22.05.2014 Views

CERN Program Library Long Writeup W5013 - CERNLIB ...

CERN Program Library Long Writeup W5013 - CERNLIB ...

CERN Program Library Long Writeup W5013 - CERNLIB ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

The functions F i (Z,X,Y) (i = σ, l) have the form:<br />

F i (Z, X, Y )=F i0 (X, Y )+ZF i1 (X, Y ) (7)<br />

where F ij (X, Y ) denotes a function constructed from two polynomials<br />

⎧<br />

⎪⎨<br />

F ij (X, Y )=<br />

⎪⎩<br />

P neg<br />

ij (X, Y ) if Y ≤ 0<br />

P pos<br />

ij (X, Y ) if Y > 0<br />

(8)<br />

and P neg<br />

ij , P pos<br />

ij fulfil the conditions:<br />

P neg<br />

ij (X, Y ) Y =0 = P pos<br />

∂P neg<br />

ij<br />

ij (X, Y ) Y =0 = ∂Ppos<br />

ij<br />

∂Y ∣ Y =0<br />

∂Y ∣ Y =0<br />

The detailed form of the P ij polynomials is:<br />

with<br />

P neg<br />

i0 (X, Y ) = (C 1 + C 2 X + ···+ C 6 X 5 )+(C 7 + C 8 X + ···+ C 12 X 5 )Y<br />

+ (C 13 + C 14 X + ···+ C 18 X 5 )Y 2 + ···+(C 31 + ···+ C 36 X 5 )Y 5<br />

P pos<br />

i0 (X, Y ) = (C 1 + C 2 X + ···+ C 6 X 5 )+(C 7 + C 8 X + ···+ C 12 X 5 )Y<br />

+ (C 37 + C 38 X + ···+ C 42 X 5 )Y 2 + ···+(C 55 + ···+ C 60 X 5 )Y 5 (9)<br />

P neg<br />

i1 (X, Y ) = (C 61 + C 62 X + ···+ C 65 X 4 )+(C 66 + C 67 X + ···+ C 70 X 4 )Y<br />

+ (C 71 + C 72 X + ···+ C 75 X 4 )Y 2 + ···+(C 81 + ···+ C 85 X 4 )Y 4<br />

P pos<br />

i1 (X, Y ) = (C 61 + C 62 X + ···+ C 65 X 4 )+(C 66 + C 67 X + ···+ C 70 X 4 )Y<br />

+ (C 86 + C 87 X + ···+ C 90 X 4 )Y 2 + ···+(C 96 + ···+ C 100 X 4 )Y 4<br />

X =ln E m µ<br />

Y =ln E c<br />

v j E<br />

j = σ, l<br />

where v σ,l are additional parameters of the fit. By a numerical (twofold) integration of the formulae (5)<br />

and (6) above, we have calculated 1800 data points in the range Z =1, 6, 13, 26, 50, 82, 92 and the energy<br />

ranges 1GeV ≤ T ≤ 10 TeV and 4m ≤ E c ≤ T and performed a least-squares fit to determine the<br />

parameters. The fitted values of the parameters are in the DATA statements in the functions GPRSGM and<br />

GPRELM, which compute the formulae (5) and (6) respectively. The accuracy of the fit is:<br />

∆σ<br />

σ<br />

∆E pair<br />

loss<br />

E pair<br />

loss<br />

{<br />

10% if T ≤ 5 GeV<br />

≤<br />

5% if T>5 GeV<br />

{<br />

10% if T ≤ 5 GeV<br />

≤<br />

4% if T>5 GeV<br />

The function GPRELM contains a second formula to calculate the total energy lost by the muon due to direct<br />

e + e − -production used when E c ≥ Emax = E − 0.75 √ em µ Z 1/3 . This formula describes the total energy<br />

loss with an error less than 1%:<br />

E pair<br />

loss<br />

(Z, T ) = Epair<br />

loss (Z, T, E c = E max ) (10)<br />

= Z(Z +1)E max [d 1 +(d 2 X + d 3 Y )+(d 4 X 2 + d 5 XY + d 6 Y 2 )+<br />

+ ···+(d 22 X 6 + d 23 X 5 Y + ···+ d 28 Y 6 )]<br />

where X =ln(E/m µ ) and Y = Z 1/3 . The fitted parameters d i can be found in the DATA statement in the<br />

function GPRELM.<br />

315 PHYS450 – 3

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!