Particle physicists currently explore the fundamental laws of Nature through very powerful machines, the LHC at CERN being one of them. The good accomplishment of this task crucially depends on our ability to implement, in appropriate simulation tools, any model physicists could dream of. This would indeed allow us to draw conclusive statements from theory-data comparisons.
[image credits: GamOI (CC0)]
A week ago, I proposed to run a full particle physics research project on Steem in this context. The aim is to design a Python program allowing for inputting any particle physics model in the simulation tools.
Thanks to a joint effort from 
The first part of this project consists in designing a data format to store the information that will have to be inputted by the users. As the amount of inputs is pretty large, I decided to organize the project in terms of one Utopian sub-task per type of inputs. The topic of the day consists in the treatment of the model parameters.
[image credits: ArXiv]
As explained in my previous post, the entire information on a particle physics model is included in an equation called a Lagrangian.
Such a Lagrangian is in generally compact, and for the Standard Model, it even fits on a t-shirt, as illustrated with the picture. Note that this t-shirt can be bought at the CERN shop.
Now let us go back to the Lagrangian. It contains various things, that include parameters. This is what we will talk about today.
In any typical particle physics model, we have two types of parameters, namely external and internal parameters.
An illustrative declaration of external parameter is provided below in the good old FeynRules syntax (which we want to adapt for the needs of this project). The parameter that is chosen as an example is named aS.
aS == {
ParameterType -> External,
Value -> 0.1184,
InteractionOrder -> {QCD, 2},
BlockName -> SMINPUTS,
OrderBlock -> 3
}
I guess the meaning of each attribute of this aS parameter is almost straightforward. Please ignore the Mathematica syntax and mentally convert it into a future Python syntax.
A remark is in order concerning three attributes. The interaction order is an optional property. It indicates the nature of a parameter with respect to the fundamental interactions embedded in the model. Here, the aS parameter has the same strength as the square (this is the 2) of the coupling strength of the strong interaction (this is the QCD part). Whilst QCD and QED are reserved keywords with very well defined meanings, the user is actually free to use anything.
All external parameters are then organized in groups (or blocks... yes, this is not invented, see here) and each entry in a block connects a counter (that consists in one integer) and a value.
It is now the time to move on with internal parameters. In the FeynRules syntax, the declaration of an internal parameter (named gs for the sake of the example) would read
gs == {
ParameterType -> Internal,
ComplexParameter -> False,
InteractionOrder -> {QCD, 1},
Value -> Sqrt[4 Pi aS],
ParameterName -> G
}
Once again, please ignore the Mathematica syntax and mentally trade it with a Python class. I need to discuss one of the above lines in detail (the rest can be guessed). Some parameters are special in the sense that one must clearly be able to identify what they are physically (physics always strikes back). This is what the ParameterName option allows us to do in the above syntax. It tags gs as a ‘G’ parameter that is well known and with well defined properties.
Some specificities exist for parameters that are matrices. First of all, their indices must be specified. In addition, some properties can optionally be turned on (unitarity, hermiticity, orthogonality).
For instance, in the FeynRules syntax, the typical declaration of a matrix would read
CKM == {
ParameterType -> Internal,
Indices -> {Index[Generation], Index[Generation]},
Unitary ->True,
ComplexParameter -> True,
Value -> { … }
}
Any unindicated option (hermiticity, orthogonality) means that it is set to false (that is the default choice). Moreover, the value of the parameter, represented by the dots, is this time a list of values, one entry for each element of the matrix.
Moreover, for external matrices, one needs as usual to provide a block name. There is however no need to specify the counter. They can be dealt with internally. The counter consists this time in a 2-tuple corresponding to the line and column numbers of each element.
Very importantly, one must be able to generalize that to any tensor (any parameter carrying at least 2 indices).
Concerning the indices, they must also be declared. In this declaration, one must define their range and their unfolding properties. The latter is a bit hard to explain. In short, if set to true, it means that if the index appears summed in the Lagrangian, the summ must be explicitly expanded when the Lagrangian will be treated.
In this post, we really start this particle physics research project at SteemSTEM/Utopian.io.
I decided to focus on the input parameters that the user will have to provide and that the code will have to read, and process internally.
The tasks that have to be done for now are quite simple.
I am totally open for the strategy to follow for the input format. The simplest option is generally the best and is the one I will choose as a default. However, if you want to get an opinion before coding, leaving a comment to this post may be helpful.
I think that for now, we are all good. To tackle this project, I have created a fresh GitHub folder. The subdirectory structure is left open for now.
Please do not hesitate to come back to me for questions.