This document discusses parton distribution functions (PDFs) relevant for a future 100 TeV hadron collider. It summarizes that such a collider would probe PDFs at smaller x values than currently possible, down to x=10-9. It would also probe higher mass scales, up to masses of 10 TeV. Current PDF determinations have little constraint for x<10-4 or masses above 1 TeV. The increased energy would require considering effects like top quark PDFs, electroweak corrections, and high-energy resummation not important at lower energies. Polarized collisions could also provide insights into PDFs.
Parton Distributions at a 100 TeV Hadron Colliderjuanrojochacon
This document discusses parton distributions for a potential future 100 TeV hadron collider. It begins with an outline of topics to be covered, including the increased kinematic coverage from 14 TeV to 100 TeV, PDF luminosities over this energy range, and tools needed for PDF studies at 100 TeV. The document then examines the kinematic coverage at 100 TeV in detail, showing how it probes PDFs at smaller x values and allows access to higher mass scales. Plots demonstrate that PDF luminosities increase much more rapidly from 14 to 100 TeV for higher mass states. The discussion covers tools needed for FCC PDF studies, including behavior of PDFs at large-x, inclusion of a top quark PDF,
Parton distributions with QED corrections and LHC phenomenologyjuanrojochacon
The document discusses parton distribution functions (PDFs) that include quantum electrodynamics (QED) corrections. It summarizes the NNPDF2.3QED PDF set, which is the first to include next-to-next-to-leading order (NNLO) QCD and leading order (LO) QED effects. The photon PDF is directly constrained by LHC data for the first time. The PDF set improves constraints on the photon PDF from both DIS and LHC Drell-Yan data. It also discusses implications for LHC phenomenology from photon-initiated contributions.
Parton Distributions at a 100 TeV Hadron Colliderjuanrojochacon
Usage of modern PDF sets with LHAPDF6 v6.1.5 is suitable for FCC studies and simulations. At a 100 TeV hadron collider, PDFs would need to be evaluated in more extreme regions of small-x, large-x, and large invariant masses than at the LHC. Photon-initiated processes could contribute significantly at the FCC due to large uncertainties in the photon PDF. Heavy quark PDFs, including for the top quark, should be included in matched calculations for FCC simulations rather than using a purely massless scheme.
This document contains the agenda for a workshop on Multi-Gbps TCP. The workshop includes presentations on high speed networks, LHC networks, TCP/AQM protocols and their duality model, control theory and stability of TCP/AQM, FAST simulations, and related TCP kernel projects. Presentations will be given by researchers from Caltech, CERN, UCLA, and INRIA on topics such as TCP protocols, active queue management, stability analysis, and simulations. There will also be discussion periods following some of the presentations.
NNPDF3.0: Next Generation Parton Distributions for the LHC Run IIjuanrojochacon
NNPDF3.0 is a new PDF release from the NNPDF collaboration that incorporates recent experimental data from HERA and the LHC, improved theory calculations, and methodological advances. Key aspects of NNPDF3.0 include the inclusion of new data like HERA structure functions, LHC jets and electroweak data, and top quark production data. It also utilizes approximate NNLO calculations for jets and NLO electroweak corrections for Drell-Yan production. The fitting methodology has been improved with a C++ rewrite of the code and validation on closure tests. Preliminary results show good agreement with NNPDF2.3 and reduced uncertainties for some PDFs from the new data and methodology
The impact of new collider data into the NNPDF global analysisJuan Rojo
The document summarizes Juan Rojo's presentation on the impact of new collider data in the NNPDF global analysis. It discusses updates and improvements to the NNPDF methodology, including adopting the public code APFEL, adding new LHC datasets like LHCb and top quark pair differential distributions, and analyzing the impact on parton distributions from including precise Tevatron and LHC Z boson data. Preliminary results from NNPDF3.1 indicate good stability compared to the previous NNPDF3.0 analysis, with reduced uncertainties and improved flavor separation from new experimental inputs.
NNPDF3.0: Next generation parton distributions for the LHC Run IIjuanrojochacon
The document provides an overview of the forthcoming NNPDF3.0 PDF release from the NNPDF Collaboration. Key points include:
1) NNPDF3.0 includes over 1000 new data points from HERA and LHC experiments like ATLAS and CMS, improving constraints on PDFs.
2) Improved theory calculations are used, including approximate NNLO corrections for jet data and full NLO electroweak corrections.
3) The NNPDF methodology has been upgraded with a C++ code rewrite, validation on closure tests, and improvements to the fitting strategy and basis choices.
Pdpta11 G-Ensemble for Meteorological Prediction EnhancementHisham Ihshaish
This document discusses using an ensemble approach called Genetic Ensemble (G-Ensemble) to improve meteorological predictions. Meteorological models use initial conditions and physical parameterizations to predict variables over a domain at future time steps. However, predictions can be imperfect due to uncertainties in initial conditions and parameterizations. G-Ensemble aims to address this by running an ensemble of meteorological models with varied initial conditions and parameterizations to generate a collective prediction. The approach was tested on hurricane Katrina predictions, showing potential to improve forecast accuracy. Future work will further evaluate G-Ensemble on additional cases.
Parton Distributions at a 100 TeV Hadron Colliderjuanrojochacon
This document discusses parton distributions for a potential future 100 TeV hadron collider. It begins with an outline of topics to be covered, including the increased kinematic coverage from 14 TeV to 100 TeV, PDF luminosities over this energy range, and tools needed for PDF studies at 100 TeV. The document then examines the kinematic coverage at 100 TeV in detail, showing how it probes PDFs at smaller x values and allows access to higher mass scales. Plots demonstrate that PDF luminosities increase much more rapidly from 14 to 100 TeV for higher mass states. The discussion covers tools needed for FCC PDF studies, including behavior of PDFs at large-x, inclusion of a top quark PDF,
Parton distributions with QED corrections and LHC phenomenologyjuanrojochacon
The document discusses parton distribution functions (PDFs) that include quantum electrodynamics (QED) corrections. It summarizes the NNPDF2.3QED PDF set, which is the first to include next-to-next-to-leading order (NNLO) QCD and leading order (LO) QED effects. The photon PDF is directly constrained by LHC data for the first time. The PDF set improves constraints on the photon PDF from both DIS and LHC Drell-Yan data. It also discusses implications for LHC phenomenology from photon-initiated contributions.
Parton Distributions at a 100 TeV Hadron Colliderjuanrojochacon
Usage of modern PDF sets with LHAPDF6 v6.1.5 is suitable for FCC studies and simulations. At a 100 TeV hadron collider, PDFs would need to be evaluated in more extreme regions of small-x, large-x, and large invariant masses than at the LHC. Photon-initiated processes could contribute significantly at the FCC due to large uncertainties in the photon PDF. Heavy quark PDFs, including for the top quark, should be included in matched calculations for FCC simulations rather than using a purely massless scheme.
This document contains the agenda for a workshop on Multi-Gbps TCP. The workshop includes presentations on high speed networks, LHC networks, TCP/AQM protocols and their duality model, control theory and stability of TCP/AQM, FAST simulations, and related TCP kernel projects. Presentations will be given by researchers from Caltech, CERN, UCLA, and INRIA on topics such as TCP protocols, active queue management, stability analysis, and simulations. There will also be discussion periods following some of the presentations.
NNPDF3.0: Next Generation Parton Distributions for the LHC Run IIjuanrojochacon
NNPDF3.0 is a new PDF release from the NNPDF collaboration that incorporates recent experimental data from HERA and the LHC, improved theory calculations, and methodological advances. Key aspects of NNPDF3.0 include the inclusion of new data like HERA structure functions, LHC jets and electroweak data, and top quark production data. It also utilizes approximate NNLO calculations for jets and NLO electroweak corrections for Drell-Yan production. The fitting methodology has been improved with a C++ rewrite of the code and validation on closure tests. Preliminary results show good agreement with NNPDF2.3 and reduced uncertainties for some PDFs from the new data and methodology
The impact of new collider data into the NNPDF global analysisJuan Rojo
The document summarizes Juan Rojo's presentation on the impact of new collider data in the NNPDF global analysis. It discusses updates and improvements to the NNPDF methodology, including adopting the public code APFEL, adding new LHC datasets like LHCb and top quark pair differential distributions, and analyzing the impact on parton distributions from including precise Tevatron and LHC Z boson data. Preliminary results from NNPDF3.1 indicate good stability compared to the previous NNPDF3.0 analysis, with reduced uncertainties and improved flavor separation from new experimental inputs.
NNPDF3.0: Next generation parton distributions for the LHC Run IIjuanrojochacon
The document provides an overview of the forthcoming NNPDF3.0 PDF release from the NNPDF Collaboration. Key points include:
1) NNPDF3.0 includes over 1000 new data points from HERA and LHC experiments like ATLAS and CMS, improving constraints on PDFs.
2) Improved theory calculations are used, including approximate NNLO corrections for jet data and full NLO electroweak corrections.
3) The NNPDF methodology has been upgraded with a C++ code rewrite, validation on closure tests, and improvements to the fitting strategy and basis choices.
Pdpta11 G-Ensemble for Meteorological Prediction EnhancementHisham Ihshaish
This document discusses using an ensemble approach called Genetic Ensemble (G-Ensemble) to improve meteorological predictions. Meteorological models use initial conditions and physical parameterizations to predict variables over a domain at future time steps. However, predictions can be imperfect due to uncertainties in initial conditions and parameterizations. G-Ensemble aims to address this by running an ensemble of meteorological models with varied initial conditions and parameterizations to generate a collective prediction. The approach was tested on hurricane Katrina predictions, showing potential to improve forecast accuracy. Future work will further evaluate G-Ensemble on additional cases.
The document discusses the NNPDF3.1 global analysis of parton distribution functions (PDFs). It provides an update to NNPDF3.0 motivated by new high-precision collider data and progress in NNLO calculations. NNPDF3.1 fits both a perturbative and fitted charm PDF and finds slightly better fit quality for the fitted charm case. Comparisons to NNPDF3.0 show agreement within uncertainties and reduced PDF errors in NNPDF3.1 due to the new LHC data.
This document provides example problems and solutions related to calculating network performance metrics like transfer time and latency. It addresses topics like message segmentation, circuit switching vs packet switching, and calculating bandwidth needs for different media types. Sample problems calculate latency for different network configurations, bandwidth required for streaming high-definition video and audio, and compare transferring a file with and without message segmentation.
The document describes a method called the "Four Russians method" to speed up Bayesian Hidden Markov Model (HMM) classification by exploiting repetition in long observation sequences. The key ideas are to break the observation sequence into blocks of length k and compute the forward variables only at block boundaries, and to sample the hidden state sequence block-by-block from the backward-forward distribution rather than the full backward distribution. This reduces the computational complexity from O(TN^2) to O(TNk/k^2) = O(TN/k).
This document discusses digital modulation techniques. It begins by listing various digital modulation types including ASK, FSK, PSK, MFSK, MPSK, and MSK. It then provides an overview of the digital modulation and demodulation process when used for wireless communication. The key digital modulation techniques of ASK, FSK, and PSK are then explained in more detail. ASK modulates the amplitude of the carrier wave, FSK modulates the frequency, and PSK modulates the phase. Diagrams and equations are provided to illustrate how each modulation type encodes data onto an analog signal. The document concludes by discussing the demodulation of ASK, FSK, and PSK signals.
This document describes using MATLAB to analyze a synthetic time series dataset representing climate data over 500,000 years. The time series contains periodic signals at 100ky, 41ky and 21ky. Random noise and a long term trend are added. Fourier analysis is used to identify the dominant periodic components in the frequency domain. A Hamming window and bandpass filter are applied to further analyze specific frequency bands like the 21ky signal. Autocorrelation is also examined to identify cyclic patterns in the time series.
The document summarizes the NNPDF3.1 global analysis which provides an updated determination of parton distribution functions (PDFs) from experimental data. Key points include:
1) NNPDF3.1 includes new high-precision measurements from the LHC as well as NNLO QCD calculations, allowing more data to be included. It also fits the charm PDF rather than assuming it is purely perturbative.
2) The new data provides stronger constraints on PDFs, particularly the gluon and down quark, significantly reducing their uncertainties. It also shows good agreement with the previous NNPDF3.0 analysis.
3) For the first time, NNPDF3.1 includes LHC
On The Fundamental Aspects of DemodulationCSCJournals
When the instantaneous amplitude, phase and frequency of a carrier wave are modulated with the information signal for transmission, it is known that the receiver works on the basis of the received signal and a knowledge of the carrier frequency. The question is: If the receiver does not have the a priori information about the carrier frequency, is it possible to carry out the demodulation process? This tutorial lecture answers this question by looking into the very fundamental process by which the modulated wave is generated. It critically looks into the energy separation algorithm for signal analysis and suggests modification for distortionless demodulation of an FM signal, and recovery of sub-carrier signals
Constraints on the gluon PDF from top quark differential distributions at NNLOjuanrojochacon
- The document discusses constraints on the gluon PDF from top quark production at hadron colliders.
- It describes using the inclusive top quark pair production cross section to reduce uncertainties in the gluon PDF, especially in the large-x region between 0.1 and 0.5.
- Cross section ratios between different beam energies, such as 8 TeV/7 TeV, are highlighted as powerful precision tests that can discriminate between PDFs and probe BSM physics.
QCD at the LHC: recent progress and open problemsjuanrojochacon
The document discusses recent progress and open problems in QCD at the LHC. It notes that improving the quantitative understanding of the Standard Model is essential, and that sharpening QCD tools could enable new discoveries at the LHC. In particular, better parton distribution functions, higher-order perturbative calculations, and matching calculations to parton showers are highlighted as important for improving both precision and sensitivity to new physics. The talk outlines the current status and future prospects for parton distribution functions, fixed-order calculations up to NNLO, matching to parton showers, and merging samples with different jet multiplicities.
Recent progress in proton and nuclear PDFs at small-xjuanrojochacon
1) The document discusses recent progress in proton and nuclear parton distribution functions (PDFs) at small values of x. PDFs describe the momentum distribution of quarks and gluons inside protons and nuclei.
2) Global analyses of experimental data from various processes are used to determine PDFs at hadronic scales, which are then evolved perturbatively to higher scales relevant for LHC predictions. Recent analyses include data from the LHC.
3) Probing PDFs at small x requires processes dominated by gluons at leading order, produced in the forward region with low invariant masses. Examples discussed are direct photon and charm production. LHCb and future forward calorimeter data provide constraints on the small-
NNPDF3.0: parton distributions for the LHC Run IIjuanrojochacon
NNPDF3.0 is a new PDF determination that includes updated data and theory improvements compared to NNPDF2.3. It includes all HERA-II data and new LHC measurements. The fitting code was rewritten in C++ and validated using closure tests. NNPDF3.0 shows reasonable agreement with NNPDF2.3 while improving descriptions of data and reducing uncertainties in some regions. It provides PDFs for use at the LHC Run II.
Parton Distributions and Standard Model Physics at the LHCjuanrojochacon
This document discusses parton distribution functions (PDFs) and recent developments. It notes that NNLO calculations are essential to reduce uncertainties in PDF analysis. Several key processes like inclusive jet production and top quark production are now available at NNLO. The document also discusses the inclusion of LHC data like W+charm, top quark, and jet data in global PDF fits. It highlights updates to various PDF fitting groups and the upcoming NNPDF3.0 release.
The document discusses the Monash 2013 tune of Pythia 8, which uses the NNPDF2.3LO parton distribution functions (PDFs). It notes that LO PDFs are important for describing non-perturbative physics in event generators. NNPDF2.3LO has a steeper gluon distribution at small values of x compared to the CTEQ6L PDF used in previous tunes. This allows the Monash 2013 tune to better describe precise forward data from experiments like TOTEM and CMS, which probe the gluon PDF in the low-x region.
News from NNPDF: QED, small-x, and alphas(MZ) fitsjuanrojochacon
Juan Rojo presented recent work from the NNPDF collaboration on three spin-off fits from their NNPDF3.1 global analysis: NNPDF3.1QED, fits including small-x resummation, and a determination of the strong coupling constant αS(mZ). For NNPDF3.1QED, they are imposing the LUXqed formalism to constrain the photon PDF rather than extracting it from data. For small-x resummation fits, they find that including NNLO+NLLx theory stabilizes the small-x gluon and improves description of HERA data. Their preliminary αS(mZ) value is consistent with other determinations.
This document discusses parton distribution functions (PDFs) with intrinsic charm. It presents the motivation for fitting a charm PDF in global analyses, including stabilizing charm mass dependence, quantifying the non-perturbative charm component, and exploring implications for LHC phenomenology. The document summarizes previous fits allowing for intrinsic charm and issues they faced. It then presents new NNPDF fits that allow the charm PDF to be fitted, finding these fits describe EMC charm data and have stable gluon and charm PDFs under charm mass variations, with implications for precision LHC calculations.
Strong Higgs Pair Production at the LHC with jet substructurejuanrojochacon
This document discusses strategies for measuring strong double Higgs boson production at the LHC and FCC to test models of electroweak symmetry breaking. In composite Higgs models, vector boson fusion Higgs pair production can be substantially enhanced compared to the Standard Model. Analyzing the di-Higgs mass distribution, especially in boosted topologies, provides the best sensitivity to deviations in Higgs self-couplings from Standard Model predictions. Preliminary results suggest the LHC could probe deviations in the hhVV coupling down to 20-50% depending on the final state, while the FCC could achieve even stronger constraints.
Parton Distributions: future needs, and the role of the High-Luminosity LHCjuanrojochacon
1) Improved PDFs are needed to match the accuracy of higher-order calculations of cross sections and characterize properties of the Higgs boson and search for new physics.
2) The HL-LHC could significantly reduce PDF uncertainties through high-statistics measurements, especially in processes sensitive to large-x gluons and quarks like top quark pair production and Drell-Yan.
3) Preliminary studies generating HL-LHC pseudo-data show PDF uncertainties on the gluon-gluon and quark-antiquark luminosities could be reduced by 10-30% from top pair and Drell-Yan measurements respectively.
PDF uncertainties the LHC made easy: a compression algorithm for the combinat...juanrojochacon
This document summarizes Juan Rojo's presentation on a new method for combining PDF sets called compressed Monte Carlo PDFs (CMC-PDFs). The method involves combining Monte Carlo replicas from different PDF sets, then compressing the large combined set into a smaller set that still accurately reproduces properties like uncertainties. Validation shows CMC-PDFs with only 25 replicas can reproduce uncertainties for a variety of LHC processes, providing a computationally efficient implementation of the PDF4LHC recommendation.
News from NNPDF: new data and fits with intrinsic charmjuanrojochacon
Juan Rojo presented recent work by the NNPDF collaboration including: 1) inclusion of the final HERA legacy dataset which provides a moderate reduction in PDF uncertainties, 2) inclusion of new LHC data which constrains the large-x gluon PDF, and 3) ongoing work to perform fits with intrinsic charm and investigate implications for LHC phenomenology.
The document summarizes the heavy-ion physics program using the Large Hadron Collider (LHC) detectors. It discusses probing novel regimes of high density saturated gluon distributions and qualitatively new physics. Key observables include jet quenching, quarkonia suppression, and heavy flavor modification to study the quark-gluon plasma produced in Pb-Pb collisions. The ALICE, ATLAS and CMS experiments are well-suited to measure bulk properties and select hard probes over a wide momentum range.
Design and Implementation of Low Ripple Low Power Digital Phase-Locked LoopCSCJournals
We propose a phase-locked loop (PLL) architecture, which reduces the double frequency ripple without increasing the order of loop filter. Proposed architecture uses quadrature numerically–controlled oscillator (NCO) to provide two output signals with phase difference of π/2. One of them is subtracted from the input signal before multiplying with the other output of NCO. The system also provides stability in case the input signal has noise in amplitude or phase. The proposed structure is implemented using field programmable gate array (FPGA), which dissipates 15.44mw and works at clock frequency of 155.8 MHz.
This chapter discusses controller design for power electronics. It begins by introducing negative feedback loops and their effects of reducing disturbances and making the output insensitive to variations in the forward path. Key terms like open-loop, closed-loop, loop gain, and transfer functions are defined. Stability is then analyzed using the phase margin test, which evaluates the phase of the loop gain at the crossover frequency to determine if the closed-loop system contains any right half-plane poles. The chapter covers designing compensators to shape the loop gain for stability and performance. It concludes with measuring loop gains using injection techniques.
The document discusses the NNPDF3.1 global analysis of parton distribution functions (PDFs). It provides an update to NNPDF3.0 motivated by new high-precision collider data and progress in NNLO calculations. NNPDF3.1 fits both a perturbative and fitted charm PDF and finds slightly better fit quality for the fitted charm case. Comparisons to NNPDF3.0 show agreement within uncertainties and reduced PDF errors in NNPDF3.1 due to the new LHC data.
This document provides example problems and solutions related to calculating network performance metrics like transfer time and latency. It addresses topics like message segmentation, circuit switching vs packet switching, and calculating bandwidth needs for different media types. Sample problems calculate latency for different network configurations, bandwidth required for streaming high-definition video and audio, and compare transferring a file with and without message segmentation.
The document describes a method called the "Four Russians method" to speed up Bayesian Hidden Markov Model (HMM) classification by exploiting repetition in long observation sequences. The key ideas are to break the observation sequence into blocks of length k and compute the forward variables only at block boundaries, and to sample the hidden state sequence block-by-block from the backward-forward distribution rather than the full backward distribution. This reduces the computational complexity from O(TN^2) to O(TNk/k^2) = O(TN/k).
This document discusses digital modulation techniques. It begins by listing various digital modulation types including ASK, FSK, PSK, MFSK, MPSK, and MSK. It then provides an overview of the digital modulation and demodulation process when used for wireless communication. The key digital modulation techniques of ASK, FSK, and PSK are then explained in more detail. ASK modulates the amplitude of the carrier wave, FSK modulates the frequency, and PSK modulates the phase. Diagrams and equations are provided to illustrate how each modulation type encodes data onto an analog signal. The document concludes by discussing the demodulation of ASK, FSK, and PSK signals.
This document describes using MATLAB to analyze a synthetic time series dataset representing climate data over 500,000 years. The time series contains periodic signals at 100ky, 41ky and 21ky. Random noise and a long term trend are added. Fourier analysis is used to identify the dominant periodic components in the frequency domain. A Hamming window and bandpass filter are applied to further analyze specific frequency bands like the 21ky signal. Autocorrelation is also examined to identify cyclic patterns in the time series.
The document summarizes the NNPDF3.1 global analysis which provides an updated determination of parton distribution functions (PDFs) from experimental data. Key points include:
1) NNPDF3.1 includes new high-precision measurements from the LHC as well as NNLO QCD calculations, allowing more data to be included. It also fits the charm PDF rather than assuming it is purely perturbative.
2) The new data provides stronger constraints on PDFs, particularly the gluon and down quark, significantly reducing their uncertainties. It also shows good agreement with the previous NNPDF3.0 analysis.
3) For the first time, NNPDF3.1 includes LHC
On The Fundamental Aspects of DemodulationCSCJournals
When the instantaneous amplitude, phase and frequency of a carrier wave are modulated with the information signal for transmission, it is known that the receiver works on the basis of the received signal and a knowledge of the carrier frequency. The question is: If the receiver does not have the a priori information about the carrier frequency, is it possible to carry out the demodulation process? This tutorial lecture answers this question by looking into the very fundamental process by which the modulated wave is generated. It critically looks into the energy separation algorithm for signal analysis and suggests modification for distortionless demodulation of an FM signal, and recovery of sub-carrier signals
Constraints on the gluon PDF from top quark differential distributions at NNLOjuanrojochacon
- The document discusses constraints on the gluon PDF from top quark production at hadron colliders.
- It describes using the inclusive top quark pair production cross section to reduce uncertainties in the gluon PDF, especially in the large-x region between 0.1 and 0.5.
- Cross section ratios between different beam energies, such as 8 TeV/7 TeV, are highlighted as powerful precision tests that can discriminate between PDFs and probe BSM physics.
QCD at the LHC: recent progress and open problemsjuanrojochacon
The document discusses recent progress and open problems in QCD at the LHC. It notes that improving the quantitative understanding of the Standard Model is essential, and that sharpening QCD tools could enable new discoveries at the LHC. In particular, better parton distribution functions, higher-order perturbative calculations, and matching calculations to parton showers are highlighted as important for improving both precision and sensitivity to new physics. The talk outlines the current status and future prospects for parton distribution functions, fixed-order calculations up to NNLO, matching to parton showers, and merging samples with different jet multiplicities.
Recent progress in proton and nuclear PDFs at small-xjuanrojochacon
1) The document discusses recent progress in proton and nuclear parton distribution functions (PDFs) at small values of x. PDFs describe the momentum distribution of quarks and gluons inside protons and nuclei.
2) Global analyses of experimental data from various processes are used to determine PDFs at hadronic scales, which are then evolved perturbatively to higher scales relevant for LHC predictions. Recent analyses include data from the LHC.
3) Probing PDFs at small x requires processes dominated by gluons at leading order, produced in the forward region with low invariant masses. Examples discussed are direct photon and charm production. LHCb and future forward calorimeter data provide constraints on the small-
NNPDF3.0: parton distributions for the LHC Run IIjuanrojochacon
NNPDF3.0 is a new PDF determination that includes updated data and theory improvements compared to NNPDF2.3. It includes all HERA-II data and new LHC measurements. The fitting code was rewritten in C++ and validated using closure tests. NNPDF3.0 shows reasonable agreement with NNPDF2.3 while improving descriptions of data and reducing uncertainties in some regions. It provides PDFs for use at the LHC Run II.
Parton Distributions and Standard Model Physics at the LHCjuanrojochacon
This document discusses parton distribution functions (PDFs) and recent developments. It notes that NNLO calculations are essential to reduce uncertainties in PDF analysis. Several key processes like inclusive jet production and top quark production are now available at NNLO. The document also discusses the inclusion of LHC data like W+charm, top quark, and jet data in global PDF fits. It highlights updates to various PDF fitting groups and the upcoming NNPDF3.0 release.
The document discusses the Monash 2013 tune of Pythia 8, which uses the NNPDF2.3LO parton distribution functions (PDFs). It notes that LO PDFs are important for describing non-perturbative physics in event generators. NNPDF2.3LO has a steeper gluon distribution at small values of x compared to the CTEQ6L PDF used in previous tunes. This allows the Monash 2013 tune to better describe precise forward data from experiments like TOTEM and CMS, which probe the gluon PDF in the low-x region.
News from NNPDF: QED, small-x, and alphas(MZ) fitsjuanrojochacon
Juan Rojo presented recent work from the NNPDF collaboration on three spin-off fits from their NNPDF3.1 global analysis: NNPDF3.1QED, fits including small-x resummation, and a determination of the strong coupling constant αS(mZ). For NNPDF3.1QED, they are imposing the LUXqed formalism to constrain the photon PDF rather than extracting it from data. For small-x resummation fits, they find that including NNLO+NLLx theory stabilizes the small-x gluon and improves description of HERA data. Their preliminary αS(mZ) value is consistent with other determinations.
This document discusses parton distribution functions (PDFs) with intrinsic charm. It presents the motivation for fitting a charm PDF in global analyses, including stabilizing charm mass dependence, quantifying the non-perturbative charm component, and exploring implications for LHC phenomenology. The document summarizes previous fits allowing for intrinsic charm and issues they faced. It then presents new NNPDF fits that allow the charm PDF to be fitted, finding these fits describe EMC charm data and have stable gluon and charm PDFs under charm mass variations, with implications for precision LHC calculations.
Strong Higgs Pair Production at the LHC with jet substructurejuanrojochacon
This document discusses strategies for measuring strong double Higgs boson production at the LHC and FCC to test models of electroweak symmetry breaking. In composite Higgs models, vector boson fusion Higgs pair production can be substantially enhanced compared to the Standard Model. Analyzing the di-Higgs mass distribution, especially in boosted topologies, provides the best sensitivity to deviations in Higgs self-couplings from Standard Model predictions. Preliminary results suggest the LHC could probe deviations in the hhVV coupling down to 20-50% depending on the final state, while the FCC could achieve even stronger constraints.
Parton Distributions: future needs, and the role of the High-Luminosity LHCjuanrojochacon
1) Improved PDFs are needed to match the accuracy of higher-order calculations of cross sections and characterize properties of the Higgs boson and search for new physics.
2) The HL-LHC could significantly reduce PDF uncertainties through high-statistics measurements, especially in processes sensitive to large-x gluons and quarks like top quark pair production and Drell-Yan.
3) Preliminary studies generating HL-LHC pseudo-data show PDF uncertainties on the gluon-gluon and quark-antiquark luminosities could be reduced by 10-30% from top pair and Drell-Yan measurements respectively.
PDF uncertainties the LHC made easy: a compression algorithm for the combinat...juanrojochacon
This document summarizes Juan Rojo's presentation on a new method for combining PDF sets called compressed Monte Carlo PDFs (CMC-PDFs). The method involves combining Monte Carlo replicas from different PDF sets, then compressing the large combined set into a smaller set that still accurately reproduces properties like uncertainties. Validation shows CMC-PDFs with only 25 replicas can reproduce uncertainties for a variety of LHC processes, providing a computationally efficient implementation of the PDF4LHC recommendation.
News from NNPDF: new data and fits with intrinsic charmjuanrojochacon
Juan Rojo presented recent work by the NNPDF collaboration including: 1) inclusion of the final HERA legacy dataset which provides a moderate reduction in PDF uncertainties, 2) inclusion of new LHC data which constrains the large-x gluon PDF, and 3) ongoing work to perform fits with intrinsic charm and investigate implications for LHC phenomenology.
The document summarizes the heavy-ion physics program using the Large Hadron Collider (LHC) detectors. It discusses probing novel regimes of high density saturated gluon distributions and qualitatively new physics. Key observables include jet quenching, quarkonia suppression, and heavy flavor modification to study the quark-gluon plasma produced in Pb-Pb collisions. The ALICE, ATLAS and CMS experiments are well-suited to measure bulk properties and select hard probes over a wide momentum range.
Design and Implementation of Low Ripple Low Power Digital Phase-Locked LoopCSCJournals
We propose a phase-locked loop (PLL) architecture, which reduces the double frequency ripple without increasing the order of loop filter. Proposed architecture uses quadrature numerically–controlled oscillator (NCO) to provide two output signals with phase difference of π/2. One of them is subtracted from the input signal before multiplying with the other output of NCO. The system also provides stability in case the input signal has noise in amplitude or phase. The proposed structure is implemented using field programmable gate array (FPGA), which dissipates 15.44mw and works at clock frequency of 155.8 MHz.
This chapter discusses controller design for power electronics. It begins by introducing negative feedback loops and their effects of reducing disturbances and making the output insensitive to variations in the forward path. Key terms like open-loop, closed-loop, loop gain, and transfer functions are defined. Stability is then analyzed using the phase margin test, which evaluates the phase of the loop gain at the crossover frequency to determine if the closed-loop system contains any right half-plane poles. The chapter covers designing compensators to shape the loop gain for stability and performance. It concludes with measuring loop gains using injection techniques.
PDFs at the LHC: Lessons from Run I and preparation for Run IIjuanrojochacon
This document summarizes parton distribution functions (PDFs) at the start of LHC Run II. It discusses the status of recent PDF sets from NNPDF, MMHT, CT, ABM, and HERAPDF. It notes some differences between these sets and the importance of PDF uncertainties for LHC measurements. The document also discusses benchmarks between PDF sets, comparisons using the APFEL online tool, and the prospects for including more ATLAS data in global PDF fits to further constrain PDFs.
Neural Network Fits of Parton DistributionsJuan Rojo
The document discusses neural network fits of parton distribution functions (PDFs). It describes the NNPDF approach, which uses artificial neural networks as universal interpolators to parametrize PDFs without theoretical bias, in contrast to traditional approaches. The NNPDF method also uses a Monte Carlo replica method to estimate PDF uncertainties without linear approximations. Recent NNPDF results include determinations of PDFs including quantum electrodynamics corrections and an investigation of the intrinsic charm content of the proton.
Parton distributions in the LHC precision erajuanrojochacon
This document summarizes Juan Rojo's presentation on parton distribution functions (PDFs) at the Zurich Phenomenology Workshop 2018. The key points are:
1) PDF fits require combining perturbative cross-sections calculated using the Standard Model Lagrangian with non-perturbative PDFs extracted from a global analysis of experimental data.
2) More precise PDFs are needed to reduce uncertainties on calculations of processes like Higgs production and measurements of its couplings at the LHC.
3) Recent PDF analyses have included new data like differential top quark production from LHC and NNLO calculations, improving determinations of the gluon PDF over a wide range of x values.
4) Small-x data
The document discusses a lecture on PID control. It begins by defining proportional, derivative, and integral control and how each component works. It then discusses tuning strategies for PID controllers, including how changing each gain affects time and frequency response. The document provides examples of implementing proportional, PI, PD, and PID control for first and second order systems. It concludes by discussing PID tuning and methods for choosing gains either with or without a model of the system.
The document discusses PID control, which combines proportional, integral and derivative control actions. It explains each control action and its effects on the system response and stability. Proportional control reduces steady-state error but can cause oscillation. Integral control eliminates steady-state error but also causes oscillation. Derivative control reduces overshoot and damping but increases sensitivity to noise. PID controllers combine these actions to achieve desired response without oscillations or steady-state error. The document provides examples of tuning the gains of each action.
Similar to New dynamics in parton distributions at a 100 TeV hadron collider (20)
Higgs Pair Production at the LHC and future collidersjuanrojochacon
Juan Rojo gave a seminar at Boston University Physics on November 26th, 2018 about Higgs pair production at the LHC and future colliders. He discussed how measuring Higgs pair production can provide insights into the Higgs sector and electroweak symmetry breaking. However, observing Higgs pair production is challenging due to small cross-sections in the standard model. Future colliders with higher energies, like the FCC, may enable more precise studies of Higgs pair production and help address open questions in particle physics.
Parton distributions from high-precision collider datajuanrojochacon
Juan Rojo gave a seminar at the Technical University of Munich on July 13, 2017 about parton distributions from high-precision collider data. He discussed how parton distribution functions are essential for calculating cross sections at hadron colliders like the LHC, since they describe the probability of finding quarks and gluons within protons. Rojo explained that global analyses fit PDFs to diverse experimental data using statistical techniques like neural networks, and the PDFs can then provide predictions for new processes. He highlighted recent updates from the NNPDF collaboration in version 3.1 to include more precise LHC data and the option to fit the charm quark distribution.
Higgs pair production in vector-boson fusion at the LHC and beyondjuanrojochacon
The document discusses Higgs pair production, which can help uncover the mechanism of electroweak symmetry breaking. Double Higgs production allows reconstructing the full Higgs potential and probing the Higgs self-interaction. While production rates are small in the Standard Model, deviations from SM couplings could significantly increase rates. The document focuses on vector boson fusion channel, where requiring two forward jets and vetoing central jets can reduce backgrounds, and sensitivity to non-SM couplings improves at high di-Higgs invariant masses. Precision studies of Higgs pair production may reveal insights into electroweak symmetry breaking and new physics.
Precision determination of the small-x gluon from charm production at LHCbjuanrojochacon
This document discusses using LHCb data on charm production to constrain the small-x gluon and improve predictions for neutrino fluxes. LHCb data at 7 TeV, 5 TeV and 13 TeV provides stringent constraints on the small-x gluon beyond HERA. This improved gluon allows more accurate predictions for signals and backgrounds at neutrino telescopes. At a 100 TeV collider, inclusive cross sections depend directly on small-x PDFs, but using LHCb data leads to stabilized predictions with reduced uncertainties.
This document discusses potential areas where lattice QCD calculations could provide input to help constrain parton distribution functions (PDFs) which are currently not well known. It identifies "benchmarks" where PDFs are already well determined, as well as "opportunities" where lattice calculations could have more impact. These include PDFs at large values of Bjorken x, the strange quark content of the proton, and charm content. The document also discusses how lattice data could be included in PDF global fits to help reduce PDF uncertainties.
Discovery through precision: perturbative QCD at the dawn of the LHC Run IIjuanrojochacon
This document summarizes a seminar given by Juan Rojo on perturbative QCD at the dawn of LHC Run II. In the seminar, Rojo discussed how recent advances in perturbative QCD, such as higher precision parton distribution functions and higher-order calculations, have improved the prospects for new physics searches at the LHC. Rojo also presented recent work on topics like PDFs with threshold resummation, Higgs pair production, and charm production that further push the boundaries of perturbative QCD and its applications at the LHC.
Parton Distributions and the search for New Physics at the LHCjuanrojochacon
Juan Rojo gave a seminar at King's College London on September 23, 2015 about parton distribution functions (PDFs) and their importance for precision physics at the Large Hadron Collider (LHC). PDFs describe the momentum distributions of quarks and gluons within protons and are crucial for determining cross sections and uncertainties for many LHC processes. The accurate determination of PDFs requires global analyses of experimental data using flexible parametrizations like neural networks to avoid biases. PDF uncertainties now limit characterization of the Higgs boson and searches for new physics at the LHC.
CERN, Particle Physics and the Large Hadron Colliderjuanrojochacon
The document discusses particle physics research done at CERN using the Large Hadron Collider (LHC). It describes the LHC as the most powerful particle accelerator ever built, with a 27km long tunnel housing four detectors. The LHC collides protons together at high energies to study their constituent particles like quarks and search for new particles like the Higgs boson. It also allows researchers to recreate conditions shortly after the Big Bang and potentially observe mini black holes or extra dimensions at very small scales. The future includes planning for an even larger successor to the LHC to continue advancing understanding of fundamental physics.
The structure of the proton in the Higgs boson erajuanrojochacon
Juan Rojo gave a seminar at SLAC on July 4th, 2015 about the structure of the proton in the Higgs boson era and the role of the Large Hadron Collider. He discussed how the discovery of the Higgs boson completed the Standard Model but also opened new questions. Determining the parton distribution functions of protons with precision is important for phenomenology at the LHC, such as characterizing Higgs couplings and searching for new physics. Over the next 20 years, the LHC will play a key role in exploring these open questions.
Particle Physics, CERN and the Large Hadron Colliderjuanrojochacon
The document discusses particle physics research done at CERN's Large Hadron Collider (LHC). It describes the LHC as the most powerful particle accelerator ever built, with a 27 km long tunnel housing detectors that observe proton collisions at very high energies. One of the LHC's major discoveries was the Higgs boson particle in 2012. The document outlines how the LHC allows scientists to study the fundamental building blocks of matter at the smallest observable scales.
PDF uncertainties and the W mass: Report from the Workshop “Parton Distributi...juanrojochacon
The document summarizes discussions from a workshop about reducing uncertainties in parton distribution functions (PDFs) that affect measurements of the W boson mass. Key topics discussed included issues modeling the Z boson's transverse momentum, inconsistencies between PDF sets, and the need for additional LHC measurements like of W/Z production to reduce PDF uncertainties in future W mass measurements to below 10 MeV. Participants agreed more work is needed to understand differences between PDF sets and include relevant LHC data in global fits.
Characterizing New Physics with Polarized Beams in Hadron Collisionsjuanrojochacon
This document discusses how polarized proton beams could help characterize new physics discovered at the LHC or FCC. Polarized and unpolarized parton distribution functions have different behaviors, so cross sections with polarized beams would provide insights into couplings to different quark flavors. Single and double spin asymmetries could distinguish between new physics models that predict similar unpolarized signatures. While more study is needed, polarized beams could significantly aid understanding of the structure and couplings of any discovered heavy new particles.
The Standard Model and the LHC in the Higgs Boson Erajuanrojochacon
The document discusses the Standard Model of particle physics and the role of the Large Hadron Collider (LHC) following the discovery of the Higgs boson. It provides background on the development of the Standard Model and discovery of its key particles like quarks, gluons, and weak bosons. It describes the LHC as the most powerful particle collider built to explore physics at the highest energies and probe unanswered questions left by the Standard Model. Four main detectors at the LHC, including ATLAS and CMS, precisely measure collision products to explore fundamental particles and forces.
The Structure of the Proton in the Higgs Boson Erajuanrojochacon
Juan Rojo gave a seminar at NIKHEF in Amsterdam on January 22, 2015 about the structure of the proton in the Higgs boson era. He discussed how the discovery of the Higgs boson completed the Standard Model but also opened new questions. He explained that the Large Hadron Collider will play a key role in exploring these questions over the next 20 years. Accurately determining the parton distribution functions of the proton is vital for phenomenology at the LHC.
Boosting Strong Higgs Pair Production at the LHCjuanrojochacon
This document summarizes Juan Rojo's presentation on boosting strong Higgs pair production at the LHC. The key points are:
1) Higgs pair production allows for stringent tests of the understanding of electroweak symmetry breaking, but has low rates in the Standard Model.
2) Higgs pair production in vector boson fusion is small in the Standard Model but provides unique information on the hhVV coupling. It can be substantially enhanced in composite Higgs models.
3) Preliminary results show the hhVV coupling can be measured with 25-30% precision at the 14 TeV LHC with 300 fb-1, and 10-15% precision with 3000 fb-1, while the FCC could achieve
aMCfast: Automation of Fast NLO Computations for PDF fitsjuanrojochacon
MadGraph5_aMCatNLO provides NLO calculations for arbitrary processes and their matching to parton showers, but existing fast interfaces are limited. A new tool called aMCfast provides a fast interface to MadGraph5_aMCatNLO, allowing its predictions to be used in global PDF fits. It precomputes matrix elements and interpolates them using grids, then reconstructs distributions for any PDFs or scales. This will increase the number and accuracy of processes in PDF fits, including electroweak corrections and photon-initiated effects, improving determination of PDFs from LHC data.
Chapter wise All Notes of First year Basic Civil Engineering.pptxDenish Jangid
Chapter wise All Notes of First year Basic Civil Engineering
Syllabus
Chapter-1
Introduction to objective, scope and outcome the subject
Chapter 2
Introduction: Scope and Specialization of Civil Engineering, Role of civil Engineer in Society, Impact of infrastructural development on economy of country.
Chapter 3
Surveying: Object Principles & Types of Surveying; Site Plans, Plans & Maps; Scales & Unit of different Measurements.
Linear Measurements: Instruments used. Linear Measurement by Tape, Ranging out Survey Lines and overcoming Obstructions; Measurements on sloping ground; Tape corrections, conventional symbols. Angular Measurements: Instruments used; Introduction to Compass Surveying, Bearings and Longitude & Latitude of a Line, Introduction to total station.
Levelling: Instrument used Object of levelling, Methods of levelling in brief, and Contour maps.
Chapter 4
Buildings: Selection of site for Buildings, Layout of Building Plan, Types of buildings, Plinth area, carpet area, floor space index, Introduction to building byelaws, concept of sun light & ventilation. Components of Buildings & their functions, Basic concept of R.C.C., Introduction to types of foundation
Chapter 5
Transportation: Introduction to Transportation Engineering; Traffic and Road Safety: Types and Characteristics of Various Modes of Transportation; Various Road Traffic Signs, Causes of Accidents and Road Safety Measures.
Chapter 6
Environmental Engineering: Environmental Pollution, Environmental Acts and Regulations, Functional Concepts of Ecology, Basics of Species, Biodiversity, Ecosystem, Hydrological Cycle; Chemical Cycles: Carbon, Nitrogen & Phosphorus; Energy Flow in Ecosystems.
Water Pollution: Water Quality standards, Introduction to Treatment & Disposal of Waste Water. Reuse and Saving of Water, Rain Water Harvesting. Solid Waste Management: Classification of Solid Waste, Collection, Transportation and Disposal of Solid. Recycling of Solid Waste: Energy Recovery, Sanitary Landfill, On-Site Sanitation. Air & Noise Pollution: Primary and Secondary air pollutants, Harmful effects of Air Pollution, Control of Air Pollution. . Noise Pollution Harmful Effects of noise pollution, control of noise pollution, Global warming & Climate Change, Ozone depletion, Greenhouse effect
Text Books:
1. Palancharmy, Basic Civil Engineering, McGraw Hill publishers.
2. Satheesh Gopi, Basic Civil Engineering, Pearson Publishers.
3. Ketki Rangwala Dalal, Essentials of Civil Engineering, Charotar Publishing House.
4. BCP, Surveying volume 1
Philippine Edukasyong Pantahanan at Pangkabuhayan (EPP) CurriculumMJDuyan
(𝐓𝐋𝐄 𝟏𝟎𝟎) (𝐋𝐞𝐬𝐬𝐨𝐧 𝟏)-𝐏𝐫𝐞𝐥𝐢𝐦𝐬
𝐃𝐢𝐬𝐜𝐮𝐬𝐬 𝐭𝐡𝐞 𝐄𝐏𝐏 𝐂𝐮𝐫𝐫𝐢𝐜𝐮𝐥𝐮𝐦 𝐢𝐧 𝐭𝐡𝐞 𝐏𝐡𝐢𝐥𝐢𝐩𝐩𝐢𝐧𝐞𝐬:
- Understand the goals and objectives of the Edukasyong Pantahanan at Pangkabuhayan (EPP) curriculum, recognizing its importance in fostering practical life skills and values among students. Students will also be able to identify the key components and subjects covered, such as agriculture, home economics, industrial arts, and information and communication technology.
𝐄𝐱𝐩𝐥𝐚𝐢𝐧 𝐭𝐡𝐞 𝐍𝐚𝐭𝐮𝐫𝐞 𝐚𝐧𝐝 𝐒𝐜𝐨𝐩𝐞 𝐨𝐟 𝐚𝐧 𝐄𝐧𝐭𝐫𝐞𝐩𝐫𝐞𝐧𝐞𝐮𝐫:
-Define entrepreneurship, distinguishing it from general business activities by emphasizing its focus on innovation, risk-taking, and value creation. Students will describe the characteristics and traits of successful entrepreneurs, including their roles and responsibilities, and discuss the broader economic and social impacts of entrepreneurial activities on both local and global scales.
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A proprietary approach developed by bringing together the best of learning theories from Psychology, design principles from the world of visualization, and pedagogical methods from over a decade of training experience, that enables you to: Learn better, faster!
Juneteenth Freedom Day 2024 David Douglas School District
New dynamics in parton distributions at a 100 TeV hadron collider
1. Parton Distributions
at a 100 TeV Hadron Collider
Juan Rojo
CERN, PH Division, TH Unit
Future Circular Colliders Kick-off Meeting
Geneva, 14.02.2014
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
2. Exploratory first study on the role of Parton Distributions at a Future Circular
Collider with CoM of 100 TeV
Concentrate on the basic results, avoid technical details (choice of PDF set etc),
and explore the new qualitative features of PDFs at the FCC
Outline of this talk:
Kinematic coverage from LHC 14 TeV to FCC 100 TeV
PDF luminosities from 14 to 100 TeV
New qualitative features of PDF in 100 TeV collisions: top-quark PDFs, LO
small-x PDFs, Electroweak corrections, high-energy BFKL resummation
Physics case for polarized collisions at the FCC
2
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
3. Kinematic Coverage and
PDF Luminosities:
From LHC14 to FCC100
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
4. At Born level, for the production of a particle at rapidity y with mass M, the PDFs are evaluated at
Going from Ecm=14 TeV to Ecm=100 TeV, for a given M and y knowledge of PDFs at smaller x is
required:
x1,20( S=100 TeV ) = 0.14 x1,20( S=14 TeV )
In addition, for fixed M, the increased range in y allows to prove even further smaller x
Conversely, fixing x1,20 and y, the increased center of mass energy implies that higher masses will
be probed:
M( S=100 TeV ) = 7.14 M( S=14 TeV )
But recall that hadronic cross-sections fall as 1/M2 so this is not how BSM mass reach scales!
Some consequences:
For Higgs and SM probes (tt, W, Z), PDFs will be proved (at least) one order of magnitude
smaller x
For possible new high-mass particles of mass M, large-x PDFs (required at 14 TeV) turn into
medium-x PDFs (at 100 TeV), not only leading to larger cross-sections but with less uncertainties
For small masses M, a completely new kinematical range opens that has never been explored
4
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
5. Kinematics of a 100 TeV FCC
Plot by J. Rojo, Dec 2013
105
FCC 100 TeV
MX ( GeV )
104
LHC 14 TeV
3
10
102
10
y=-8
1 -10
10
5
Juan Rojo
-9
10
y=-4
-8
10
10-7
y=0
-6
10
-5
10
x
y=4
10-4
-3
10
y=8
10-2
10-1
FCC Kick-off Meeting, Geneva, 14/02/2014
6. Kinematics of a 100 TeV FCC
Plot by J. Rojo, Dec 2013
105
20 TeV Z’
FCC 100 TeV
MX ( GeV )
104
2 TeV squarks
LHC 14 TeV
3
10
Higgs, top
102
W,Z
DY, low-pt jets
10
y=-8
1 -10
10
6
Juan Rojo
-9
10
y=-4
-8
10
10-7
y=0
-6
10
-5
10
x
y=4
10-4
-3
10
y=8
10-2
10-1
FCC Kick-off Meeting, Geneva, 14/02/2014
7. NNPDF2.3 dataset
Kinematics of a 100 TeV FCC
Plot by J. Rojo, Dec 2013
105
107
NMC-pd
NMC
SLAC
BCDMS
6
5
10
LHC 14 TeV
103
HERAI-AV
CHORUS
FLH108
Q2 / M2 / p2 [ GeV2 ]
T
MX ( GeV )
10
FCC 100 TeV
104
ZEUS-H2
ZEUSF2C
H1F2C
104
102
NTVDMN
DYE605
DYE886
CDFWASY
3
10
CDFZRAP
D0ZRAP
CDFR2KT
D0R2CON
102
10
ATLAS-WZ-36pb
CMS-WEASY-840PB
LHCB-WZ-36pb
ATLAS-JETS-10
y=-8
1 -10
10
-9
10
y=-4
-8
10
10-7
y=0
-6
10
-5
10
x
y=4
10-4
-3
10
y=8
10-2
10-1
10
1 -5
10
10-4
-3
10
x
10-2
10-1
Compare kinematical coverage to that of the NNPDF2.3 set:
Current PDF determinations have essentially no constraints for x < 10-4
The region of masses for M>1 TeV also unconstrained: rely on DGLAP evolution extrapolation
Poor constraints on high-x PDFs, relevant for high masses M
For M > 10 GeV, constraints from HERA only available for x > 10-3
Global PDF fits rely on QCD evolution, but EW effects will be required in multi-TeV region
7
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
1
8. Compare the ratio of PDF luminosities between 100 TeV and 14 TeV in different channels as a
function of the final state mass
100 TeV vs 14 TeV PDF Luminosities, NNPDF2.3 NNLO
PDF luminosity ratio 100 TeV / 14 TeV
108
107
For final state masses M < 1
TeV moderate increase in PDF
luminosity, between a factor 10
and 100
106
105
104
For M > 1 TeV, much steeper
increase (since 14 TeV lumis
damped by large-x PDFs), up
to a factor 108 for M = 10 TeV
103
102
10
1
8
gg lumi ratio
102
Juan Rojo
10
3
MX [ GeV ]
104
Qualitative similar behavior
for other PDF luminosities
FCC Kick-off Meeting, Geneva, 14/02/2014
9. New qualitative features of
PDFs in 100 TeV collisions
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
10. At FCC100, the production of 100 GeV particles might require knowledge of PDFs down to x=1e-6, 1e-7,
depending on acceptance
For other processes, both perturbative (low mass Drell-Yan, Quarkonium production, low pt photons
and jets) and non-perturbative (Underlying Event, Minimum Bias) we need PDFs down to x=1e-8, 1e-9
Compare various PDFs at very small x out of the box using LHAPDF5.9.0: small-x PDFs frozen between
1e-6 and 1e-8 depending on the PDF set
Small-x NNLO PDFs for FCC studies
NNPDF2.3
CT10
cteq6
MSTW08
2
103
102
10-9
10
NNPDF2.3
CT10
cteq6
MSTW08
104
x u ( x, Q2)
104
x g ( x, Q )
Small-x NNLO PDFs for FCC studies
103
102
10-8
10-7
Juan Rojo
10-6
x
10-5
10-4
10-3
10-9
10-8
10-7
10-6
x
10-5
10-4
FCC Kick-off Meeting, Geneva, 14/02/2014
10-3
11. This is not a fundamental problem: is easy enough to provide a extrapolation down to very small-x ...
... but this extrapolation must be driven by theory + methodology, since no data available
The NNPDF2.3LO set can be extrapolated down to 1e-9 using the neural network extrapolation: huge
PDF uncertainties, but central values turn out to have a reasonable behavior
NNPDF2.3LO PDF set is already available as standalone code in Pythia8, where there is an ongoing
tuning effort. Torbjorn has been using it to provide UE predictions for FCC finding reasonable results
xg(x,Q), NNPDF23_lo_as_0119_qed.LHgrid members
500
Members
Generated by APFEL2.0.0: V.Bertone, S.Carrazza, J.Rojo (arXiv:1310.1394)
Central value
Std. deviation
400
68% c.l.
Q = 1.41 GeV
300
200
100
0
-9
10
11
Juan Rojo
-8
10
10-7
-6
10
-5
10
x
10-4
-3
10
10-2
10-1
1
FCC Kick-off Meeting, Geneva, 14/02/2014
12. In the Variable-Flavor-Number (VFN) scheme, heavy quark PDFs for charm and bottom are generated
radiatively from the gluon PDF
For very high-mass production at a 100 TeV FCC, the top quark can be considered as approximately
massless, and thus we need to generate a top quark PDF t(x,Q) just as we have a charm and bottom PDF
Note that missing the top PDF also feeds back into all other PDFs due to the different DGLAP evolution
Ratio to NNPDF2.1 GM-VFN, x=10-2
Ratio to NNPDF2.1 GM-VFN, x=10-2
1.15
missing charm
1.1
NNPDF2.1
1.2
NNPDF2.1 FFN NF=3
1.1
NNPDF2.1 FFN NF=4
x (x, Q 2)
xg (x, Q2)
1.05
1
1
0.9
0.95
NNPDF2.1
NNPDF2.1 FFN NF=3
0.9
missing charm
0.8
NNPDF2.1 FFN NF=4
0.85
10
12
Juan Rojo
102
Q 2 [ GeV 2 ]
3
10
104
0.7
10
102
Q 2 [ GeV 2 ]
3
10
FCC Kick-off Meeting, Geneva, 14/02/2014
104
13. Currently, only the NNPDF Collaboration provides sets with top quark PDF included (as well as sets in
the other VFN schemes, NF=3, NF=4 and NF=5)
At 10 TeV, the top quark PDF t(x,Q) is only a factor 2 smaller that all other quark PDFs (charm and
bottom are very close to light quark PDFs): should be included in theoretical predictions
2
x PDF ( x, Q = 10 TeV )
NNPDF2.3 NNLO NF = 6
102
Gluon PDF
Up quark PDF
10
Top PDF
1
10-1 -5
10
13
Gluon
Up
Charm
Bottom
Top
Juan Rojo
10-4
-3
10
x
10-2
10-1
FCC Kick-off Meeting, Geneva, 14/02/2014
14. As mentioned in the case of top quark, when Q >> mt it makes sense computationally to resum
large collinear-like logarithms into a top PDF
With a similar motivation, it might be efficient to resum multiple initial state emissions of W and Z
bosons into the corresponding parton distributions, FW(x,Q), FZ(x,Q)
The analogous of DGLAP evolution equations in QCD can be derived in the electroweak sector of
the Standard Model, but the resulting equations are very different (Ciafaloni and Comelli,
2002,2005)
The purely electroweak evolution equations must be supplemented with the QED evolution
equations and the determination of the photon PDF
(x,Q2) from experimental data
(NNPDF2.3QED)
An important difference between QED and EW evolution is that in the later case W and Z boson
PDFs are always generated dynamically, while there is an intrinsic photon PDF in the proton
14
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
15. The analogous of DGLAP evolution equations in QCD can be derived in the electroweak sector of
the Standard Model, but the resulting equations are very different (Ciafaloni and Comelli, 2002,2005)
Evolution equation for the structure function of W bosons
No numerical implementation of EW evolution equations exist. Very different flavor/coupling
structure as compared to QCD evolution equations
In addition, EW must be combined with pure QED evolution, and then combined with QCD into
a complete set of Standard Model PDF evolution equations
15
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
16. Once QED corrections to PDFs are taken into account, photon-initiated contributions are relevant
at the LHC, could be even more the case at the FCC
Many examples, like photon-initiated corrections substantially modify the lepton pt in high-mass
Drell-Yan
They also induce substantial uncertainties for high-mass WW production, up to 100%
More FCC-specific studies required
WW production @ LHC 100 TeV, 68% CL
high-mass DY
σ(WW) [QCD+QED] / σ(WW) [QCD]
2.5
2
WW at FCC100
1.5
1
NNPDF2.3 QED, qq
0.5
(QCD+QED)/QCD
MRST04 QED, qq
NNPDF2.3 QED, qq + γ γ
MRST04 QED, qq + γ γ
0
0
16
Boughezal, Li, Petriello 2013
Juan Rojo
1000
2000
3000
4000
5000
Mcut ( GeV )
WW
6000
7000
8000
Snowmass QCD report
FCC Kick-off Meeting, Geneva, 14/02/2014
17. The kinematical coverage of the FCC reaches the small-x region where the usual DGLAP PDF
evolution might need to be completed with BFKL high-energy (small-x) resummation
Combining DGLAP and BFKL stabilizes the perturbative expansion of DGLAP evolution at small-x
gluon-gluon DGLAP kernel
The theory for DIS known (Altarelli, Ball, Forte 08, Ciafaloni, Colferai, Salam, Stasto 07), more
theoretical progress is required for computation of relevant hadronic cross sections at the FCC
17
Juan Rojo
DGLAP+BFKL
DGLAP NNLO
FCC Kick-off Meeting, Geneva, 14/02/2014
18. Crucial milestone for the next years is to produce a global PDF fit which combines NNLO DGLAP
evolution with NLL BFKL resummation
This would be a pre-requisite to study the relevance of high-energy resummation at the FCC,
specially for benchmark processes like Higgs, W, Z and top production
Ratio g(x,Q)/gNLO(x,Q)
High-energy resummation affects mostly the gluon PDF, and then feeds to all the quark PDFs
18
Juan Rojo
DGLAP NNLO
DGLAP+BFKL
x=10-4
FCC Kick-off Meeting, Geneva, 14/02/2014
19. The Physics Case for
Polarized Collisions at the FCC
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
20. What are the BSM opportunities for the polarized option of a 100 TeV machine?
Polarized beams could provide a useful tool for BSM characterization, where differences in polarized
asymmetries provide a handle on SM vs BSM discrimination
NNPDF2.3, Q2 = 104 GeV2
0.8
0.6
xd
xs
0.5
2
x ∆ q ( x, Q )
0.5
x∆g
x∆u
x∆d
x∆s
0.7
xu
0.6
2
0.8
xg
0.7
x q ( x, Q )
NNPDFpol1.1, Q2 = 104 GeV2
0.4
0.3
0.2
0.4
0.3
0.2
0.1
0.1
0
0
-0.1
-0.1
10-2
10-1
x
10-2
10-1
x
Different qualitative behaviors of PDFs wrt unpolarized PDFs
Polarized PDFs smaller than unpolarized due to positivity condition
and suppressed at small-x due to different DGLAP splitting functions
Only asymmetries which involve high-x polarized PDFs (final states with large invariant mass)
will be large enough to be accessible experimentally
20
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
21. Fuks, Proudom, Rojo, Schienbein,
in preparation
Measurement of sign of AL will discriminate between different BSM scenarios (different production modes)
21
A more precise measurement of AL leads to enhanced discrimination, ie, qq vs gg production mechanisms
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
22. Parton Distributions play a central role at the LHC program, will continue to do so
at a Future Circular Collider at 100 TeV
Many new qualitative features of PDFs need to be studied: top PDF, PDFs at very
large-x, PDFs with electroweak corrections, PDFs with high-energy resummation
It will be useful to provide specific PDF sets for FCC studies, with suitable
extrapolations at very small and very large-x as well as to a very large Q2 (and
include top PDF)
A polarized mode of the FCC might provide a unique way of characterizing BSM
dynamics uncovered in unpolarized collisions
22
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
23. High-mass production at FCC will probe PDFs at very high-x, we want to make sure that available PDF
sets properly extrapolate in this region
Michelangelo reported some weeks ago that using CTEQ at very large x returns zero
I have tried using LHAPDF5.9.0 with CT10, MSTW08 and NNPDF2.3. Consider only central PDF sets
(ignore for the time being PDF uncertainties), for Q = 10 TeV
Large-x PDFs seems to behave properly at very large-x, though MSTW08 extrapolation has a peculiar
behavior, at least using the LHAPDF library
Note substantial differences for d(x,Q) at high-x
Large-x NNLO PDFs for FCC studies
Large-x NNLO PDFs for FCC studies
NNPDF2.3
10-1
10-1
CT10
-2
CT10
-2
10
MSTW08
-3
10
MSTW08
-3
10
x d ( x, Q2)
10
x g ( x, Q2)
NNPDF2.3
10-4
10-4
10-5
10-5
10-6
10-7
10-7
10-8
0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95
x
23
10-6
10-8
0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95
x
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014
24. At 10 TeV, the top quark PDF t(x,Q) is only a factor 2/3 smaller that all other quark PDFs (charm and
bottom are very close to light quark PDFs): should be included in theoretical predictions
The missing contribution from t(x,Q) also feeds back to the gluon PDF: up to 4% differences due to the
missing top quark PDF
NNPDF2.3 NNLO, x = 10-2
1.06
1.04
F
Ratio ( N = 5 ) / ( N = 6 )
1.05
Gluon
Up
Down
NF=6 vs NF=5
1.03
F
1.02
1.01
1
0.99
0.98
102
24
Juan Rojo
3
Q10GeV )
(
104
FCC Kick-off Meeting, Geneva, 14/02/2014
25. 100 TeV vs 14 TeV PDF Luminosities, NNPDF2.3 NNLO
PDF luminosity ratio 100 TeV / 14 TeV
108
107
106
GG
QG
QQbar
QQ
105
104
103
102
10
1
102
10
3
MX [ GeV ]
104
Gluon-initiated processes grow faster than quark initiated from 14 to 100 TeV
Very large PDF uncertainties affect QQbar luminosities since large-x antiquarks poorly
known
Using these results, it is possible to estimate how the cross-sections for different processes
will increase when going from 14 TeV to 100 TeV
25
Juan Rojo
FCC Kick-off Meeting, Geneva, 14/02/2014