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11

0

P P

0

,

,

P

 

parameters

 

 

 

P

P

1

0

en

1

0

0

0

e

e

i

i

n

parameterization

E

E z

z z

i

i

P z

P

E

 

  

 

 

 

S S

1

0

en

1

0

0

0

e

e

i

i

n

parametrization

E

E z

z z

i

i

i

S z

S

E

E

  

Instead of integrating over energy, the collision kerma and scerma distributions

can be calculated directly by raytracing with parameterized exponentials. Effect

of spectral changing with depth, i.e.

depth hardening

is described by means of

the hardening coefficients

P

and

S

The parameters derived using a (depth dose effective) spectrum. Only

P

and

P

are directly measurable quantities.

Heterogeneities considered by using different sets of parameters

for each tissue type, mapped by using lookup tables from the

Hounsfield numbers!

Handling the beam spectrum – depth changes

0

S S

0

,

,

S

 

e.g. Pinnacle, Raystation

e.g. Oncentra