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David Fritz [email protected] du LUSI DOE Review July 23-24, 2007 Damage Considerations Damage Considerations David Fritz FEL Source Propagation Absorbed Energy Dose Damage Processes in Solids Damage Thresholds FLASH Results Summary

Damage Considerations David Fritz

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Damage Considerations David Fritz. FEL Source Propagation Absorbed Energy Dose Damage Processes in Solids Damage Thresholds FLASH Results Summary. Comparison to Synchrotron Sources. Average heat load is not a concern but instantaneous energy deposition must be considered. - PowerPoint PPT Presentation

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Page 1: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 1

Damage ConsiderationsDavid Fritz

Damage ConsiderationsDavid Fritz

FEL Source Propagation Absorbed Energy DoseDamage Processes in SolidsDamage ThresholdsFLASH ResultsSummary

FEL Source Propagation Absorbed Energy DoseDamage Processes in SolidsDamage ThresholdsFLASH ResultsSummary

Page 2: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 2

Comparison to Synchrotron SourcesComparison to Synchrotron Sources

Parameter APS LCLS

Repetition Rate 6,500,000 Hz 120 Hz

Pulse Length 70 ps 0.25 ps

Average Power 1,000 W 0.25 W

Peak Power 2.2 MW 8,000 MW

Average heat load is not a concern but instantaneous energy deposition must be considered

Average heat load is not a concern but instantaneous energy deposition must be considered

Page 3: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 3

FEL Source PropagationFEL Source Propagation

2/12

0

1)(

z

zzW

2

00

Wz

Distance

rangeRayleigh

waistbeamGaussian

0

z

z

W

A diffraction limited Gaussian source is assumed

A diffraction limited Gaussian source is assumed

Page 4: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 4

Peak FluencePeak Fluence

densityphoton Peak

densityPhoton

pulse ain photons ofNumber

)(

2)(

2

)()(

),,(

)(),,(

2

2

)(2

2

22

peak

photon

peak

peak

photon

zw

yx

peakphoton

A

N

zw

NzA

zwzA

dydxzyxN

ezAzyx

Page 5: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 5

Radiation Dose per AtomRadiation Dose per Atom

photoionpeakphoton AEDose section crossron photoelect Atomic

energyPhoton

photoion

photonE

Page 6: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 6

Solid State Damage ProcessesSolid State Damage Processes

Thermal meltingPresure effects

SpallationShear

AblationNon-thermal melting

Multi-pulse fatigue effectsThermomechanical stressChemical Phase transition

Thermal meltingPresure effects

SpallationShear

AblationNon-thermal melting

Multi-pulse fatigue effectsThermomechanical stressChemical Phase transition

Page 7: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 7

Thermal Damage ThresholdsThermal Damage Thresholds

M

R

T

T

TM dTCD QdTCDM

R

T

T

M

Heat Capacity - Energy required to raise the temperature of one gram of a substance by 1° K.Enthalphy of Transformation (a.k.a. Latent Heat) – the amount of energy released or absorbed by a substance during a change of phase.

Heat Capacity - Energy required to raise the temperature of one gram of a substance by 1° K.Enthalphy of Transformation (a.k.a. Latent Heat) – the amount of energy released or absorbed by a substance during a change of phase.

meltingofheatLatent

etemperaturMelting

etemperaturRoom

heatSpecific

melttoDose

etemperaturmeltingreachtoDose

Q

T

T

C

D

D

M

R

M

TM

Page 8: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 8

Thermal Damage Thresholds (2)Thermal Damage Thresholds (2)

Beryllium Silicon

Page 9: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 9

Thermal Damage Thresholds (3)Thermal Damage Thresholds (3)

Material Dose to Tmelt † Dose to Melt † Dose in NEH3 † * Dose in FEH1 † *

Be 0.34 0.42 0.0002 0.00004

B 0.54 1.06 0.0005 0.0001

Al 0.19 0.30 0.03 0.007

Si 0.37 0.89 0.04 0.01

Ti 0.50 0.65 0.24 0.06

Cu 0.31 0.45 0.15 0.03

Ge 0.29 0.68 0.12 0.03

Mo 0.93 1.32 0.36 0.08

Ag 0.41 0.43 0.56 0.13

Ta 0.98 1.36 0.72 0.16

W 1.24 1.78 0.76 0.17

Pb 0.09 0.14 1.17 0.26

* 8265 eV Photon Energy, 1.1 x 1012 ph/pulse† Units of eV/atom

Page 10: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 10

FLASH ResultsFLASH Results

32.5 nm wavelength25 fs pulse duration5.5 μJ pulse energyB4C, C, Si, SiC were exposed to focused FLASH FELUp to 2.2 J/cm2

Threshold for surface damage is on the order of the fluence required for themal melting

32.5 nm wavelength25 fs pulse duration5.5 μJ pulse energyB4C, C, Si, SiC were exposed to focused FLASH FELUp to 2.2 J/cm2

Threshold for surface damage is on the order of the fluence required for themal melting

S. Hau-Riege et al., Applied Physics Letters 90, 173128 (2007).

Page 11: Damage Considerations David Fritz

David [email protected]

LUSI DOE Review July 23-24, 2007Damage Considerations 11

SummarySummary

Instantaneous energy deposition must be consideredHigh melting point, low-Z materials will be most resistent to damageThermal model predicts that some materials can be safely placed in the NEH and FEH beam at normal incidenceFLASH damage results are consistent with the thermal model

Instantaneous energy deposition must be consideredHigh melting point, low-Z materials will be most resistent to damageThermal model predicts that some materials can be safely placed in the NEH and FEH beam at normal incidenceFLASH damage results are consistent with the thermal model