# 10 Oct 2017

Still working our way through this tutorial based on C++ and MINUIT:

http://www.desy.de/~rosem/flc_statistics/data/04_parameters_estimation-C.pdf

Now, we tackle the L3 LEP data. L3 was an experiment at the Large Electron Positron collider, at CERN, near Geneva. Until 2000, it recorded the decay products of e+e- collisions at center of mass energies up to 208 GeV.

An example is the muon pair production:

$$e^+ e^- \rightarrow \mu^+\mu^-$$

Both muons are mainly detected and reconstructed from the tracking system. From the measurements, the curvature, charge and momentum are determined.

The file L3.dat contains recorded muon pair events. Every line is an event, a recorded collision of a $$e^+e^-$$ pair producing a $$\mu^+\mu^-$$ pair.

The first three columns contain the momentum components $$p_x$$, $$p_y$$ and $$p_z$$ of the $$\mu^+$$. The other three columns contain the momentum components for the $$mu^-$$. Units are in $$GeV/c$$.

## Forward-Backward Asymmetry

An important parameter that constrains the Standard Model (the theoretical framework that models our current understanding of Physics) is the forward-backward asymmetry A:

$$A = (N_F - N_B) / (N_F + N_B)$$

where:

• $$N_F$$ are the events in which the $$\mu^-$$ flies forwards ($$\cos \theta_{\mu^-} > 0$$);
• $$N_B$$ are the events in which the $$\mu^-$$ flies backwards.

Given the L3.dat dataset, we would like to estimate the value of $$A$$ and determine its statistical error.

In a simple counting experiment, we can write the statistical error as:

$$\sigma_A = \sqrt{ \frac{(1-A^2)}{N} }$$

where $$N = N_F + N_B$$.

So, as a first step, we can simply count the forward events.

## First estimation

Let’s look at that data:

$> head -n 5 L3.dat 4.584 -9.763 -18.508 -24.171 50.464 95.865 62.570 184.448 -175.983 -28.392 -83.491 70.656 7.387 101.650 13.531 -7.853 -108.002 -14.472 43.672 56.083 -77.367 -40.893 -52.481 72.804 -36.620 -60.832 -46.156 35.863 59.591 -3.220  First we need to assemble a bit of code to read in that file: func read(fname string) []float64 { f, err := os.Open(fname) if err != nil { log.Fatal(err) } defer f.Close() var costh []float64 sc := bufio.NewScanner(f) for sc.Scan() { var pp, pm [3]float64 _, err = fmt.Sscanf( sc.Text(), "%f %f %f %f %f %f", &pp[0], &pp[1], &pp[2], &pm[0], &pm[1], &pm[2], ) if err != nil { log.Fatal(err) } v := pm[0]*pm[0] + pm[1]*pm[1] + pm[2]*pm[2] costh = append( costh, pm[2]/math.Sqrt(v), ) } if err := sc.Err(); err != nil { log.Fatal(err) } plot(costh) return costh }  Now, with the $$\cos \theta_{\mu^{-}}$$ calculation out of the way, we can actually compute the asymmetry and its associated statistical error: func asym(costh []float64) (float64, float64) { n := float64(len(costh)) nf := 0 for _, v := range costh { if v > 0 { nf++ } } a := 2*float64(nf)/n - 1 sig := math.Sqrt((1 - a*a) / n) return a, sig }  Running the code gives: events: 346 A = 0.231 +/- 0.052  OK. Let’s try to use gonum/optimize and a log-likelihood. ## Estimation with gonum/optimize To let optimize.Minimize loose on our dataset, we need the angular distribution: $$f(\theta, A) = \frac{3}{8} (1 + \cos^2 \theta) + A \cos\theta$$ we just need to feed that through the log-likelihood procedure: func main() { costh := read("L3.dat") log.Printf("events: %d\n", len(costh)) a, sig := asym(costh) log.Printf("A= %5.3f +/- %5.3f\n", a, sig) fcn := func(x []float64) float64 { lnL := 0.0 A := x[0] const k = 3.0 / 8.0 for _, v := range costh { lnL += math.Log(k*(1+v*v) + A*v) } return -lnL } grad := func(grad, x []float64) { fd.Gradient(grad, fcn, x, nil) } hess := func(h mat.MutableSymmetric, x []float64) { fd.Hessian(h.(*mat.SymDense), fcn, x, nil) } p := optimize.Problem{ Func: fcn, Grad: grad, Hess: hess, } var meth = &optimize.Newton{} var p0 = []float64{0} // initial value for A res, err := optimize.Minimize(p, p0, nil, meth) if err != nil { log.Fatal(err) } display(res, p) }  which, when run, gives: $> go build -o fba fba.go
\$> ./fba
events: 346
A= 0.231 +/- 0.052

minimal function value:  230.817
number of parameters: 1
hess=[429.2102851867676]
errs= [0.04826862636461834]
par-000: 2.196444e-01 +/- 4.826863e-02


ie: the same answer than the MINUIT-based code there:

Results of MINUIT minimisation
-------------------------------------

Minimal function value:               230.817
Estimated difference to true minimum:   9.044e-11
Number of parameters:           1
Error definition (Fmin + Delta):         0.500
Exact covariance matrix.

Parameter     Value       Error    positive    negative    L_BND    U_BND
0          A  2.196e-01  4.827e-02 +4.767e-02 -4.879e-02  0.0e+00  0.0e+00

Covariance matrix:
2.330e-03

Correlation matrix:
1.000