Developments at LCLS Joachim Stöhr ...but long before LCLS there was SSRL and Herman left his mark…..

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Transcript Developments at LCLS Joachim Stöhr ...but long before LCLS there was SSRL and Herman left his mark…..

Developments at LCLS

Joachim Stöhr

...

but long before LCLS there was SSRL and Herman left his mark…..

Unconventional Herman

with dreadlocks

April 1, 1976 3

Herman lights up on experimental floor tries to do an experiment

Herman - a man of fashion

in sportsgear with infamous cap

5

Herman as cheerleader

leading “happy hour” with staff

6

Proud Herman first beam out of SSRL wiggler on BL4

02/28/79

Herman pushes a SASE X-FEL at SLAC

1992

February, 1992 Proposal for a hv > 300 eV FEL Based on the SLAC Linac by C. Pellegrini, UCLA February, 1992 – LCLS Technical Design Group formed by H. Winick August, 1996 – The LCLS Design Study Group, under the leadership of Max Cornacchia, begins work on the first LCLS Design Report

1998

December 1998 – The first edition of the LCLS Design Study Report is published

XFELs - a third powerful type of lightsource

J. Ullrich, A. Rudenko, R. Moshammer Ann. Rev. Phys. Chem.

63

, 635 (2012)

X-Ray Lasers are the latest light revolution

LCLS:

the world’s first x-ray free electron laser

Injector electron beam 1km linac 14GeV x-ray beam Undulator hall Near-hall: 3 stations Far-hall: 3 stations AMO SXR XPP XCS CXI MEC

SASE versus self seeded x-ray beam Intense x-ray source with spiky spectrum SASE Monochromator creates seed with controlled spectrum FEL amplifier (exponential intensity gain) 8.3 keV 40 pC seeded

G E ~ 0.5 eV

SASE

LCLS is rapidly gaining steam

On site users Publications by year 703 proposals

(~15 scientists/proposal)  31 countries  only 1 in 5 proposals gets beam time ~ 60% of papers in high impact journals

Beam delivery is ~95% of scheduled beam time < July

- The size and speed of things: from “structure” to “function” --

The speed of things – the smaller the faster

macro molecules molecular groups atoms “electrons” & “spins”

the technology gap

optical laser pulse

Light pulses can be used to capture (or beat) all motion…

Atoms: Speed of sound: 1 nm / 1 ps

Electrons: Fermi velocity: 1 nm / 1 fs

Light: Speed of light: 1 nm / 3 as

Three Strategic Science Areas of LCLS

Biological structure and function drug design, health Chemical structure and function energy, environment Material structure and function information technology Mn 4 CaO 5 cluster

Atoms Atoms/Electrons Atoms/Electrons/Spins

Biological Structure:

X-Rays are the key tool (courtesy H. Chapman) Cumulative number of structures in the PDB

ribosome myosin virus nucleosome antibody transfer RNA hemoglobin actin myoglobin

2011

Year C. Zardecki - PDB C. Abad-Zapatero - Acta Cryst D68 (2012)

Femtosecond Protein Nanocrystallography

beating the speed of sound with the speed of light atomic structure shape of nanocrystal

Liquid jet

Nanocrystals (~500nm) contained in water jet - developed at ASU Patterns of single nanocrystals recorded in single, intense and fast <50 fs x-ray shots Atoms move after shot (“speed of sound”) crystal blows up - new crystal for new shot Complete structure from ~1 million shots

First X-FEL solved protein structure Cathepsin B enzyme protein - part of the African sleeping sickness parasite

Cathepsin B glyco-protein: Famously difficult to crystallize and solve by conventional methods # shots: 4 million # of hits 10% 2Å resolution

The structure of Cathepsin B – 2 Å resolution

sugar moiety in pro-peptide Pro-peptide sugar moiety in

in-vivo

TbCatB Water R factor = 18.7% R free = 21.0%

in-vivo

TbCatB

S. Boutet (SLAC) Karol Nass (CFEL) Lars Redecke (U. Hamburg) Nano crystallography appears to be the first “killer app” of LCLS

Chemical structure: Understanding Photosynthesis

( )

Not Understood Understood

 Has created our

atmosphere

and ozone layer    Only fundamental source of

food

on earth Has created

fossil energy

sources (crude oil, coal, gas)

Photosystem II: Where Plants Split Water

Photosystem II [ ] 1 ms

Mn 4 CaO 5

X-ray damage has prevented conclusive structure determination Beat damage with intense, fast pulses

First results: room temperature study of S 1 state X-ray diffraction: atomic structure X-ray emission: electronic structure single shot diffraction pattern – 5 Å single shot pattern

• 

50 fs pulses, 3.4 × 10 11 photons∕pulse at 9 keV undamaged room temperature atomic/electronic structure

future studies will reveal reaction dynamics

Technology: Switching of information “bits”

Today’s roadmap for data storage:

Magnetic “1” and “0” bits are switched by weak field pulse aided by heat from laser

Magnetic “bits” have nanoscale dimensions

The dream: magnetic switching by a laser pulse All-optical magnetic writing

Stanciu PRL

99,

et al.,

047601 (2007) Ostler

et. al.,

Nature Comm . 3, 1 (2012)

Switching works:

  ultrafast -

40 fs optical light pulses

but only for one material – ferrimagnetic metallic GdFeCo alloy

What is the secret that makes GdFeCo work?

Use x-ray pulses to probe optical switching X-ray probe pulse 50 fs

l

~ 1.5 nm Optical pump pulse 40 fs

l

~ 800 nm CCD detector fast readout

Obtain information what happens after optical pulse  as function of D t (time)  as function of q (size)

GdFeCo not “amorphous” but inhomogeneous on nanoscale

TEM image consistent with X-ray scattering C. Graves

et al

(submitted)

nanoregions switch first – drive macroscopic switching

LCLS is being extended by LCLS-II project

Expand capacity and capability

  New injector plus 1 km linac Two new undulator sources  (TW power option) Extended spectral range from  250eV to 13 keV Experimental hall for > 4 instruments

First light in fall of 2018 Assures international competitiveness (Japan, Germany, Korea, Switzerland)

The end

The Future

Atomic structure

     Pursue first killer application: nanocrystal diffraction “Structure” of whole proteins (biology) and reaction centers (chemistry) Extend to “function” through pump-probe studies of dynamics Explore crystal size limits toward “single molecule imaging” Explore transient atomic structure of matter (e.g. liquids) Develop terawatt, femtoseconds pulses •

Electronic and spin structure

   Understand electronic/spin structure of excited states Key systems are chemical reaction centers and complex materials Understand x-ray/electronic interactions with controlled pulses (damage limits, non-linear processes) Develop soft x-ray seeding and pulse manipulation toolbox (split, delay, pol. control, etc)

The central problem in structural molecular biology High radiation dose causes changes in molecular structure

typical mitigation strategies:

Use large crystals: keeps dose small, periodicity enhances diffraction

Cryogenically cool crystals

Tolerable dose in cryogenically-cooled crystals ≈ 0.02 eV / atom ≈ 6 ⨉ 10 10 ph/μm 2

Data for crystals < 1 μm 2 limited by poor (s/n) data or x-ray beam damage

Elspeth Garman, U. Oxford micrograph of crystal after exposing to x-rays and warming up

Nano-crystal diffraction provides access to new class of proteins e.g. cell membrane proteins that are hard to crystallize

Materials Science: The new paradigm Structure and Properties Long range order Static disorder Equilibrium States

1900

• most reliably calculated

Function and Control Nanoscale order Dynamic order Transient excited states

2000 future

• difficult to measure and calculate

Deep Science

Mining for Matter 33