Operation of a free-electron laser from the extreme ultraviolet to the water window
W. Ackermann
,
G. Asova
,
V. Ayvazyan
,
A. Azima
,
N. Baboi
,
J. B|[auml]|hr
,
V. Balandin
,
B. Beutner
,
A. Brandt
,
A. Bolzmann
,
R. Brinkmann
,
O. I. Brovko
,
M. Castellano
,
P. Castro
,
L. Catani
,
E. Chiadroni
,
S. Choroba
,
A. Cianchi
,
J. T. Costello
,
D. Cubaynes
,
J. Dardis
,
W. Decking
,
H. Delsim-Hashemi
,
A. Delserieys
,
G. Di Pirro
,
M. Dohlus
,
S. D|[uuml]|sterer
,
A. Eckhardt
,
H. T. Edwards
,
B. Faatz
,
J. Feldhaus
,
K. Fl|[ouml]|ttmann
,
J. Frisch
,
L. Fr|[ouml]|hlich
,
T. Garvey
,
U. Gensch
,
Ch. Gerth
,
M. G|[ouml]|rler
,
N. Golubeva
,
H.-J. Grabosch
,
M. Grecki
,
O. Grimm
,
K. Hacker
,
U. Hahn
,
J. H. Han
,
K. Honkavaara
,
T. Hott
,
M. H|[uuml]|ning
,
Y. Ivanisenko
,
E. Jaeschke
,
W. Jalmuzna
,
T. Jezynski
,
R. Kammering
,
V. Katalev
,
K. Kavanagh
,
E. T. Kennedy
,
S. Khodyachykh
,
K. Klose
,
V. Kocharyan
,
M. K|[ouml]|rfer
,
M. Kollewe
,
W. Koprek
,
S. Korepanov
,
D. Kostin
,
M. Krassilnikov
,
G. Kube
,
M. Kuhlmann
,
C. L. S. Lewis
,
L. Lilje
,
T. Limberg
,
D. Lipka
,
F. L|[ouml]|hl
,
H. Luna
,
M. Luong
,
M. Martins
,
M. Meyer
,
P. Michelato
,
V. Miltchev
,
W. D. M|[ouml]|ller
,
L. Monaco
,
W. F. O. M|[uuml]|ller
,
O. Napieralski
,
O. Napoly
,
P. Nicolosi
,
D. N|[ouml]|lle
,
T. Nu|[ntilde]|ez
,
A. Oppelt
,
C. Pagani
,
R. Paparella
,
N. Pchalek
,
J. Pedregosa-Gutierrez
,
B. Petersen
,
B. Petrosyan
,
G. Petrosyan
,
L. Petrosyan
,
J. Pfl|[uuml]|ger
,
E. Pl|[ouml]|njes
,
L. Poletto
,
K. Pozniak
,
E. Prat
,
D. Proch
,
P. Pucyk
,
P. Radcliffe
,
H. Redlin
,
K. Rehlich
,
M. Richter
,
M. Roehrs
,
J. Roensch
,
R. Romaniuk
,
M. Ross
,
J. Rossbach
,
V. Rybnikov
,
M. Sachwitz
,
E. L. Saldin
,
W. Sandner
,
H. Schlarb
,
B. Schmidt
,
M. Schmitz
,
P. Schm|[uuml]|ser
,
J. R. Schneider
,
E. A. Schneidmiller
,
S. Schnepp
,
S. Schreiber
,
M. Seidel
,
D. Sertore
,
A. V. Shabunov
,
C. Simon
,
S. Simrock
,
E. Sombrowski
,
A. A. Sorokin
,
P. Spanknebel
,
R. Spesyvtsev
,
L. Staykov
,
B. Steffen
,
F. Stephan
,
F. Stulle
,
H. Thom
,
K. Tiedtke
,
M. Tischer
,
S. Toleikis
,
R. Treusch
,
D. Trines
,
I. Tsakov
,
E. Vogel
,
T. Weiland
,
H. Weise
,
M. Wellh|[ouml]|fer
,
M. Wendt
,
I. Will
,
A. Winter
,
K. Wittenburg
,
W. Wurth
,
P. Yeates
,
M. V. Yurkov
,
I. Zagorodnov
&
K. Zapfe
Abstract
We report results on the performance of a free-electron laser operating at a wavelength of 13.7|[nbsp]|nm where unprecedented peak and average powers for a coherent extreme-ultraviolet radiation source have been measured. In the saturation regime, the peak energy approached 170|[nbsp]||[micro]|J for individual pulses, and the average energy per pulse reached 70|[nbsp]||[micro]|J. The pulse duration was in the region of 10|[nbsp]|fs, and peak powers of 10|[nbsp]|GW were achieved. At a pulse repetition frequency of 700 pulses per second, the average extreme-ultraviolet power reached 20|[nbsp]|mW. The output beam also contained a significant contribution from odd harmonics of approximately 0.6|[percnt]| and 0.03|[percnt]| for the 3rd (4.6|[nbsp]|nm) and the 5th (2.75|[nbsp]|nm) harmonics, respectively. At 2.75|[nbsp]|nm the 5th harmonic of the radiation reaches deep into the water window, a wavelength range that is crucially important for the investigation of biological samples.
To read this article in full you may need to log in, make a payment or gain access through a site license (see right).