/******************************************************************************************** * Public members, functions and properties ********************************************************************************************/ public void Initialize( JobOrganizer jobOrganizer, ToolTipMaker toolTipMaker ) { Initialize(jobOrganizer); MakeToolTips(toolTipMaker); }
private void MakeToolTips( ToolTipMaker toolTipMaker ) { toolTipMaker.Add( "Choose which decay widths are used by specifying the potential types used in SingleQQ." + " The choice should be unique for every temperature.", LblPotentialTypes, MsxPotentialTypes); }
private void MakeToolTips( ToolTipMaker toolTipMaker ) { toolTipMaker.Add( "Chosen approximation for the calculation of the electromagnetic field.", LblEMFCalculationMethod, CbxEMFCalculationMethod); toolTipMaker.Add( "Name of the output file. The standard output path can be set" + Environment.NewLine + "in the menu \"File\" using \"Set output path\".", LblDataFileName, TbxDataFileName); }
private void SetToolTipMaker() { ToolTip prototype = new ToolTip { AutoPopDelay = 15000, InitialDelay = 500, ReshowDelay = 500, ShowAlways = true }; ToolTipMaker = new ToolTipMaker(prototype); }
private void MakeToolTips( ToolTipMaker toolTipMaker ) { toolTipMaker.Add( "In-medium bottomium decay widths depend on temperature, velocity and angle" + Environment.NewLine + "relative to the velocity vector. The decay width as a function of temperature and" + Environment.NewLine + "velocity is calculated as an average over the solid angle. The average is calculated" + Environment.NewLine + "from samples of dedicated azimuthal angles given by the user.", GbxGeneralParams); toolTipMaker.Add( "Temperatures in MeV to be considered in the calculation.", LblMediumTemperatures, TbxMediumTemperatures); toolTipMaker.Add( "Velocities of the QGP medium in the bottomium rest frame in units of c.", LblMediumVelocities, TbxMediumVelocities); toolTipMaker.Add( "Number of angles relative to the velocity vector from which the angular average is calculated.", LblNumberAveragingAngles, TbxNumberAveragingAngles); toolTipMaker.Add( "DopplerShiftEvaluationTypes to be considered in the calculation.", LblDopplerShiftEvaluationTypes, MsxDopplerShiftEvaluationTypes); toolTipMaker.Add( "DecayWidthType to be considered in the calculation.", LblDecayWidthType, CbxDecayWidthType); toolTipMaker.Add( "PotentialTypes to be considered in the calculation.", LblPotentialTypes, MsxPotentialTypes); toolTipMaker.Add( "BottomiumStates to be considered in the calculation.", LblBottomiumStates, MsxBottomiumStates); toolTipMaker.Add( "Name of the output file. The standard output path can be set" + Environment.NewLine + "in the menu \"File\" using \"Set output path\".", LblDataFileName, TbxDataFileName); toolTipMaker.Add( "Critical temperature for the formation of the quark-gluon medium.", LblQGPFormationTemperature); }
private void MakeToolTips( ToolTipMaker toolTipMaker ) { toolTipMaker.Add( "Desired shooting accuracy in the running coupling AlphaSoft," + Environment.NewLine + "equals the difference in AlphaSoft between two consecutive" + Environment.NewLine + "steps. AccuracyAlpha > 0.", LblAccuracyAlpha, TbxAccuracyAlpha); toolTipMaker.Add( "Desired shooting accuracy in the wave function, equals the" + Environment.NewLine + "absolute value of the wave function at the origin." + Environment.NewLine + "AccuracyWaveFunction > 0.", LblAccuracyWaveFunction, TbxAccuracyWaveFunction); toolTipMaker.Add( "Controls the strength with which the shooting algorithm reacts to changes" + Environment.NewLine + "in the running coupling. 0 <= AggressivenessAlpha < 1.", LblAggressivenessAlpha, TbxAggressivenessAlpha); toolTipMaker.Add( "Running coupling evaluated at the hard scale (QuarkMass).", LblAlphaHard, TbxAlphaHard); toolTipMaker.Add( "Running coupling evaluated at the soft scale (<1/r>).", LblAlphaSoft, TbxAlphaSoft); toolTipMaker.Add( "Running coupling evaluated at the thermal scale.", LblAlphaThermal, TbxAlphaThermal); toolTipMaker.Add( "Running coupling evaluated at the ultra soft scale.", LblAlphaUltraSoft, TbxAlphaUltraSoft); toolTipMaker.Add( "Total mass of the bottomium.", LblBoundMass, TbxBoundMass); toolTipMaker.Add( "Binding energy of the bottomium, defined relative to the potential-at-infinity" + Environment.NewLine + "for converging potentials. Otherwise it is defined as the real part of the" + Environment.NewLine + "eigenvalue of the Schroedinger equation.", LblEnergy, TbxEnergy); toolTipMaker.Add( "Decay width due to collisional damping, defined as twice the negative imaginary" + Environment.NewLine + "part of the eigenvalue of the Schroedinger equation.", LblGammaDamp, TbxGammaDamp); toolTipMaker.Add( "Maximum number of trials when the Schroedinger equation is solved by the shooting" + Environment.NewLine + "method. If MaxShootingTrials <= 0, the Schroedinger equation is solved only once.", LblMaxShootingTrials, TbxMaxShootingTrials); toolTipMaker.Add( "Color state of the bottomium. Can be color-singlet or color-octet.", LblColorState, CbxColorState); toolTipMaker.Add( "Spin state of the bottomium. Can be spin-singlet or spin-triplet.", LblSpinState, CbxSpinState); toolTipMaker.Add("Debye mass due to color screening in the quark-gluon plasma.", LblDebyeMass, TbxDebyeMass); toolTipMaker.Add( "Name of the output file. The standard output path can be set" + Environment.NewLine + "in the menu \"File\" using \"Set output path\".", LblDataFileName, TbxDataFileName); toolTipMaker.Add( "Different interaction potentials:" + Environment.NewLine + Environment.NewLine + "Complex - Complex potential used e.g. in Nendzig, Wolschin (2014)," + Environment.NewLine + "LowT - Also complex, valid for low temperatures (Brambilla et al., 2008)," + Environment.NewLine + "Real - Obtained from the real part of \"Complex\"," + Environment.NewLine + "Tzero - Cornell potential," + Environment.NewLine + "SpinDependent - Cornell potential with spin interaction term." + Environment.NewLine + Environment.NewLine + "All potentials except the spin-dependent one are also available with vanishing" + Environment.NewLine + "string coupling. The \"Tzero\"-potential becomes a simple Coulomb potential in" + Environment.NewLine + "this case.", LblPotentialType, CbxPotentialType); toolTipMaker.Add( "Angular momentum quantum number, L = 0, 1, 2, ...", LblQuantumNumberL, TbxQuantumNumberL); toolTipMaker.Add( "Principle momentum quantum number, N > L, N = 1, 2, 3, ...", LblQuantumNumberN, TbxQuantumNumberN); toolTipMaker.Add( "Temperature of the quark-gluon plasma.", LblTemperature, TbxTemperature); toolTipMaker.Add( "Chemical freeze-out temperature of the hadronic medium.", LblTchem, TbxTchem); toolTipMaker.Add( "Critical temperature for the transition between hadronic medium" + Environment.NewLine + "and quark-gluon plasma.", LblTcrit, TbxTcrit); toolTipMaker.Add( "Distance scale of the exponentially damped spin coupling.", LblSpinCouplingRange, TbxSpinCouplingRange); toolTipMaker.Add( "Scaling factor for the strength of the spin coupling. The absolute value of the" + Environment.NewLine + "coupling term differs by a factor of order one at the origin.", LblSpinCouplingStrength, TbxSpinCouplingStrength); toolTipMaker.Add( "Different parameterizations of the running coupling:" + Environment.NewLine + Environment.NewLine + "LOPerturbative - Leading order perturbative calculations," + Environment.NewLine + "LOPerturbative_Cutoff1 - Leading order perturbative calculations cut off at 1," + Environment.NewLine + "LOPerturbative_Cutoff3 - Leading order perturbative calculations cut off at 3," + Environment.NewLine + "NonPerturbative_Fischer - Fit to non-perturbative calculations," + Environment.NewLine + "NonPerturbative_ITP - Fit to non-perturbative calculations.", LblRunningCouplingType, CbxRunningCouplingType); toolTipMaker.Add( "Distance of radial steps at which the wave function is calculated.", LblStepNumber, TbxStepNumber); toolTipMaker.Add( "String tension in the Cornell- and similar potentials.", LblSigma, TbxSigma); toolTipMaker.Add( "Mass of a single bottom quark in vacuum.", LblQuarkMass, TbxQuarkMass); }