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UGO F
FANO SYMP
USY
Antonio
POSIUM 201
UGOYMP
2
Bianconi, A
Supers
16 edited by
O FAPOS
2016
edited by
Augusto Ma
stripes Press
y A. Biancon
ANOSIU
6
arcelli, Andr
s, Rome
ni, A. Marce
O M
rea Perali
elli, A. Peralali
1
UGO F
U
FANO SYMP
Ugo F
B
Antonio
Ugo Fano
POSIUM 201
Fano SM
Comple
Fan
Book o
Bianconi, A
Symposium
Supers
ISBN
16 edited by
SympMetamateria
ex Quantum
no Resonan
of Ab
edited by
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stripes Press
N 978886683
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m Matter
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arcelli, Andr
taly) Dec. 1
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30610
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9-21, 2016
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Giorgio Pae physics of jory
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POSIUM 201
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POSIUM 201
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mples will bean der Waalsrum.
POSIUM 201
s, surface p
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surface plaseometry. Forial with a ron optics to n this way we given of ss forces and
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POSIUM 201
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POSIUM 201
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face plasmowave-lengthoparticles, fble. Hybridacting speciplasmons oical propertiMNP buildinoherent (difnsferred bacvicinity of t
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ur method bery large hybantum Mechht needed toconsider a res sections fralence electdielectric fu
POSIUM 201
es for optics and metal
dei
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becomes extbrid networhanics and Mo fully explenormalizatrom molecutrons of the unction, wh
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cal responsllic nanopa
rsity, Boston
rticle (MNPenhance the known to exd semicondueractions benovel effectetwork comgration in a avelike). In
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ni, A. Marce
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onic modeshas been invlism, and is pression an
w building bl equations. linear von Nx of each SQhin the discthe standardcan be cast
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itations of tlastic scattertallic nanoponant x-ray x-ray edges
L. Hayati, C245411 (
B. Barbielli
B. Barbielli(2017).
B. BarbielliT. Schmi
B. Barbielli
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the metallic ring is prodarticles. Siminelastic sc
s [5].
C. Lane, B. 2016).
ini and P. N
ini, Low Te
ini, J. N. Haitt, Phys. Re
ini, Y. Joly,
POSIUM 201
nanoparticlduced by themilar theorieattering [4]
Barbiellini,
Nicolini, Phy
emperature P
ancock, C. Mev. B 89, 23
, and Kenji
16 edited by
les [3]. Thee resonant ees have bee and the beh
, A. Bansil,
ys. Rev. A 8
Physics/Fiz
Monney, Y.35138 (2014
Tamasaku,
y A. Biancon
e source of texcitation ofen successfuhavior of no
and H. Mo
84, 022509
zika Nizkikh
. Joly, G. G4).
Phys. Rev.
ni, A. Marce
he enhancef surface plaully used to onlinear sus
sallaei, Phy
(2011).
h Temperatu
hiringhelli,
B 92, 1551
elli, A. Peral
ed photon asmons at thexplain the
sceptibilities
ys. Rev. B 9
ur 43, to app
L. Braicov
119 (2015).
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Uncloaking nsition of Fd interactio
los A. R. Sá
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los.sademel
investigatemensional (2
he two-bodyeric form oflution betwes. We shownsition tempding energy
mpared to thsity tensor bse-fluctuatiome circulaerimental siition, we sh
mperatures ininct uniformerfluid phasuced by the
Jeroen P. At. 113, 1653
Jeroen P. Aview A 92, 0
Jeroen P. Aparation, so
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topologicaFermi superons.
á de Melo
sics, Georgi
o@physics.
e the BerezinD) neutral Fy binding enf the SOC,
ween the equw that in theperature TBK
y. We also fihe case withbecomes anon action th
ar in the ROignature for
how that then the vicinitm superfluidses which inpresence o
A. Devreese,304 (2014).
A. Devreese,043618 (20
A. Devreese,on to appea
POSIUM 201
al phases inrfluids: An
a Institute o
.gatech.edu
nskii-KosteFermi systenergy and aas a functio
ual Rashba-De ERD case,KT is increasfind a signifiout SOC. F
nisotropic (ehat describe
O limit. Thisr superfluidie anisotropicty of quantud phases. Finvolve the cf spin-orbit
, Jacques Te
, Jacques Te15).
, Jacques Tear at the ArX
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n the Berezin interplay
of Technolo
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um phase trainally, we dcoupling of and Zeema
empere, and
empere, and
empere, andXiv (2016)
y A. Biancon
inskii-Kostof spin-orb
ogy, Atlanta
ess (BKT) tn-orbit coupular Zeemana and Dresss (ERD) andon-zero Zeeffect of the
ase in the vae, we demone RO case),ortices and aon constituteFermi systeocity exhibiansitions be
discuss new “charge” an
an fields.
d Carlos A.
d Carlos A.
d Carlos A.
ni, A. Marce
terlitz-Thoubit coupling
a, GA, 3033
transition inpling (SOC)n field [1]. Bselhaus termd the Rashbman field, tSOC for all
alue of the Cnstrate that t leading to anti-vorticees an impor
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ms, we studyba-only (ROthe BKT l values of t
Clogston limthe superfluan anisotro
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RD SOC. In s at low
ologically more exotic ortices [3]
Melo, Phys. R
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POSIUM 201
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POSIUM 201
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POSIUM 201
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e strange mectron systeme difficultiesthematical fsity, the “feng theory botter physics lso the first
ese holograpiety, at the sese are quanmputable witmonstrate thsible. I will
ucture of theReferences
J. Zaanen, ondensed M
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hic duality,
tz for Theor
etals as obsems are arguas are rooted framework termion sign oils down tocan be commethod yie
phic strangesame time dntum criticalth conventiat their groupresent the
ese vacua.
Y.-W. SunMatter Physi
POSIUM 201
strange me
retical Physi
erved in higably the grea
in the fundto deal withproblem”.
o the remarkmputed usingelding a prece metals are defeating thel phases witonal methodund states ae case that th
, Y. Liu, K.ics (Cambri
16 edited by
etals and e
ics, Leiden
gh Tc supercatest enigm
damentals ofh strongly inThe hologrkable fact thg the equaticise descrip suggestivee basic printh scaling pds. Remark
are more denhis is rooted
. Schalm, Hidge Univ. P
y A. Biancon
ntanglemen
University,
conductors ama of conden
f physics: thnteracting feaphic dualithat all of coions of geneption of nonly similar to
nciples of boproperties alkably their ensely entangd in a highly
Holographic Press, 2015)
ni, A. Marce
nt.
, The Nethe
and other consed matter he lack of a ermions at fty as discovonventional erality relatin-Fermi liquo the laboraosonic field ien to thosentanglemengled than dey unconvent
Dualtity for)
elli, A. Peral
erlands
orrelated physics.
a general finite vered in
condensed ivity, but it uids [1]. atory
theory. e nt entropies eemed
ntional sign
r
ali
19
13.
Igor
Dep
Col
Hypof odembehinclelecgravmetmethypTc tmetsuggsubjformstanphyand may
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Hyperbolic
r I. Smolyan
partment of
llege Park, M
perbolic meoptical imagmonstrate a n
avior of thelude super rctrodynamicvitation theotamaterial sutamaterials bperbolic metthat is threetamaterial sugested modjected to a mm small hypndpoint behaysics”, such
different ray be used to
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c Metamat
ninov
f Electrical a
MD 20742,
etamaterials ging. Soon tnumber of neir density oresolution imc effects, theory analoguuperconducbased on fetamaterial sue times that uperconduc
del of a multmodest exteperbolic metave as indivas different
adiation lifeo study mod
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erials
and Compu
USA
were originthereafter itnovel phenoof photonic maging, newermal hyper
ues. I will rectors and selrrofluids. Auperconducof pure alum
ctors will betiverse baseernal magnetamaterial dvidual “Mint strength ofetimes. Thusdels of MON
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ter Enginee
nally introdut was realizeomena resulstates. Thes
w stealth tecrconductivieview in molf-assemble
Aluminum-bctors exhibitminum. Proe discussed.ed on a ferroetic field, thdomains, whnkowski spaf effective gs, the ferrof
ND and to il
y A. Biancon
ering, Unive
uced to oveed that hypelting from thse novel phechnologies, ty, supercon
ore detail reed three-dimbased epsilot supercond
omising fracI will also
ofluid. Whehe nanopartihich from thacetimes” exgravity, difffluid-based llustrate the
ni, A. Marce
ersity of Ma
ercome the derbolic metahe broadbanenomena anenhanced qnductivity, cent researc
mensional hyon near zeroducting criticctal geometrconsider then the ferrofcles inside the electromxhibiting different versiometamateri fine-tuning
elli, A. Peral
aryland,
diffraction lamaterials nd singular nd applicatioquantum-and interestch on yperbolic
o (ENZ) andcal temperaries of e recently fluid is the ferroflu
magnetic fferent “lawons of MONial “multiveg mechanism
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limit
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ws of ND rse” m.
14. M. IMax We 203of zinfrpresThenumprosbe d 1. DNatu2. E
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High temp
I. Eremets, Ax Planck Ins
will presen K[1] in dif
zero resistanared and Rasented. e observed amerous theorspects for acdiscussed to
Drozdov, A.ure 2015. 5
Einaga, M.,
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perature co
A. P. Drozdstitute of Ch
nt our recentfferent hydrnce, Meissnaman studie
apparently cretical workchieving hig
oo.
P., et al., Co25: p. 73-77et al., Cryst
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nventional
dov hemistry, M
t results on rides. The suer effect, iso
es. Results o
conventionaks. Recent pgher critical
onventional7. t
16 edited by
supercond
Mainz, Germ
the high temuperconducotope effecton studies o
al supercondproposals ofal temperatu
l supercond
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ductivity
many
mperature sctivity has bt, X-ray diff
of pure hydr
ductivity wif new super
ures of super
ductivity at 2
ni, A. Marce
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ffraction studrogen also w
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203 K at hig
elli, A. Peral
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tallic hydroerconductortallic state interials are ex
wer pressuresterials are doer metallizath materials adrogen-based
re, we theorerconductor
S can be form
2S+H2→2Hstant transitasurements[
erconductiv
D. Duan, Y, Sci. Rep., , B. Liu, T.
A. P. Drozd, 73-76 (20
M. Einaga, Troyan, N. H
X. Huang, XT. Cui, arX
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-rich materors
oratory of S30012, P. R.
gen under hr. However,n the pressuxtensively es because oominated bytion, such asare expectedd supercond
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3S [1]. Then,
tion, isotope2-4]. Further
vity in other
Y. Liu, F. Tia4, 6968 (20Cui, Phys. R
dov, M. I. E15).
M. Sakata, Hirao, Y. O
X. Wang, DXiv:1610.02
POSIUM 201
rials under
uperhard M. China E-
high pressur, there are nure range upexplored sinf chemical py hydrogen s high-tempd to becomeductor.
dicted H3S aching as hih pressure b, these resule effect, Mermore, we ar hydrogen-r
an, D. Li, X014); D. DuRev. B, 91,
Eremets, I. A
T. IshikawOhishi, Natu
D. Duan, S. B2630 (2016)
16 edited by
high press
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re is believeno experimep to 388 GPnce their mepre-compre elements, m
perature supe a new mem
with Im-3migh as 200 K
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X. Huang, Zuan, X. Huan, 180502 (20
A. Troyan, V
wa, K. Shimiure Phys., 12
Bertil., L. X).
y A. Biancon
sure: towar
College of phss: cuitian@
ed to be a roental evidenPa. As an altetallization cessions. Mormost novel pperconductivmber of sup
m symmetry K at high pr
n ways: 3H2
en confirmect and synchd the crystaals at high p
Z. Zhao, H. Yng, F. Tian,015).
V. Ksenofon
izu, M. I. Er2, 835-838 (
Xin, Y. Hua
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hysics, Jilin @jlu.edu.cn
oom-tempernce for the pternative, hycan happen reover, becaproperties cvity. Therefperconducto
to be a highressure and S→2H3S+Sd by in situhrotron X-raal structure apressures.
Yu, B. Liu, , D. Li, H. Y
ntov, S. I. S
remets, A. P(2016).
ng, F. Li, Q
elli, A. Peral
emperature
n University,
rature predicted ydrogen-ric
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W. Tian, TYu, Y. Liu,
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POSIUM 201
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which allpairs, with hlogical tran
POSIUM 201
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nics was dethe macroscphysics. Hoysics of livine range betcale cohereeractions inperconductivunity in thecoherence inow temperathrough towphysics of ctors dvanced ouario wherence betweeng Lifshitz ge from atomparation (NPS scenario NPS was oFS methodctrons fluctperconductiphase the m
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omplex systoexist. Finauperconduct
eferences: A. Bianconidoi:10.1142N. Poccia, e
10.1073/pnaA. Bianconi2614(78)856A. BianconiA. BianconiA. Bianconi005-0047-5.A. Bianconi2048/28/2/0K I Kugel et2048/22/1/0G. Campi, DMagnetism
G. CamInnocenti, J.(2015) doi:1
FANO SYMP
extrinsic diand shape rature superctem in the ally I willivity at 203
i, Int. J. Mo2/S02179792et al., Proc. as.12084921i, et al. Chem629-2. i et al. Physi et al Europi, Journal of. i et al. Supe024005 t al Superc
014007 D. Innocenti28, 1355 (2
mpi, A. Bian. Karpinski,10.1038/natu
POSIUM 201
sorder giveresonance [6conductivityintermediat
l show thaK in the pre
d. Phys. B 1200003769.Nat. Acad.
109. mical Physi
Rev. B 44, phys. Lett. 3f Supercond
rcond. Sci.
cond. Sci. Te
i, and A. Bi2015) http://nconi, N. Po, N. D. Zhigure14987
16 edited by
es both phas6] in a comy emerges wte regime wat this sceessurized su
14, 3289 (2. Sci. 109, 1
ics Letters 5
10126 (19931 411 (199ductivity 18
Technol. 28
echnol. 22 0
ianconi, Jou/dx.doi.org/occia, G. Biagadlo, S. M
y A. Biancon
se separatiomplex geomwhere shapwhere localenario provulfur hydrid
000),
5685 (2012
59, 121 (197
91), doi: 10.95) doi:10.1, 625 (2005
8 024005 (2
014007 (200
urnal of Sup/10.1007/s10anconi, L. B. Kazakov,
ni, A. Marce
n [7,8,9,10,metry [2]. Wpe resonanclization andvide the e
des
2), doi:
78) doi:10.1
1103/physr209/0295-5
5), doi: 10.1
2015) doi:10
09) doi:10.1
perconductiv0948-015-2
Barba, G. Aet al., Natur
elli, A. Peral
,11] with CWe propose ces dominatd delocalizaexplanation
1016/0009-
revb.44.1015075/31/7/0007/s10948
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Novel comperiors of gianNovel comp
Na2HeO.
ferences Oganov A.RLyakhov AZhu Q. et aZhou X.-F. Qian G.R. eZhu Q. et aOganov A.RMa Y. et alZhang W.W] Zhu Q. et
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h-pressure p
nov
tute of Sciek University
ds of crystalerials at extroptimal pro
ery powerfuble compounchemical eleextensions
d large structechnique csults that I wand experim
ulating and oability of “imNa3Cl, Na2
ounds in thent planets. ounds of he
R. et al, J.C.O. et al., Cl, Acta Cryset al, Phys.
et al. Sci.Repl, Cryst.EngR. et al, Nat, Nature 45
W. et al, Scieal., Phys. C
POSIUM 201
phenomena
nce and Tecy, NY 11794
structure preme conditoperties for l evolutionands and theements. Recto low-dimectures to be called evoluwill discuss
mental evideoptically trampossible”
2Cl, Na3Cl2,e C-H-O, N
elium, stable
Chem.Phys. Comp. Phys.st. B68, 215 Rev. Lett. 1
ep. 4, 5606 (g.Comm. 14ture 457, 868, 182 (200ence 342, 15
Chem. Chem
16 edited by
a discovere
chnology, 54-2100
prediction hations and pevarious appary algoritheir crystal stcent developensional syshandled ea
utionary mets include: ence for a nansparent fochemical c
, NaCl3, NaCN-H and Mg
e at experim
124, 24470 Comm. 184
5-226 (2012109, 24550(2014). 4, 3596-36063 (2009). 09). 502-1505 (2
m. Phys. 15,
y A. Biancon
ed through
5 Nobel St.,
ave opened erform compplications. Inm USPEX tructures at pments inclstems and msily, e.g. Mtadynamics
new partiallyorm of sodiuompounds tCl7 [9], Mg
g-Si-O syste
mentally rea
4 (2006). 4, 1172-118
2). 3 (2012).
01 (2012).
2013). 7796-7700
ni, A. Marce
crystal str
Moscow 14
wide opporputational sn my labora[1,2], enablarbitrary coude major i
molecular crg(BH4)2 [4] [6].
y ionic phasum [8]. that become3O2 and Mg
ems, and imp
achable pres
82 (2013).
(2013).
elli, A. Peral
ructure
43026, Rus
rtunities forscreening foatory, we haling predictionditions, giincrease of rystals [3] ] and H2O-H
se of boron,
e stable undgO2 [10].
mplications f
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drogen-rich -compressiocently, both ssure exhibierconductiv
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which has Tc
POSIUM 201
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Tc with 200 Kogen-rich m
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2Br are supeogen hydridmolecular u
ni, A. Marce
halogen hyd
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ressures duegh Tc superculfur hydrideefforts to re
gen polyhydio calculationd H5Br comclearly seen
pressure. SimGPa. Furthe
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elli, A. Peral
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POSIUM 201
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uan and Tia
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etallization ompounds arent discoverresearch hyhydrogen-ri
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ni, A. Marce
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in solid hydcandidates fr hydrides wds. Howeverally the hyd
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molecule, ins of severalng in situ hi
methods. By ydrogen-bonw perspective
elli, A. Peral
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POSIUM 201
ctronic top
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n characteriETP (USSR)ation effectsnsition”, K.
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ter of primadization in aand shape o
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metal in the h1960) n revealed bt al., Phys. R
nic topologic) onductor-to-pl. Phys. Lelogical, and hys. Lett. 10es/xpress.htm
ni, A. Marce
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version of 2102 (2013)uctor to meta(2016)
ali
29
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“A reinvestosphorus”, Bnostructuresn: 97888668“Pressure-in
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tigation of thB. Joseph ets” edited by830597 nduced elect. 115, 1864
POSIUM 201
he high preal., in “Ato
y A. Biancon
ctronic trans403 (2015)
16 edited by
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diagram of brfaces Interfstripes Press
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elli, A. Peral
black rfaces and s, Rome 20
Xiang et al.
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S. CaprarS. CaprarLesueur, Caprara, N. ScopigGrilli, PhS. CaprarBucheli, 195448 (J. BiscaraM. GrilliS. Caprar425701 (S. HuranRastogi, AGrilli, J. G. Seibol8. M. V.
FANO SYMP
ra, et al., Phra, D. Buchand M. Griand M. Grigno, D. Buc
hys. Rev. Lera, F. PeronM. Grilli, F2014). as, N. Berge, S. Caprarara, N. Berge2015) d, J. BiscaraA. Dogra, PLesueur, ald, S. CapraMazziotti, N
POSIUM 201
hys. Rev. B eli, N. Scopilli, Superc. lli, Superc. cheli, S. Capett. 116, 026naci, and M.F. Peronaci,
eal, S. Huraa, J. Lesueueal, J. Lesue
as, N. BergeP. Kumar, RarXiv:1506.ara, M. GrillN. Scopigno
16 edited by
(Rapid Compigno, N. BeSc. and TeSc. and Tecprara, J. Bis6804 (2016). Grilli, PhyG. Seibold
and, C. Feuiur, Nature Meur, and M.
eal, C. FeuiR. C. Budha06874 li and R. Rao, M. Grilli
y A. Biancon
mmunicatioergeal, J. Bich. 28, 0140ch. 28, 0450scaras, N. B).
ys. Rev. Lettd, and S. Cap
illet-Palma, Materials 12,
Grilli, Phy
illet-Palma, ani, N. Scop
aimondi EP, and S. Cap
ni, A. Marce
ons) 88, 020iscaras, S. H002 (2015);004 (2015).
Bergeal, J. L
t. 109, 1964prara, Phys.
A.Rastogi, , 542 (2013)s.: Condens
G. Singh, Aigno, S. Cap
L, 112 1700prara, prepr
elli, A. Peral
0504(R) (20Hurand, J. ; D. Buchel.
Lesueur, and
401 (2012); . Rev. B 89
R. C. Budh). s. Matter 27
A. Jouan, Aaprara, M.
04 (2015). rint.
ali
33
13);
i, S.
d M.
D. ,
hani,
7
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24. J. L
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sed matter ef cuprate supof charge acsolvent" plaorientationhin a Montee polymer mwith the addal order leavferronematicermodynament of soft-mxperiments uperconducGrilli, S. Ca
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G Seibold, J
ni, A. Marce
ment, Sapien
effects emerperconductocompanied
ayed by anti(and direct
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mic transitionmatter physand reconc
ctors. Work aprara, G. S
es
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J Lorenzana
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nza, Univer
rge on a harors. We shoby a non-
iferromagnetion) as the dy, we find nses first in aversion st inversion anied by ven. Such
sics, produccile the phas
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Capati, C Di
conductors,(2014)
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34
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Tre Via della
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has been stueavy normalto the diffeng may be ain Hall effecch a mechane effect. Aft
part I will aible with thth C. Gorin).
ni, A. Marce
a Vasca Nav
nd Perel, is s effect, whof spintronis based on s
udied extenl metal. In arent microsactive. ct due to thenism yields er a brief re
also report ohe theoreticani and U. E
elli, A. Peral
vale 84, I-
the generathich arises anics spin-charge
nsively in a real systemscopic
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eview of the
on some recal predictionEckern and
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tion as a
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27. and
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smons, the ce a strong inmparison witperties are aich are now tunable and
e graphene, ouple of exaed on Bi2Se
perconductosed light and
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collective onteraction wth that of exat the basis routinely u
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POSIUM 201
plasmonic uctors
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scillations oith the electxciting lightof surface-e
used in manyices, plasmo
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materials:
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of electronstromagnetict and a hugeenhanced Ry bio-sensinonics shoul
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y A. Biancon
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ni, A. Marce
of Topologic
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show notabduced waveeld enhancenfrared specons. Howevon more exoIn this talkn the TerahgB2 High-Terved and m
elli, A. Peral
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no
di Fisica, Salab.it
ted photonicocessing. Inices may opfor novel te
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mechanical pstrate the corthermore wch leads to anumber of p
POSIUM 201
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apienza Uni
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emented a smerference in predictions. omputationawe report a nan exponentphoton sourc
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ave a strongability to maspectives boal applicatio
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ni, A. Marce
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o perform quantum statedamental tes
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m systems osk, scattersf the quantuic down-con
elli, A. Peral
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quantum es of light bsts of quant
nsformationase the numeter naturallyevelopment n large ng problemeter, confirmare a promi
over classicshot boson um device, nversion.
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well as on thogap. I will tor is domin
also presentn the formati
POSIUM 201
antum mate
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erials.
California, Bce Berkeley
copy techniqaths to disell present noprate supercdent dynamd momentumcenario in wmulated em
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Berkeley National L
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n. Howevernsition reman XANES snic changesS may inveral phase tras the existin
mission, optiwill report pynamics of t
POSIUM 201
aration andectron syst
ali di Frasca
ly separatedscribed as acomparable y may exten
ested phase s form compphenomena
hanges, and f phase-sepaffer a wide scan be obseptical transmattice, and che vanadiumystems becage near roomstructural phvity by seveo V− V dimctural twist ansition andchanisms, ha, in spite ofains an openspectroscopys associatedstigate simuansition. ng scenario cal and tranpreliminary the different
16 edited by
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ensitivity to T transition.both the m
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Resonant Phntributions
ni, A. Marce
n VO2, a co
044, Italy
structural, mration that oge coherench domains r
f transition mains play a rrmations, tr strong anom
of phase-seprvable quantmena origindom. tainly one oheating or c
K), to a hystonoclinic tode. xis forming
edrons. An -driven Peieexplain the its the drivin
probe the l. Moreover,etal–insulat
formed on Vt different tehotoemissioof the DOS
elli, A. Peral
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metal oxiderole in the ransport, omalies in th
parated ntities such anate from
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VO2 films usemperatures
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31.
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School of PItaly
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chool of SciUniversit
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show that imimetallic poere is an effeticular the d
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ows openingeffect for eway for the
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ariglia 1,2,3 R
Pharmacy, P
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in AB stackoints are deective recondimension pene sheet an
he Eisenhartd spin 1/2parture of the bands, switchhen curvatu
g or closing electronic dee beginning
POSIUM 201
layer graph
Roberto Gia
Physics Uni
ca, Univers
ca e Astronoadova, Italy
Technology,rino, 62032 ia, 06123 -
ked bilayer gescribed by mnstruction operpendiculand the intera-Duval lift orticles near
bilayer sheehing from a
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hene in an
ambo 4 And
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idade Feder
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graphene lomassless, fof the 4 dimear to the sheactionsexpeof the dynathe Dirac p
et induces a a conductingve. In particgap betwee
us using curvonics in bilay
y A. Biancon
effective 4D
drea Perali 1
t`a di Camer
ral de Ouro
ersit`a degli
ics Divisiono, Italy aly
w energy exour dimensiensional spaeet, that ariserienced by mics experi
points. We fchange in thg regime forcular, curvinen conductiovature as a tyer graphen
ni, A. Marce
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ienced by Gfind thatchanhe energy ler negative cng grapheneon and valentunable parane.
elli, A. Peral
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around the fermions.
cluding in cally from ths. The effectGaliei invaringing the evel of curvature toe bilayers nce bands, ameter open
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ction of dopdies. A strononent �T* s(1.1) for x =nsition tempendence wito zero) at x
E of xc with ping dependmation of therconductiv
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otope (16O/1
* is investigping x by mng x dependsystematical= 0.06, correperature Tc. ith differentxc(
16O) = 0.an exponenent OIE on
he pseudogavity and the
POSIUM 201
attice effecn the pseudo
8O) effect (gated for the
means of x-radent and siglly decreaseesponding t Both T*(16
t slopes and .201(4) and nt of �xc = 0T* signals
ap, consistenvibronic ch
16 edited by
cts as reveaogap temp
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gn reversed es from �T*
to increasing6O) and T*(
d critical endd xc(
18O) = 00.84(22). Tha substantiant with a poharacter of i
y A. Biancon
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* = - 0.6(1.3g T* and de(18O) exhibid points (wh0.182(3), indhe remarkabal involvemolaronic appits ground st
ni, A. Marce
uge unconvLa2-xSrxCu
p (charge-stor La2-xSrxCe structure (is observed) for x = 0.1
ecreasing suit a linear dohere T*(16Odicating a lably large an
ment of the laproach to cutate.
elli, A. Peral
ventional uO4
tripe orderinCuO4 as a (XANES)
d. The OIE 15 to �T* =
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O) and T*(18
arge positivnd strongly attice in the
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Ref
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Complexityb)micron be
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titute of Cry
tstanding strir dynamic hrelated mateperties. Theribution and
play a centrachrotron radnanoscale p
mplex scenarmesoscale. Wmplex and hem material s
ferences
M. Fratini, NBianconi, Nhttp://dx.doiG. Campi, DMagnetism G. Campi, AInnocenti, J.(2015) doi:1G. Campi, MTromba, M.http://dx.doiN. Poccia, GBianconi, Sc
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y in heterogeam techniq
pi
ystallograph
ructure-funcheterogeneoerials constie competitiod electronical role for mdiation featuphase separrio where H
We also shoeterogeneouscience to b
N. Poccia, ANature, 466,
i.org/10.107D. Innocenti28, 1355 (2
A. Bianconi. Karpinski,10.1038/natuM. Fratini, I Mastrogiaci.org/10.101
G. Campi, Acientific rep
POSIUM 201
geneous funques
hy, CNR, via
ction relatioous structureitute an impon between c textures gimaterial funcures and froration with fHTS emergeow the possius structureiomedicine
A. Ricci, G.841-844 (2
73/pnas.120i, and A. Bi
2015) http://, N. Poccia,, N. D. Zhigure14987
I. Bukreeva,como, A. C16/j.actbio.2
A. Ricci, A. ports, 4, 543
16 edited by
nctional ma
a Salaria K
onship of nee and comp
portant classcompeting
ives mesoscctionality [3om optical ffine details es in networibility to extes at nano/m [4, 5].
Campi, M.2010) 08492109. ianconi, Jou/dx.doi.org/, G. Biancongadlo, S. M
, G. Ciasca,edola Acta 2015.05.033S. Caporale
30 (2014) do
y A. Biancon
aterials as s
Km 29.300, 0
ew functionposition [1, 2s of materiaorders due t
cale phase se3]. Taking afocusing devin real spac
rks competitend our me
mesoscopic s
. Burghamm
urnal of Sup/10.1007/s10ni, L. Barba. Kazakov,
, M. BurghaBiomateria3 e, E. Di Coloi:10.1038/
ni, A. Marce
een by sync
00015 Roma
al materials2]. Strongly
als showing to defects speparation th
advances frovices, we cace. The resung with elecethodology scale in diff
mer, G. Aep
perconductiv0948-015-2a, G. Arrighet al., Natur
ammer, F. Blia, 23, 309
la, T. A Haw/srep05430
elli, A. Peral
chrotron x-
a, Italy
s are often dy electrons intriguing patial
hat is believom X ray an visualizeults suggest ctronic textto visualize
ferent fields
ppli & A.
vity and No2955-3 hetti, D. re 525, 359
Brun, G. 9 (2015)
wkins, A.
ali
42
-ray
due
ved
e a
tures e s
ovel
34. A.CMar
aIsti001bDepKing
We MicdiagElecoesoresoThetopowavand impproddevcancand com
Ref
[1]
[2]
[3] SiggKyrHirsNatu
UGO F
Early canc
Cricentia* , Mrtinb, P. We
ituto di Stru33 Rome, It
epartment ofgdom
present a fucroscopy (SNgnostics. Thctron Laser ophageal adolution and e optical fibrographical avelengths (p
Scanning Nportant tool duce a majoelopment ocer. It is alschemical s
mponents, re
ferences:
Cricent3 (2011
Smith AMartin ThompsWeight
Halliwellgel-King Mrgiou Mariasch Pierre Lure Scientif
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cer diagnos
M. Lucea, Meightmanb
uttura della taly f Physics, U
ully implemNOM) in sp
he SNOM hat the ALIC
denocarcinohas been abre has been and optical protein/glycNear-field Ofor tissue im
or advance if portable d
so planned tpecificity o
esponsible f
ti A, Luce M1) 913;
AD, Siggel-DS, Surmanson NR, Satman P; App
l Diane E, MMichele RF, a, Mitra AniL, Cricenti Afic Reports;
POSIUM 201
stics by IR-
M. Ortenzia,
Materia (IS
University of
mented Infrapectroscopic
has been couCE facility ioma have shble to disting
driven in pimages havoprotein, D
Optical Micrmaging and in imaging o
diagnostic dto utilise theof the mentiofor cancer fo
M, Tolk NH
-King MRF,n M, Craig veliev Y, Prplied Physic
Morais CamCraig Tim, ta, Paraskev
Antonio, Lu 6 (2016) 29
16 edited by
-SNOM spe
M.R.F. Sigg
SM-CNR), v
f Liverpool,
ared (IR) Scc mode for
upled with ain Daresbur
hown that thguish betwe
particular arve been colleDNA). This c
roscopy, in early cance
of malignandevices for he powerful coned methoormation.
H, Margarito
, Holder GMT, Barrett Sritchard DMcs Letters; 1
milo LM, LimIngham Jam
vaidis Evanuce Marco, W9494.
y A. Biancon
ectroscopy
gel-Kingb, T
via del Foss
, Liverpool
canning Neatissue imag
an infrared lry [1]. Resuhe system caeen healthy eas of the oected simulcombinationits spectros
er diagnostint tissues [3hospital use combinationodologies to
ondo G; Nan
M, Cricenti SD, Wolski M, Varro A,102 (2013) 0
ma Kássio Mmes, Martinngelos, TheoWeightman
ni, A. Marce
T. Craigb, J.
so del Caval
L69 7ZE, U
ar-field Optiging and earlight source
ults of IR-SNan operate aand malignesophageal taneously an of InfraRescopic modecs. It is exp], leading tofor various
n of high sp study the k
nosci. Nanot
A, Luce M,A, Dunning Chattopadh053701.
MG, Trevisn David S, Hophilou Geon Peter, Mar
elli, A. Peral
J. Inghamb, D
liere 100,
United
ical rly cancer e, based on FNOM on at nanometenant tissues l tissue and at different ed radiatione, can be an
pected to o the s types of patial resolukey
otechnol. Le
, Harrison Pg DJ, hyay S,
san Julio, Heys Kelly Aorgios, Martrtin Francis
ali
43
D.
Free
er [2].
n n
ution
ett.;
P,
A, tin-L;
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16 edited by
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44
35Bi
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1BAc2IN3RSaEm
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Thein eE1 cdichaniscontX-rastrustruthe strudichstrucouis fo
1) loc
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Wei Xu1,3*, F
Beijing Synccademy of SNFN - Labo
RICMASS, Rabelli 119A,mail: * mar
ey words:
e circular diclectic dipolchannle (pahroism (whesotropic laytroversy ovay or neutro
ucture more uctures that icrystallogra
uctural in dehoism absoructures. It is ld not descround that:
the X-ray dcal coordina
the XMCDspect to CuOoms (sitting
the XMCDspect to CuO
xygen atoms
with rhombwards loweagonal of sq
with rhombe absolute vcreases from
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agnetic Dicrconductor
ederico gald
hrotron RadSciences, Beoratori NaziRome Intern 00185 Rom
XMCD, Cu
chroism in e-quadrupo
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ribe the true
dischroism sates than XA
D signal canO4 square p
g in the diag
D signal is qO4 square ps are movin
bic distortior energy as quare) incre
bic distortiovalue of z fom 0.2 angstr
POSIUM 201
chroism spers
denzi2, Aug
diation Faceijing, 10004ionali di Fraational Cen
me, Italy. nfn.it, anton
u K-edge, L
absorption cole (E1-E2) XMCD). TheXNCD or XM
commesura. There werons attempti[2-10] Thecrucial for sure. Hence in, we perfo
u K-edge andthe crystall
e structures
signal is moANES or its
be evident plane) of thegonal of squ
quite weak ~plane) of theng either up
ons, the peakthe absolut
eases from 0
ons, the XMor two oxygrom to 0.6 a
16 edited by
ectroscopy
gusto Marce
cility, Institu49, China. ascati, Via Enter for Mat
nio.biancon
L-edge, Bi22
can be induchannel (XNere is a debMCD) in Biate structurere lots of crying to descr
e emergencesuperconduit is still of
ormed theord L-edge uslographic strof Bi2212.
ore senstives first deriv
above 10-4
e oxygen couare) are mo
~10-6 or 10-7
e oxygen coor down sim
k position ote value of z0.2 angstrom
MCD signal gen atom (siangstrom.
y A. Biancon
at Cu K-ed
elli2,3* and A
ute of High E
E. Fermi 40terials Scien
ni@ricmass.
212
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e to the symvative spectr
for the rhoboordination, oving out of
7 for the recoordination, mulatenousl
of maximumz for two oxm to 0.6 ang
of the maxiitting in the
ni, A. Marce
dge and L-e
Antonio Bia
Energy Phy
0, Frascati, nce Superst
eu
er the nonmy magnetic sthe nature o
ch possesseshad been un
hyic investigmmesurate density wavl related to
ests to invesulations of thnt crystallogreported in heoretical ca
metry breakrum.
bic distortioi.e. when tw
f plane. Figu
tangular disi.e. when tw
ly.
m peak XMCxygen atom gstrom.
imum peak diagonal of
elli, A. Peral
edge of
anconi3*,
ysics, Chine
00044, Italtripes, Via d
magnetic effsignal in E1of the circuls strongly
under gations usinmodulated
ve and stripcomplexity
stigate the the X-ray graphic literatures alculations,
king of the
on (with wo oxygen ure.1(a)
sortion (witwo adjacent
CD shifts (sitting in t
increases asf square)
ali
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Hemasyori
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[1]cu[2]Refro[3]Strdif[4]incSe[5]AsBi[6]moato[7]dif19[8]Inc19[9]J.L
UGO F
ence it is imaximum pea
ymmtry, parigin of the s
(
gure.1 The xygen atomsoms moving
eferences
] S. Di Mattuprates, Phy] P.A. Mileefinement oom a neutro] A. Biancoripe structuffraction, Ph] X.B. Kan,commensurect. B: Struc] A. Yamamsano, Rietvei2(Sr,Ca)3C] V. Petriceodulation inoms, Phys. ] A.I. Beskrffraction stu
990; 166: 79] Y. Gao, Pcommensur
988; 241: 95] P. Bordet,L. Hodeau,
FANO SYMP
mportant to vak in XMCDity breakingsupercondu
a) rhombic
distortions s moving reg either up o
teo, M.R. Nys. Rev. B 2s, S.J. Kenn
of the incomon diffractiooni, M. Lusiure of the Cuhys. Rev. B, S.C. Mossrate modulact. Sci 1992moto, M. Oneld analysis
Cu2O8+x, Pek, Y. Gao, Pn the 2:2:1:2Rev. B 199rovnyi, M. Dudy of the m9-86. . Lee, P. Corate Modula54. , J.J. CappoM. Marezio
POSIUM 201
verify the inD signal in g very well,ctivity of th
distortion
of the localespectively uor down.
Norman, X-r007; 76: 01nedy, G.J. M
mmensurate on study, Phignoli, N.L. uO2 plane in
B 1996; 54: 4, Four-dime
ation in a Bi; 48: 122-13noda, E. Taks of the modhys. Rev. BP. Lee, P. C2 Bi-Sr-Ca-0; 42: 387-3Dlouhá, Z. J
modulated st
oppens, M.Aation of the
ni, C. Chailo, J.L. Thole
16 edited by
ntensity as wBi2212 so a
, which is bhis sytem.
l oxygen coup and dow
ray dichrois4510.
McIntyre, Gstructure of
hysica C 199 Saini, P. Bn Bi2 Sr2C4310-4314.ensional cryi2Sr2CaCu234.
akayama-Mudulated strucB 1990; 42: Coppens, X--Cu-O super392. Jirák, S. Vrtructure of B
A. Subrama2212 Bi-Sr
llout, J. Cheence, D. Tra
y A. Biancon
well as the pas to underselieved to b
(b)
ordinates (awn ; and (b)
sm and the p
G.D. Gu, G.Jf high qualit98; 294: 275
Bordet, Å. KaCu2O8+y
ystallograph2O8 single c
uromachi, Fcture in the 4228-4239.-ray analysirconductor i
ratislav, E. PBi2(Sr, Ca)
ania, A.W. Sr-Ca-Cu-O S
enavas, A.Wanqui, Powd
ni, A. Marce
peak positiostand the locbe correlated
rectangular
a) with two with two ad
pseudogap p
J. Russell, Nty Bi-2212 5-288.
Kvick, P.G. Rby anomalo
hic analysis crystal, Acta
F. Izumi, T. supercondu
. is of the incoincluding th
Pollert, Neu)3Cu2O8+y
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W. Hewat, Eder X-ray an
elli, A. Peral
on of the cal structurd with the
r distoriton
diagnonal djacent oxyg
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of the ta Crystallog
Ishigaki, Hucting oxide
ommensurahe oxygen
utron y, Physica C
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E.A. Hewat,and neutron
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46
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FANO SYMP
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tani, C. RizBi2Sr3− xCan data, Phys
POSIUM 201
uperconduc
zzoli, M.t. FaxCu2O8: Asica C 1989
16 edited by
ctor Bi2Sr2C
Francesconi,A commens9; 161: 598-
y A. Biancon
CaCu2O8, P
, G. Andreeurate mode
-606.
ni, A. Marce
Physica C 1
tti, The modl from singl
elli, A. Peral
1988; 153:
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47
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d theoreticauperuidity inw system haong pairing nem consistiner[2]. We usnd systems wion as functe energy banharacterize tas function oablish doubliagram of sts.
, D.Neilson uble few-layand A.R.Hamne, Phys.Rev
16 edited by
iband doub
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al e_orts havn a bilayer gas been theonecessary fong of two pase the meanwith intra-btion of the cnd gap as pthe crossovof the carriele bilayer grtrongly inte
and F. M. Pyer grapheneamilton, Higv.Letters 11
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system with rmalism we]. We foundn-like transfinterband paenerate caser with a phaCooper pairdiscuss the
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84 (1993). M. V. Milos
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31013. ] Xu, S. Y., hang, C. (20senide. Natu] Souma, S.
egawa, K. (2pposite surfa
93(16), 16] S.-Y. Xu e
aP, arXiv:15] Xu, B., Da. A (2016). 9
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sano1, Friedhto di Fisica,I-00133 Ro
Festkörpert 07743 Jena
te electronicaAs, TaP, Nergies by mion and withcussed. Theonduction ato electron
Weyl nodes, tand the smaeir occupatiohey give risection and, hThe high-ene. The energuencies, at wdetails of thP, we direct
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Alidoust, N015). Discovure Physics., Wang, Z.,2016). Direcaces in the n1112. et al., Exper508.03102.pai, Y. M., ZOptical spe
POSIUM 201
cal propertAb initio stu
helm Bechs Università
ome, Italy theorie und a, Germany
c, optical anNbAs and Nb
eans of the hin the indee four band and As4p/P3
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ties of Weyludies of TaA
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., Sato, T., Nion of noneqymmetric W
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X. P., Miao, Hmetal TaAs. P
n, Z., Bian, Gn state with
Nakayama, quivalent Fe
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Yang, R., Zsemimetal
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H., Ma, J., .Physical Re
G., Chang, TFermi arcs
K., Tanaka,ermi-arc staetal NbP. Ph
al Weyl sem
Zhang, W., .TaAs, Phys
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n transitionbP
Ricerca
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covered Wery for small y with spin-Chemical y separated rgetical F at the 8 Wrticular for tnodes. The d optical part of the optical nsitions in ttion define nounced pe
PES results fr TaAs[5].
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