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Nur für internen Gebrauch / © Siemens AG 2008. Alle Rechte vorbehalten. Medical and industrial applications of linear electron accelerators Dr. Roland Schmidt Siemens AG Sector Healthcare 27.04.2009

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Page 1: Schmidt Linacs Medical Industrial Applicationsheraeus-technology.desy.de/e8/e44867/SchmidtLinacs... · Multi-element collimation device located inside the gantry head to shape the

Nur für internen Gebrauch / © Siemens AG 2008. Alle Rechte vorbehalten.

Medical and industrial applications of linear elect ron accelerators

Dr. Roland SchmidtSiemens AGSector Healthcare 27.04.2009

Page 2: Schmidt Linacs Medical Industrial Applicationsheraeus-technology.desy.de/e8/e44867/SchmidtLinacs... · Multi-element collimation device located inside the gantry head to shape the

430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 2

Abstract

Medical and industrial applications of linear electron acceleratorsRoland Schmidt, Siemens Healthcare

The first industrial applications of linear electron accelerators showed up in the Fifties of the last century. We will give a short overview about the history of this technology, especially about their rise in medical industry for cancer treatment.

In the second chapter, we will talk about the basic physics, the functionality, the main components and limitations of this technology. This will be explained at the model of a typical S-band accelerator, as it is used at Siemens and other competitorsfor medical applications.

In a side view, we will look at the necessary assemblies, which are used to operate this type of accelerators appropriately, like modulators, injectors or dose chambers. An example of a complete system in a clinical environment will be shown.

The third part of this talk will open a window in the industrial fields like security business (e.g. cargo screening) or NDT (non destructive testing) and point out how worldwide linear electron accelerators might become more and more important.

A brief look at our facility in Rudolstadt, Thuringia, will close this talk.

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 3

Introduction

History and basics of Radiation Therapy

Linear Accelerator: Concepts & Technologies

Industrial Applications

Closing remarks and discussion

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 4

History of Radiation Oncology

First articles about treatment with X-rays in the early 20th century.This therapy with standard X-ray tubes was the only choice until the Fifties.

Since late Fifties until end of the last century the use of Co60 (or Cs137) was very popular but lost its attractiveness due to safety and environmetal reasons.

At the same time accelerators for electron had been developed – 3 main types:a. Van-de-Graaf (1954): minor importanceb. Betatron: circular acceleration in a strong magnetic field: until the late 70iesc. Linac: Linear accelerator, driven by high frequency: since 1970 until today

Recent technologies are based on high energy accelerators for protons or heavy ions.

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 5

Cancer basicsTreatment choices

3 different treatment modalities

Surgical OncologyWorks best for tumors that are well-contained and accessible; some are

neither

Radiation OncologyTele-therapy is radiation delivered

from a distanceBrachy-therapy is radioactive seeds

that are placed inside the body

Medical Oncology (Chemotherapy)Anti-mitotic Drugs - prevent cell divisionAnti-angiogenesis drugs - prevent formation of new blood vesselsBiologic Response Modifiers – enhance normal immune response

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 6

Purpose of Radiation Therapy

Radiation Therapy is used in Cancer treatment to destroy tumor cells, while minimizing damage to normal cells.

Radiation is not selective, it damages both normal cells and tumor cells !

Fortunately, healthy cells can repair themselves more readily than tumor cells, under some conditions.

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 7

Depth Dose in Water

0

20

40

60

80

100

120

0 5 10 15 20 25 30 35

depth [cm]

dose

[%] 6MeV e

17MeV e

6MV X

15MV X

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 8

Depth in Water (cm)

Surface Dose

Penetration Depth for

Electrons

10 MeV Electron Beam

Field Size: 15 x 15 cmR

elat

ive

Dos

e %

Dmax

Definition : Depth in water at which 80% of maximum ionization occurs. Field size 15 x 15 cm at surface.

Characteristics: High surface dose, shallow penetration, steep fall-off.

X-Rays Produced by Electrons in Scatter Foils, Air, Water

Up to 5%

110

100

90

80

70

60

50

40

30

20

10

0 5 10 15 20

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 9

10 MV Photon Beam

Field Size: 10 x 10 (cm)

Dmax

Rel

ativ

e D

ose

%

Surface Dose

Build-up Region Depth in Water

Definition: Percentage ionization of Dmax at 10 cm depth in water

Characteristics: Low surface dose, Deep penetration, Gradual Fall-off

110

100

90

80

70

60

50

40

30

20

10

0 5 10 15 20

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 10

Radiation TherapyWorkflow

DIAGNOSE

Cancer diagnosis

� Diagnostic imaging from MR, CT, PET/CT� Patient is diagnosed with cancer

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 11

Radiation TherapyWorkflow

DIAGNOSE PRESCRIBE

Treatment decision

� Surgery, Chemotherapy, Radiation Therapy??� Depends on tumor type, tumor progression, location� Ideally, decision is agreed upon

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 12

Radiation TherapyWorkflow

DIAGNOSE PRESCRIBE PLAN &SIMULATE

Preparation of treatment plan

� Cancer outlining, definition of critical structures� Calculation of required dose & placement of beam angles� Virtual simulation of treatment plan & fitting of immobilization

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 13

Radiation TherapyWorkflow

DIAGNOSE PRESCRIBE PLAN &SIMULATE

POSITION

Radiation therapystarts

� Patient set-up� Portal imaging� Radiation treatment

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 14

Radiation TherapyWorkflow

DIAGNOSE PRESCRIBE PLAN &SIMULATE

POSITION TREAT

Treatment delivery

� Automatic gantry movement to planned gantry angles

� Automatic positioning of MLC leaves to conform to tumor PTV

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 15

Introduction

History and basics of Radiation Therapy

Linear Accelerator: Concepts & Technologies

Industrial Applications

Closing remarks and discussion

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 16

LINAC Key Components

GantryRF SourcesWaveguideBeam CollimationTreatment TableImaging Device

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 17

Schematic view of a Magnetron Linac

MEVATRON

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 18

RF Sources

Magnetron

� e.g. Model 6250 (E2V)� Nominal peak power 2.6 MW� Covers up to medium energies� Self oscillating/Amplifier� 4-15MV photon (x-ray) energies� 5-14 MeV electron energies

Klystron

� e.g. Model 2157 (Thales)� Nominal peak power 7.5 MW� Delivers up to high energies� Only amplifies, needs RF Driver� 4-25MV photon energies� 5-21 MeV electron energies

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 19

Types of linear accelerators (waveguides)

A. TRAVELLING WAVE

� RF power input near head (or gun) of the waveguide� Particle “rides” the wave down the waveguide� Unused RF power recycled at the end of waveguide

+ Low RF power required- Beam time formation, beam stability

B. STANDING WAVE

� RF power input near center of waveguide (or any other position)� RF standing waves set up in cavities

+ Fast operation and mode changes; high stability- High RF power required

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 20

Electron Accelerators (standing wave)

Photon and Electron modeswith one single accelerator

Multi energy operation:� Photon mode from 4 to 23 MV� Electron mode from 5 to 21 MeV

Photon mode operation only

Fixed tungsten targetEnergies up to 6 MeV

Type 8067Siemens

Type 6MeVSiemens

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 21

Parts of an accelerating waveguide

Electron

gun

Buncher

WaveguideEnvelope

(Bending magnet)Lens coil Steering coils

External X-ray target

Primary collimators

Flattening Filters

X & Y Jaws

RF Input

from

Magnetron

or Klystron4 Port

circulator

Ion pump

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 22

Source: Electron Gun

12,500Volts

Barium Impregnated Tungsten

E-

E-

E-

E-

E-

E-

E-

E-

E-

E-

Electron Control Grid

Filament (Heater)Heats The Cathode ≅1050ºC E-

E-

E-

E-

E-

E-

E-

E-Free ElectronsBarium

Anode &1st cavity

E-

E-

E-E-

E-

E-E-

Ground

Electron gun

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 23

Design of the waveguide

Electron Stream

Electron Bunch

Drift Space

Electron Gun

Cavity Nose

Buncher.drw

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 24

Accelerating the electrons

Pulses of Radiofrequency Power (3000MHz)

Electric Field

Electron Bunch

RF Input

Side Cavity WGrfin.drw

Centerline Cavity

Direction of Electron Travel

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430. WE-Heraeus-SeminarRoland Schmidt

e-

CAVITYFIELD

VOLTAGE0

-

+

ELECTRONINJECTION

Standing wave acceleration

Page 26: Schmidt Linacs Medical Industrial Applicationsheraeus-technology.desy.de/e8/e44867/SchmidtLinacs... · Multi-element collimation device located inside the gantry head to shape the

430. WE-Heraeus-SeminarRoland Schmidt

+

- +

- +

-+

- +

- +

- +

-+

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

Page 27: Schmidt Linacs Medical Industrial Applicationsheraeus-technology.desy.de/e8/e44867/SchmidtLinacs... · Multi-element collimation device located inside the gantry head to shape the

430. WE-Heraeus-SeminarRoland Schmidt

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

- +

- +

-+

- +

- +

- +

-+

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

Page 30: Schmidt Linacs Medical Industrial Applicationsheraeus-technology.desy.de/e8/e44867/SchmidtLinacs... · Multi-element collimation device located inside the gantry head to shape the

430. WE-Heraeus-SeminarRoland Schmidt

+

-+

- +

- +

- +

-+

- +

- +

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

-+

-

+

++

-

-

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

-+

- +

- +

- +

-+

- +

- +

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

- +

- +

-+

- +

- +

- +

-+

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

- +

- +

-+

- +

- +

- +

-+

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

-+

- +

- +

- +

-+

- +

- +

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

-+

-

+

++

-

-

+

-

+

++

--

-

+

-

+

++

--

-

+

-

+

++

--

-

e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

+

-+

- +

- +

- +

-+

- +

- +

-e-

CAVITYFIELD

VOLTAGE0

-

+

Standing wave acceleration

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430. WE-Heraeus-SeminarRoland Schmidt

CAVITYFIELD

VOLTAGE0

-

+

e-

Standing wave acceleration

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 42

Bending magnet and envelope

ENERGYTOOHIGH

ENERGYTOOLOW

e-

ELECTRONENERGYDISTRIBUTION

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 43

Beam spot measurement 6MeV Linac

Measurement setup spot size measure

Photon mode operationIntegrated tungstentargetEnergies up to

6 MeV

Accelerator

Slit Collimator

Pb film layer collimator

Film

5.1

0

0.05

0.1

0.15

0.2

-6 -5 -4 -3 -2 -1 0 1 2 3 4 5 6x [mm]

Sch

wär

zung

[a.u

.] Profile 80%68.27%50%

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 44

Beam Formation for Electrons

Electrons exit window Primary scattering foil(s) Secondary scattering foilElectron dose chamberPrimary jaws beam cuttingElectron applicator

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 45

Beam Formation for Photons

Electrons exit window Strike external W TargetPhotons generatedCarbon electron absorberPrimary collimationFlattening filterPhoton dose chamberField light mirrorPrimary jaw (s) beam cutting

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430. WE-Heraeus-SeminarRoland Schmidt

Multileaf Collimator (MLC)

Multi-element collimation device located inside the gantry head to shape the aperture of a treatment field.

Can substitute for a patient-specific, custom-built block used in 3-D conformal radiation therapy. This was the original intent of MLC.

Can also be used as a fluence modulator by varying the aperture across the target volume as a function of dose delivered. Such usage is called Intensity Modulated Radiation Therapy (IMRT). This is today’s most important use of MLC.

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 47

Introduction

History and basics of Radiation Therapy

Linear Accelerator: Concepts & Technologies

Industrial Applications

Closing remarks and discussion

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 48

Linear Electron Accelerators are used in industrial applications too:

�NDT (non destructive testing)

�CARGO INSPECTION

�FOOD IRRADIATION

�STERILISATION

�PROCESSING SEWAGE WATERS OR INFECTED WASTES BEFORE DISPOSAL

�IRRADIATION OF CABLES, PIPES, PRODUCTS OF COMPLEX SHAPE, etc.

�RESEARCH

Industrial applications

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 49

Some examples:

Industrial applications

Cargomobil

Cargo stationary Cargo stationary

NDT

Sterilization Surface Bonding

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 50

Examples: Cargo Scannerat Customs (Hamburg)(Source: Ph.D. Thesis from Peter Carsten Lotz)

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 51

Examples: Cargo Scannerat Customs (Hamburg)(Source: Ph.D. Thesis from Peter Carsten Lotz)

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 52

Introduction

History and basics of Radiation Therapy

Linear Accelerator: Concepts & Technologies

Industrial Applications

Closing remarks and discussion

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 53

Surface Area 23 tsqm

Employees 220

Founded 1919

Apprentices 35

Welcome to Rudolstadt, Thuringia

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 54

Key Technologies @ H IM CVG

Vacuum components

X-ray Products

Therapy components

Cleanroomhigh precision

assembly

Vacuumprocesses

High energyfinal test

Vacuumprocesses

High voltagefinal test

Precisionmachiningof special

alloys

Cleaning and coating of

vacuumcomponents

High temperature

annealing and brazing

Cleanroomhigh precision

assembly

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 55

Mechanical components

High temperature processes

Glass treatment

Galvanik processes

Vacuum components

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 56

Manufacturing of X-Ray Tubes

Brazing Assembly

Degassing Final Test

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 57

Manufacturing of cavities

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 58

Therapy Components / Waveguides

BeamtestBakeout

StackingBrazing

Tuning

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 59

Thank you for attention

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430. WE-Heraeus-Seminar28.04.2009 Roland SchmidtSeite 60