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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,

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nanoparticlduced by themilar theorieattering [4]

Barbiellini,

Nicolini, Phy

emperature P

ancock, C. Mev. B 89, 23

, and Kenji

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les [3]. Thee resonant ees have bee and the beh

, A. Bansil,

ys. Rev. A 8

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and H. Mo

84, 022509

zika Nizkikh

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Phys. Rev.

ni, A. Marce

he enhancef surface plaully used to onlinear sus

sallaei, Phy

(2011).

h Temperatu

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B 92, 1551

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POSIUM 201

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ese holograpiety, at the sese are quanmputable witmonstrate thsible. I will

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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

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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

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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

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conductors ama of conden

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nciples of boproperties alkably their ensely entangd in a highly

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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

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Igor

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Hyperbolic

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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

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magnetic fferent “lawons of MONial “multiveg mechanism

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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

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supercond

Mainz, Germ

the high temuperconducotope effecton studies o

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ductivity

many

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of pure hydr

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ni, A. Marce

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tallic hydroerconductortallic state interials are ex

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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

Materials, C-mail addres

re is believeno experimep to 388 GPnce their mepre-compre elements, m

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by two mainlts have beeeissner effecalso explorerich materia

X. Huang, Zuan, X. Huan, 180502 (20

A. Troyan, V

wa, K. Shimiure Phys., 12

Bertil., L. X).

y A. Biancon

sure: towar

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ed to be a roental evidenPa. As an altetallization cessions. Mormost novel pperconductivmber of sup

m symmetry K at high pr

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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

ni, A. Marce

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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

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n University,

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W. Tian, TYu, Y. Liu,

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POSIUM 201

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POSIUM 201

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es both phas6] in a comy emerges wte regime wat this sceessurized su

14, 3289 (2. Sci. 109, 1

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se separatiomplex geomwhere shapwhere localenario provulfur hydrid

000),

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8 024005 (2

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urnal of Sup/10.1007/s10anconi, L. B. Kazakov,

ni, A. Marce

n [7,8,9,10,metry [2]. Wpe resonanclization andvide the e

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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

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h-pressure p

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ds of crystalerials at extroptimal pro

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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

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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

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a discovere

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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

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m. Phys. 15,

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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

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82 (2013).

(2013).

elli, A. Peral

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POSIUM 201

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POSIUM 201

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POSIUM 201

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POSIUM 201

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POSIUM 201

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POSIUM 201

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POSIUM 201

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cts as reveaogap temp

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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

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A. Bianconi. Karpinski,10.1038/natuM. Fratini, I Mastrogiaci.org/10.101

G. Campi, Acientific rep

POSIUM 201

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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.

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Early canc

Cricentia* , Mrtinb, P. We

ituto di Stru33 Rome, It

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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

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M.R.F. Sigg

SM-CNR), v

f Liverpool,

ared (IR) Scc mode for

upled with ain Daresbur

hown that thguish betwe

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roscopy, in early cance

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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

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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

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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

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liere 100,

United

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, Harrison Pg DJ, hyay S,

san Julio, Heys Kelly Aorgios, Martrtin Francis

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hrotron RadSciences, Beoratori NaziRome Intern 00185 Rom

rcelli@lnf.in

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POSIUM 201

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diation Faceijing, 10004ionali di Fraational Cen

me, Italy. nfn.it, anton

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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

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mportant to vak in XMCDity breakingsupercondu

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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

Sleight, TheSupercondu

W. Hewat, Eder X-ray an

elli, A. Peral

on of the cal structurd with the

r distoriton

diagnonal djacent oxyg

phase of

N. Koshizuksingle cryst

Radaelli, ous x-ray

of the ta Crystallog

Ishigaki, Hucting oxide

ommensurahe oxygen

utron y, Physica C

e uctor, Scienc

E.A. Hewat,and neutron

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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:

dulated le crystal X

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36 Sa1 Usar SegemaacBEbytemtheena_theexto the [1]ho[2]Do

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nergy. We in_ects the paie condensat

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] M. Zareniole superflui] A.Perali, Double-Bilay

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S crossover

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rimental andtron-hole sucently a newgime of stroer in a systeulating layefor multibans gap equatintroduce theiring. We chte fraction aresults estaich phase divestigations

ia, A.Perali,idity in douD.Neilson a

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POSIUM 201

r in a multi

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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

ndrea Peraliamerino (M

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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i1 C), Italy

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graphene

ne to search nd in relatedemonstratede investigateyers graphenoximation atg. We presentential and t

nd we invesnew parameOur fundin

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and to d nano-thin d to be able e the BCS-ne separatedt zero nt results fothe Fermi

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POSIUM 201

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er, S. Pons, r, and D. Ro

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Italy

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of the Fermiconfinemention of the dding to multting energyuantum-size

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or different m

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system with rmalism we]. We foundn-like transfinterband paenerate caser with a phaCooper pairdiscuss the

ov. Phys. - JE. Vagov, M. 015). omponent S

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two identice obtain expd that there ifer of Coopeairing and thes we found ase shift betwrs in the intrexperiment

ETP 104, 308D. Croitoru,

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ni, A. Marce

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cal bands. Uressions foris not coexier pairs for the crosspairtwo coexis

ween the twraband and tal signature

84 (1993). M. V. Milos

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onductivity. and structureasmon frequ

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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

Weng, H. Mrimental dis

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POSIUM 201

cal propertAb initio stu

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c, optical anNbAs and Nb

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rimental dispdf Zhao, L. X., ectroscopy o

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ties of Weyludies of TaA

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B., Wang, XWeyl semim

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., Sato, T., Nion of noneqymmetric W

scovery of a

Wang, K., of the Weyl

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X. P., Miao, Hmetal TaAs. P

n, Z., Bian, Gn state with

Nakayama, quivalent Fe

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a topologica

Yang, R., Zsemimetal

ni, A. Marce

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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

elli, A. Peral

n transitionbP

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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

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... & Fang, Zeview X, 5(3

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