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Lorenzo Avaldi CNR-Istituto di Struttura della Materia Area della Ricerca di Roma 1 Institute of Structure of Matter Outlook dynamical energy flow in uracil ISM and LNF SPARC-Lab Eurofel Lab

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Page 1: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Lorenzo Avaldi

CNR-Istituto di Struttura della Materia Area della Ricerca di Roma 1

Institute of Structure of Matter

Outlook

• dynamical energy flow in uracil

• ISM and LNF

• SPARC-Lab

• Eurofel Lab

Page 2: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Nucleobases absorb sytrongly UV radiation

Photo excited states are reactive

How does the molecule survive ?

Time resolved experiments - the question and the approach

Page 3: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Image credit to

Markus Gühr

(Pulse Inst., SLAC)

conical

intersection

Page 4: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Our approach : to record inner shell

photoelectron spectra as a function

of pump-probe delay

Advantages

1) XPS above threshold ionizes

molecule at any nuclear geometry ( no

yield reduction due to FC overlap as in

optical valence shell ionization)

2) element and site selectivity

Page 5: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

LCLS hv= 346 eV (150 pC, 80-100 fs, 120 Hz)

Electron spectrometer : 2 m long magnetic

bottle (R. Feifel, Uppsala University)

Uracil molecules

evaporated in an

inductive oven at

140° (density

1011 cm-3 )

Alignment tools

Time resolved experiments : where and how

Page 6: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Simulation of the experiment C 1s BE (eV) ΔE (eV) label

C5 291.0 - A

C6 292.8 1.8 B

C4 294.4 3.4 C

C2 295.4 4.4 D

O. Takahashi, Hiroshima University, Japan K. Ueda, Tohoku University, Sendai, Japan

287 288 289 290 291 292 293 294 295 296 297

0.0

0.5

1.0

1.5

2.0

C5 C

4C

6

Inte

nsi

ty (

arb

itra

ry u

nits

)

S0

Binding energy (eV)

C2

288 290 292 294 296

0

2 n* S1

288 290 292 294 296

0

2

4

S2*

10 % excited

molecules

FWHM =0.5 eV 288 290 292 294 296

0

1

2

Inte

nsi

ty (

arb

itra

ry u

nits

)

Binding energy (eV)

S0

288 290 292 294 296

0

1

2

3

S1

288 290 292 294 296

0

1

2

3 S2

288 290 292 294 296

-0.2

-0.1

0.0

0.1

0.2288 290 292 294 296

-0.2

-0.1

0.0

0.1

0.2

Diff

eren

ce

Binding energy (eV)

Difference spectra

Calculations and simulations

Page 7: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

LCLS SASE Fel : spectral width + spectral jitter

338 340 342 344 346 348 350

0

50000

100000

150000

200000

250000

pu

lse

en

erg

y d

istr

ibu

tion

photon energy (eV)

SumAll

Gauss fit of hvHist_A

FWHM=2,5eV

280 285 290 295 300 305

0.0

0.2

0.4

0.6

Binding energy (eV)

280 285 290 295 300 305

0.0

0.2

0.4

0.6

S0

S1

280 285 290 295 300 305

0.0

0.2

0.4

0.6 S2

280 285 290 295 300 305

-0.02

0.00

0.02Diff

ere

nce

Binding energy (eV)

280 285 290 295 300 305

-0.02

0.00

0.02

Difference spectra

-1,0 -0,8 -0,6 -0,4 -0,2 0,0 0,2 0,4 0,6 0,8 1,0

0

200

400

600

800

1000

1200

Tim

eP

ixE

dge H

isto

gra

m

delay (ps)

Pump-probe : measurement of actual delay shot by shot to

take into account the time jiiter between XFel and UV laser

Page 8: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

delay 500 fs

280 285 290 295 300 305

-0.02

0.00

0.02Diffe

rence

Binding energy (eV)

280 285 290 295 300 305

-0.02

0.00

0.02

Difference spectra

0 50 100 150 200 250 300 350

0

2

4

6

8

10

12

14

Valence

C Auger

yiel

d (a

rb.u

nits

)

kinetic energy (eV)

C(1s)

280 285 290 295 300 305 310

0

2

4

6

8

280 285 290 295 300 305 310

-0,10

-0,05

0,00

0,05

0,10

diff

ere

nce

binding energy (eV)

Results

Page 9: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

280 285 290 295 300 305

-0.02

0.00

0.02Diff

ere

nce

Binding energy (eV)

280 285 290 295 300 305

-0.02

0.00

0.02

Difference spectra

Page 10: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

287

288

289

290

291

292

293

294

295

296

297

0.0

0.5

1.0

1.5

2.0

C5

C4

C6

Intensity (arbitrary units)

S0

Bin

din

g e

nerg

y (e

V)

C2

288

290

292

294

296

02S

1

288

290

292

294

296

024

S2

0 2 4 6 8 10

0.0

0.1

0.2

Dife

fre

nce

(a

rbita

rry

un

its)

Delay (ps)

0 2 4 6 8 10

0.0

0.1

0.2

Delay (ps)

Dife

fre

nce

(a

rbita

rry

un

its)

0 2 4 6 8 10

0.0

0.1

0.2

Delay (ps) D

ifefr

en

ce (

arb

itarr

y u

nits

)

mean=0.00154

uncertainty=0.007

min=-0.013

max=0.014

𝜏1 =200 fs

𝜏2 =6 ps

𝜏2 =6 ps

Resorting on shot-to-shot

delay (slots 30fs*n )

287 288 289 290 291 292 293 294 295 296 297

0.0

0.5

1.0

1.5

2.0

C5

C4

C6

Inte

nsi

ty (

arb

itra

ry u

nits

)

S0

Binding energy (eV)

C2

288 290 292 294 296

0

2 S1

288 290 292 294 296

0

2

4

S2

b c

280 285 290 295 300 305 310

0

2

4

6

8

4 eV

binding energy (eV)

C(1s)

photo

ele

ctr

on y

ield

(arb

. units)

a b c

Page 11: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

X-ray photoelectron and Auger electron spectroscopies have been used to investigate

energy relaxation in UV excited uracil → Advent of seeded Fel’s

Fast and slow dynamics have been observed : fast dynamics attributed to nuclear

dynamics (vibrational relaxation in the ππ* state) + slow dynamics due to tunneling

(coupling of electronic states via conical intersection)

To be proved/disproved by molecular

dynamics calculations

Conclusions

Page 12: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

CNR-ISM & INFN-LNF

A high-resolution VUV beamline @ SPARC-Lab A. Marcelli, INFN – LNF E. Pace INFN, Università di Firenze M. Coreno, CNR-ISM L. Poletto, CNR-IFN, Padova

• wavelength range (with high harmonics) 250-40nm

• repetition rate: 1-10 Hz

• radiation spectrum «slightly» tunable

• higher harmonics linearly polarized sources with high temporal

and spatial coherence

• pulse duration: 100 fs

Page 13: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

The scientific case (October 2008)

Topics

• Atomic and molecular physics

• Astronomy

• Nanostructure

• Anelastic scattering

• Biology and astrobiology

• UV induced damaging

• Photochemistry

• Quantum coherence and entanglement

Page 14: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Ref. Marcello Coreno Figure 1. Pictorial crossing between the two lowest-energy electronic

states of [(BZC2H5)R]+ (full lines) and [(BZC2H5)R . Csolv]

+ (broken lines).

Electronic properties of biomolecules and their clusters

Solvent-free environment :

→ easier modeling of different intermolecular forces

→ results comparable with theoretical calculations

Variable polarization and λ < 150 nm from SPARC extends investigation to σ-bonded systems like sugars and non aromatic aminoacids and implement valence photoemission techniques for the study of chiral recognition.

Page 15: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Raman spectroscopy on isolated building blocks of nanostructured films

Raman spectroscopy is among most popular methods for characterization of nano-structured systems. The ability of the VUV-FEL to shift the wavelength of scattered light from visible into deep UV will allow to probe new electronic transitions well within the 7-10 eV range for classes of cluster materials such as nano-carbons and potential gap dielectrics from metal oxides

Raman Imaging…!

Ref. Claudio Marcelli

Correlation map between band gap and dielectric constant in many insulators and semiconductor materials. The dotted line points out the gap value of 220 nm (~5.64 eV).

Page 16: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Monochromator High-resolution high-spectral

purity 5m McPherson

Normal Incidence

UV-VUV monochromator

from SRS-Daresbury,

beamline 3.2

Page 17: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

TOF-300 set-up

Test with rare gas discharge lamp [21.22 eV (He I), 16.67 eV (Ne I) and 11.62 eV (Ar I)]

CH2I2 diiodomethane

Page 18: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

“(2012) Il consorzio EuroFEL nasce da un approccio globale…… L'infrastruttura di ricerca distribuita su piu' sorgenti diverse tra di loro permetterà la realizzazione di linee di luce tra loro complementari, con la possibilità di aprire l'infrastruttura nel suo complesso a campi di ricerca non tradizionali e quindi a nuove utenze…. Il tempo di luce disponibile presso le linee di FEL è e rimarrà limitato e quindi esperimenti preparatori e complementari da svolgersi presso linee di luce di sincrotrone e laboratori CNR saranno essenziali per garantire un utilizzo efficiente da parte della comunità scientifica CNR e più in generale italiana delle nuove sorgenti pulsate.”

CW Pump laser

Ti:sapphire oscillator 1 KHz regenerative amplifier (>2 mJ)

1 KHz Pump laser

Pulse diagnostic

(ENEA)

XUV Spectrometer

for HHG diagnostic

HHG generation chamber

Duplication optics /OPA

Variable delay stage

Experimental stations ( UV-XUV time resolved)

Eurofel support Lab @ISM

Page 19: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Optical parametric amplifier (OPA) 240 – 15000 nm Output ≥220 uJ for 1 mJ input Input (800 nm: 2 mJ)

Page 20: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima
Page 21: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Monochromatic beamline for ISM-Roma Luca Poletto and Fabio Frassetto CNR – Institute of Photonics and Nanotechnologies, Padova (Italy)

Page 22: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima
Page 23: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

ACKNOWLEDGMENTS

M. Coreno, P. Bolognesi, D. Catone, P. O’Keeffe, S. Turchini,

N. Zema, D. Rau, S. Colonna, C. Quaresima, A. Cricenti, A.

Paladini, S. Priori, M. Brolatti, M. Luce

Area di Ricerca Roma 2

Area di Ricerca Roma 1 Sincrotrone Elettra - Area Science Park-

Area di Ricerca Potenza

Page 24: Institute of Structure of Matter · Simulation of the experiment C 1s BE (eV) ΔE (eV) label C 5 291.0 - A C 6 292.8 1.8 B C 4 294.4 3.4 C C 2 295.4 4.4 D O. Takahashi, Hiroshima

Studies of dynamical energy flow in molecules using covariance mapping

LCLS Beamtime L508

Paola Bolognesi

Patrick O’Keefe

Lorenzo Avaldi

Valerio Rossi Albertini

Robert Richter

Kevin Prince

Melanie Mucke

V. Zhaunerchyk

M.N. Piancastelli

John Eland

Raimund Feifel Timur Osipov

Brendan Murphy

Li Fang

Nora Berrah

Subhendu Mondal

Kyioshi Ueda

Tommaso Mazza

Michael Meyer

Catalin Miron

Peter v.d. Meulen

Peter Salen

Mats Larsson

John Bozek

C. Bostedt

Ryan Coffee

S. Carron

Emily F. Sistrunk Jakob

Grilj

Brian K. McFarland

Markus Koch

Markus Guehr

L.J. Frasinsky