 0.78 MBq, i.e. 2.6 % of the administered activity. This corresponds to literature data (average about 2.4 %) for scintigraphic studies of children with neuroblastomas. When using the known calculation method for analytical formula without the introduction of corrections for the absorption and scattering of radiation was obtained a result of 1.02 MBq, i.e. overestimation was 31 %.&#x0D; Conclusions: Introduction calculated by the Monte Carlo method for the absorption and scattering of radiation during scintigraphy patient can improve the accuracy of dosimetry planning of radionuclide therapy.
DOI: 10.21470/1678-9741-2021-0074
2023
Long-Term Radial Artery Grafts with Previous Midterm Proven Patency
Left internal thoracic artery to left anterior descending artery (LITA-LADA) grafting has become a fundamental part of coronary artery bypass grafting (CABG). This grafting has led to an increased use of other arterial conduits, of which the radial artery (RA) is the most popular. Whether RA can have the same long-term patency as LITA is controversial. The objective of this study is to access the long-term clinical follow-up and, when available, the patency rate of RA grafts.Twenty-six patients from a previous study with critical stenosis in all target vessels underwent complete arterial CABG with LITA and RA grafts from 1996 to 2003. They all underwent midterm multidetector computed tomography after surgery with the association of at least one patent LITA and one patent RA graft.Twelve patients (46%) are alive with no angina symptoms. Six patients underwent a second image exam 12 to 16 years (average of 14 years) after surgery, with a total of six LITA-LADA and 14 RA grafts with 100% patency rate. Clinical follow-up five to 23 years after surgery (average of 14 years) showed only one death 12 years after surgery related to coronary artery disease (CAD) (3,8%). Another 12 patients died of non-CAD.Patients with midterm associated LITA and RA patent grafts show similar optimal long-term patency rates of both types of grafts with excellent clinical outcome.
DOI: 10.1016/0375-9601(94)91047-2
1994
Cited 7 times
Dynamics of Josephson vortices in a temperature gradient
We have studied the underdamped dynamics of vortices in a long Josephson junction in the presence of a temperature gradient along the junction. The flux-flow voltage was found to depend on the mutual orientation of the temperature gradient and the external magnetic field. This effect is caused by the difference in viscosity coefficient on the hot and the cold junction sides. The motion of Josephson vortices is simulated using the perturbed sine-Gordon model with the spatially dependent loss term. Simulation results are in good agreement with experimental data.
2018
Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s = 13 TeV
2016
Search for pair-produced vectorlike B quarks in proton-proton collisions at √s = 8 TeV
2016
Search for long-lived charged particles in proton-proton collisions at √s=13 TeV
DOI: 10.1103/physrevd.63.012001
2000
Cited 4 times
Search for light-to-heavy quark flavor changing neutral currents in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>N</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mover><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover><mml:mrow><…
We report on a search for flavor-changing neutral-currents (FCNC) in the production of heavy quarks in deep inelastic νμN and ν¯μN scattering by the NuTeV experiment at the Fermilab Tevatron. This measurement, made possible by the high-purity NuTeV sign-selected beams, probes for FCNC in heavy flavors at the quark level, and is uniquely sensitive to neutrino couplings of potential FCNC mediators. All searches are consistent with zero, and limits on the effective mixing strengths |Vuc|2, |Vdb|2, and |Vsb|2 are obtained.Received 31 July 2000DOI:https://doi.org/10.1103/PhysRevD.63.012001©2000 American Physical Society
DOI: 10.1142/s0217751x01008035
2001
Cited 4 times
OBSERVATION OF NEUTRAL CURRENT CHARM PRODUCTION IN ν<sub>μ</sub>Fe SCATTERING AT THE TEVATRON
We report on the first observation of open charm production in neutral current deep inelastic neutrino scattering as seen in the NuTeV detector at Fermilab. The production rate is shown to be consistent with a pure gluon-Z 0 boson production model, and the observed level of charm production is used to determine the effective charm mass.
2007
Measurement of the Inclusive Jet Cross Section using the {\boldmath $k_{\rm T}$} algorithmin{\boldmath $p\overline{p}$} Collisions at{\boldmath $\sqrt{s}$} = 1.96 TeV with the CDF II Detector
2015
Measurements of jet multiplicity and differential production cross sections of Z + jets events in proton-proton collisions at √s = 7 TeV
DOI: 10.1142/s0217751x05027539
2005
NuTeV Structure Function Measurement
The NuTeV experiment obtained high statistics samples of neutrino and antineutrino charged current events during the 1996-1997 Fermilab fixed target run. The experiment combines sign-selected neutrino and antineutrino beams and the upgraded CCFR iron-scintillator neutrino detector. A precision continuous calibration beam was used to determine the muon and hadron energy scales to a precision of 0.7% and 0.43% respectively. The structure functions F 2 (x, Q 2 ) and xF 3 (x, Q 2 ) obtained by fitting the y-dependence of the sum and the difference of the ν and [Formula: see text] differential cross sections are presented.
2017
Inclusive search for supersymmetry using razor variables in pp collisions at √s = 13 TeV
2017
Observation of Charge-Dependent Azimuthal Correlations in p-Pb Collisions and Its Implication for the Search for the Chiral Magnetic Effect
2003
The CDF-II Tau Physics Program - Triggers, $\tau$ ID and Preliminary Results
The study of processes containing T leptons in the final state will play an important role at Tevatron Run II. Such final states will be relevant both for electroweak studies and measurements as well as in searches for physics beyond the Standard Model. The present paper discusses the physics opportunities and challenges related to the implementation of a new set of triggers able to select events containing tau candidates in the final state. We illustrate, in particular, the physics capabilities for a variety of new physics scenarios such as supersymmetry (SUSY), SUSY with Rp-parity violation, with Bilinear parity violation or models with the violation of lepton flavor. Finally, we present the first Run II results obtained using some of the described tau triggers.
2009
Search for new particles decaying into dijets in proton-antiproton collisions at sqrt[s]=1.96 TeV
DOI: 10.1063/1.57764
1999
Cited 3 times
Heavy quark production in neutrino deep-inelastic scattering
Charm production by neutrino charged-current interactions produces two muon (dimuon) events which are easily identified. This signal provides an important method to measure the strange sea and the mass of the charm quark. Several experiments, including CCFR, CDHS and CHARM II, have performed analyses of such events. The results of these analyses are summarized with emphasis on CCFR and improvements made by NuTeV.
DOI: 10.1016/s0920-5632(00)00549-1
2000
Recent QCD results from NuTeV/CCFR Collaboration
Fermilab experiments CCFR and its successor NuTeV study nucleon structure through deep inelastic scattering of neutrino beams off an iron target. We report on the most recent CCFR measurement of the νN differential cross section and resulting structure functions ΔxF3 = xFν3 − xFν3, and Rlong = σLσT, in the framework of massive charm quark. ΔxF3 in sensitive to strange and charm content of the nucleon. NuTeV's preliminary direct measurement of the strange sea, from dimuon charged-current production, and nucleon charm content probed by neutral-current νN interaction, are also presented.
DOI: 10.48550/arxiv.hep-ex/0205080
2002
A Departure from Prediction: Electroweak Physics at Nutev
The NuTeV experiment has performed precision measurements of the ratio of neutral-current to charged-current cross-sections in high rate, high energy neutrino and anti-neutrino beams on a dense, primarily steel, target. The separate neutrino and anti-neutrino beams, high statistics, and improved control of other experimental systematics, allow the determination of electroweak parameters with significantly greater precision than past neutrino-nucleon scattering experiments. Our null hypothesis test of the standard model prediction measures sin2thetaW=0.2277+/-0.0013(stat)+/-0.0009(syst), a value which is 3.0 standard deviations above the prediction. We discuss possible explanations for and implications of this discrepancy.
DOI: 10.1142/s0217751x01006486
2001
NEW MESUREMENTS OF NUCLEON STRUCTURE FUNCTIONS FROM CCFR/NuTeV
We report on the extraction of the structure functions F_2 and Delta xF_3 = xF_3nu-xF_3nub from CCFR neutrino-Fe and antineutrino-Fe differential cross sections. The extraction is performed in a physics model independent (PMI) way. This first measurement for Delta xF_3, which is useful in testing models of heavy charm production, is higher than current theoretical predictions. Within 5% the F_2 (PMI) values measured in neutrino and muon scattering are in agreement with the predictions of Next-to-Leading-Order PDFs (using massive charm production schemes), thus resolving the long-standing discrepancy between the two measurements.
DOI: 10.1007/s41781-021-00054-2
2021
Dynamo: Handling Scientific Data Across Sites and Storage Media
Abstract Dynamo is a full-stack software solution for scientific data management. Dynamo’s architecture is modular, extensible, and customizable, making the software suitable for managing data in a wide range of installation scales, from a few terabytes stored at a single location to hundreds of petabytes distributed across a worldwide computing grid. This article documents the core system design of Dynamo and describes the applications that implement various data management tasks. A brief report is also given on the operational experiences of the system at the CMS experiment at the CERN Large Hadron Collider and at a small-scale analysis facility.
DOI: 10.48550/arxiv.hep-ex/9906038
1999
Strange Content of the Nucleon (NuTeV)
The NuTeV experiment uses neutrino deep-inelastic scattering from separate neutrino and anti-neutrino beams to study the structure of the nucleon. Charged-current production of charm is sensitive to the strange content of the nucleon while neutral-current charm production probes the charm content. Preliminary analyses of both topics are presented along with discussion of possible momentum asymmetry in the strange sea.
2015
Search for a standard model-like Higgs boson in the μ[superscript +]μ[superscript −] and e[superscript +]e[superscript −] decay channels at the LHC
2014
Differential cross section measurements for the production of a W boson in association with jets in proton–proton collisions at √s = 7 TeV
2014
Measurement of the t[bar over t] production cross section in pp collisions at √s = 8 TeV in dilepton final states containing one τ lepton
2015
Search for narrow high-mass resonances in proton–proton collisions at √s = 8 TeV decaying to a Z and a Higgs boson
2015
Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in ℓ[superscript +]ℓ[superscript −]b[bar over b] final states
2015
Measurement of the cross section ratio σ[subscript t[bar over t]b[bar over b]]/σ[subscript t[bar over t]jj] in pp collisions at √s = 8 TeV
2014
Modification of Jet Shapes in PbPb Collisions at √s[subscript NN] = 2.76 TeV
2015
Measurement of the production cross section ratio σ ([subscript χb2](1P))/σ ([subscript χb1](1P)) in pp collisions at √s = 8 TeV
2014
Measurement of the top-quark mass in all-jets t[bar over t] events in pp collisions at √s =7 TeV
2014
Measurement of the pp → ZZ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at √s = 8 TeV
2015
Search for heavy majorana neutrinos in μ[superscript ±]μ[superscript ±] + jets events in proton–proton collisions at √s = 8 TeV
2014
Evidence of b-Jet Quenching in PbPb Collisions at √s[subscript NN] = 2.76 TeV
2016
Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at t √s = 8 TeV
2016
Measurement of the t[bar over t] production cross section in the all-jets final state in pp collisions at √s = 8 TeV
2014
Inclusive Search for a Vector-Like T Quark with Charge 2/3 in pp Collisions at √s = 8 TeV
2016
Measurement of the integrated and differential t[bar over t] production cross sections for high- pT top quarks in pp collisions at √s = 8 TeV
2015
Angular coefficients of Z bosons produced in pp collisions at √s = 8 TeV and decaying to μ[superscript +]μ[superscript −] as a function of transverse momentum and rapidity
2015
Nuclear effects on the transverse momentum spectra of charged particles in pPb collisions at √s[subscript NN] = 5.02 TeV
2016
Study of B meson production in p + Pb collisions at √s[subscript NN] = 5.02 TeV using exclusive hadronic decays
2015
Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies
2014
Search for new resonances decaying via WZ to leptons in proton–proton collisions at √s = 8 TeV
2014
Measurement of the production cross section for a W boson and two b jets in pp collisions at √s = 7 TeV
2015
Search for stealth supersymmetry in events with jets, either photons or leptons, and low missing transverse momentum in pp collisions at 8 TeV
2016
Search for New Phenomena in Monophoton Final States in Proton–proton Collisions at √s = 8 TeV
2014
Search for baryon number violation in top-quark decays
2016
Measurement of the forward–backward asymmetry of top-quark and antiquark pairs using the full CDF Run II data set
2016
Search for Narrow Resonances in Dijet Final States at √s = 8 TeV with the Novel CMS Technique of Data Scouting
2014
Measurement of pseudorapidity distributions of charged particles in proton–proton collisions at √s = 8 TeV by the CMS and TOTEM experiments
2014
Studies of dijet transverse momentum balance and pseudorapidity distributions in pPb collisions at √s[subscript NN] = 5.02 TeV
2015
Search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks using a matrix element method
2014
Observation of the diphoton decay of the Higgs boson and measurement of its properties
2014
Searches for electroweak production of charginos, neutralinos, and sleptons decaying to leptons and W, Z, and Higgs bosons in pp collisions at 8 TeV
2014
Search for heavy neutrinos and W bosons with right-handed couplings in proton–proton collisions at √s = 8 TeV
2014
Measurement of differential cross sections for the production of a pair of isolated photons in pp collisions at √s = 7 TeV
2016
Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at √s=8 and 13 TeV
2014
Search for excited quarks in the γ + jet final state in proton-proton collisions at √s = 8 TeV
2015
Search for a light charged Higgs boson decaying to c[bar over s] in pp collisions at √s = 8 TeV
2015
Measurements of the ϒ(1S), ϒ(2S), and ϒ(3S) differential cross sections in pp collisions at √s = 7 TeV
2014
Measurement of higher-order harmonic azimuthal anisotropy in PbPb collisions at √s[subscript NN] = 2.76 TeV
2015
Searches for supersymmetry based on events with b jets and four W bosons in pp collisions at 8 TeV
2012
Study of W boson production in PbPb and pp collisions at √s[subscript NN] = 2.76 TeV
2012
Combined search for the quarks of a sequential fourth generation
2012
Search for scalar top quark production in p[bar over p] collisions at √s = 1.96 TeV
2012
Jet momentum dependence of jet quenching in PbPb collisions at √s[subscript NN] = 2.76 TeV
2011
Search for B[subscript s][superscript 0]→μ[superscript +]μ[superscript -] and B[superscript 0]→μ[superscript +]μ[superscript - ] Decays in pp Collisions at √s=7 TeV
2011
Dijet Azimuthal Decorrelations in pp Collisions at √s=7 [square root of s=7] TeV
2012
Observation of long-range, near-side angular correlations in pPb collisions at the LHC
2011
Observation of the Baryonic Flavor-Changing Neutral Current Decay Λ[subscript b][superscript 0]→Λμ[superscript +]μ[superscript -]
2011
Search for New Physics in High p [subscript T] Like-Sign Dilepton Events at CDF II
2012
Measurement of B[subscript s][superscript 0]→D[subscript s](*)[superscript +]D[subscript s](*)[superscript -] Branching Ratios
2012
Measurement of CP-violation asymmetries in D[superscript 0]→K[subscript S][superscript 0]π[superscript +]π[superscript -]
2011
Measurement of W[superscript +]W[superscript −] production and search for the Higgs boson in pp collisions at √s = 7 TeV