15
John Arthur X-Ray Optics Specs [email protected] d.edu October 12, 2004 X-Ray Prototype Optics Specifications John Arthur

John Arthur X-Ray Optics [email protected] October 12, 2004 X-Ray Prototype Optics Specifications John Arthur

  • View
    223

  • Download
    0

Embed Size (px)

Citation preview

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-Ray Prototype Optics Specifications

John Arthur

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

The Project scope includes

facilities for production and transport of a bright, high-current electron beaman undulator system in which the electron beam will generate the x-ray beamfacilities for transport, diagnostics and optical manipulation of the x-ray beamendstations and related facilities for x-ray experimentsconventional facilities for the accelerator systems and x-ray experimentsa central lab office building to house support staff and researchers

From the LCLS Global Requirements document:

This talk will elaborate on the specifications for the LCLS x-ray optics and diagnostics

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

The X-ray Optics

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

Functions of the x-ray optics

Confinement  (masks, slits, local apertures)

Intensity attenuation  (gas attenuator, solid attenuator)

Focusing  (K-B mirror)

Spectral filter  (mirror low-pass filter, monochromator)

Beam direction (flipper mirrors)

Temporal filter  (pulse split/delay)

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

High peak power (fluence) poses a challenge for x-ray optics

Response of material to ultra-high power x-ray pulse is untested

LLNL codes can describe all aspects of the response EXCEPT

initial conversion of x-ray energy into hot electrons. Uncertainty due

only to lack of understanding of non-linear response

We have good arguments that the non-linear response will be

negligible

Therefore, we will use linear absorption cross sections with

confidence

LLNL will do precise calculations (assuming linear cross sections)

as part of optics design

Until those calculations are done, use conservative approximation

based on known melting points of materials

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

0.01

0.1

1

10

100

100 1000 10000

Photon energy (eV)

Flu

en

ce (

J/cm

^2

)

undulatorexitexperimentalhall A

experimentalhall B

C

Si

W

Au

Be

NEH

FEH

FEE

LLNLLLNL

Expected LCLS fluence compared with melt fluence for various materials

Approximation assumes FEL

pulse energy instantly

deposited in atoms within

absorption volume (using

linear absorption cross

section). If resulting

energy/atom much less than

melt energy/atom, then the

material will not be

damaged.

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

Some proposed solutions to the peak power problem

Grazing-incidence slits

Graded-density absorber

Low-z materials (Be, B4C, C)

Grazing incidence

Gas attenuator

Distance from source

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

Basic specifications for slits and attenuators

Slit aperture range 2 x 4 beam size @ 800 eV

Slit precision 1 µm

Attenuator range up to 104 at any energy 800-8000 eV

Attenuator precision 1% of attenuation, steps 3/10/100/103/104

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-ray focusing (DESCOPED)

K-B focusing mirrors

Produce high flux density

Useful energy range 800 - 24000 eV

Focus size < 1 µm

Efficiency >10%

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-ray mirrors for LCLS (DESCOPED)

Double-mirror low-pass filter

Energy low-pass filter

Beam redirection

Low-pass mirror critical energy variable 1200 eV -9000 eV

Mirror mechanical stability beam jitter < 10% of beam size

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-ray monochromators

Energy bandpass filter

Energy range 800 eV -24000 eV

Bandpass < 2 x10-4

Rapid scan range 10%

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-ray pulse split and delay

Provides precise time delay between pulses

Pulse split/delay using thin Si crystals

Energy 8000, 24000 eV

Delay range 0-200 ps

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

X-ray diagnostics are required for characterization of the FEL and spontaneous radiation, as means of assessing SASE performance

The X-ray Diagnostics

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

Specifications for the x-ray diagnostics

Position of beam centroid 5% of beam size

Beam transverse dimensions 10% of beam size

Beam divergence 10% of divergence

Photon energy 0.02% of energy

Photon energy spread 20% of energy spread

John Arthur

X-Ray Optics Specs [email protected]

October 12, 2004

Summary

The XTOD group will provide facilities for transporting the LCLS

x-ray beam, for measuring the beam characteristics, and for

manipulating the characteristics in controlled ways

X-ray optical elements will aperture, attenuate, focus, and

monochromate the x-rays

Some of the desired optical components are not in the current

project scope

A suite of x-ray diagnostics will allow characterization of SASE

performance