High resolution RIXS from cuprates:
results and perspectives
L.
Bra
icovic
h
CN
R S
OF
T a
nd U
LT
RA
S,
Dip
. di F
isic
a,
Po
litecn
ico
di M
ilano,
Italy
,
Acknowledgments
-The
rese
arch
ers of M
ilan
o P
olite
cnic
o
Cla
udia
Dal
lera
Gia
com
oG
hirin
ghel
liA
lber
to T
agliaf
erri
-The
ERSF (G
renoble
) direc
tion
and the
staf
f of th
e ESRF-EX
AFS g
roup
(N.B
. Bro
okes
, J. G
oulo
nan
d c
o.)
-A
ll c
o-a
uth
ors
liste
d in the
follow
ing v
iew
gra
phs
-A
ll m
y stu
den
ts
-The
Sw
issLig
htSourc
e (S
LS)direc
tion
and the
staf
f of th
e A
DRESS-S
AX
ES g
roup
(T. Sch
mitt an
d V
. Stroco
v a
nd c
oll.)
-The
theo
rists (J
. van
den
Brink, L. A
men
tan
d c
oll.)
-The
EPFL g
roup (M
. G
rionian
d c
oll.)
-The
pre
siden
t of th
e M
ilan
o P
olite
cnic
o
and the
direc
tors
of D
ptm
of Physics
Lay-o
ut
PA
RT
1 C
upra
tes
His
tory
Spectr
osco
py o
f colle
ctive m
agne
tic e
xcitatio
ns
The inte
rpla
y b
etw
ee
n R
IXS
at vario
us e
dg
es
The c
ross fert
ilization w
ith n
eutr
ons
PA
RT
2 W
hat
do w
e n
ee
d t
o d
o b
ett
er
?
The n
ew
pro
ject
at th
e E
SR
F (
RIX
S +
XM
CD
)
The im
port
ance o
f cupra
tes
doe
s n
ot
need t
o b
e d
em
onstr
ate
d
Som
e h
isto
ry
Energ
y loss (
eV
)
La
2C
uO
4excited a
t C
u-3
d
-4-3
-2-1
02
1
AX
ES
@ ID
08, 2003. G
. G
hir
inghelliet al.,
Ph
ys R
ev L
ett. 92, 117406 (
2004).
∆ ∆∆∆E~0.8 eV
L. C
. D
udaet al., J. E
lectr
on S
pectr
osc.
Rela
t. P
henom
. 110–111, 275 (
2000).
∆ ∆∆∆E~1.2 eV
K. Ic
hik
aw
a et al., J. E
lectr
on
Spectr
osc. R
ela
t. P
henom
.
78, 183 (
1996).
∆ ∆∆∆E~1.6 eV
AX
ES
@ ID
08, 2007. L. B
raic
ovic
het al.,
arX
iv:0
807:1
140v1, (2
008).
∆ ∆∆∆E~0.45 eV
SA
XE
S @
SLS
, 2008. G
. G
hirin
ghe
lli, L.
Bra
icovic
h, T
. S
chm
itet al., unpublis
hed
∆ ∆∆∆E~0.13 eV
Incid
ent photo
n e
nerg
y ~
931 e
V
Com
bin
ed r
esolv
ing p
ow
er
incre
ase b
y a
facto
r of 12
World
record
2003
World
record
spring
2007
World
record
spring
2008
World
record
2000
Mila
no
Up
psa
la
ES
RF
SLS
La
2C
uO
4=
LC
O
Energ
y loss (
eV
)
La
2C
uO
4excited a
t C
u-3
d
-20
AX
ES
@ I
D08
, 2003
. G
. G
hirin
gh
elliet al.,
Ph
ys R
ev L
ett
. 92
, 11740
6 (
20
04
).
G.
Gh
irin
gh
elli
, N
. B
. B
roo
ke
s,
E.
Anne
se
, H
. B
erg
er,
C.
Da
llera
, M
. G
rio
ni, L
. P
erf
ett
i, A
. T
aglia
ferr
i, a
nd
L.
Bra
ico
vic
h
ES
RF
First L2,3
evid
ence
of th
e d
d
dependence
on the
str
uctu
re
x 2
00
Very
sm
all
cro
ss s
ection
Essentially
no K
of th
e p
hoto
n
(< 7
% o
f th
e B
Z a
round (
0,0
))
Energ
y loss (
eV
)
La
2C
uO
4excited a
t C
u-3
d
-20
FIR
ST
EV
IDE
NC
E O
F D
ISP
ER
SIO
N
AX
ES
@ ID
08 (
ES
RF
)
fall
of 2007.
L. B
raic
ovic
het al.,.
L. B
raic
ovic
h,
L. J. A
ment, V
. B
isog
ni, F
. F
ort
e, C
. A
ruta
, G
. B
ale
str
ino, N
. B
. B
rookes, G
. M
. D
e L
uca,
P. G
. M
edag
lia,
F. M
iletto G
ranozio
, M
. R
adovic
, M
. S
allu
zzo,
J. van d
en B
rink, and G
. G
hirin
ghelli
Phys.
Rev.
Lett. 102, 167401 (
2009)
ES
RF
Energ
y loss (
eV
)
La
2C
uO
4excited a
t C
u-3
d
-20
1.0
0.5
0.0
010
20
A
B
CD
Ene
rgy lo
ss (
eV
)LC
O a
t 15
K a
nd
q// 1
.85
5
Normalized intensity
(b)
XA
S 933
92
9 Ph
oto
n e
nerg
y (
eV
)
L. B
raic
ovic
h,
J. van d
en B
rink, V
. B
isog
ni, M
. M
ore
tti S
ala
, L.A
ment, N
.B. B
rookes, G
.M. de L
uca,
M.
Sallu
zzo, T
. S
chm
itt, a
nd G
. G
hirin
ghelli
(to
be p
ublis
hed)
FIR
ST
Dis
en
tan
glin
g o
f m
agn
on
and
bim
ag
no
n
SA
XE
S @
AD
RE
SS
(SLS
)
fall
of 2008.
SL
S
Mila
n +
The N
eth
erland +
ES
RF
+ S
LS
+ N
aple
s
-3-2
-10
12
3
0
100
200
300
q
Energy (meV)
400
LC
O a
t 15 K
RIX
S
L. B
raic
ovic
h,
J. van d
en B
rink, V
. B
isog
ni, M
. M
ore
tti S
ala
, L.A
ment, N
.B. B
rookes, G
.M. de L
uca,
M.
Sallu
zzo, T
. S
chm
itt, a
nd G
. G
hirin
ghelli
(to
be p
ublis
hed)
RIX
S b
y
Neu
tro
ns
Ne
utr
ons b
y
SLS
What about bim
agnons
?
Any o
ther
way t
o e
xp
lore
bim
agn
ons
?
Yes
Direct
exp
lora
tion
if there
is
NO
SP
IN-O
RB
IT
in t
he
inte
rmed
iate
sta
te
Cu K
-ed
ge R
IXS
(J. H
ill e
t al.)
Oxy K
-edg
e R
IXS
-1.0
-0.5
0.0
Tra
nsfe
rred e
nerg
y
-10
Tra
nsfe
rred e
nerg
y
SLS
Cu-L
3
RIX
S
8.97
8.98
8.99
9.00
9.01
ener
gy (K
eV)
0-0
.5-1
.0
transfe
rred
energ
y
Cu-K
RIX
SID
16 –
ID12 –
Mila
no c
oll.
V.
Bis
ogni, L
. S
imonelli
et al.
ES
RF
Cu-K
RIX
S
528
530
532
534
Energ
y (
eV
)
XA
S
SLS
ES
RF
Oxygen
-0.5
0.0
Cu-L
3
Oxy-K
Go
to
Oxyg
en
K-e
dg
e
(ES
RF
)
Diffe
rent sam
plin
g !!!!
Sum
marizin
g p
art
I
The h
ighlig
ht
is t
he D
ISP
ER
SIO
N
at
all
edge
s (
in p
art
icula
r S
OF
T x
-ra
ys)
Cro
ss f
ert
ilization w
ith n
eutr
ons
Very
sm
all
sa
mple
s (
a f
ew
monola
yers
)
Goal: m
onola
yer
sensitiv
ity
Dra
matic e
xp
ansio
n o
f th
e f
ield
with r
espect
to n
eutr
ons
What
do w
e n
eed ?
A c
onsid
era
ble
incre
ase o
f re
solu
tio
n
in t
he s
oft r
ang
e
7000
10000
20000
3000
0
4000
0
ela
st
ph
ma
gb
ima
g
Aro
und
½of
the B
Z
-0.3
-0.2
-0.1
0.0
0.1
energ
y loss (
eV
)
ES
RF
+ M
ilano
goa
l
Sca
ling u
p b
y a
facto
r of
2 i.e.
10 m
ete
rs s
pectr
om
ete
r
Movable
Pla
tform
SAXES, a high resolution spectrometer
for resonant x-ray emissionin the 400–1600 eVenergy range
G. G
hirin
ghelli
, A
. P
iazzalu
nga, C
. D
alle
ra, G
. T
rezzi, a
nd L
. B
raic
ovic
h
DipartimentodiFisica, PolitecnicodiMilano, Piazza Leonardo daVinci 32, I-20133 Milano, Italy
T.
Schm
itt,
V. N
. S
trocov, R
. B
ete
mps, and L
. P
atthey
Swiss Light Source, Paul ScherrerInstitut, CH-5232 VilligenPSI, Switzerland
X.
Wang a
nd M
. G
rioni
Institutde Physique des Nanostructures, EcolePolytechniqueFédéderalede Lausanne,CH-1015 Lausanne,
RE
VIE
W O
F S
CIE
NT
IFIC
IN
ST
RU
ME
NT
S 77, 11
3108,2006
Mila
no
Up
psa
la
ES
RF
SLS
ES
RF
Framework: Electronic and magnetic properties of matter.
Goal: To understand the interplay between the electronic, spin and orbital
degrees of freedom which determ
ine the physical properties of materials.
Evo
lutio
n o
f B
L8 o
f th
e E
SR
F in a
ne
w a
mbitio
us p
roje
ct
Ne
ed
of
a v
ery
lo
ng
be
am
-lin
e (
typ
ica
lly 1
20
m)
pro
ba
bly
with
tw
o m
on
och
rom
. (R
IXS
an
d X
MC
D)
Ne
ed
of
a n
ew
bu
ildin
g
RIX
S X
MC
D
ESRF Upgrade:
Magnetism
“vill
ag
e”
Incre
ased f
lux.
Incre
ased s
tabili
ty.
Lon
g b
eam
line
with s
pace
for
experim
enta
l in
fra-s
tructu
re
even w
ith s
mall
beam
s.
Ne
w instr
um
ents
.
High DC magnetic field lab.?
RIX
S: very
hig
h c
om
bin
ed e
nerg
y r
esolu
tion (
at le
ast 30000).
Beam
siz
es (
e.g
. 3 x
50 m
icro
ns)
A LOT OF SPACE
aro
und the instr
um
ent A
ND
AR
OU
ND
TH
E S
AM
PLE
for
q d
ependent m
easure
ments
and
experim
enta
l fa
cili
ties e
.g. a h
igh m
agnetic fie
ld.
“XM
CD
”: s
mall
spots
mic
rons. S
pace for
instr
um
enta
tion,
sam
ple
pre
para
tion e
.g. puls
ed laser
depositio
n
An inte
llige
nt
com
bin
ation o
f te
chno
logie
s w
ill a
llow
un
ique p
erf
orm
ances o
f th
e instr
um
ents
The p
ers
pe
ctive is t
o tell
som
eth
ing
really
ne
w in t
he m
ediu
m p
erio
d
Past
and f
utu
re o
f th
e c
olla
bora
tion w
ith M
ilano P
olit
ecnic
o
tim
e
Gre
ek n
am
e o
f th
e G
od o
f w
ar
No w
ar.
“W
ars
are
not
wo
n b
ut
only
lost”
(W.
Churc
hill
)
Fair c
om
petitio
n
AX
ES
rebuild
ing at th
e E
SR
F201
0
AX
ES
at
the E
SR
F (
Advance
d X
-ra
y E
mis
sio
n S
pectr
osco
py)
199
5
201
3N
ew
RIX
S p
roje
ct
at th
e E
SR
F
AR
ES
(A
dvance
d R
Esona
nt
Scattering)
SuperA
XE
S=
SA
XE
S
at
SLS
(S
AX
ES
= s
uccess)
200
7-8
MA
KE
P
HY
SIC
S N
OT
W
AR