/********************************************************************************************
* 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);
}
